1. Introduction
Let A be an
$E_1$
-algebra spectrum, and let
$a \in \pi_{mk}(A)$
with
$m\gt 0$
and even
$k\geq0$
. In this paper we define, under Hypothesis 4.1, an
$E_1$
-algebra extension
$A\to A(\!\sqrt[m]{a})$
realizing the adjunction of an mth root of a in homotopy rings,
and then study how the algebraic K-theory of
$A(\!\sqrt[m]{a})$
, or its topological Hochschild and cyclic homology, relates to that of A. Hypothesis 4.1 holds, for example, if A is an
$E_2$
-ring for which
$\pi_* A$
is concentrated in even degrees.
In general, the existence of a suitable root adjunction to a ring spectrum and its effect on such invariants is an intriguing question. As shown in [Reference Schwänzl, Vogt and WaldhausenSVW99, Proposition 2], there is no Gaussian sphere
$\mathbb{S}[i]$
; see [Reference LawsonLaw20] for a discussion of root adjunctions in degree 0.
For classes in positive degrees, examples exist and have been shown to be relevant, in particular in studying redshift for algebraic K-theory. We have the Adams splitting of connective complex K-theory ku completed at an odd prime p,
and the extension
$\ell_p\to ku_p$
can be interpreted, on homotopy rings, as the root adjunction
were
$v_1\mapsto u^{p-1}$
, giving
Sagave [Reference SagaveSag14, 4.15] showed that
$ku_p$
can be constructed as an extension of
$\ell_p$
, establishing how
$\ell_p\to ku_p$
qualifies as a tamely ramified extension in
$E_\infty$
-rings. In [Reference Ausoni and RognesAR02, Reference AusoniAus10], Rognes and the first author computed the algebraic K-theory of
$\ell_p$
and
$ku_p$
with coefficients in a Smith–Toda complex
$V(1)=\mathbb{S}/(p,v_1)$
, for
$p\geq5$
. Taking
$T(2)=V(1)[v_2^{-1}]$
, we have the formula
relating the two computations, hinting at a chromatic shift (or redshift) of this tamely ramified root adjunction.
After our construction of root adjunctions in
$E_1$
-rings, we offer an investigation of how the resulting extension is reflected in algebraic K-theory. In particular, we have the following spectrum-level splitting of algebraic K-theory in the tamely ramified case, which applies to a wide array of examples.
Theorem 1.1 (Theorem 5.5). Assume Hypothesis 4.1 with
$p\nmid m$
and
$\lvert a \rvert \gt 0$
. Furthermore, assume that A is p-local and connective. In this situation, the map in algebraic K-theory
induced by the extension
$A\to A(\!\sqrt[m]{a})$
is the inclusion of a wedge summand.
This is deduced from the corresponding result for topological cyclic homology, see Theorem 5.4. An analogous splitting result for algebraic K-theory in the non-connective case is provided in Corollary 5.6.
For an integer
$n\gt 0$
, we say that a spectrum E is height n if
$L_{T(n)}E \not \simeq 0$
and
$L_{T(m)}E \simeq 0 $
for
$m\gt n$
, where T(n) denotes a height-n telescope. We say an
$E_1$
-ring A of height n exhibits redshift if K(A) is of height
$n+1$
. Owing to [Reference Land, Mathew, Meier and TammeLMM+24, Purity Theorem], K(A) is of height at most
$n+1$
, so A will exhibit redshift if
$L_{T(n+1)} K(A)\not\simeq0$
. The following result is thus an immediate consequence of our splitting results, Theorem 5.5 and Corollary 5.6.
Corollary 1.2.
Assume Hypothesis 4.1 with
$p\nmid m$
and
$\lvert a \rvert \gt 0$
. If A exhibits redshift, then so does
$A(\!\sqrt[m]{a})$
.
A key feature of the defined root adjunction is that
$A(\!\sqrt[m]{a})$
is endowed with the structure of an
$E_1$
-algebra in the symmetric monoidal category
$\operatorname{Fun}(\mathbb{Z}/m,\operatorname{Sp})$
of m-graded spectra, which is reflected in an Adams-type splitting of spectra
Such a grading on a spectrum, compatible with further additional algebraic structures, has already proven to be very useful: let us mention the computations of Hesselholt and Madsen [Reference Hesselholt and MadsenHM97] of the K-theory of truncated polynomial algebras, and of the second and third authors [Reference Bayndr and MoulinosBM22] of the K-theory of the free
$E_1$
-algebras in degree 2 over finite fields. In the present paper, the grading corresponding to the root adjunction, and the induced splitting of the topological Hochschild homology (THH) as developed in [Reference Antieau, Mathew, Morrow and NikolausAMM+22, Appendix A], are essential ingredients in the proofs of our various splitting results.
We use the theory of logarithmic THH for an in-depth study of the THH of
$A(\!\sqrt[m]{a})$
. Hesselholt and Madsen [Reference Hesselholt and MadsenHM03] introduced log THH for studying the algebraic K-theory of complete discrete valuation rings in mixed characteristic, and proved a descent property of log THH in the case of tamely ramified extensions. Rognes [Reference RognesRog09] then initiated a study of logarithmic structures, logarithmic André–Quillen homology, and log THH in the context of
$E_\infty$
-ring spectra. With Sagave and Schlichtkrull [Reference Rognes, Sagave and SchlichtkrullRSS15, Reference Rognes, Sagave and SchlichtkrullRSS18], they then established the existence of localization sequences for log THH and proved that it satisfies tamely ramified descent in the example of the extension
$\ell_p\to ku_p$
.
Here, we offer an alternative definition of log THH that applies to a more general class of ring spectra. More precisely, we define log THH for a given
$E_1$
-ring spectrum A and a class
$a\in\pi_{mk}(A)$
satisfying Hypothesis 4.1, associated to the pre-log structure given by the monoid generated, under multiplication, by
$a\in \pi_*(A)$
(see Definition 6.5); it is denoted
$\operatorname{THH}(A \mid a)$
. For instance, this applies to the Morava K-theory spectrum k(n) for
$v_n \in \pi_* k(n)$
. We prove the following form of tamely ramified descent (see also Theorem 6.14).
Theorem 1.3 (Theorem 6.21). If A is p-local and
$p\nmid m$
, then there is an equivalence of spectra
\[\operatorname{THH}(A(\!\sqrt[m]{a})) \simeq \operatorname{THH}(A) \vee \bigg(\bigvee_{0\lt i\lt m}\Sigma^{ik}\operatorname{THH}(A \mid a) \bigg).\]
We also prove the existence of a localization cofiber sequence
see Theorem 6.19. This is an analogue in the present setting of the localization sequences constructed in [Reference Rognes, Sagave and SchlichtkrullRSS15], but note that our definition only applies to the case of a pre-log structure given by a monoid on a single generator. We would like to point out also the recent preprint of Binda et al. [Reference Binda, Lundemo, Park and ØstværBLP+23], where a version of logarithmic Hochschild homology for simplicial commutative rings is constructed.
We now mention examples of application of the above results.
1.1 Topological K-theory
We prove in Theorems 4.6 and 7.5 that, at an odd prime p, there are equivalences of
$E_1$
-ring spectra
These equivalences upgrade the splitting result of Adams into a
$\mathbb{Z}/(p-1)$
-graded, respectively
$\mathbb{Z}/({p-1}/{2})$
-graded,
$E_1$
-ring structure. We prove that when
$p=1$
in
$\mathbb{Z}/m$
, the splitting in Theorem 1.1 can be improved to a more refined splitting of
$K(A(\!\sqrt[m]{a}))$
. In the case of
$ku_p\simeq \ell_p (\!\sqrt[p-1]{v_1})$
, this more refined splitting reads as
Here,
$K(ku_p)_0 \simeq K(\ell_p)$
and, for
$p\gt 3$
, we can compute the V(1)-homotopy groups of each of the ith-graded pieces
$V(1)_*K(ku_p)_i$
using the first author’s computation of
$V(1)_* K(ku_p)$
.
Using this refined splitting, the second author makes a simplified computation of
$T(2)_*K(ku)$
in [Reference BayndrBay24]. We also obtain complete descriptions of
$V(1)_*K(ko_p)$
and
$T(2)_* K(ko_p)$
; see Theorem 7.7.
We note that the splitting (1.1) can be considered as a version of Adams-type splitting for the cohomology theory represented by K(ku), with classes corresponding to 2-categorical complex vector bundles, as developed in [Reference Baas, Dundas, Richter and RognesBDR+11].
1.2 Johnson–Wilson spectra and Morava E-theory
Let
$n\geq 1$
be an integer, and let E(n) and
$E_n$
be the Johnson–Wilson and Morava E-theory spectra. Let
$\widehat{E(n)}$
be the K(n)-localization of E(n). These spectra have coefficient rings given as
and
$\pi_* \widehat{E(n)} \cong \pi_* E(n)^{\wedge}_{I_n}$
, where
$\lvert u_i\rvert = 0$
,
$\lvert u\rvert = -2$
and
$I_n=(p,v_1,\ldots,v_n)$
. The Galois group
${Gal}=\operatorname{Gal}(\mathbb{F}_{p^n} | \mathbb{F}_p)$
acts on
$E_n$
, and let
$E_n^{\operatorname{hGal}}$
be the homotopy fixed-point spectrum with coefficients
$\pi_* E_n^{\operatorname{hGal}} \cong \mathbb{Z}_p[\lvert u_1,\ldots,u_{n-1}\rvert][u^{\pm 1}]$
.
We prove in Theorem 9.3 that there are equivalences of
$E_1$
-rings
\begin{equation}\begin{aligned}E_n& \simeq \mathbb{S}_{W(\mathbb{F}_{p^n})} \wedge_{\mathbb{S}_p} \widehat{E(n)}(\!\sqrt[p^n-1]{v_n})\\E_n^{\operatorname{hGal}}&\simeq \widehat{E(n)}(\!\sqrt[p^n-1]{v_n}).\end{aligned}\end{equation}
This promotes the
$E_1$
-ring structure on Morava E-theories to a non-trivial
$\mathbb{Z}/(p^n-1)$
-graded
$E_1$
-ring structure.
Using this description of
$E_n$
and the log-THH-étaleness of root adjunction, we show in Theorem 9.9 that the canonical map
is an equivalence after p-completion. The relationship between such equivalences and the Galois descent question for THH is studied in [Reference MathewMat17].
Applying Corollary 5.6 to these root adjunctions of non-connective spectra, we deduce the following result.
Theorem 1.4 (Theorem 9.4). The canonical maps
\begin{align*}K(E(n)) \to& K(E_n^{\operatorname{hGal}}),\\K(\mathbb{S}_{W(\mathbb{F}_{p^n})} \wedge E(n)) \to & K(E_n)\end{align*}
are inclusions of wedge summands after
$T(n+1)$
-localization.
1.3 Lubin–Tate spectra
We can also apply our results to Lubin–Tate spectra that can be constructed, in several steps, from the truncated Brown–Peterson spectra
$BP \langle n \rangle$
, with coefficients
$\pi_*BP \langle n \rangle\cong\mathbb{Z}_{(p)}[v_1,\ldots,v_n]$
. In more precise terms, we consider an
$E_3$
$MU[\sigma_{2(p^n-1)}]$
-algebra form of
$BP \langle n \rangle$
as constructed by Hahn and Wilson [Reference Hahn and WilsonHW22, Remark 2.1.2]. In this situation, we can construct
$BP \langle n \rangle(\!\sqrt[p^n-1]{v_n})$
as an
$E_3$
$MU[\sigma_2]$
-algebra (Remark 4.7).
Let k be a perfect field of characteristic p, and let
$\mathbb{S}_{W(k)}$
denote the spherical Witt vectors spectrum. We prove in Proposition 8.3 that the
$MU[\sigma_2]$
-orientation above provides a formal group law
$\Gamma$
of height n over k, and that there is an equivalence of
$E_3$
-rings
where
$E_{(k,\Gamma)}$
denotes the Lubin–Tate spectrum corresponding to
$\Gamma$
. Owing to [Reference Land, Mathew, Meier and TammeLMM+24, Purity Theorem], we have an equivalence
By [Reference Hahn and WilsonHW22],
$BP \langle n \rangle$
satisfies the redshift conjecture; following an argument suggested to us by Hahn, we show that
$\mathbb{S}_{W(k)} \wedge BP \langle n \rangle$
also satisfies the redshift conjecture, cf. Proposition 8.1. By Corollary 1.2, we deduce that
$E_{(k,\Gamma)}$
satisfies the redshift conjecture. Indeed, we deduce from this (see Theorem 8.6) a new proof of Yuan’s result [Reference YuanYua21] that all Lubin–Tate spectra satisfy the redshift conjecture. We also obtain the following from Corollary 5.6.
Theorem 1.5 (Theorem 8.5). The induced map
is the inclusion of a non-trivial wedge summand.
We expect the above result to be relevant also for explicit computations. For example, in [Reference Angelini-Knoll, Ausoni, Culver, Höning and RognesAAC+25], the authors compute
$V(2)_*\operatorname{TC}(BP\langle2\rangle)$
for
$p\geq 7$
, which provides an explicit description of
$T(3)_*K(BP\langle 2 \rangle)$
. Through the inclusion above, we deduce that
$T(3)_*K(BP\langle 2 \rangle)$
maps isomorphically to a summand of
$T(3)_*K(E_{(\mathbb{F}_p,\Gamma)})$
for a height-2 formal group law
$\Gamma$
over
$\mathbb{F}_p$
. To our knowledge, this is the first explicit, quantitative result on the algebraic K-theory groups of Lubin–Tate spectra for height larger than 1.
Note that it is not known if the
$E_3$
MU-algebra forms of
$BP \langle n \rangle$
constructed in [Reference Hahn and WilsonHW22] map into the Morava E-theories mentioned in the preceding subsection.
Remark 1.6. In [Reference Burklund, Schlank and YuanBSY22, Theorem G], the authors construct an
$E_\infty$
-map
$MU[\sigma_2] \to E_{(\overline{\mathbb{F}}_p,\Gamma')}$
for the unique height-n formal group law
$\Gamma'$
on
$\overline{\mathbb{F}}_p$
, solving an open question on the existence of orientations on Lubin–Tate spectra. Our constructions provide a similar orientation for a ‘smaller’ form of Lubin–Tate spectra. Namely, we obtain that
$E_{(\mathbb{F}_p,\Gamma)}$
is an
$E_3$
$MU[\sigma_2]$
-algebra where
$\sigma_2$
acts through
$u^{-1} \in \pi_* E_{(\mathbb{F}_p,\Gamma)}$
; see Example 8.4. Moreover, there is a grading on
$E_{(\mathbb{F}_p,\Gamma)}$
that respects this structure. To be precise,
$E_{(\mathbb{F}_p,\Gamma)}$
is an
$E_3$
$MU[\sigma_2]$
-algebra in the
$\infty$
-category of
$\mathbb{Z}/(p^n-1)$
-graded spectra, where
$u^{-1} \in \pi_* E_{(\mathbb{F}_p,\Gamma)}$
is of weight 1.
Remark 1.7. The above construction of Lubin–Tate spectra by root adjunction is used in an essential way in the construction of a counter-example to the telescope conjecture in forthcoming work by Burklund, Hahn, Levy and Schlank.
1.4 Morava K-theory
In § 9.3, we construct two-periodic Morava K-theories from Morava K-theories through root adjunction. By Corollary 1.2, we deduce that two-periodic Morava K-theories satisfy the redshift conjecture if the redshift conjecture holds for Morava K-theories (Corollary 9.6).
For
$p\gt 3$
, the V(1)-homotopy of K(k(1)) is computed by the first author and Rognes in [Reference Ausoni and RognesAR12], where it is also shown that k(1) satisfies the redshift conjecture. From this, we deduce that the two-periodic first Morava K-theory
$ku/p$
also satisfies the redshift conjecture (Corollary 9.7). Moreover, through the interpretation of
$ku/p$
as
$k(1)(\!\sqrt[p-1]{v_1})$
, the second author makes the first computation of
$T(2)_*K(ku/p)$
in [Reference BayndrBay24].
1.5 Outline
We begin with a quick introduction of graded objects in § 2. In § 3, we construct a family of graded
$E_2$
‘polynomial’ algebras and establish their even cell decompositions. In § 4, we provide our central construction for root adjunctions (Construction 4.3) and prove our first splitting result on the THH of ring spectra obtained via a root adjunction. In § 5, we prove Theorem 1.4. Section 6 is devoted to studying the variant of log THH we set forth, as well as the log-THH-étaleness of root adjunctions. Section 7 contains our results on the algebraic K-theory of real and complex topological K-theories. We apply our results to Lubin–Tate spectra in § 8. In § 9, we study the THH and the algebraic K-theory of Morava E-theories.
Notation 1.8.
-
(1) We work freely in the setting of
$\infty$
-categories and higher algebra from [Reference LurieLur09, Reference LurieLur17]. -
(2) For an
$E_2$
-algebra R in a symmetric monoidal
$\infty$
-category, when we say T is an R-algebra (or an
$E_1$
R-algebra), we mean that it is an
$E_1$
-algebra in right R-modules. If we mean an
$E_1$
-algebra in left R-modules, we call this a left
$E_1$
R-algebra. If R is
$E_\infty$
, we do not need to denote the distinction. -
(3) When we say
$E_n$
-ring, we mean an
$E_n$
-algebra in the
$\infty$
-category of spectra
$\operatorname{Sp}$
.
2. Recollections on graded objects
Let
$m\geq 0$
be an integer and let
$\mathbb{Z}/m$
denote the discrete
$\infty$
-groupoid whose objects are the elements of the set of integers modulo m. For a presentably symmetric monoidal
$\infty$
-category
${{\mathcal{V}}}$
, we define the
$\infty$
-category of m-graded objects in
$$\mathcal{V}$$
to be the functor category
$\operatorname{Fun}(\mathbb{Z}/m, {{\mathcal{V}}})$
. For a functor F in
$\operatorname{Fun}(\mathbb{Z}/m,{{\mathcal{V}}})$
, we denote F(i) by
$F_i$
for every
$i \in \mathbb{Z}/m$
. Since
$\mathbb{Z}/m$
is discrete, we have
For
$m=0$
, this is given by
$\operatorname{Fun}(\mathbb{Z}, {{\mathcal{V}}})$
, where
$\mathbb{Z}$
is the corresponding discrete
$\infty$
-groupoid. In this case, we omit m and call
$\operatorname{Fun}(\mathbb{Z}, {{\mathcal{V}}})$
the
$\infty$
-category of graded objects in
${{\mathcal{V}}}$
. We are mainly interested in the case
${{\mathcal{V}}} = \operatorname{Sp}$
. We call an object of
$\operatorname{Fun}(\mathbb{Z}/m,\operatorname{Sp})$
an m-graded spectrum; for
$m=0$
, we drop m and call it a graded spectrum.
Using the symmetric monoidal structure on
$\mathbb{Z}/m$
given by addition, we equip
$\operatorname{Fun}(\mathbb{Z}/m, {{\mathcal{V}}})$
with the Day convolution closed symmetric monoidal structure [Reference GlasmanGla16]. Since
$\mathbb{Z}/m$
is discrete, this boils down to the following:
2.1 Algebras in graded spectra
We are interested in
$E_n$
-algebras in the
$\infty$
-category of m-graded spectra and the algebras over these
$E_n$
-algebras.
Definition 2.1. An m-graded
$E_n$
-ring A is an
$E_n$
-algebra in
$\operatorname{Fun}(\mathbb{Z}/m, \operatorname{Sp})$
. For
$k\lt n$
, an m-graded
$E_k$
A-algebra is an
$E_k$
A-algebra in
$\operatorname{Fun}(\mathbb{Z}/m, \operatorname{Sp})$
. Similarly, an m-graded (left) right A-module is a (left) right A-module in
$\operatorname{Fun}(\mathbb{Z}/m, \operatorname{Sp})$
.
Remark 2.2. Note that the notion of an m-graded
$E_k$
-algebra in
$\operatorname{Sp}$
is, in general, different from the notion of an m-graded object in the
$\infty$
-category of
$E_k$
-algebras in
$\operatorname{Sp}$
.
2.2 Manipulations on graded objects
For a symmetric monoidal functor
$\mathbb{Z}/m\to \mathbb{Z}/m'$
(i.e. a group homomorphism), there is an induced adjunction between the
$\infty$
-categories
$\operatorname{Fun}(\mathbb{Z}/m,\operatorname{Sp})$
and
$\operatorname{Fun}(\mathbb{Z}/m',\operatorname{Sp})$
where the left adjoint is symmetric monoidal and given by left Kan extension [Reference NikolausNik16, Corollary 3.8]. The right adjoint is given by restriction. This provides the following adjunctions, which allow us to move between various gradings. Let
$n\gt 0$
and
$s \geq 0$
be integers.
-
– We let
$D^n_{sn} \dashv Q$
denote the adjunction induced by the quotient map
$\mathbb{Z}/sn \to \mathbb{Z}/n$
sending 1 to 1. -
– We often use
$D^{n}_{sn}$
for
$s=0$
, which allows us to obtain an n-graded object out of a graded object X in
$\operatorname{Sp}$
. We let
$D^{n}$
denote
$D^n_{0} \colon \operatorname{Fun}(\mathbb{Z},\operatorname{Sp}) \to \operatorname{Fun}(\mathbb{Z}/n,\operatorname{Sp})$
and we have
\[D^n(X)_i \simeq \bigvee_{j\in \mathbb{Z} \mid j \equiv i\ \operatorname{mod}\,n}X_j.\]
-
– For
$n = 1$
, we denote
$D^1_s$
by D. In this case, is given by
\[D \colon \operatorname{Fun}(\mathbb{Z}/s,\operatorname{Sp}) \to \operatorname{Sp}\]
$D(X) \simeq \vee_{j \in \mathbb{Z}/s} X_j$
, i.e. left Kan extension along
$\mathbb{Z}/s \to 0$
. For an s-graded (spectrum)
$E_n$
-ring X, we call D(X) the underlying (spectrum)
$E_n$
-ring of X. We often omit D in our notation.
-
– For
$s \in \mathbb{Z}$
, let
$L_s \dashv R_s $
denote the adjunction on
$\operatorname{Fun}(\mathbb{Z}, \operatorname{Sp})$
induced by the map
$\mathbb{Z} \xrightarrow{\cdot s} \mathbb{Z}$
given by multiplication by s. For a graded spectrum X, we have for every i and
\[L_s(X)_{si} \simeq X_i\]
$L_s(X)_{j} \simeq 0$
whenever
$s \nmid j$
; furthermore,
$R_s(X)_j \simeq X_{sj}$
for every j.
-
– Let
$F\dashv G$
denote the adjunction induced by the trivial map
$0 \to \mathbb{Z}/m$
. We have
$G(X) = X_0$
. For an m-graded
$E_n$
-ring A, F(G(A)) is given by
$A_0$
in weight 0 and it is trivial on the other degrees. Therefore, we sometimes abuse notation and denote the m-graded
$E_n$
-ring F(G(A)) by
$A_0$
. The counit of this adjunction provides a map of m-graded
\[A_0 \to A\]
$E_n$
-rings. If
$A_i \simeq 0$
for
$i \neq 0$
, then this map is an equivalence and we say that A is concentrated in weight 0. The following lemma states that, in this situation, there is an equivalence of
$E_n$
-rings between the underlying
$E_n$
-ring of A and the weight-0 piece
$G(A) = A_0$
of A. Therefore, we often do not distinguish between A,
$G(A) = A_0$
and D(A) in our notation when A is concentrated in weight 0.
Lemma 2.3.
Let A be an m-graded
$E_n$
-ring concentrated in weight 0. There is an equivalence of
$E_n$
-rings
where
$A_0$
denotes G(A). In particular, we have
$F(D(A)) \simeq A$
as m-graded
$E_n$
-rings.
Proof. Since A is concentrated in weight 0, we have
$D(A)\simeq DFG(A)$
. As
$D \circ F$
Kan extends through the composite
$0\to \mathbb{Z}/m \to 0$
, it is equivalent to the identity functor. We obtain that
$DFG(A) \simeq G(A) \simeq A_0$
.
For the second statement, note that
$F(D(A)) \simeq F(G(A))$
due to the first statement. Since A is concentrated in weight 0, we have
$F(G(A))\simeq A$
.
3. A family of
$E_2$
polynomial rings in graded spectra
In this section, we introduce the construction of a family of
$E_2$
-algebras in graded spectra. These have appeared in the work of Hahn and Wilson [Reference Hahn and WilsonHW22] and are also studied in greater depth by Devalpurkar and Moulinos (Logarithmic structures for
$E_2$
-algebras, in progress, 2022). These will be central to our constructions. For every
$r, w \in \mathbb{Z}$
, one constructs a graded
$E_2$
-ring
$\mathbb{S}[\sigma_{2r}]$
, which may be thought of as a ‘polynomial’ algebra with a generator in homotopical degree 2r and grading weight w. However, these are not polynomial algebras in the precise sense, as they are only demonstrated to admit
$E_2$
structures. By mapping these
$E_2$
-rings into each other, we will be able to construct
$E_2$
-ring extensions.
3.1 Shearing preliminaries
The main mechanism underlying this construction is that of shearing, which we now briefly review. It has appeared in [Reference RaksitRak20], and is also studied by Devalpurkar and Moulinos, Logarithmic structures for
$E_2$
-algebras, in progress, 2022). In what follows,
$\operatorname{Gr}(\operatorname{Sp})$
denotes
$\operatorname{Fun}(\mathbb{Z},\operatorname{Sp})$
, i.e. the
$\infty$
-category of graded spectra.
Proposition 3.1. There exists an endofunctor on graded spectra
given by
with the following properties:
-
– sh is an equivalence, with inverse given by
$\operatorname{sh}^{-1}(M_i) = M_{i}[2i]$
; -
– sh admits an
$E_2$
-monoidal structure, with respect to the Day convolution product on
$\operatorname{Gr}(\operatorname{Sp})$
.
Proof. This appears in the
$\mathbb{Z}$
-linear setting in [Reference RaksitRak20] and also appears in [Reference Devalapurkar, Hahn, Lawson, Senger and WilsonDHL+23]. For the sake of completeness, we sketch the basic ideas underlying the construction. In [Reference LurieLur15], Lurie constructs an
$E_2$
-monoidal map of spaces
sending
$n \mapsto \mathbb{S}^{-2n}$
. We now define
$\operatorname{sh}$
as the functor, obtained by adjunction, from the assignment
given by the composition
Here, the first map sends
$(n,M) \mapsto (\phi(n),M_n)$
. The fact that this latter composition is
$E_2$
follows from the fact that
$\phi$
is itself
$E_2$
. This further implies that
$\operatorname{sh}$
is itself
$E_2$
monoidal. To see that this is an equivalence, one displays, as in [Reference RaksitRak20], an inverse in the same way by precomposing
$\phi$
with the map
$\mathbb{Z}\xrightarrow{-1\cdot}\mathbb{Z}$
.
Variant 3.2. One can precompose the map
$\phi: \mathbb{Z} \to \operatorname{Pic}(\operatorname{Sp})$
with the map
$\cdot (k) : \mathbb{Z} \to \mathbb{Z}$
. We denote the composition by
As in the above, we use this to define an endofunctor
This acquires the same formal properties as above, e.g. it will be an
$E_2$
-monoidal autoequivalence on
$\operatorname{Gr}(\operatorname{Sp})$
. Furthermore, one has the description
$(\operatorname{sh}^k M)_i \simeq M_i[-2ki]$
.
3.2 Sheared polynomial algebras
Recall that there exists an
$E_\infty$
-algebra
$\mathbb{S}[t] \in \operatorname{Gr}(\operatorname{Sp})$
, which gives a graded enhancement of the ‘flat’ polynomial algebra. One can obtain this, for example, by observing that the restriction map from filtered spectra to graded spectra
is lax symmetric monoidal. In more detail, this will be the restriction
along
$\mathbb{Z} \hookrightarrow (\mathbb{Z}, \leq)$
so that, in particular, we forget the structure maps of the filtration; cf. [Reference LurieLur15]. We remind the reader that this is different from the associated graded functor. One then sets
$\mathbb{S}[t] := \operatorname{Res}(\mathbf{1})$
, where 1 denotes the unit of the symmetric monoidal structure on
$\operatorname{Fil}(\operatorname{Sp})$
. Thus,
$\mathbb{S}[t]$
(which is given by
$\mathbb{S}$
in nonpositive weights and 0 in positive weights) acquires the structure of an
$E_{\infty}$
-algebra in graded spectra.
Construction 3.3. As described in Proposition 3.1, there exists an
$E_2$
-monoidal autoequivalence
$\operatorname{sh}$
. We set
and more generally, for
$k\gt 0$
,
that is, one applies
$\operatorname{sh}^{k}$
to
$\mathbb{S}[t]$
to obtain a family of
$E_2$
-algebras in graded spectra. For
$k=0$
, we set
$\mathbb{S}[\sigma_0] := \mathbb{S}[t]$
. It follows by inspection that the underlying graded
$E_1$
-ring of
$\mathbb{S}[\sigma_{2k}]$
is the free graded
$E_1$
-ring on
$\mathbb{S}^{2k}(-1)$
, where
$\mathbb{S}^{2k}(-1)$
is
$\mathbb{S}^{2k}$
concentrated in weight
$-1$
.
Remark 3.4. For
$w\in \mathbb{Z}$
and even
$k\geq 0$
, we apply the functor
$L_{-w}$
which left Kan extends along the multiplication map
to obtain weight-sifted variants of
$\mathbb{S}[\sigma_k]$
. We often omit
$L_{-w}$
when the weight of
$\sigma_k$
is clear from the context but when we wish to be explicit, we write
$\mathbb{S}[\sigma_{k, w}]$
for the graded
$E_2$
-ring
$L_{-w}\mathbb{S}[\sigma_k]$
, where
$\sigma_{k,w}$
is in weight w. As before, the underlying graded
$E_1$
-ring of
$\mathbb{S}[\sigma_{k, w}]$
is the free graded
$E_1$
-ring
$\operatorname{Free}_{E_1}( \mathbb{S}^{k}(w))$
.
To adjoin roots, we often start with
$\mathbb{S}[\sigma_{mk}]$
and
$\mathbb{S}[\sigma_k]$
with
$\sigma_{mk}$
and
$\sigma_k$
in weights m and 1, respectively, where
$m\gt 0$
and
$k\gt 0$
is even.
Proposition 3.5.
In the situation above, there exists a map of graded
$E_2$
-rings
that carries
$\sigma_{mk}$
to
$\sigma_k^m$
in homotopy. This provides a map of m-graded
$E_2$
-rings
where
$\sigma_k \in \pi_* D^m(\mathbb{S}[\sigma_k])$
is of weight 1 and
$D^m(\mathbb{S}[\sigma_{mk}])$
is concentrated in weight 0.
Furthermore, we have
$D^m(\mathbb{S}[\sigma_{mk}])\simeq F(D(\mathbb{S}[\sigma_{mk}]))$
as m-graded
$E_2$
-rings; here, F Kan extends through
$0 \to \mathbb{Z}/m$
.
Proof. We first remind the reader that there is an identification
of graded
$E_2$
-rings. This follows from the very definition of the kth shearing functor
$\operatorname{sh}^{k}$
, in particular that it sends
$\mathbb{S}[t]$
to the negative weight part of the graded spectrum given by the map
Thus we may identify
$\mathbb{S}[\sigma_{mk,-1}]$
with
$R_m\mathbb{S}[\sigma_{k,-1}] \simeq R_m\operatorname{sh}^{k}(\mathbb{S}[t])$
, negative-weight part of the graded spectrum given by the map
Therefore, the counit of the adjunction
$L_m \dashv R_m$
provides a map of graded
$E_2$
-rings
Here,
$\mathbb{S}[\sigma_{mk,-m}]$
is the free graded
$E_1$
-algebra on a class
$\sigma_{mk,-m}$
of degree mk and weight
$-m$
and by inspection on the adjunction
$L_m \dashv R_m$
, this map carries
$\sigma_{mk,-m}$
to
$\sigma_{k,-1}^m$
. Applying the functor
$L_{-1}$
to this map, we obtain the map of graded
$E_2$
-rings
$\mathbb{S}[\sigma_{mk}] \to \mathbb{S}[\sigma_k]$
claimed in the proposition.
The functor
$D^m$
gives the desired map
of m-graded
$E_2$
-algebras. Note that
$\sigma_{mk} \in \pi_{*}D^m(\mathbb{S}[\sigma_{mk}])$
is of weight 0, which ensures that
$D^m(\mathbb{S}[\sigma_{mk}])$
is concentrated in weight 0.
To see the last statement, we have
due to Lemma 2.3, since
$D^m(\mathbb{S}[\sigma_{mk}])$
is concentrated in weight 0. Furthermore,
$D D^m$
is the Kan extension through the composite
$\mathbb{Z}\to \mathbb{Z}/m \to 0$
, which is the same as the Kan extending through
$\mathbb{Z}\to 0$
. Therefore,
$DD^m(\mathbb{S}[\sigma_{mk}]) \simeq D(\mathbb{S}[\sigma_{mk}])$
. This, together with (3.1), provides the desired equivalence
$D^m(\mathbb{S}[\sigma_{mk}]) \simeq F(D(\mathbb{S}[\sigma_{mk}]))$
.
We often omit the functor
$D^m$
in our notation and denote the map of m-graded
$E_2$
-rings
$D^m(\mathbb{S}[\sigma_{mk}]) \to D^m(\mathbb{S}[\sigma_k])$
as
$\mathbb{S}[\sigma_{mk}] \to \mathbb{S}[\sigma_k]$
.
Remark 3.6. To adjoin a root to a degree-0 class, we need the
$k=0$
case of the proposition above. In other words, we need an analogous
$E_2$
-map
$\mathbb{S}[\sigma_{mk}] \to \mathbb{S}[\sigma_k]$
for
$k=0$
. For this, we start with the graded
$E_2$
-map
$\mathbb{S}[\sigma_{m2}] \to \mathbb{S}[\sigma_2]$
and apply the functor
$\operatorname{sh}$
. This procedure provides a graded
$E_2$
-map
$\mathbb{S}[\sigma_{{0},m}] \to \mathbb{S}[\sigma_{0,1}]$
that carries
$\sigma_{0,m}$
to
$\sigma_{0,1}^m$
as desired.
3.3 Cell structures on sheared polynomial algebras
A key technical result for us will be the even cell decomposition of
$\mathbb{S}[\sigma_{k}]$
as an
$E_2$
-algebra. As we show in the remainder of this section, this is what will allow us to define
$E_2$
-algebra maps to a given
$E_2$
-algebra A, along which we will then adjoin roots.
Remark 3.7. In the second arXiv version of [Reference Hahn and WilsonHW22], Hahn and Wilson also construct
$E_2$
even cell decompositions on the free
$E_1$
-algebra
$\mathbb{S}[\sigma_k]$
using a Koszul duality argument for even
$k \geq 0$
. However, they removed this result in the later versions of their paper since they found a simpler argument for their redshift results that avoids the use of these even cell decompositions. Since this does not appear in the published version of [Reference Hahn and WilsonHW22], we give a proof of the
$E_2$
even cell decompositions on
$\mathbb{S}[\sigma_k]$
that we use. We would like to note that our methods are different from the ones used in [Reference Hahn and WilsonHW22, arXiv version 2].
Before doing this, we make precise what exactly we mean by even cell decomposition. The following notions are heavily inspired by § 6.3 of [Reference Galatius, Kupers and Randal-WilliamsGKR25].
Definition 3.8. Let
$f: S \to R \in \operatorname{Alg}_{E_2}(\operatorname{Sp}^{\mathbb{Z}})$
be a map of
$E_2$
-algebras in graded spectra. We say f has a filtered cellular decomposition if there exists a tower in
$\operatorname{Alg}_{E_2}(\operatorname{Fil}(\operatorname{Gr}(\operatorname{Sp})))$
for which
such that each
$\operatorname{sk}_{i}(f)$
is obtained from
$\operatorname{sk}_{i-1(f)}$
via the following pushout diagram.

The notation X[n] in the above means that the object X is placed in filtering degree n.
In particular, in each degree i of the tower, we are adding cells in increasing dimension
$n_i$
. Thus, if
$i \leq j$
, then
$n_i \leq n_j$
and
$I_{n_i}$
refers to the set of
$n_i$
cells of R. It may be the case that
$n_i = i$
, but we do not require this for the sake of flexibility of the definition, which is a point of departure from the notion in [Reference Galatius, Kupers and Randal-WilliamsGKR25]. If
$f: \mathbf{1} \to R$
is the map from the unit, we call this a filtered cellular decomposition of R.
Definition 3.9. A map
$f\colon S \to R$
of graded
$E_2$
-rings admits a cell decomposition if it is the colimit of a tower
in graded
$E_2$
-rings, where each stage is obtained from the previous via a cell attachement in graded
$E_2$
-rings. In particular, if f admits a filtered cellular decomposition, then taking levelwise colimits provides a cellular decomposition of f.
Our first step is to establish the decomposition for
$\mathbb{S}[t]$
.
Proposition 3.10.
As an
$E_2$
-algebra in graded spectra,
$\mathbb{S}[t]$
admits a (filtered) cellular decomposition with cells in even degrees.
Proof. The two key inputs for our argument are Theorems 11.21 and 13.7 of [Reference Galatius, Kupers and Randal-WilliamsGKR25]. The former result applied to the map
$f: 0 \to I$
of non-unital
$E_2$
-algebras in graded spectra (where I is the augmentation ideal of the map
$\mathbb{S}[t] \to \mathbb{S}$
) says that there exists a relative CW decomposition
Moreover, the proof of this fact in the same work constructs a minimal cell structure, one that has the smallest possible number of cells in a given bidegree (the extra degree here arises since we are working in graded spectra). In particular, the colimit they construct,
$\operatorname{colim} \operatorname{sk}_n(f)$
, will have cells precisely in bidegree
$b^{E_2}_{g,d}(\mathbb{S}[t]):= \operatorname{dim}_k H^{E_2}_{g,d}(\mathbb{S}[t], \mathbb{S}, k) \in \mathbb{N} \cup \{ \infty\}$
, where
$H^{\mathcal{O}}_{g,d}(R ; k)$
is the
$\mathcal{O}$
-homology of an
$\mathcal{O}$
-algebra R, with coefficients in the ring k; we will, in fact, set
$k = \mathbb{Z}$
.
We sketch the argument given there applied to our particular case for the sake of completeness. One proceeds by inductively constructing a factorization
in the
$\infty$
-category of (increasingly) filtered objects of
$\operatorname{Fun}(\mathbb{Z}, \operatorname{Sp})$
. Here,
$h_e: \operatorname{sk}_{e-1} \to \operatorname{sk}_{e}$
comes with the structure of a (filtered) CW attachment of dimension e, where
$\operatorname{sk}_{i}$
denotes the ith skeleton equipped with the skeletal filtration leading up to that degree. Taking the colimit along
$\epsilon$
gives an induced map
$f_\infty: \operatorname{colim} sk_\epsilon(f) \to I$
, which is an equivalence.
For the inductive step in their argument, they show that the Hurewicz map
from relative homotopy to relative
$E_2$
-homology with coefficients in k is surjective. Using this, one is able to choose a set of maps
whose images generate
$H_{*, \epsilon}^{E_2}(\mathbb{S}[t], \operatorname{sk}_{\epsilon -1}; k)$
as a k-module. The boundary maps are then used to attach filtered cells
$(g, \epsilon)$
to
$\operatorname{sk}_{\epsilon -1}$
to form
$\operatorname{sk}_{\epsilon}$
, and the corresponding
$E_\alpha$
is used to extend
$f_{\epsilon -1}$
to
$f_{\epsilon}$
. Putting all this together, we see that the attachment of the cells is parameterized by the dimensions of the
$E_2$
-algebra homology groups with coefficients in k. To see, in our particular setup, that this cell decomposition is concentrated in even degrees, it is therefore enough to verify that
$H^{E_2}_{g, e}(\mathbb{S}[t], k)$
vanishes whenever
$e \cong1\operatorname{mod} 2$
. For this, we apply [Reference Galatius, Kupers and Randal-WilliamsGKR25, Theorem 13.7], which states that the k-fold iterated bar construction of an
$E_k$
-algebra is equivalent to the k-suspension of the
$E_k$
-cotangent complex. By [Reference LurieLur15, Proposition 5.4.9], there is an equivalence
$\operatorname{Bar}^{(2)}(\mathbb{S}[t]) \simeq \operatorname{gr}(\mathbb{S}[\mathbb{C}P^{n}]_{n \geq 0}) $
in graded spectra, where the right-hand side is the associated grading of the filtration on spherical chains on
$\mathbb{C}P^\infty$
, with filtration induced by the skeletal filtration on infinite projective space. Tensoring this with
$k = \mathbb{Z}$
in our particular situation, we obtain (a 2-fold shift) of chains on
$\mathbb{C}P^\infty$
with coefficients in
$\mathbb{Z}$
which has a cell in each bidegree
$(-n, 2n-2)$
. By taking into account units, we conclude that
$\mathbb{S}[t]$
may be constructed from
$\mathbb{S}$
by attaching the same cells.
We begin with the particular filtered cellular decomposition on
$\mathbb{S}[t]$
given in the proof above and apply levelwise colimits to obtain a cellular decomposition for
$\mathbb{S} \to \mathbb{S}[t]$
in the sense of Definition 3.9. In the following corollary, we use this particular cellular decomposition.
Corollary 3.11.
The degree-0 piece of the above cellular decomposition is the free algebra
$\operatorname{Free}_{E_2}(\mathbb{S}(-1))$
, i.e. the free
$E_2$
-algebra with generator in degree 0 and weight
$-1$
. Moreover, the map
$f_0: \operatorname{Free}_{E_2}((\mathbb{S}(-1)) \to \mathbb{S}[t]$
itself admits a cellular decomposition with even cells of positive dimension.
Proof. In degree 0, we have the following pushout square in
$\operatorname{Alg}_{E_2}(\operatorname{Fun}(\mathbb{Z}, \operatorname{Sp}))$
.

Since this is a pushout square, we obtain an equivalence
Moreover, by starting in degree 0 with the zero cells already attached, we may conclude that the map
itself admits a cellular decomposition with even cells of positive dimension.
By the above corollary, we have a cellular decomposition on the map of graded
$E_2$
-rings
$\operatorname{Free}_{E_2}(\mathbb{S}(-1)) \to \mathbb{S}[t]$
. We can apply shearing to this map to obtain a map
Proposition 3.12.
Let
$k\gt 0$
be even. The map
$f_0: \operatorname{Free}_{E_2} \mathbb{S}^{k}(-1) \to \mathbb{S}[\sigma_k] $
admits a cell decomposition with cells concentrated in even degrees. Left Kan extending along the multiplication map
$\mathbb{Z} \xrightarrow{\times -w} \mathbb{Z} $
, we conclude that
$f_0: \operatorname{Free}_{E_2} \mathbb{S}^{k}(w) \to \mathbb{S}[\sigma_{k,w}] $
admits a cell decomposition with cells concentrated in even degrees.
Proof. By Corollary 3.11,
$\mathbb{S}[t]$
may be written as a filtered colimit of a diagram of
$E_{2}$
-algebras,
where each
$\operatorname{sk}_{i}(f)$
is formed as a pushout from
$\operatorname{sk}_{i-1}$
along a map
$\operatorname{Free}_{E_2}(\mathbb{S}^{2n+1}) \to \mathbb{S}$
. We may apply
$\operatorname{sh}^{k/2}$
to this diagram, and take note of the fact that this will commute with colimits along the filtered diagram, together with the free
$E_2$
-algebra functor. Thus, we conclude with an even cell presentation for the induced map:
By left Kan extending along the multiplication by the
$-w$
map on
$\mathbb{Z}$
(i.e. applying
$L_{-w}$
), we conclude analogously for the map
Proposition 3.13.
Let A be a (graded)
$E_2$
-ring whose homotopy groups are concentrated in even degrees and let
$a \in \pi_{k} A$
be a weight-w class for some even
$k\geq0$
. Then there is a (graded)
$E_2$
-ring map
which carries
$\sigma_{k}$
to a.
Proof. By Proposition 3.12, the map
admits an even cell decomposition. Let
$a \in \pi_{k}(A)$
be as in the hypothesis of the proposition. This induces an
$E_2$
-algebra map
$\operatorname{Free}_{E_2}(\mathbb{S}^{k}(w)) \to A $
, which we would like to extend inductively along the above tower. In order to do this, it is enough to note that in degree i, we would need to trivialize the induced map
$\operatorname{Free}_{E_2}(\mathbb{S}^{k + 2i -1}) \to A$
. Using the free/forgetful adjunction between
$\operatorname{Alg}_{E_2}(\operatorname{Gr}(\operatorname{Sp}))$
and
$\operatorname{Gr}(\operatorname{Sp})$
algebras and graded spectra, this will now follow from the fact that
$\pi_{2n-1}(A)= 0$
for all n.
Remark 3.14. In Remark 3.6, we mentioned that we are going to use
$\operatorname{sh}(\mathbb{S}[\sigma_{m2,m}])$
to adjoin roots to degree-0 classes. We remark that
$\operatorname{sh}(\mathbb{S}[\sigma_{m2,m}])$
also satisfies the lifting property in the proposition above. This follows from the fact that the even cell decomposition for
$\mathbb{S}[\sigma_{m2,m}]$
provides an even cell decomposition for
$\operatorname{sh}(\mathbb{S}[\sigma_{m2,m}])$
, since
$\operatorname{sh}$
is an
$E_2$
-monoidal left adjoint functor.
Remark 3.15. We remark that another way to construct an
$E_2$
-algebra map
$\mathbb{S}[t] \to A$
comes from the filtration on
$\mathbb{S}[t]$
given its filtered cell decomposition. The mapping space
obtains a filtration from the filtration on the source; this will have associated grading
$$\operatorname{gr}\operatorname{Map}_{\operatorname{Alg}_{E_2}}(\mathbb{S}[t], A )\simeq {\operatorname{Map}}\bigg({\operatorname{Free}_{E_2}}\bigg(\bigoplus_{n \geq 1} \mathbb{S}^{2n }, A\bigg)\bigg) \simeq {\operatorname{Map}}\bigg(\bigoplus_{n \geq 1} \mathbb{S}^{2n }, A\bigg).$$
Now, if X has even homotopy groups, then so does the associated grading, so the resulting spectral sequence computing the homotopy groups of the limit collapses. Thus,
$a \in \pi_{0}(A)$
gives a class in
$x \in \pi_0 \operatorname{Map}(\mathbb{S}^{2k}, X) \subset \pi_0 \operatorname{Map}(\bigoplus_{n \geq 1} \mathbb{S}^{2n +2nk -2}, X) $
, which will be an infinite cycle, and thus corresponds to an
$E_2$
-algebra map
$\mathbb{S}[t] \to A$
. We remark that this approach should allow for one to define maps
$ \mathbb{S}[\sigma_k] \to A$
in the general case as well. We thank Oscar Randal-Williams for suggesting this approach.
4. Adjoining roots and THH
Here, we introduce our construction for adjoining roots to ring spectra and prove our first results on the THH of ring spectra obtained through this construction.
4.1 Background on algebras over
$E_n$
-algebras
Here is a quick background on some of the standard facts that we often use from [Reference LurieLur17].
For an
$E_\infty$
-algebra R in a presentably symmetric monoidal
$\infty$
-category
${{\mathcal{C}}}$
, the
$\infty$
-category of
$E_n$
R-algebras is a symmetric monoidal
$\infty$
-category with the pointwise tensor product [Reference LurieLur17, Example 3.2.4.4]. Therefore, for two
$E_n$
R-algebras A and B,
$A \otimes_R B$
is an
$E_n$
R-algebra.
In this work, we often consider algebras over an
$E_n$
-algebra R and in this case, the
$\infty$
-category of
$E_m$
R-algebras (for
$m\leq n-1$
) are not known to carry an appropriate
$E_{n-1}$
-monoidal structure. To work around this problem, we use the following facts which can be extracted from [Reference LurieLur17, Corollary 4.8.5.20].
The
$\infty$
-category of (left) right R-modules is an
$E_{n-1}$
-monoidal
$\infty$
-category. We call an
$E_m$
-algebra in the
$\infty$
-category of right R-modules an
$E_m$
R-algebra, where
$m\leq n-1$
.
Furthermore, for a map
$f\colon R \to S$
of
$E_n$
-algebras in
${{\mathcal{C}}}$
, one obtains an
$E_{n-1}$
-monoidal functor
$-\otimes_{R} S$
between the respective
$\infty$
-categories of modules. For every
$m\leq n-1$
, this induces a functor
In particular, for an
$E_m$
R-algebra A,
$A \otimes_R S$
is an
$E_{m}$
S-algebra. Furthermore, the forgetful functor induced by f, i.e. the right adjoint of
$- \otimes_R S$
, is
$E_{n-1}$
-lax monoidal, and therefore it induces a functor
The unit of this adjunction provides a map of
$E_m$
R-algebras
Since S is the monoidal unit in
$\operatorname{RMod}_S$
, S is an
$E_{n-1}$
S-algebra, and forgetting through (4.2), it is an
$E_{n-1}$
R-algebra. In summary, an
$E_n$
-algebra map
$R \to S$
equips S with the structure of an
$E_{n-1}$
R-algebra.
4.2 A construction for adjoining roots to ring spectra
We now introduce our construction for adjoining roots to ring spectra. For this, we use the following hypothesis. Recall that we often omit the functor D and let
$\mathbb{S}[\sigma_k]$
denote the underlying
$E_2$
-ring of the graded
$E_2$
-ring
$\mathbb{S}[\sigma_k]$
.
Hypothesis 4.1 (Root adjunction hypothesis). Given an
$E_1$
-ring A with
$a \in \pi_{mk}A$
, there is a chosen
$\mathbb{S}[\sigma_{mk}]$
-algebra structure on A for which the structure map
$\mathbb{S}[\sigma_{mk}] \to A$
carries
$\sigma_{mk}$
to
$a \in \pi_{mk}A$
. Here,
$m\gt 0$
and
$k\geq 0$
is even. See Proposition 4.2 for the cases of interest where this is satisfied.
The hypothesis above may not seem very natural but it is satisfied in the following general situations.
Proposition 4.2.
Let
$k\geq 0$
be even and
$m\gt 0$
, an
$E_1$
-ring A satisfies Hypothesis 4.1 for
$a \in \pi_{mk}A$
if:
-
(1) A is an
$E_2$
-ring for which
$\pi_* A$
is concentrated in even degrees; or -
(2) A is an R-algebra for an
$E_2$
-ring R where
$\pi_* R$
is concentrated in even degrees and a is in the image of the map
$\pi_* R \to \pi_* A$
.
Proof. Assume that A is as in part (2), and let
$r\in \pi_{mk}R$
detect a through the map
$\pi_* R \to \pi_* A$
. We choose an
$E_2$
-ring map
$g\colon \mathbb{S}[\sigma_{mk}] \to R$
that carries
$\sigma_{mk}$
to r; see Proposition 3.13. Forgetting through g, see (4.2), one obtains a
$\mathbb{S}[\sigma_{mk}]$
-algebra structure on A. Indeed, through this structure,
$\sigma_{mk}$
acts through a as desired.
If A is as in part (1), then A is an A-algebra and A satisfies the assumption in part (2). Therefore, A satisfies Hypothesis 4.1.
For instance, the Morava K-theory spectrum K(n) and all
$E_1$
$MU_{(p)}$
-algebra forms of
$BP \langle n \rangle$
satisfy Hypothesis 4.1 with respect to their non-negative degree homotopy classes.
Note that we are not assuming any pre-existing non-trivial grading on A; in fact, this will allow us to view it as an m-graded spectrum concentrated in weight 0. Given
$a \in \pi_{mk} A$
, the following construction adjoins an m-root to a.
Construction 4.3. Assume Hypothesis 4.1. We consider
$\mathbb{S}[\sigma_{mk}]$
as an m-graded
$E_2$
-ring and A as an m-graded
$\mathbb{S}[\sigma_{mk}]$
-algebra, both concentrated in weight 0, using the functor F from § 2.2; we omit F in our notation.
Owing to Proposition 3.5 (Remark 3.6 for
$k=0$
), there is a map
of m-graded
$E_2$
-rings that carries
$\sigma_{mk}$
to
$\sigma_k^m$
in homotopy, where
$\sigma_k$
is of weight 1 and
$\sigma_{mk}$
is of weight 0. Note that we omit the functor
$D^m$
in our notation. Considering the corresponding extension of scalars functor
$- \wedge_{\mathbb{S}[\sigma_{mk}]} \mathbb{S}[\sigma_k]$
between the
$\infty$
-categories of m-graded
$\mathbb{S}[\sigma_{mk}]$
-algebras and m-graded
$\mathbb{S}[\sigma_k]$
-algebras (see (4.1)), we define the m-graded
$E_1$
$\mathbb{S}[\sigma_k]$
-algebra
$A(\!\sqrt[m]{a})$
through
This comes equipped with a map
$A \to A(\!\sqrt[m]{a})$
of m-graded
$E_1$
$\mathbb{S}[\sigma_{mk}]$
-algebras; see (4.3).
Since
$\pi_* (\mathbb{S}[\sigma_k])$
is free as a
$\pi_* (\mathbb{S}[\sigma_{mk}])$
-module, one obtains an isomorphism of rings
Therefore, we say
$A(\!\sqrt[m]{a})$
is obtained from A by adjoining an m-root to a.
When A is p-local, observe that we have an equivalence of m-graded
$E_1$
$\mathbb{S}[\sigma_k]$
-algebras
where
$\mathbb{S}_{(p)}[\sigma_i]$
denotes the p-localization of
$\mathbb{S}[\sigma_i]$
.
It follows that the weight pieces of
$A(\!\sqrt[m]{a})$
are given by the following:
for each
$0\leq i\lt m$
.
Note that
$A(\!\sqrt[m]{a})$
might possibly depend on the
$\mathbb{S}[\sigma_{mk}]$
-algebra structure chosen on A. Therefore, every time we apply Construction 4.3, we fix an
$\mathbb{S}[\sigma_{mk}]$
-algebra structure on A.
Remark 4.4. If A is an
$E_3$
-ring with even homotopy, we may start with an
$E_2$
-map
$\mathbb{S}[\sigma_{mk}] \to A$
for a given
$a \in \pi_{mk}A$
with
$k\geq 0$
. By extending scalars, we obtain an
$E_2$
-ring map
$A \wedge \mathbb{S}[\sigma_{mk}] \to A$
that equips A with the structure of an
$A \wedge \mathbb{S}[\sigma_{mk}]$
-algebra. Through this,
$A(\!\sqrt[m]{a})$
is weakly equivalent as an m-graded
$\mathbb{S}[\sigma_k]$
-algebra to
In particular,
$A(\!\sqrt[m]{a})$
admits the structure of an m-graded
$A \wedge \mathbb{S}[\sigma_k]$
-algebra.
Remark 4.5. In general, we do not expect the root adjunction
$A\ \to A(\!\sqrt[m]{a})$
to satisfy a universal property. On the other hand, if A is an
$E_3$
-ring,
$A(\!\sqrt[m]{a})$
is an A-algebra and the map
$\pi_* A \to \pi_* A(\!\sqrt[m]{a})$
is étale, then it follows by [Reference Hesselholt and PstragowskiHP25, Theorem 1.10] that there is a bijection between homotopy classes of A-algebra maps
$A(\!\sqrt[m]{a}) \to B$
and
$\pi_* A$
-algebra maps
$\pi_* A(\!\sqrt[m]{a}) \to \pi_* B$
for any étale A-algebra B.
For the following, we fix an
$E_2$
-map
$\mathbb{S}_{(p)}[\sigma_{2(p-1)}] \to \ell$
carrying
$\sigma_{2(p-1)}$
to
$v_1$
.
Theorem 4.6. There is an equivalence
of
$E_1$
$\ell_p$
-algebras.
Proof. By Remark 4.4 above,
$\ell_p(\!\sqrt[p-1]{v_1})$
is an
$\ell_p$
-algebra. Let
$L_p$
denote the non-connective p-completed Adams summand. The
$E_1$
$L_p$
-algebra
is an étale
$E_1$
$L_p$
-algebra in the sense of Hesselholt and Pstragowski [Reference Hesselholt and PstragowskiHP25], and there is an isomorphism of
$\pi_* (L_p)$
-algebras
It follows by [Reference Hesselholt and PstragowskiHP25, Theorem 1.10] that there is an equivalence of
$L_p$
-algebras
Through this,
$\ell_p(\!\sqrt[p-1]{v_1})$
serves as the connective cover of
$KU_p$
in
$E_1$
$\ell_p$
-algebras. Hence, there is an equivalence of
$E_1$
$\ell_p$
-algebras
$ku_p \simeq \ell_p(\!\sqrt[p-1]{v_1})$
.
In Theorem 9.3, we show that the Morava E-theory spectrum
$E_n$
is given by
$\mathbb{S}_{W(\mathbb{F}_{p^n})} \wedge_{\mathbb{S}_{p}} \widehat{E(n)}(\!\sqrt[p^n-1]{v_n})$
as an
$E_1$
-ring, where
$\widehat{E(n)}$
is the K(n)-localized Johnson–Wilson spectrum.
Remark 4.7. In certain cases, it is possible to equip
$A(\!\sqrt[m]{a})$
with the structure of an
$E_n$
-algebra for
$n\gt 1$
. For this, one may use the graded
$E_\infty$
MU-algebra
$MU[\sigma_k]$
[Reference Hahn and WilsonHW22, Construction 2.6.1], where
$k\gt 0$
is even. Indeed,
$MU[\sigma_k]$
is the free graded
$E_1$
MU-algebra over
$\Sigma^kMU$
. There is a map of graded
$E_\infty$
-rings
and Proposition 3.13 provides maps
$\mathbb{S}[\sigma_k] \to MU[\sigma_k]$
of graded
$E_2$
-rings.
It follows by [Reference Hahn and WilsonHW22, Remark 2.1.2] that a form of
$BP \langle n \rangle$
admits the structure of an
$E_3$
$MU[\sigma_{2(p^n-1)}$
]-algebra, where
$\sigma_{2(p^n-1)}$
acts through
$v_n \in \pi_* BP \langle n \rangle$
. We obtain an equivalence of
$p^n-1$
-graded
$E_1$
$\mathbb{S}[\sigma_2]$
-algebras
This equips
$BP \langle n \rangle(\!\sqrt[p^n-1]{v_n})$
with the structure of a
$p^n-1$
-graded
$E_3$
$MU[\sigma_2]$
-algebra.
4.3 The weight-0 piece of THH
Here, we prove our first result regarding the THH of the ring spectra obtained via root adjunction. Namely, we show that
$\operatorname{THH}(A(\!\sqrt[m]{a}))$
contains
$\operatorname{THH}(A)$
as a summand whenever A is p-local and
$p \nmid m$
.
It follows by [Reference Antieau, Mathew, Morrow and NikolausAMM+22, Example A.10] that for an m-graded
$E_1$
-ring Y, the m-grading on
$\operatorname{THH}(Y)$
is obtained by applying the cyclic bar construction
$b_\bullet(Y)$
of Y in the
$\infty$
-category of m-graded spectra. In simplicial level s and weight i, the m-graded cyclic bar construction of Y is given by the following:
Owing to [Reference Antieau, Mathew, Morrow and NikolausAMM+22, Corollary A.15], we have the following equality:
where the functor
$D(-)$
provides the underlying spectrum as usual; we often omit D in our notation. Furthermore,
$\operatorname{THH}(Y)$
is an
$S^1$
-equivariant m-graded spectrum in a canonical way and the equivalence above is an equivalence of
$S^1$
-equivariant spectra.
Construction 4.8. Let R be an
$E_2$
-ring and S an
$E_1$
R-algebra. For us, this will mean that the pair
$(R,S) \in \operatorname{RMod}^{(2)}(\operatorname{Sp})$
, where
for an arbitrary symmetric monoidal
$\infty$
-category
$\mathcal{C}$
. Here,
$\operatorname{RMod}(\mathcal{C})$
is the
$\infty$
-category of pairs (A,M), where A is an
$E_1$
-algebra and
$M \in \operatorname{RMod}_A(\mathcal{C})$
. Thus, objects in
$\operatorname{RMod}^{(2)}(\mathcal{C})$
may be identified with pairs (A,M), where A is an
$E_2$
-algebra and M is an
$E_1$
A-algebra in
$\mathcal{C}$
.
We remark that, in general,
$\operatorname{RMod}^{(2)}(\mathcal{C})$
may be written as
$\operatorname{Alg}_{\mathcal{O}}(\mathcal{C})$
, where
$\mathcal{O}$
is the tensor product of operads
This tensor product of operads, studied in depth in [Reference LurieLur17, 2.2.5], is symmetric and satisfies the following universal property at the level of algebra objects:
Hence, applying the discussion to
$\mathcal{C} = \operatorname{Sp} $
and R and S as above, we may view S as a right R-module in
$E_1$
-algebras.
Since
$\operatorname{THH}$
is a symmetric monoidal functor from
$E_1$
-rings to spectra [Reference Nikolaus and ScholzeNS18, § IV.2], we deduce that
$\operatorname{THH}(S)$
is a right
$\operatorname{THH}(R)$
-module.
Proposition 4.9.
Let F be an m-graded
$E_1$
E-algebra and
$E\to F'$
a map of m-graded
$E_2$
-rings. There is a natural equivalence of m-graded right
$\operatorname{THH}(F')$
-modules in
$S^1$
-equivariant spectra,
whose underlying ungraded equivalence is that of right
$\operatorname{THH}(F')$
-modules in cyclotomic spectra. If E and F are concentrated in weight 0, then we have the following:
Proof. Let us recall that the functor
is symmetric monoidal. Furthermore, it commutes with sifted colimits; indeed, this can be seen from the fact that it can be decomposed into a composition of functors comprised of taking tensor products and realizations of simplicial objects, both of which commute with sifted colimits. Thus, there will be a natural equivalence
\begin{align*} \operatorname{THH}(F \wedge_{E} F') &\simeq \operatorname{THH}( ||\operatorname{Bar}_\bullet(F,E,F')||) \\ &\simeq ||\operatorname{Bar}_{\bullet}(\operatorname{THH}(F)_\bullet, \operatorname{THH}(E)_\bullet, \operatorname{THH}(F')_\bullet)|| \\ &\simeq \operatorname{THH}(F) \wedge_{\operatorname{THH}(E)}\operatorname{THH}(F').\end{align*}
This allows us to deduce that
$\operatorname{THH}$
preserves the sifted colimit given by the double-sided bar construction; this can be computed at the level of underlying spectra by the bilinear pairing
corresponding to the relative tensor product. Furthermore, as
$\operatorname{THH}$
preserves the sifted colimits corresponding to this relative tensor product, the above equivalence is compatible with right
$\operatorname{THH}(F')$
module structures. The analogous claims all hold when accounting for additional gradings, by recalling that
$\operatorname{THH}$
promotes to a sifted colimit preserving symmetric monoidal functor from algebras in graded spectra to
$S^1$
-equivariant objects in graded spectra. In particular, if E and F are concentrated in weight 0, we deduce the equivalence
of graded
$\operatorname{THH}(F)$
-modules.
Remark 4.10. The
$m=1$
case of the proposition above provides the non-graded case.
One may consider
$\mathbb{S}[\sigma_k]$
as an
$E_1$
-ring obtained by adjoining an m-root to
$\mathbb{S}[\sigma_{mk}]$
. Proposition 4.12 identifies the weight-0 piece of
$\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_k])$
. Before Proposition 4.12, we state and prove a well-known fact.
Lemma 4.11.
Let
$\varphi \colon M \to N$
be a map between bounded-below spectra. Then
$\varphi$
is an equivalence if and only if
$H\mathbb{Z} \wedge \varphi$
is an equivalence. If, furthermore, M and N are p-local, then
$\varphi$
is an equivalence if and only if
$H\mathbb{Z}_{(p)} \wedge \varphi$
is an equivalence.
Proof. Let K be the fiber of
$\varphi$
and let i be the smallest i such that
$\pi_iK \neq 0$
. Owing to the Tor spectral sequence of [Reference Elmendorf, Kriz, Mandell and MayEKM+97, Theorem .4.1], we have
$\pi_i (H\mathbb{Z} \wedge K)= \pi_iK$
. Therefore, if
$H\mathbb{Z} \wedge K \simeq 0$
, then
$K \simeq 0$
and
$\varphi$
is an equivalence.
If M and N are p-local, then
$\varphi$
is an equivalence if and only if
$\mathbb{S}_{(p)} \wedge \varphi$
is an equivalence. It follows by the previous result that
$\varphi$
is an equivalence if and only if
$H\mathbb{Z} \wedge \mathbb{S}_{(p)} \wedge \varphi \simeq H\mathbb{Z}_{(p)} \wedge \varphi$
is an equivalence.
For the following, let
$k\geq0$
be even and let
$m\gt 1$
. Furthermore, fix a map of m-graded
$E_2$
-rings
$\mathbb{S}_{(p)}[\sigma_{mk}] \to \mathbb{S}_{(p)}[\sigma_k]$
provided by Proposition 3.5 (Remark 3.6 for
$k=0$
).
Proposition 4.12.
In the situation above, assume that
$p \nmid m$
. The induced map
is an equivalence of
$E_1$
-rings. Since
$\mathbb{S}_{(p)}[\sigma_{mk}]$
is concentrated in weight 0, we obtain the following chain of equivalences:
of
$E_1$
-rings using Lemma 2.3.
Proof. It suffices to prove that the map
is an equivalence; see Lemma 4.11.
By the base-change formula for THH, this is equivalent to the following map,
being an equivalence in weight 0. Here,
$H\mathbb{Z}_{(p)}[\sigma_{k}]$
denotes the free
$H\mathbb{Z}_{(p)}$
-algebra on
$\mathbb{S}_{(p)}^k$
given by
$H\mathbb{Z}_{(p)} \wedge \mathbb{S}_{(p)}[\sigma_k]$
.
The map
$H\mathbb{Z}_{(p)}[\sigma_{mk}] \to H\mathbb{Z}_{(p)}[\sigma_{k}]$
induces a map
from the Bökstedt spectral sequence computing
$\operatorname{THH}^{H\mathbb{Z}_{(p)}}(H\mathbb{Z}_{(p)}[\sigma_{mk}])$
to the Bökstedt spectral sequence computing
$\operatorname{THH}^{H\mathbb{Z}_{(p)}}(H\mathbb{Z}_{(p)}[\sigma_{k}])$
. Since the weight grading on the THH of an m-graded ring spectrum comes from a weight grading on the corresponding cyclic bar construction, the Bökstedt spectral sequence computing THH of an m-graded ring spectrum admits an m-grading, i.e. it splits into m summands in a canonical way. Therefore, in our situation, it is sufficient to show that
$\phi^2$
is an isomorphism on weight 0.
We have
where d denotes the Connes operator. The degrees of the classes above are given by the following:
Furthermore,
$\sigma_{mk}$
and
$d(\sigma_{mk})$
are in weight 0 and
$\sigma_k$
and
$d(\sigma_k)$
are in weight 1. In particular, all of
$E^2$
is weight 0 and the weight-0 piece of
$F^2$
is the
$\mathbb{Z}_{(p)}$
-module generated by the classes
$\sigma_k^{im}$
and
$\sigma_k^{(i+1)m-1}d(\sigma_k)$
over
$i \geq 0$
.
Since
$\phi^2(\sigma_{mk}) = \sigma_k^{m}$
, we obtain that
Therefore, we have
Since
$p\nmid m$
, we have that m is a unit. Using this, one observes that
$\phi^2$
is an isomorphism after restricting and corestricting to weight 0 as desired.
In the situation of Hypothesis 4.1,
$A \to A(\!\sqrt[m]{a})$
is a map of m-graded
$E_1$
-rings and A is concentrated in weight 0. Therefore, there is a map
where A above denotes the underlying
$E_1$
-ring of A. This map is
$S^1$
-equivariant since it is the restriction of the
$S^1$
-equivariant m-graded map
$\operatorname{THH}(A) \to \operatorname{THH}(A(\!\sqrt[m]{a}))$
along
$0 \to \mathbb{Z}/m$
as
$\operatorname{THH}(A)$
is concentrated in weight 0.
Theorem 4.13.
Assume Hypothesis 4.1 and that A is p-local and
$p\nmid m$
. Then (4.7) is an equivalence.
Proof. Recall that
$A(\!\sqrt[m]{a})$
is given by
where A and
$\mathbb{S}_{(p)}[\sigma_{mk}]$
are concentrated in weight 0. Owing to Proposition 4.9, we have
and it follows by Proposition 4.12 that the map
is an equivalence. This identifies
$\operatorname{THH}(A(\!\sqrt[m]{a}))_0$
with
$\operatorname{THH}(A)$
as desired.
Remark 4.14. It should be possible to relax the hypothesis on A that it is p-local by assuming that m is invertible in
$\pi_0A$
. Our results assuming A is p-local and
$p \nmid m$
should be true under this weaker assumption as well, but we do not pursue this here. We would like to thank the anonymous referee for pointing this out.
5. Adjoining roots and algebraic K-theory
We now prove Theorem 1.1 from the introduction. For the rest of this section, assume Hypothesis 4.1. We established that
$A(\!\sqrt[m]{a})$
is an m-graded ring spectrum and therefore
$\operatorname{THH}(A(\!\sqrt[m]{a}))$
is an
$S^1$
-equivariant m-graded spectrum; see (4.5). One might define
${{\operatorname{TC}^{-}}}(A(\!\sqrt[m]{a}))$
as an m-graded spectrum given by
Since m is finite, the underlying spectrum of an m-graded spectrum, provided by the functor D, is given by a finite coproduct which is equivalent to the corresponding finite product. In particular, D commutes with all limits and colimits. Because of this, we have
and, therefore, we often omit D in our notation.
Similarly,
$\operatorname{TP}(A(\!\sqrt[m]{a}))$
and
$(\operatorname{THH}(A(\!\sqrt[m]{a}))^{tC_p})^{hS^1}$
admit the structure of m-graded spectra and these constructions commute with the functor D as above. Combining this with Theorem 4.13, we obtain the following result.
Theorem 5.1.
Assume Hypothesis 4.1, that A is p-local and
$p\nmid m$
. The maps
\begin{align*} {{\operatorname{TC}^{-}}}(A) &\xrightarrow{\simeq} {{\operatorname{TC}^{-}}}(A(\!\sqrt[m]{a}))_0,\\ \operatorname{TP}(A) &\xrightarrow{\simeq} \operatorname{TP}(A(\!\sqrt[m]{a}))_0,\\ (\operatorname{THH}(A)^{tC_p})^{hS^1} &\xrightarrow{\simeq} ((\operatorname{THH}(A(\!\sqrt[m]{a}))^{tC_p})^{hS^1})_0 \end{align*}
induced by
$A \to A(\!\sqrt[m]{a})$
are all equivalences.
When A is connective and p-local,
$A(\!\sqrt[m]{a})$
is also connective and p-local. By [Reference Nikolaus and ScholzeNS18, Corollary 1.5] (and the discussion afterwards), the topological cyclic homology of
$A(\!\sqrt[m]{a})$
is defined via the following fiber sequence:
As mentioned previously, the middle term and the third term above admit canonical splittings into m-cofactors. Furthermore, can respects this splitting since it only depends on the
$S^1$
-equivariant structure of
$\operatorname{THH}(A(\!\sqrt[m]{a}))$
.
However,
$\operatorname{TC}(A(\!\sqrt[m]{a}))$
do not necessarily split into m-cofactors. This is due to the fact that the Frobenius map does not necessarily respect the grading. Indeed, the Frobenius is given by maps
see [Reference Antieau, Mathew, Morrow and NikolausAMM+22, Corollary A.9]. On the other hand, we obtain the following splitting of
$\operatorname{TC}(A(\!\sqrt[m]{a}))$
.
Construction 5.2. Assume Hypothesis 4.1 and that A is connective and p-local where
$p \nmid m$
. In this situation, p is a non-zero divisor in
$\mathbb{Z}/m$
. Therefore, the Frobenius map on
$\operatorname{THH}(A(\!\sqrt[m]{a}))$
carries pieces of non-zero weight to non-zero weight pieces. Moreover,
$\varphi_p$
carries zero weight to zero weight. Therefore, the map
$\varphi_p -can$
splits as a coproduct of their restriction to zero weight and their restriction to non-zero weight. In particular, the fiber sequence in (5.1) admits a splitting as follows:
\begin{multline*}\operatorname{TC}(A(\!\sqrt[m]{a}))_0 \vee \operatorname{TC}(A(\!\sqrt[m]{a}))_1 \to \operatorname{THH}(A(\!\sqrt[m]{a}))_0^{hS^1}\vee\operatorname{THH}(A(\!\sqrt[m]{a}))_{\gt 0}^{hS^1} \\ \xrightarrow{(\varphi_p)_0 -can_0 \vee (\varphi_p)_{\gt 0} - can_{\gt 0}} (\operatorname{THH}(A(\!\sqrt[m]{a}))_0^{tC_p})^{hS^1} \vee (\operatorname{THH}(A(\!\sqrt[m]{a}))^{tC_p})_{\gt 0}^{hS^1}.\end{multline*}
Here,
$(-)_{\gt 0}$
denotes restriction to
$\rm{weight}\neq0$
. We have
where
$\operatorname{TC}(A(\!\sqrt[m]{a}))_0$
denotes the fiber of the map
$(\varphi_p)_0 - can_0$
and
$\operatorname{TC}(A(\!\sqrt[m]{a}))_1$
denotes the fiber of the map
$(\varphi_p)_{\gt 0} - can_{\gt 0}$
.
Remark 5.3. There are interesting cases where one obtains further splittings of the topological cyclic homology spectrum
$\operatorname{TC}(A(\!\sqrt[m]{a}))$
. For instance, if
$p =1$
in
$\mathbb{Z}/m$
, one obtains that
$\operatorname{TC}(A(\!\sqrt[m]{a}))$
splits into m-summands. This happens to be the case when
$m=p-1$
or when p is odd and
$m=2$
. We exploit this in Construction 7.3 to obtain a splitting of
$\operatorname{TC}(ku_p)$
into
$p-1$
summands. Moreover, if
$m = p^n-1$
, then one obtains an underlying
$p-1$
-grading of
$\operatorname{THH}(A(\!\sqrt[m]{a}))$
by Kan extending through
$\mathbb{Z}/(p^n-1) \to \mathbb{Z}/(p-1)$
. This provides a
$p-1$
-grading for
$\operatorname{TC}(A(\!\sqrt[m]{a}))$
.
Theorem 5.4.
Assume Hypothesis 4.1 with
$p\nmid m$
and that A is p-local and connective. Under the equivalence (5.2), the canonical map
is equivalent to the inclusion of the first wedge summand.
Proof. Since A is concentrated in weight 0, the map
$\operatorname{TC}(A) \to \operatorname{TC}(A(\!\sqrt[m]{a}))$
factors through the map
induced by the canonical map
$\operatorname{THH}(A) \to \operatorname{THH}(A(\!\sqrt[m]{a}))_0$
. The map
$\operatorname{THH}(A) \to \operatorname{THH}(A(\!\sqrt[m]{a}))_0$
of cyclotomic spectra is an equivalence due to Theorem 4.13. Considering the construction of
$\operatorname{TC}(A(\!\sqrt[m]{a}))_0$
, one observes that this equivalence induces an equivalence between the fiber sequences defining
$\operatorname{TC}(A)$
and
$\operatorname{TC}(A(\!\sqrt[m]{a}))_0$
. In other words, (5.3) is an equivalence as desired.
Finally, we obtain the desired splitting for
$K(A(\!\sqrt[m]{a}))$
.
Theorem 5.5 (Theorem 1.1). Assume Hypothesis 4.1 with
$p\nmid m$
and
$k\gt 0$
. Furthermore, assume that A is p-local and connective. In this situation, the following map:
is the inclusion of a wedge summand.
Proof. Since
$\lvert a \rvert = mk$
and
$k\gt 0$
, we have
We start by constructing a map of m-graded
$E_1$
-algebras
that induces an isomorphism on
$\pi_0$
, where
$H\pi_0A$
is concentrated in weight 0. Weight-0 Postnikov truncation [Reference Hahn and WilsonHW22, Lemma B.0.6] provides a map of graded
$E_2$
-rings
$\mathbb{S}[\sigma_k] \to \mathbb{S}$
that we consider as a map of m-graded
$E_2$
-rings by left Kan extending through
$\mathbb{Z}\to\mathbb{Z}/m$
.
This provides a map of m-graded
$E_1$
-rings
(see (4.3)), where the right-hand side is concentrated in weight 0. Postcomposing with the ordinary Postnikov truncation, we obtain (5.5).
Owing to the Dundas–Goodwillie–McCarthy theorem [Reference Dundas, Goodwillie and McCarthyDGM13], there is the following pullback square provided by the map (5.5).

The equivalence in the upper-right corner follows by Construction 5.2 and Theorem 5.4.
The map
$A(\!\sqrt[m]{a}) \to H\pi_0A$
induces a map of m-graded spectra
Since
$H\pi_0A$
is concentrated in weight 0,
$\operatorname{THH}(H\pi_0A)$
is also concentrated in weight 0. Therefore, the map f is trivial on
$\operatorname{THH}(A(\!\sqrt[m]{a}))_{\gt 0}$
. This shows that the right vertical map above induces the trivial map on
$\operatorname{TC}(A(\!\sqrt[m]{a}))_1$
. Using this, we obtain that the pullback square above splits as a coproduct of the following pullback squares.

By the naturality of the pullback squares provided by the Dundas–Goodwillie–McCarthy theorem and Theorem 5.4, we see that the inclusion of the first cofactor in the coproduct of pullback squares above is indeed induced by the map
$A\to A(\!\sqrt[m]{a})$
. This shows that
as desired, where the inclusion of the first cofactor above is given by
$K(A) \to K(A(\!\sqrt[m]{a}))$
.
Using the purity theorem for algebraic K-theory, we obtain the following for non-connective A.
Corollary 5.6.
Assume Hypothesis 4.1 with
$p\nmid m$
and
$k\gt 0$
. If A is p-local, then the map
is the inclusion of a wedge summand for every
$i\geq 2$
. In particular, if A is of height larger than 0 and A satisfies the redshift conjecture, then
$A(\!\sqrt[m]{a})$
also satisfies the redshift conjecture.
Proof. Let cA denote the connective cover of A in
$\mathbb{S}[\sigma_{mk}]$
-algebras. We consider the following commuting diagram of m-graded
$E_1$
-rings.

Every spectrum with bounded-above homotopy is T(i)-locally trivial for every
$i\geq1$
. Taking fibers, one obtains that the horizontal arrows above are T(i)-equivalence for every
$i\geq1$
; see (4.4).
It follows by [Reference Land, Mathew, Meier and TammeLMM+24, Corollary E] that the horizontal maps above induce T(i)-equivalences in algebraic K-theory for every
$i\geq 2$
. The result follows by applying Theorem 5.5 to the left vertical map.
6. A variant of logarithmic THH
Here, we introduce our definition of log THH and identify
$\operatorname{THH}(A(\!\sqrt[m]{a}))$
using
$\operatorname{THH}(A)$
and log THH of A whenever A is p-local and
$p \nmid m$
. Through our definition, log THH admits a canonical structure of a cyclotomic spectrum; in upcoming work, Devalapurkar and the third author develop a very general notion of logarithmic structures for
$E_2$
-algebras and a corresponding theory of log THH which subsumes the definition we use here. In particular, this will recover the variant due to Rognes, which is defined by way of the replete bar construction; cf. [Reference RognesRog09, Reference Rognes, Sagave and SchlichtkrullRSS15]
Our definition of log THH starts with a definition of log THH of the free algebra
$\mathbb{S}[\sigma_k]$
, where
$k\geq0$
is even as before. We consider
$\sigma_k$
to be in weight 1.
For a graded
$E_n$
-ring spectrum E, we denote the weight connective cover of E by
$E_{\geq 0}$
. Indeed, the weight connective cover is obtained by restricting and then left Kan extending through the inclusion
$\mathbb{N} \to \mathbb{Z}$
. The counit of this adjunction provides a map
$E_{\geq 0}\to E$
of graded
$E_n$
-algebras.
Construction 6.1. Analogous to Construction 3.3, let
$\mathbb{S}[\sigma_k^{{\pm 1}}]:= \operatorname{sh}^k(\mathbb{S}[t^{\pm 1}])$
. The graded
$E_\infty$
-map
$\mathbb{S}[t] \to \mathbb{S}[t^{\pm 1}]$
provides a graded
$E_2$
-map
$\mathbb{S}[\sigma_k] \to \mathbb{S}[\sigma_k^{\pm 1}]$
. Furthermore, by the definition of the shearing functor,
$\mathbb{S}[\sigma_k^{\pm 1}]$
is indeed given by
$\phi^k$
of Variant 3.2; in particular,
$\mathbb{S}[\sigma_{mk}^{\pm 1}]$
is the restriction of
$\mathbb{S}[\sigma_k^{\pm 1}]$
along
$\mathbb{Z} \xrightarrow{\cdot m} \mathbb{Z}$
. Applying the adjunction
$L_m \dashv R_m$
induced by
$\cdot m$
to the map
$\mathbb{S}[\sigma_{mk}] \to \mathbb{S}[\sigma_k]$
, one observes that
$\mathbb{S}[\sigma_{mk}]$
is also the restriction of
$\mathbb{S}[\sigma_k]$
along
$\cdot m$
. Therefore, the counit of
$L_m \dashv R_m$
provides a commutative diagram of graded
$E_2$
-rings.

Remark 6.2. One may also take weight connective covers in the
$\infty$
-category of graded
$S^1$
-equivariant spectra by using the left Kan extension/restriction adjunction induced by
$\mathbb{N}^{ds} \to \mathbb{Z}$
. This provides a map
of graded
$E_1$
-algebras in
$S^1$
-equivariant spectra factoring the map
$ \operatorname{THH}(\mathbb{S}[\sigma_k]) \to \operatorname{THH}(\mathbb{S}[\sigma_k^{\pm 1}])$
.
The following is analogous to the description of the replete bar construction of commutative
$\mathcal{J}$
-space monoids generated by a single element; cf. [Reference RognesRog09, Proposition 3.21], [Reference Sagave and SchlichtkrullSS19, § 8.5] and [Reference Rognes, Sagave and SchlichtkrullRSS15, §§ 6 and 7].
Definition 6.3. Let
$k \geq 0$
be even. The log THH of
$\mathbb{S}[\sigma_k]$
with respect to
$\sigma_k \in \pi_k \mathbb{S}[\sigma_k]$
is the weight connective cover of the THH of
$\mathbb{S}[{\sigma_k}^{{\pm 1}}]$
. In other words, it is the
$S^1$
-equivariant
$E_1$
-algebra
Similarly, the p-local counterpart is defined as follows:
The following example provides a justification for this definition of log THH by showing that its
$H\mathbb{Z}$
-homology provides what should be the logarithmic Hochschild homology of the free algebra
$\mathbb{Z}[\sigma_k]$
; cf. [Reference Krause and NikolausKN22, Example 10.3].
Example 6.4. Considering
$H\mathbb{Z}$
as a graded
$E_\infty$
-algebra concentrated in weight 0, we deduce that
Therefore,
$H\mathbb{Z}_*\operatorname{THH}(\mathbb{S}[\sigma_k]\mid \sigma_k)$
is given by the weight connective cover of
where
$d \sigma_k$
is of weight 1 and degree
$k+1$
and
$\sigma_k$
is of weight 1 and degree k. The isomorphism above follows by the usual Bökstedt spectral sequence considerations applied together with the Hochschild–Kostant–Rosenberg (HKR) theorem. Taking the weight connective cover of (6.1), we obtain
where
$d\log \sigma_k$
is of weight 0 and homotopical degree 1 and corresponds to
$(d \sigma_k) /\sigma_k$
. Furthermore, the map
carries
$d\sigma_k$
to
$d\sigma_k = \sigma_k d\log \sigma_k$
.
Recall from Construction 4.8 that when A is a
$\mathbb{S}[\sigma_k]$
-algebra,
$\operatorname{THH}(A)$
admits the structure of a right
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-module. We use this structure in the following definition. Recall that Proposition 4.2 provides various cases of interest where the assumptions on A in the following definition are satisfied.
Definition 6.5. Let A be an
$E_1$
$\mathbb{S}[\sigma_k]$
-algebra and assume that the unit map
$\mathbb{S}[\sigma_k] \to A$
carries
$\sigma_k \in \pi_k \mathbb{S}[\sigma_k]$
to
$a \in \pi_k A$
with even
$k \geq 0$
. We define the log THH of A with respect to a as the following
$S^1$
-equivariant spectrum:
If A is assumed to be p-local, we use the following equivalent definition:
The definition of log THH we provide above is analogous to the definitions used in [Reference RognesRog09, Reference Sagave and SchlichtkrullSS19, Reference Rognes, Sagave and SchlichtkrullRSS15].
Remark 6.6. We remark that
$\operatorname{THH}(\mathbb{S}[\sigma_k] \mid \sigma_k)$
should be a cyclotomic spectrum as the Frobenius maps of THH multiply the weight by p and this should provide
$\operatorname{THH}(A \mid a)$
above with the structure of a cyclotomic spectrum. However, since we don’t explicitly need this for our application, displaying this will take us too far afield, and so we leave the details to the future work of Devalapurkar and the third author.
Since the definition of log THH is given by the extension of scalars functor
corresponding to the
$E_1$
-algebra map
$\operatorname{THH}(\mathbb{S}[\sigma_k]) \to \operatorname{THH}(\mathbb{S}[\sigma_k]\mid \sigma_k)$
, we deduce that
$\operatorname{THH}(A \mid a)$
is equipped with the structure of a right
$\operatorname{THH}(\mathbb{S}[\sigma_k] \mid \sigma_k)$
-module. Furthermore, the unit of the adjunction given by the extension of scalars functor above and the corresponding forgetful functor provides a map
of right
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-modules; see (4.3).
Remark 6.7. Using
$MU[\sigma_k]$
mentioned in Remark 4.7, it is possible to equip log THH with the structure of an
$E_n$
-algebra for
$n\gt 0$
in favorable cases. For instance, for the
$E_3$
$MU[\sigma_{2(p^n-1)}]$
-algebra form of
$BP \langle n \rangle$
constructed in [Reference Hahn and WilsonHW22],
$\operatorname{THH}(BP \langle n \rangle \mid v_n)$
admits the structure of an
$E_1$
-ring. Indeed, using the map of
$E_2$
-rings
$\operatorname{THH}(MU[\sigma_{2(p^n-1)}]) \to \operatorname{THH}(BP \langle n \rangle)$
, we obtain an
$E_1$
-ring
equivalent to
$\operatorname{THH}(BP \langle n \rangle \mid v_n)$
. This equivalence follows by the following chain of equivalences:
\begin{align*} &\operatorname{THH}(BP \langle n \rangle) \wedge_{\operatorname{THH}(MU[\sigma_{2(p^n-1)}])} \operatorname{THH}(MU[\sigma_{2(p^n-1)}^{\pm 1}])_{\geq 0} \\ &\quad \simeq \operatorname{THH}(BP \langle n \rangle) \wedge_{\operatorname{THH}(MU) \wedge \operatorname{THH}(\mathbb{S}[\sigma_{2(p^n-1)}])} \operatorname{THH}(MU) \wedge \operatorname{THH}(\mathbb{S}[\sigma_{2(p^n-1)}^{\pm 1}])_{\geq 0} \\ &\quad \simeq \operatorname{THH}(BP \langle n \rangle) \wedge_{\operatorname{THH}(\mathbb{S}[\sigma_{2(p^n-1)}])} \operatorname{THH}(\mathbb{S}[\sigma_{2(p^n-1)}]),\end{align*}
obtained from the equivalence of
$E_2$
MU-algebras
$MU[\sigma_{2(p^n-1)}] \simeq MU \wedge \mathbb{S}[\sigma_{2(p^n-1)}]$
mentioned in Remark 4.7.
Furthermore, Hahn and Yuan [Reference Hahn and YuanHY20, 1.11 and 1.12] show that there is an
$E_\infty$
-map
$MU[\sigma_2]\to ku_p$
for
$p=2$
and claim that their methods provide such a map for odd primes too. In this situation,
$\operatorname{THH}(ku_p \mid u_2)$
is equipped with the structure of an
$E_\infty$
-ring (by arguing as above) where
$u_2$
denotes the Bott element. Note that log THH of
$ku_p$
with respect to
$u_2$
is also constructed as an
$E_\infty$
-ring in [Reference Rognes, Sagave and SchlichtkrullRSS18].
Remark 6.8. In work in progress, Devalapurkar and the second author show that, in a general context, for every
$E_2$
-ring with even homotopy, log THH, as in our definition, may be equipped with a canonical
$E_1$
-algebra structure in cyclotomic spectra.
To study the log THH of
$E_1$
-rings obtained via root adjunctions, we use the following constructions.
Construction 6.9. Using Construction 6.1 and the weight connective cover adjunction mentioned in Remark 6.2, we obtain the following commuting diagram of graded
$E_1$
-algebras.

Construction 6.10. Assume Hypothesis 4.1. By Proposition 4.9, there is an equivalence
This equips
$\operatorname{THH}(A(\!\sqrt[m]{a}))$
with the structure of a right
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-module in m-graded spectra. Considering the map
as a map of m-graded
$E_1$
-ring spectra, Definition 6.5 may be employed at the level of m-graded spectra. This shows that
$\operatorname{THH}(A(\!\sqrt[m]{a}) \mid \sqrt[m]{a})$
admits a canonical structure of a right
$\operatorname{THH}(\mathbb{S}[\sigma_k] \mid \sigma_{k})$
-module in m-graded spectra. Furthermore, the map
$\operatorname{THH}(A(\!\sqrt[m]{a})) \to \operatorname{THH}(A(\!\sqrt[m]{a}) \mid \sqrt[m]{a})$
is a map of m-graded
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-modules.
6.1 Logarithmic THH-étale root adjunctions
Here, our goal is to show that when A is p-local and
$p \nmid m$
, root adjunction is log-THH-étale. In other words, we show that there is an equivalence of m-graded spectra
Remark 6.11. A notion of log-THH-étalenes is already defined in [Reference Rognes, Sagave and SchlichtkrullRSS18]. In the language of Rognes, Sagave and Schlichtkrull [Reference Rognes, Sagave and SchlichtkrullRSS18], log-THH-étaleness of
$A\to A(\!\sqrt[m]{a})$
would be expressed by an equivalence
Since we only assume A to be
$E_1$
,
$\operatorname{THH}(A\mid a)$
may not admit an A-module structure and, therefore, the right-hand side above may not be defined in our generality. On the other hand, if one starts with an
$E_3$
-algebra A with even homotopy, the log THH of A may be given an A-module structure and we obtain that
$A\to A(\!\sqrt[m]{a})$
is log-THH-étale in the sense of (6.4) whenever A is p-local and
$p \nmid m$
.
Proposition 6.12.
For
$k \geq 0$
, the spectra
$\operatorname{THH}(\mathbb{S}[\sigma_k] \mid \sigma_k)$
and
$\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_k] \mid \sigma_k)$
are connective in homotopy.
Proof. This follows by the fact that the weight connective part of the cyclic bar construction on
$\mathbb{S}[\sigma_k^{\pm 1}]$
(
$\mathbb{S}_{(p)}[\sigma_k^{\pm 1}]$
) is connective in homotopy in each simplicial degree.
We start by proving a log-THH-étaleness result for the p-localized free
$E_1$
-algebra
$\mathbb{S}_{(p)}[\sigma_{mk}]$
.
Proposition 6.13.
Let
$k\geq 0$
be even and let
$m\gt 0$
with
$p \nmid m$
. In this situation, there is an equivalence of left
$\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}] \mid \sigma_{mk})$
-modules in m-graded spectra:
where the left
$\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}] \mid \sigma_{mk})$
-module structure on the right-hand side is provided by Construction 6.9.
Proof. We start by constructing the desired map. First, there is a composite map of m-graded
$E_1$
-ring spectra
which is, in particular, a map of left
$\mathbb{S}_{(p)}[\sigma_{mk}]$
-modules in m-graded spectra by forgetting structure through the m-graded
$E_1$
-ring map
$\mathbb{S}_{(p)}[\sigma_{mk}] \to \mathbb{S}_{(p)}[\sigma_k]$
. Using the extension of scalars functor induced by the map
of m-graded
$E_1$
-algebras, we obtain the desired map:
of left
$\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}] \mid \sigma_{mk})$
-modules in m-graded spectra from (6.5). Here, we used the fact that the left
$\mathbb{S}_{(p)}[\sigma_{mk}]$
-module structure on
$\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_k] \mid \sigma_{k})$
used in (6.5) is compatible with the one obtained by forgetting the canonical left
$\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}] \mid \sigma_{mk})$
-module structure on
$\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_k] \mid \sigma_{k})$
through (6.6); this follows by the p-local version of (6.3).
What remains is to show that f is an equivalence. Since f is a map between p-local connective spectra (Proposition 6.12), it is sufficient to show that
$H\mathbb{Z}_{(p)} \wedge f$
is an equivalence; see Lemma 4.11.
By inspection on the two-sided bar construction defining relative smash products, one obtains that
\begin{align*}& H\mathbb{Z}_{(p)} \wedge \operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}] \mid \sigma_{mk}) \wedge_{\mathbb{S}_{(p)}[\sigma_{mk}]} \mathbb{S}_{(p)}[\sigma_k] \\&\quad \simeq (H\mathbb{Z}_{(p)} \wedge \operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}] \mid \sigma_{mk}) ) \wedge_{H\mathbb{Z}_{(p)}[\sigma_{mk}]} H\mathbb{Z}_{(p)}[\sigma_{k}].\end{align*}
Using the base-change formula for THH, we obtain that
$H\mathbb{Z}_{(p)} \wedge f$
is given by the canonical map
To prove that
$H\mathbb{Z}_{(p)} \wedge f$
is an equivalence, we argue as in the proof of Proposition 4.12. The map of Bökstedt spectral sequences computing the map
is given on the second page, due to the HKR theorem, by the ring map
satisfying
where m is a unit as
$p \nmid m$
. In particular,
Here,
$\sigma_{mk}$
and
$\sigma_k$
are in degrees (0,mk) and (0,k), respectively, and
$d(\sigma_{mk})$
and
$d(\sigma_k)$
are in degrees (1,mk) and (1,k), respectively. Furthermore,
$\sigma_{mk}$
and
$d(\sigma_{mk})$
are of weight m and
$\sigma_k$
and
$d(\sigma_k)$
are of weight 1. In particular, both Bökstedt spectral sequences degenerate on the second page and the map
$\phi$
provides the map (6.7).
Taking connective covers in weight direction and identifying
$\sigma_{mk}^{-1} d(\sigma_{mk})$
as
$d\log \sigma_{mk}$
and
$\sigma_k^{-1} d(\sigma_k)$
as
$d\log \sigma_k$
, we obtain that the map
is given by a map
that carries
$\sigma_{mk}$
to
$\sigma_{k}^m$
and
$d\log \sigma_{mk}$
to
$d\log \sigma_k$
up to a unit due to (6.9) as
$p \nmid m$
.
Upon extending scalars with respect to the map
$\mathbb{Z}_{(p)}[\sigma_{mk}] \to \mathbb{Z}_{(p)}[\sigma_{k}]$
, this map becomes an isomorphism. In other words,
$\pi_*(H\mathbb{Z}_{(p)} \wedge f)$
is an isomorphism and, therefore, f is an equivalence.
The following theorem provides the log-THH-étaleness of root adjunction in ring spectra.
Theorem 6.14.
Assume Hypothesis 4.1 with
$p\nmid m$
and that A is p-local. In this situation, there is an equivalence of m-graded spectra
In other words, as an m-graded spectrum,
$\operatorname{THH}(A(\!\sqrt[m]{a}) \mid \sqrt[m]{a})$
is given by
for every
$0\leq i\lt m$
.
Proof. We have the following chain of equivalences:
\begin{equation*} \begin{split} &\operatorname{THH}(A(\!\sqrt[m]{a}) \mid \sqrt[m]{a}) \simeq \operatorname{THH}(A(\!\sqrt[m]{a})) \wedge_{\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_k])} \operatorname{THH}(\mathbb{S}_{(p)}[\sigma_k] \mid \sigma_k)\\ &\quad\simeq (\operatorname{THH}(A) \wedge_{\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}])}\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_k]) ) \wedge_{\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_k])} \operatorname{THH}(\mathbb{S}_{(p)}[\sigma_k] \mid \sigma_k)\\ &\quad\simeq \operatorname{THH}(A) \wedge_{\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}])} \operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}] \mid \sigma_{mk}) \wedge_{\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}] \mid \sigma_{mk})} \operatorname{THH}(\mathbb{S}_{(p)}[\sigma_k] \mid \sigma_k)\\ &\quad\simeq \operatorname{THH}(A \mid a) \wedge_{\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}] \mid \sigma_{mk})} \operatorname{THH}(\mathbb{S}_{(p)}[\sigma_k] \mid \sigma_k)\\ &\quad\simeq \operatorname{THH}(A \mid a) \wedge_{\operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}]\mid \sigma_{mk})} ( \operatorname{THH}(\mathbb{S}_{(p)}[\sigma_{mk}] \mid \sigma_{mk}) \wedge_{\mathbb{S}_{(p)}[\sigma_{mk}]} \mathbb{S}_{(p)}[\sigma_k] )\\ &\quad\simeq \operatorname{THH}(A\mid a) \wedge_{\mathbb{S}_{(p)}[\sigma_{mk}]} \mathbb{S}_{(p)}[\sigma_k].\\ \end{split}\end{equation*}
The first and fourth equivalences follow by the definition of log THH, the second equivalence follows by our definition of root adjunction and Proposition 4.9 and the fifth equivalence follows by Proposition 6.13.
Remark 6.15. In [Reference Rognes, Sagave and SchlichtkrullRSS18], the authors show that
$\ell \to ku_{(p)}$
is log-THH-étale. This compares to our result above, since we show that
$ku_p \simeq \ell_p(\!\sqrt[p-1]{v_1})$
in Theorem 4.6.
6.2 Relating THH and logarithmic THH
The goal of this section is to show that there is a fiber sequence
under our usual assumptions. The
$E_1$
-ring
$A/a$
above is described in the following construction, which is analogous to [Reference Rognes, Sagave and SchlichtkrullRSS15, Lemmas 6.14 and 6.15].
Construction 6.16. Let A be an
$\mathbb{S}[\sigma_k]$
-algebra where
$\sigma_k$
acts through
$a \in \pi_kA$
, where
$k \geq 0$
is even. The weight-0 Postnikov section of
$\mathbb{S}[\sigma_k]$
provides a map
$\mathbb{S}[\sigma_k] \to \mathbb{S}$
of
$E_2$
-rings [Reference Hahn and WilsonHW22, B.0.6]. Considering the extension of scalars functor
$- \wedge_{\mathbb{S}[\sigma_k]}\mathbb{S}$
from the
$\infty$
-category of
$E_1$
$\mathbb{S}[\sigma_k]$
-algebras to the
$\infty$
-category of
$E_1$
$\mathbb{S}$
-algebras, one equips
with the structure of an
$E_1$
-ring spectrum. Since
$\mathbb{S}$
is the cofiber of the map
$\Sigma^{k}\mathbb{S}[\sigma_k] \xrightarrow{\cdot \sigma_k } \mathbb{S}[\sigma_k]$
,
$A/a$
is indeed the cofiber of the map
$\Sigma^{k} A \xrightarrow{\cdot a} A$
.
Considering
$\mathbb{S}[\sigma_k]$
as a graded
$E_2$
-ring, we have
This can be observed by inspection of the cyclic bar construction on
$\mathbb{S}[\sigma_k]$
or by computing the
$H\mathbb{Z}$
-homology of the left-hand side above. This is used in the statement of the following proposition.
Remark 6.17. The following proposition is analogous to [Reference Rognes, Sagave and SchlichtkrullRSS15, Proposition 6.11]. We remark that, unlike there, we do not take
$S^1$
-equivariance into account, which leads to a simpler proof.
Proposition 6.18. The cofiber of the map
is given by
$\Sigma \mathbb{S}$
concentrated in weight 0 as a left
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-module in graded spectra. Here, the left
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-module structure on
$\mathbb{S}$
is given by the weight-Postnikov truncation map of graded
$E_1$
-rings
Proof. Let M be the cofiber of the map f below in left
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-modules in graded spectra:
We start by computing
$H\mathbb{Z}_*M$
. The map
is given by the ring map
that carries
$\sigma_k$
to
$\sigma_k$
and
$d(\sigma_k)$
to
$\sigma_k d\log \sigma_k$
; this follows by the Böksedt spectral sequences in (4.6) and (6.8). This map is injective and the only class that is not in the image is
$d\log \sigma_k$
. We obtain an equivalence of graded
$H \mathbb{Z}$
-modules
where the right-hand side is concentrated in weight 0.
Since M is connective in homotopy (by Proposition 6.12), we deduce that it is concentrated in weight 0 by the equivalence above. Again, since M is connective, the Tor spectral sequence shows that the lowest-degree non-trivial homotopy group of
$H\mathbb{Z} \wedge M$
is given by the lowest-degree non-trivial homotopy group of M. By this, and (6.10), there is a map of graded spectra
$\Sigma \mathbb{S} \to M$
(with
$\Sigma \mathbb{S}$
placed in weight 0), which when smashed with
$H \mathbb{Z}$
gives the degree-1 class in
$H \mathbb{Z}$
homology. This map
is an equivalence (by Lemma 4.11) because one gets an equivalence after smashing with
$H \mathbb{Z}$
.
We need to improve this to an equivalence of left
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-modules in graded spectra. Since M is a left
$\operatorname{THH}(\mathbb{S}[\sigma_{k}])$
-module in graded spectra, there is a map (by adjunction)
of left
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-modules in graded spectra carrying 1 to 1 in homotopy. Taking weight-0 Postnikov sections [Reference Hahn and WilsonHW22, B.0.6], we obtain an equivalence of left
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-modules in graded spectra
This map is an equivalence because it carries 1 to 1 in homotopy by construction and since both sides are equivalent as spectra to
$\Sigma \mathbb{S}$
.
We are ready to provide the cofiber sequence relating THH to log THH.
Theorem 6.19.
Let A be an
$\mathbb{S}[\sigma_k]$
-algebra where
$\sigma_k$
acts through
$a \in \pi_kA$
with even
$k \geq 0$
. In this situation, there is a cofiber sequence of spectra
The corresponding cofiber sequence for
$\operatorname{THH}(A(\!\sqrt[m]{a}) \mid \sqrt[m]{a})$
is a cofiber sequence of m-graded spectra.
Proof. Proposition 6.18 provides the following cofiber sequence of left
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-modules in graded spectra:
Applying the functor
$\operatorname{THH}(A)\wedge_{\operatorname{THH}(\mathbb{S}[\sigma_k])} -$
to this cofiber sequence, we obtain the following cofiber sequence:
What is left is to identify the cofiber above as
$\operatorname{THH}(A/a)$
. We have
Here,
$\mathbb{S}$
on the right-hand side denotes the de-suspension of
$\Sigma\operatorname{THH}(\mathbb{S}[\sigma_k])_0$
as a left
$\operatorname{THH}(\mathbb{S}[\sigma_k])$
-module in graded spectra; see Proposition 6.18. This is
$\operatorname{THH}(\mathbb{S}[\sigma_k])_0$
, which admits the structure of a graded
$E_1$
-ring spectrum equipped with a map
$\operatorname{THH}(\mathbb{S}[\sigma_k]) \to \operatorname{THH}(\mathbb{S}[\sigma_k])_0$
of graded
$E_1$
-ring spectra given by the relevant weight-0 Postnikov section map. Indeed, owing to the universal property of Postnikov sections, this weight-0 Postnikov section map factors the map of graded
$E_1$
-rings
$\operatorname{THH}(\mathbb{S}[\sigma_k]) \to \operatorname{THH}(\mathbb{S})$
induced by the weight-0 Postnikov section map
$\mathbb{S}[\sigma_k] \to \mathbb{S}$
; i.e. we have a factorization of this map of graded
$E_1$
-algebras as
The second map above is an equivalence as its domain and codomain are equivalent to
$\mathbb{S}$
as spectra and it carries the unit to the unit by construction. In particular, we can replace
$\mathbb{S}$
on the right-hand side of (6.12) with
$\operatorname{THH}(\mathbb{S})$
. This provides the first equivalence below:
\begin{align} \Sigma \operatorname{THH}(A) \wedge_{\operatorname{THH}(\mathbb{S}[\sigma_k])} \mathbb{S} & \simeq \Sigma \operatorname{THH}(A) \wedge_{\operatorname{THH}(\mathbb{S}[\sigma_k])} \operatorname{THH}(\mathbb{S})\nonumber\\ &\simeq \Sigma \operatorname{THH}(A \wedge_{\mathbb{S}[\sigma_k]} \mathbb{S})\nonumber\\ & \simeq \Sigma \operatorname{THH}(A/a).\end{align}
The second equivalence follows by Proposition 4.9 and the third equivalence follows by our description of the
$E_1$
-algebra
$A/a$
in Construction 6.16. Equations (6.12) and (6.13) identify the cofiber in (6.11) as
$\operatorname{THH}(A/a)$
, providing the cofiber sequence claimed in the theorem.
The statement regarding the cofiber sequence in m-graded spectra for
$A(\!\sqrt[m]{a})$
follows by utilizing the same arguments.
Remark 6.20. The above localization sequence is of fundamental importance in the theory of log THH. A proof of the above localization sequence for general
$E_2$
log structures, using more general methods, will be supplied by Devalpurkar and Moulinos (Logarithmic structures for
$E_2$
-algebras, personal communication, 2022).
6.3 THH after root adjunction
Here, we identify
$\operatorname{THH}(A(\!\sqrt[m]{a}))$
in terms of
$\operatorname{THH}(A)$
and
$\operatorname{THH}(A \mid a)$
.
Theorem 6.21 (Theorem 1.3). Assume Hypothesis 4.1 with
$p\nmid m$
and that A is p-local. In this situation, the m-graded spectrum
$\operatorname{THH}(A(\!\sqrt[m]{a}))$
is given by
and
In particular, there is an equivalence of spectra:
\[\operatorname{THH}(A(\!\sqrt[m]{a})) \simeq \operatorname{THH}(A) \vee \bigg(\bigvee_{0\lt i\lt m}\Sigma^{ik}\operatorname{THH}(A \mid a) \bigg).\]
Proof. The identification of
$\operatorname{THH}(A(\!\sqrt[m]{a}))_0$
is provided by Proposition 4.13. Therefore, it is sufficient to provide the identification of
$\operatorname{THH}(A(\!\sqrt[m]{a}))_i$
for
$i\neq 0$
.
Owing to Theorem 6.14,
Therefore, it is sufficient to show that
whenever
$i \neq 0$
. This follows once we show that the cofiber of the map
of m-graded spectra is concentrated in weight 0. From Theorem 6.19, the cofiber of this map is given by
where
$A(\!\sqrt[m]{a})/\sqrt[m]{a}$
is defined to be
$A(\!\sqrt[m]{a}) \wedge_{\mathbb{S}[\sigma_k]} \mathbb{S}$
. Therefore, we have
Since A,
$\mathbb{S}[\sigma_{mk}]$
and
$\mathbb{S}$
are concentrated in weight 0, we obtain that
$A(\!\sqrt[m]{a})/\sqrt[m]{a}$
and therefore
$\operatorname{THH}(A(\!\sqrt[m]{a})/\sqrt[m]{a})$
are also concentrated in weight 0. This proves that the cofiber of (6.16) is concentrated in weight 0, which proves (6.15), and this, together with (6.14), proves the theorem.
7. Algebraic K-theory of complex and real topological K-theories
Here, we start by showing that
$K(ku_p)$
splits into
$p-1$
non-trivial summands. Afterwards, we show that
$ku_p$
may be constructed from
$ko_p$
via root adjunction. We use this to obtain an explicit description of the V(1)-homotopy of
$K(ko_p)$
from the first author’s computation of
$V(1)_*K(ku_p)$
(see [Reference AusoniAus10]).
7.1 Adams’ splitting result for 2-vector bundles
Recall that
$\pi_* ku_p \cong \mathbb{Z}_p[u]$
and
$\pi_* \ell_p \cong \mathbb{Z}_p[v_1]$
, where
$\lvert u \rvert = 2$
and
$\lvert v_1 \rvert = 2p-2$
. The
$E_\infty$
-map
$\ell_p \to ku_p$
carries
$v_1$
to
$u^{p-1}$
in homotopy. For the rest of this section, we fix a map
$\mathbb{S}[\sigma_{2(p-1)}] \to \ell_p$
of
$E_2$
-algebras carrying
$\sigma_{2(p-1)}$
to
$v_1$
and perform root adjunction using this map. Recall from Theorem 4.6 that there is an equivalence of
$E_1$
$\ell_p$
-algebras
This equips
$ku_p$
with the structure of a
$p-1$
-graded
$E_1$
$\ell_p$
-algebra, which further equips
$\operatorname{THH}(ku_p)$
with the structure of a
$p-1$
-graded
$S^1$
-equivariant spectrum.
Let
$p\gt 3$
be a prime and let V(1) denote the type-2 finite spectrum used in [Reference AusoniAus05]; V(1) is a homotopy ring spectrum.
There is another grading on
$V(1)_*\operatorname{THH}(ku_p)$
that the first author calls the
$\delta$
-grading [Reference AusoniAus05]. The group
$\Delta := \mathbb{Z}/(p-1)$
acts on the
$E_\infty$
-ring
$ku_p$
through Adams operations. Let
$\delta \in \Delta$
be a chosen generator and let
$\alpha \in \mathbb{F}_p^\times$
satisfy
$\pi_* (\mathbb{S}/p \wedge \delta )(u) = \alpha u$
, where
We say
$u^i$
has
$\delta$
-weight i as
$\pi_* (\mathbb{S}/p \wedge\delta)(u^i) = \alpha^i u^i$
. Similarly, one says
$x \in V(1)_*\operatorname{THH}(ku_p)$
has
$\delta$
-weight i if the self map of
$V(1)_*\operatorname{THH}(ku_p)$
induced by
$\delta$
carries x to
$\alpha^ix$
. One defines
$\delta$
-weight in a similar way on other invariants of
$ku_p$
(see [Reference AusoniAus05, Definition 8.2]).
Proposition 7.1.
The group
$V(1)_*\operatorname{THH}(ku_p)_i$
is given by the classes of
$\delta$
-weight i in
$V(1)_* \operatorname{THH}(ku_p)$
.
Proof. Since
$H\mathbb{F}_p \wedge ku_p$
is a
$p-1$
-graded
$E_1$
$H\mathbb{F}_p$
-algebra, there is a
$p-1$
-grading on
${{\text{HH}^{\mathbb{F}_p}_*}}(H{\mathbb{F}_p}_*ku_p)$
. By inspection on the Hochschild complex, one observes that the
$\delta$
-weight grading on
${{\text{HH}^{\mathbb{F}_p}_*}}(H{\mathbb{F}_p}_* ku_p)$
agrees with the weight grading. In particular, the
$\delta$
-weight grading and the weight grading agree on the second page of the Bökstedt spectral sequence computing
${{\text{HH}^{\mathbb{F}_p}}}(H\mathbb{F}_p \wedge ku_p)$
. From [Reference AusoniAus05, Proof of Theorem 9.15], this shows that the
$\delta$
-weight grading and the weight grading agree on
${{\text{HH}_*^{\mathbb{F}_p}}}(H\mathbb{F}_p \wedge ku_p)$
. Furthermore, there is a basis of
${{\text{HH}_*^{\mathbb{F}_p}}}(H\mathbb{F}_p \wedge ku_p)$
as an
$\mathbb{F}_p$
-module where
$\delta$
-weight is defined for each basis element. Therefore, the
$H\mathbb{F}_p$
-module
${{\text{HH}^{H\mathbb{F}_p}}}(H\mathbb{F}_p \wedge ku_p)$
splits as a coproduct of suspensions of
$H\mathbb{F}_p$
in such a way that the map
${{\text{HH}^{H\mathbb{F}_p}}}(H\mathbb{F}_p \wedge \delta)$
is given by the respective multiplication map corresponding to the
$\delta$
-weight on each cofactor. Using this, one observes that the
$\delta$
-weight and the weight grading agree on
$H_*(V(1) \wedge \operatorname{THH}(ku_p);\mathbb{F}_p)$
.
The Hurewicz map
is injective and this map preserves both gradings. From this, we deduce that the weight grading and the
$\delta$
-weight grading agree on
$V(1)_* \operatorname{THH}(ku_p)$
.
In general, THH of m-graded ring spectra may not result in an m-graded cyclotomic spectrum as the Frobenius map does not preserve the grading; it multiplies the grading by p. On the other hand, for
$ku_p$
,
$\operatorname{THH}(ku_p)$
is
$p-1$
-graded and
$p= 1$
in
$\mathbb{Z}/(p-1)$
. In particular, the Frobenius map preserves the grading and one obtains that
$\operatorname{THH}(ku)$
is a
$p-1$
-graded cyclotomic spectrum.
Proposition 7.2.
The
$S^1$
-equivariant structure on
$\operatorname{THH}(ku_p)_i$
lifts to a cyclotomic structure for which there is an equivalence
of cyclotomic spectra.
Proof. The monoid
$\mathbb{Z}/ (p-1)$
satisfies the conditions in [Reference Antieau, Mathew, Morrow and NikolausAMM+22, Lemma A.7] needed to endow
$\operatorname{THH}(ku)$
with an
$L_p$
twisted cyclotomic structure [Reference Antieau, Mathew, Morrow and NikolausAMM+22, Corollary A.9]. However, since
$ p \cong 1 \mod p-1$
, this ends up being the identity functor on
$\mathbb{Z} /(p-1)$
-graded spectra. Thus, one obtains a sequence of
$S^1$
-equivariant maps
for each
$i \in \mathbb{Z} / (p -1)$
, which is precisely the relevant additional piece of structure needed to view this as a cyclotomic object.
Construction 7.3. Here, we construct a splitting of
$K(ku_p)$
using Proposition 7.2. Since the product mentioned in Proposition 7.2 is a finite product, it is at the same time a coproduct. In particular, it commutes with all limits and colimits. Therefore, the fiber sequence defining
$\operatorname{TC}(ku_p)$
splits into a product of fiber sequences
Hence, there is a splitting of
$\operatorname{TC}(ku_p)$
:
where
$\operatorname{TC}(ku_p)_i :=\operatorname{TC}(\operatorname{THH}(ku_p)_i)$
. Arguing as in the proof of Theorem 5.5, one obtains a map
$ku_p \to H\mathbb{Z}_p$
of
$p-1$
-graded
$E_1$
-rings where
$H\mathbb{Z}_p$
is concentrated in weight 0. Therefore, the induced map
$\operatorname{THH}(ku_p) \to \operatorname{THH}(\mathbb{Z}_p)$
of
$p-1$
-graded spectra is trivial in non-zero weight. By inspection on the product splitting of the fiber sequence defining
$\operatorname{TC}(ku_p)$
, we consider
$\operatorname{TC}(ku_p) \to \operatorname{TC}(\mathbb{Z}_p)$
as a map of
$p-1$
-graded spectra, where
$\operatorname{TC}(\mathbb{Z}_p)$
is concentrated in weight 0. Again, as in the proof of Theorem 5.5, this splits the pullback square (from the Dundas–Goodwillie–McCarthy theorem) relating
$\operatorname{TC}(ku_p)$
to
$K(ku_p)$
, resulting in a splitting of
$K(ku_p)$
that we denote by
Here,
$K(ku_p)_0 \simeq K(\ell_p)$
due to Theorem 5.5.
To understand the resulting splitting of
$K(ku_p)$
, we identify the V(1)-homotopy of each weight piece. The computation of
$V(1)_*K(ku_p)$
is due to the first author [Reference AusoniAus10, Theorem 8.1] and these groups are given below:
\begin{align} V(1)_* K(ku_p) &\cong \mathbb{F}_p[b] \otimes \Lambda(\lambda_1,a_1) \oplus \mathbb{F}_p[b] \otimes \mathbb{F}_p \{\partial \lambda_1,\partial b, \partial a_1, \partial \lambda_1 a_1\} \nonumber\\ &\oplus \mathbb{F}_p[b] \otimes \Lambda(a_1) \otimes \mathbb{F}_p \{t^d \lambda_1 \mid 0\lt d\lt p \} \nonumber\\ &\oplus \mathbb{F}_p[b] \otimes \Lambda(\lambda_1) \otimes \mathbb{F}_p \{\sigma_n, \lambda_2 t^{p^2-p} \mid 1 \leq n \leq p-2 \}\nonumber\\ &\oplus \mathbb{F}_p \{s \}.\end{align}
Here,
$\lvert b \rvert = 2p+2$
,
$\lvert \partial \rvert = -1$
,
$\lvert \lambda_1 \rvert = 2p-1$
,
$\lvert a_1 \rvert = 2p+3$
,
$\lvert \sigma_n \rvert = 2n+1$
,
$\lvert t \rvert = -2$
,
$\lvert \lambda_2 \rvert = 2p^2-1$
and
$\lvert s \rvert = 2p-3$
. We assign weights to these classes in a way that turns
$V(1)_*K(ku_p)$
into a
$p-1$
-graded abelian group. The weights of
$\sigma_n$
, b,
$a_1$
,
$ \partial$
,
$\lambda_1$
, t,
$\lambda_2$
and s are given by n, 1, 1, 0, 0, 0, 0 and 0, respectively. Classes denoted by tensor products or products above have the canonical degrees and weights. Furthermore, the isomorphism above is that of
$\mathbb{F}_p[b]$
-modules and
$b^{p-1} = -v_2$
.
Theorem 7.4. For the equivalence of spectra
provided by Construction 7.3, there is an equivalence
and there are isomorphisms
for each
$i \in \mathbb{Z}/(p-1)$
, where the right-hand side denotes the weight-i piece of the
$p-1$
-grading on
$V(1)_* K(ku_p)$
described above.
Proof. The identification of
$K(ku_p)_0$
is given in Construction 7.3. This provides the identification of
$V(1)_* K(ku_p)_0$
as
$(V(1)_*K(ku_p))_0$
, since this is precisely the image of the map
see [Reference AusoniAus05, Theorem 10.2]. The identification of
$V(1)_* (K(ku_p)_i)$
for
$i \neq 0 $
follows by noting, from Proposition 7.1, that it is sufficient to keep track of the contribution of
$\delta$
-weight i classes in
$V(1)_* \operatorname{THH}(ku_p)$
to
$V(1)_* \operatorname{TC}(ku_p)$
. This follows by inspection of [Reference AusoniAus10, §§ 5 and 7].
7.2 Algebraic K-theory of real K-theory
Let
$p\gt 3$
. Using Theorem 5.5, the splitting of
$K(ku_p)$
discussed above and our root adjunction formalism, we obtain a straightforward computation of
$V(1)_*K(ko_p)$
from our knowledge of
$V(1)_* K(ku_p)$
from [Reference AusoniAus10]. Here,
$ko_p$
denotes the connective cover of the p-completed real topological K-theory spectrum
$KO_p$
. We have
$\pi_* KO_p \cong \mathbb{Z}_p[\alpha^{\pm 1}]$
with
$\lvert \alpha \rvert = 4$
.
There is a subgroup
$C_2$
of
$\Delta\cong \mathbb{Z}/(p-1)$
such that
$KO_p \simeq KU_p^{hC_2}$
. Through this, the induced map
$KO_p \to KU_p$
carries
$\alpha$
to
$u^2$
up to a unit that we are going to omit. Since
$L\simeq (KU_p)^{h\Delta}$
, we obtain a sequence of
$E_\infty$
-maps
where the first map carries
$v_1$
to
$\alpha^{{p-1}/{2}}$
in homotopy.
Theorem 7.5
For
$p\gt 3$
, there is an equivalence
of
$E_1$
$\ell_p$
-algebras.
Proof. This follows as in the proof of Theorem 4.6 by noting that
$p \nmid {p-1}/{2}$
.
Furthermore,
$ku_p$
may also be obtained from
$ko_p$
via root adjunction; for this root adjunction, we use the
$\mathbb{S}_{p}[\sigma_4]$
-algebra structure on
$ko_p$
provided by Theorem 7.5. To identify the resulting 2-graded
$E_1$
-ring structure on
$ku_p$
, we use the symmetric monoidal functor
given by left Kan extension through the canonical map
$\mathbb{Z}/(p-1) \to \mathbb{Z}/2$
.
Proposition 7.6.
For
$p\gt 3$
, there is an equivalence
of 2-graded
$E_1$
-algebras, where D’ is defined above and the
$p-1$
-grading on
$ku_p$
is given by Theorem 4.6.
Proof. From Theorem 7.5,
$ko_p$
is an
$\mathbb{S}[\sigma_4]$
-algebra given by
To adjoin a root to
$ko_p$
using this structure, we use the sequence of maps
of 2-graded
$E_2$
-ring spectra, where
$\mathbb{S}[\sigma_{2(p-1)}]$
and
$\mathbb{S}[\sigma_4]$
are concentrated in weight 0 and
$\mathbb{S}[\sigma_2]$
above is given its canonical
$p-1$
-grading so that
$\sigma_2$
in
$D'(\mathbb{S}[\sigma_2])$
lies in weight 1.
We obtain the following equivalences of 2-graded
$E_1$
-rings:
The functor D’ is a left adjoint and it is symmetric monoidal. Therefore, it commutes with the two-sided bar construction defining relative smash products. This provides the second equivalence in the following equivalences of 2-graded
$E_1$
-algebras:
The first equivalence above follows by Theorem 4.6 and the relative smash product in the middle is taken in
$p-1$
-graded spectra. Since
$\ell_p$
and
$\mathbb{S}[\sigma_{2(p-1)}]$
are concentrated in weight 0, the right-hand side above is equivalent to the right-hand side of (7.2); this follows by Lemma 2.3. In other words, (7.2) and (7.3) agree.
Recall that the spectra
$K(ku_p)_i$
are given in Construction 7.3 and the groups
$V(1)_*K(ku_p)_i$
are identified in Theorem 7.4.
Theorem 7.7.
For
$p\gt 3$
, there is an equivalence of spectra
Therefore, we have
and
$V(1)_*K(ko_p)$
, as an abelian group, is given by
\begin{align*} V(1)_* K(ko_p) \cong &\, \mathbb{F}_p[b^2] \otimes \Lambda(\lambda_1,ba_1) \oplus \mathbb{F}_p[b^2] \otimes \mathbb{F}_p \{\partial \lambda_1,b\partial b, b\partial a_1, b\partial \lambda_1 a_1\} \\ &\oplus \mathbb{F}_p[b^2] \otimes \Lambda(ba_1) \otimes \mathbb{F}_p \{t^d \lambda_1 \mid 0\lt d\lt p \} \\ & \oplus \mathbb{F}_p[b^2] \otimes \Lambda(\lambda_1) \otimes \mathbb{F}_p \{b^{\epsilon(n)}\sigma_n, \lambda_2 t^{p^2-p} \mid 1 \leq n \leq p-2 \}\\ &\oplus \mathbb{F}_p \{s \},\end{align*}
where
$\epsilon(n) = 1$
if n is odd and
$\epsilon(n) = 0$
if n is even. Here, the class denoted by
$(b^2)^{(p-1)/2}$
is
$ -v_2$
.
As a consequence, we have an isomorphism of abelian groups
Proof. We start by identifying
$\operatorname{THH}(ko_p)$
as a cyclotomic spectrum. We have the following chain of equivalences:
\begin{align*} \operatorname{THH}(ko_p) &\simeq \operatorname{THH}(ko_p(\!\sqrt[2]{\alpha}))_0 \\ &\simeq \operatorname{THH}(D'(ku_p))_0\\ &\simeq (D'(\operatorname{THH}(ku_p)))_0\\ &\simeq \prod_{0 \leq i \lt (p-1)/2} \operatorname{THH}(ku_p)_{2i}. \end{align*}
The first equivalence above follows by Theorem 4.13, the second equivalence follows by Proposition 7.6 and the third equivalence is a consequence of [Reference Antieau, Mathew, Morrow and NikolausAMM+22, Corollary A.15]. The last equivalence above follows by the description of D’ as a left Kan extension; see § 2.2. Indeed, this shows that the following composite map of cyclotomic spectra is an equivalence:
Here, the equivalence in the middle follows by Proposition 7.2. The last map above is the canonical projection.
The composite equivalence of cyclotomic spectra above shows that
\[\operatorname{TC}(\operatorname{THH}(ko_p)) \simeq{\operatorname{TC}}\bigg(\prod_{0\leq i\lt(p-1)/2} \operatorname{THH}(ku_p)_{2i}\bigg) \simeq \prod_{0\leq i\lt(p-1)/2} \operatorname{TC}(ku_p)_{2i}.\]
Considering the Dundas–Goodwillie–McCarthy theorem with respect to the composite
$ko_p\to ku_p \to H\mathbb{Z}_p$
, we obtain that the splitting of the pullback square relating
$K(ku_p)$
with
$\operatorname{TC}(ku_p)$
(mentioned in Construction 7.3) provides a splitting for
$K(ko_p)$
given by
The first and second statements in the theorem follow from this splitting. The third statement follows by this, and by inspection of (7.1).
For the last statement, note that
$T(2)_*K(ko) \cong T(2)_*K(ko_p)$
due to the purity of algebraic K-theory and [Reference Land, Mathew, Meier and TammeLMM+24, Lemma 2.2 (6)]. It follows, by Theorem 7.4, that the map
carries
$T(2)_*K(ku_p)_0$
to
$T(2)_*K(ku_p)_i$
for
$i\lt p-1$
, where the map above multiplies by
$b^i$
. Using this fact, together with [Reference AusoniAus10, Proposition 1.2 (b)], provides isomorphisms
given by
$\cdot b^i$
for
$i\lt p-1$
. This, together with (7.4), provides the desired identification of
$T(2)_*K(ko)\cong T(2)_*K(ko_p)$
as
$T(2)_* K(\ell_p)[b^2]/((b^2)^{(p-1)/2}+v_2)$
.
8. Root adjunction and Lubin–Tate spectra
Recall that in [Reference Hahn and WilsonHW22], Hahn and Wilson prove that there are
$E_3$
MU-algebra forms of
$BP \langle n \rangle$
. Furthermore, their constructions provide an
$E_3$
$MU[\sigma_{2(p^n-1)}]$
-algebra form of
$BP \langle n \rangle$
, where
$\sigma_{2(p^n-1)}$
acts through
$v_n$
(see [Reference Hahn and WilsonHW22, Remark 2.1.2]).
To relate particular forms of
$BP \langle n \rangle$
to Lubin–Tate spectra, we use the spherical Witt vectors constructed by Lurie [Reference LurieLur18, Example 5.2.7]. For a given discrete perfect
$\mathbb{F}_p$
-algebra
$B_0$
, this provides an
$E_\infty$
-ring
$\mathbb{S}_{W(B_0)}$
that is flat over
$\mathbb{S}$
in the sense of [Reference LurieLur17, Definition 7.2.2.10]. Therefore, it follows by [Reference LurieLur17, Proposition 7.2.2.13] and [Reference MaoMao23, Proposition 2.7] that
for every spectrum F. We would like to thank Jeremy Hahn for showing us the proof of the following proposition.
Proposition 8.1.
Fix an
$E_3$
MU-algebra form of
$BP \langle n \rangle$
. Then
$\mathbb{S}_{W(B_0)} \wedge BP \langle n \rangle$
satisfies the redshift conjecture for every discrete perfect
$\mathbb{F}_p$
-algebra
$B_0$
.
Proof. There is an equivalence of
$E_2$
-algebras in
$S^1$
-equivariant spectra
Therefore, it follows by (8.1) that we have
and this is a polynomial algebra over
$W(B_0)[v_1,\ldots,v_n]$
due to [Reference Hahn and WilsonHW22, Theorem 2.5.4], where one of the generators is denoted by
$\sigma^2v_{n+1}$
. The rest of the argument follows as in the proofs of [Reference Hahn and WilsonHW22, Theorems 2.5.4 and 5.0.1, Corollary 5.0.2] by considering
instead of
$\pi_*(\operatorname{THH}^{MU}(BP \langle n \rangle)^{hS^1})$
.
Namely, we obtain from [Reference Hahn and WilsonHW22, Theorem 2.5.4] that (8.2) is concentrated in even degrees. Therefore, the corresponding homotopy fixed-point spectral sequence degenerates on the second page, providing the
$W(B_0)[v_1,\ldots,v_n]$
-algebra (8.3) as
since (8.2) is polynomial. Using the map from
$\pi_* (\operatorname{THH}^{MU}(BP \langle n \rangle)^{hS^1}\big )$
to (8.3), we deduce from [Reference Hahn and WilsonHW22, Theorem 5.0.1] that
$v_{n+1}$
in (8.3) is represented by the class
$t\sigma^2v_{n+1}$
.
Considering the action of
$v_0,\ldots,v_{n+1}$
on (8.3) described above, one observes that
Using this and the
$E_2$
-map
we deduce that
$L_{T(n+1)}K(\mathbb{S}_{W(B_0)} \wedge BP \langle n \rangle) \not \simeq *$
as desired.
Construction 8.2. Fix an
$E_3$
$MU[\sigma_{2(p^n-1)}]$
-algebra form of
$BP \langle n \rangle$
where
$\sigma_{2(p^n-1)}$
acts through
$v_n$
and let k be a perfect field of characteristic p. Recall that in this situation, degree
$p^n-1$
-root adjunction to
$v_n$
provides a
$p^n-1$
-graded
$E_3$
$MU[\sigma_2]$
-algebra; see Remark 4.7. We consider the
$E_3$
MU-algebra
It follows by [Reference HoveyHov97, Theorem 1.5.4] and [Reference HoveyHov95, Theorem 1.9] that
where
$\lvert u_i \rvert = 0$
and
$\lvert u \rvert = -2$
. Furthermore, the resulting
$E_3$
-map
$MU\to BP \langle n \rangle \to E$
provides a formal group law over
$\pi_* E$
.
For a given perfect
$\mathbb{F}_p$
-algebra
$B_0$
and a height-n formal group law
$\Gamma$
over
$B_0$
, we let
$E_{(B_0,\Gamma)}$
denote the corresponding Lubin–Tate spectrum. By Lurie’s generalization [Reference LurieLur18, § 5] of the Goerss–Hopkins–Miller theorem [Reference RezkRez98, Reference Goerss and HopkinsGH04],
$E_{(B_0,\Gamma)}$
is an
$E_\infty$
-ring.
Proposition 8.3.
In the setting of Construction 8.2, E is equivalent to
$E_{(k,\Gamma)}$
as an
$E_1$
-ring for some height-n formal group law
$\Gamma$
over k.
Proof. By construction, the map
$\pi_* MU_{(p)} \to \pi_* E$
carries
$v_i$
to
$u_iu^{-(p^i-1)}$
for
$0\lt i\lt n$
and
$v_n$
to
$u^{-(p^n-1)}$
. Therefore, the corresponding formal group law on
$\pi_0E$
is the universal deformation of the resulting height-n formal group law
$\Gamma$
over k. This follows by [Reference LurieLur10, Theorem 5 in Lecture 21]. Alternatively, one can directly check the conditions given in [Reference Lubin and TateLT66, Proposition 1.1]. It follows from the Hopkins–Miller theorem that there is an equivalence of
$E_1$
-rings
$E\simeq E_{(k,\Gamma)}$
(see [Reference RezkRez98, Theorem 7.1]).
Burklund et al. are going to use the following example in their construction of a counter-example to the telescope conjecture.
Example 8.4. Let k be a perfect algebraic extension of
$\mathbb{F}_p$
. We know from [Reference RamziRam23, Corollary 4.31] that the
$E_1$
-algebra structure on
$E_{(k,\Gamma)}$
lifts to a unique
$E_d$
-algebra structure for every
$1 \leq d\leq \infty$
. Since E in Construction 8.2 is an
$E_3$
-ring, it follows from Proposition 8.3 that there is an
$E_3$
-equivalence
for
$\Gamma$
as in Proposition 8.3. Through this equivalence, we may equip
$E_{(k,\Gamma)}$
with the structure of an
$E_3$
MU-algebra. In particular, we obtain a map of
$E_3$
MU-algebras
Furthermore,
$E_{(k,\Gamma)}$
is a
$\mathbb{Z}/(p^n-1)$
-graded
$E_3$
$MU[\sigma_2]$
-algebra where the weight-1 class
$\sigma_2$
acts through
$u^{-1}$
.
Theorem 8.5. In the setting of Construction 8.2 and Proposition 8.3, the canonical map
is the inclusion of a non-trivial wedge summand.
Proof. It follows by Corollary 5.6 and Proposition 8.3 that
is the inclusion of a wedge summand. Since
is a
$T(n) \vee T(n+1)$
-equivalence, the result follows by [Reference Land, Mathew, Meier and TammeLMM+24, Purity Theorem].
We finally prove the following theorem.
Theorem 8.6 (Yuan [Reference YuanYua21]). For every perfect
$\mathbb{F}_p$
-algebra
$B_0$
and height-n formal group law
$\Gamma$
over
$B_0$
, the Lubin–Tate spectrum
$E_{(B_0,\Gamma)}$
satisfies the redshift conjecture.
Proof. There is an
$E_\infty$
-map
$E_{(B_0,\Gamma)} \to E_{(k,\Gamma')}$
for some algebraically closed field k of characteristic p and
$\Gamma'$
is the corresponding height-n formal group law on k. Since there is an induced
$E_\infty$
-map
$K(E_{(B_0,\Gamma)}) \to K(E_{(k,\Gamma')})$
, it suffices to prove the redshift conjecture for
$E_{(k,\Gamma')}$
.
Since k is algebraically closed, there is a unique formal group law of height n over k (see [Reference LazardLaz55, Theorem IV]). Using Proposition 8.3, we deduce that
$E_{(k,\Gamma')} \simeq E$
for E as in Construction 8.2. Combining Proposition 8.1 and Theorem 8.5, we obtain that
$E_{(k,\Gamma')}$
satisfies the redshift conjecture as desired.
We remark that it should be possible to prove the redshift conjecture for all
$E_1$
MU-algebra forms of
$BP \langle n \rangle$
by constructing maps
$BP \langle n \rangle \to E_{(k,\Gamma)}$
through root adjunction.
9. Algebraic K-theory and THH of Morava E-theories
In this section, we work with a particular form of Lubin–Tate spectra. This is the Morava E-theory spectrum
$E_n$
, and
$E_n$
is central in the Ausoni–Rognes program for the computation of
$K(\mathbb{S})$
. When we say Morava E-theory
$E_n$
, we mean the Lubin–Tate spectrum corresponding to the height-n Honda formal group. This formal group is characterized by its p-series
and admits a canonical form over
$\mathbb{F}_{p^n}$
, in the sense that all of its endomorphisms are defined over this field. In this section, we prove a splitting result for the algebraic K-theory of the Morava E-theory
$E_n$
and the corresponding two-periodic Morava K-theory. Furthermore, we show that the THH of
$E_n$
may be obtained from the THH of the K(n)-localized Johnson–Wilson spectrum through base change.
9.1 An identification of Morava E-theory
Here, we provide an alternate description of
$E_n$
in terms of its fixed points and spherical Witt vectors. We have
where
$\lvert u_i \rvert = 0$
and
$\lvert u \rvert = -2$
.
Proposition 9.1. The map
obtained via the map
$\pi_* \mathbb{S}_{p} \to \pi_* E_n$
and the canonical
$W(\mathbb{F}_{p^n})$
-module structure on
$\pi_* E_n$
lifts to a map of
$E_\infty$
$\mathbb{S}_{p}$
-algebras
Proof. This is a consequence of Lurie’s theory of thickenings of relatively perfect morphisms [Reference LurieLur18, § 5.2]. Indeed,
$\mathbb{S}_{p} \to \mathbb{S}_{W(\mathbb{F}_{p^n})}$
is an
$\mathbb{S}_{p}$
-thickening of
$H\mathbb{F}_p \to H\mathbb{F}_{p^n}$
in the sense of [Reference LurieLur18, Definition 5.2.1]; see [Reference LurieLur18, Example 5.2.7].
In particular, this implies that the space of
$E_\infty$
$\mathbb{S}_{p}$
-algebra maps from
$\mathbb{S}_{W(\mathbb{F}_{p^n})}$
to the connective cover
$cE_n$
of
$E_n$
is given by the set of
$\mathbb{F}_p$
-algebra maps
where this correspondence is given by the functor
$\pi_0(-)/p$
.
Let
$f \colon \mathbb{S}_{W(\mathbb{F}_{p^n})} \to cE_n$
be the map of
$E_\infty$
$\mathbb{S}_{p}$
-algebras corresponding to the canonical
$\mathbb{F}_p$
-algebra map in (9.1); in particular,
$\pi_0 (f)/p$
is the canonical map in (9.1). We first show that
$\pi_0 f$
is given by the canonical inclusion
Since
$W(\mathbb{F}_p)$
is the ring of integers of the unique unramified extension
$\mathbb{Q}_p[\mu_{p^n-1}]$
of
$\mathbb{Q}_p$
of degree d,
$W(\mathbb{F}_{p^n})$
is generated as a
$\mathbb{Z}_p$
-algebra by a primitive
$p^n-1$
root of the unit. Since the roots of the unit of
$\pi_0 cE_n$
are all in the image of the canonical inclusion
$W(\mathbb{F}_{p^n}) \to W(\mathbb{F}_{p^n})[\lvert u_1,\ldots, u_{n-1} \rvert]$
, one observes that the map
$\pi_0 f$
has to factor through the canonical inclusion
$W(\mathbb{F}_{p^n}) \to W(\mathbb{F}_{p^n})[\lvert u_1,\ldots, u_{n-1} \rvert] $
. Furthermore, there is a unique ring map
$W(\mathbb{F}_{p^n}) \to W(\mathbb{F}_{p^n})$
that lifts the identity map on
$\mathbb{F}_{p^n}$
. This shows that
$\pi_0 f$
is given by the canonical inclusion
$W(\mathbb{F}_{p^n}) \to W(\mathbb{F}_{p^n})[\lvert u_1,\ldots, u_{n-1} \rvert]$
. Since
$\pi_* f$
is a map of
$\pi_* \mathbb{S}_{p}$
-modules, it follows that the composition of f with the map
$c E_n \to E_n$
provides the map claimed in the proposition.
Let Gal denote the Galois group
$\operatorname{Gal}(\mathbb{F}_{p^n},\mathbb{F}_p)$
. From the Goerss–Hopkins–Miller theorem, there is an action of Gal on the
$E_\infty$
-algebra
$E_n$
for which
where the degrees of the generators are as in
$\pi_*E_n$
.
Proposition 9.2.
There is an equivalence of
$E_\infty$
-
$\mathbb{S}_{p}$
-algebras
Proof. This equivalence is given by the following composite map of
$E_\infty$
$\mathbb{S}_{p}$
-algebras:
where the first map is induced by the map provided by Proposition 9.1 and the second map is given by the multiplication map of
$E_n$
. Owing to the flatness of
$\mathbb{S}_{W(\mathbb{F}_{p^n})}$
, this map induces the canonical map
at the level of homotopy groups [Reference LurieLur17, 7.2.2.13]. Since
$W(\mathbb{F}_{p^n})$
is a free
$\mathbb{Z}_p$
-module of finite rank, the functor
$W(\mathbb{F}_{p^n}) \otimes_{\mathbb{Z}_p} - $
is given by taking an n-fold product of
$-$
. In particular, the functor
$W(\mathbb{F}_{p^n}) \otimes_{\mathbb{Z}_p} - $
commutes with completions. This shows that (9.3) is an isomorphism, as desired.
9.2 Algebraic K-theory of Morava E-theories
There is a finite subgroup
$\mathbb{F}_{p^n}^\times$
of the Morava stabilizer group such that
$K = \mathbb{F}_{p^n}^\times \rtimes Gal$
acts on the
$E_\infty$
-algebra
$E_n$
. Furthermore,
where
$\widehat{E(n)}$
denotes the K(n)-localization of the Johnson–Wilson spectrum E(n); see [Reference RognesRog08, 5.4.7]. We have
where I denotes the ideal
$(p,v_1,\ldots,v_{n-1})$
. Since
$\widehat{E(n)}$
is given by
$E_n^{hK}$
, there is a K-equivariant map of
$E_\infty$
-algebras
$\widehat{E(n)} \to E_n$
. In particular, this provides a map
of
$E_\infty$
-algebras. This map carries
$v_n$
to
$u^{-(p^n-1)}$
and
$v_i$
to
$u_i u^{-(p^i-1)}$
for
$0\lt i\lt n$
.
For the following, we fix an
$E_2$
-map
$\mathbb{S}[\sigma_{2(p^n-1)}] \to \widehat{E(n)}$
to adjoin roots. Recall from Remark 4.4 that in this situation,
$\widehat{E(n)}(\!\sqrt[p^n-1]{v_n})$
is an
$\widehat{E(n)}$
-algebra.
Theorem 9.3.
There are equivalences of
$E_1$
$\widehat{E(n)}$
-algebras
\begin{align*} E_n^{\operatorname{hGal}} &\simeq \widehat{E(n)}(\!\sqrt[p^n-1]{v_n}), \\ E_n &\simeq \mathbb{S}_{W(\mathbb{F}_q)} \wedge_{\mathbb{S}_{p}}\widehat{E(n)}(\!\sqrt[p^n-1]{v_n}),\end{align*}
where the class
$u^{-1}$
corresponds to
$\sqrt[p^n-1]{v_n}$
at the level of homotopy groups for both of these equivalences.
In particular,
$E_n^{\operatorname{hGal}}$
and
$E_n$
are
$p^n-1$
-graded
$E_1$
$\widehat{E(n)}$
-algebras with
and
for every
$0\leq i\lt p^n-1$
.
Proof. By the description of
$\pi_* (\widehat{E(n)}) \to \pi_* (E_n^{\operatorname{hGal}})$
given above, this map is an order
$p^n-1$
root adjunction to
$v_n$
followed by a change of variables on
$v_i$
(with
$u_i$
) for
$i\lt n$
. In particular, we have
Furthermore, the map of rings
is a map of étale rings as
$v_n$
and
$p^n-1$
are invertible in
$\pi_* \widehat{E(n)}$
. Through [Reference Hesselholt and PstragowskiHP25, Theorem 1.10], we obtain the first equivalence in the theorem. The second equivalence follows by the first equivalence and Proposition 9.2. The statement on graded ring structures follows by the fact that root adjunction results in m-graded ring spectra; see Construction 4.3.
We are ready to prove our result on the K-theory of Morava E-theories. For this, we use the following composite map:
of
$E_1$
-rings, where the last map above is given by Theorem 9.3. Using Proposition 9.2, we obtain the following composite:
Theorem 9.4. The maps
\begin{align*}K(E(n)) &\to K(E_n^{\operatorname{hGal}}),\\K(\mathbb{S}_{W(\mathbb{F}_{p^n})} \wedge E(n)) &\to K(E_n)\end{align*}
induced by those above are inclusions of wedge summands after
$T(n+1)$
-localization.
Proof. The first map in (9.4) is a
$T(n) \vee T(n+1)$
-equivalence and hence induces a
$T(n+1)$
-equivalence in algebraic K-theory [Reference Land, Mathew, Meier and TammeLMM+24, Purity Theorem]. Therefore, the first equivalence in the theorem follows by applying Corollary 5.6 to
$\widehat{E(n)}(\!\sqrt[p^n-1]{v_n})$
.
Similarly, the first and third maps in (9.5) induce
$T(n+1)$
-equivalences in algebraic K-theory. The second equivalence in the theorem follows by observing that there is an equivalence of
$E_1$
-algebras
and then applying Corollary 5.6.
9.3 Two-periodic Morava K-theories
We obtain analogous results for two-periodic Morava K-theories. Taking a quotient with respect to a regular sequence in
$\pi_* \mathbb{S}_{W(\mathbb{F}_{p^n})} \wedge_{\mathbb{S}_p} \widehat{E(n)}$
, one obtains an
$\widehat{E(n)}$
-algebra K(n) (see [Reference LazarevLaz03, Reference AngeltveitAng08, Reference Hahn and WilsonHW18]). Here, K(n) is the Morava K-theory spectrum with coefficients in
$\mathbb{F}_{p^n}$
. We have
Using the
$\widehat{E(n)}$
-algebra structure on K(n), we adjoin roots and define the two-periodic Morava K-theory as follows:
In this case
where
$\lvert u \rvert = -2$
. Together with Theorem 9.3, this provides the following commuting diagram of
$E_1$
-rings, which justifies our definition of
$K_n$
.

In particular,
$K_n$
is a
$p^n-1$
-graded
$E_1$
-ring in a non-trivial way and we obtain the following from Corollary 5.6.
Theorem 9.5. The map
is the inclusion of a wedge summand after T(i)-localization for every
$i\geq 2$
.
Corollary 9.6.
If K(n) satisfies the redshift conjecture, then so does
$K_n$
.
The V(1)-homotopy of K(k(1)) is computed by Ausoni and Rognes in [Reference Ausoni and RognesAR12] for
$p\gt 3$
. In particular, their computation shows that K(1) satisfies the redshift conjecture. We obtain the following.
Corollary 9.7.
The two-periodic Morava K-theory
$K_1$
of height 1 satisfies the redshift conjecture for
$p\gt 3$
.
9.4 THH descent for Morava E-theories
Theorem 6.19 identifies THH of various periodic ring spectra with their log THH. For instance, the Morava E-theory spectrum
$E_n$
is periodic with unit u in degree
$-2$
. Since
$E_n/(u^{-1}) \simeq 0$
, the canonical map
is an equivalence. Using this, together with our result on log-THH-étaleness of root adjunction, we show that
$\operatorname{THH}(E_n)$
may be obtained from
$\operatorname{THH}(\widehat{E(n)})$
via base change up to p-completion. Such base-change formulas and their relationship with Galois descent problems for THH were studied by Mathew [Reference MathewMat17].
Theorem 9.8. The canonical map
is an equivalence.
Proof. Recall from Theorem 9.3 that there is an equivalence of
$\widehat{E(n)}$
-algebras
Therefore, it follows by Construction 4.3 that
\begin{align} \operatorname{THH}(\widehat{E(n)})\wedge_{\widehat{E(n)}} E_n^{\operatorname{hGal}} &\simeq \operatorname{THH}(\widehat{E(n)})\wedge_{\widehat{E(n)}} \widehat{E(n)} \wedge_{\mathbb{S}_{(p)}[\sigma_{2(p^n-1)}]} \mathbb{S}_{(p)}[\sigma_2] \nonumber\\ &\simeq \operatorname{THH}(\widehat{E(n)}) \wedge_{\mathbb{S}_{(p)}[\sigma_{2(p^n-1)}]} \mathbb{S}_{(p)}[\sigma_2].\end{align}
Since
$v_n$
is a unit in
$\widehat{E(n)}$
and
$u^{-1}$
is a unit in
$E_n^{\operatorname{hGal}}$
, Theorem 6.19 provides the equivalences
Using these equivalences, together with Theorem 6.14, we obtain that the following canonical map is an equivalence:
This, together with (??), provides the desired result.
Theorem 9.9. The canonical map
is an equivalence after p-completion.
Proof. The first equivalence below follows by Proposition 9.2 and the second follows by Theorem 9.8:
\begin{align*} \operatorname{THH}(\widehat{E(n)}) \wedge_{\widehat{E(n)}} E_n &\simeq \operatorname{THH}(\widehat{E(n)})\wedge_{\widehat{E(n)}}( E_n^{\operatorname{hGal}} \wedge_{\mathbb{S}_p} \mathbb{S}_{W(\mathbb{F}_{p^n})}) \\ & \simeq \operatorname{THH}(E_n^{\operatorname{hGal}}) \wedge_{\mathbb{S}_p} \mathbb{S}_{W(\mathbb{F}_{p^n})}.\end{align*}
Therefore, it is sufficient to show that the canonical map
is an equivalence after p-completion. This follows by the following canonical diagram of
$\mathbb{S}/p$
-equivalences.

The right-hand vertical map and the upper-left vertical map are
$\mathbb{S}/p$
-equivalences due to [Reference MaoMao23, Lemma 5.20]. The fact that the lower-left vertical map is an
$\mathbb{S}/p$
-equivalence follows by [Reference MaoMao23, proof of Lemma 5.20] and the fact that the composite
$\mathbb{S}_{W(\mathbb{F}_{p^n})} \to \operatorname{THH}(\mathbb{S}_{W(\mathbb{F}_{p^n})}) \to \mathbb{S}_{W(\mathbb{F}_{p^n})}$
is an equivalence. This shows that the upper horizontal map is an
$\mathbb{S}/p$
-equivalence, proving the theorem.
Acknowledgements
We would like to thank Sanath Devalapurkar for many of the ideas in § 3. We also thank Jeremy Hahn for showing us the proof of the redshift conjecture for
$BP \langle n \rangle$
with Witt vector coefficients. We benefited from various conversations with Andrew Baker and Robert Burklund and we would like to thank them as well. We are very grateful to Robert Burklund for pointing out a mistake in the proof of the claim, in a previous version of this paper, that the Morava K-theories satisfy redshift; the claim has been removed from the present version. We would like to thank Oscar Randal-Williams for explaining to us in depth the constructions in [Reference Galatius, Kupers and Randal-WilliamsGKR25]. Finally, we would like to thank the anonymous referees for many very useful suggestions or corrections.
Conflicts of interest
None.
Financial support
The first and second authors acknowledge support from the project ANR-16-CE40-0003 ChroK. The second author acknowledges support from the Engineering and Physical Sciences Research Council (EPSRC), grant EP/T030771/1. The third author acknowledges support from the grant NEDAG ERC-2016-ADG-741501.
Journal information
Compositio Mathematica is owned by the Foundation Compositio Mathematica and published by the London Mathematical Society in partnership with Cambridge University Press. All surplus income from the publication of Compositio Mathematica is returned to mathematics and higher education through the charitable activities of the Foundation, the London Mathematical Society and Cambridge University Press.
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