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Combinatorics of the geometry of Wilson loop diagrams II: Grassmann necklaces, dimensions, and denominators

Published online by Cambridge University Press:  23 July 2021

Susama Agarwala
Affiliation:
Applied Physics Laboratory, Johns Hopkins University, Laurel, MD, USA e-mail: susama@alum.mit.edu
Siân Fryer
Affiliation:
UC Santa Barbara, Department of Mathematics Yeats, Santa Barbara, CA, USA e-mail: fryer@math.ucsb.edu
Karen Yeats*
Affiliation:
University of Waterloo, Department of Combinatorics and Optimization, Waterloo, ON, Canada
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Abstract

Wilson loop diagrams are an important tool in studying scattering amplitudes of SYM $N=4$ theory and are known by previous work to be associated to positroids. In this paper, we study the structure of the associated positroids, as well as the structure of the denominator of the integrand defined by each diagram. We give an algorithm to derive the Grassmann necklace of the associated positroid directly from the Wilson loop diagram, and a recursive proof that the dimension of these cells is thrice the number of propagators in the diagram. We also show that the ideal generated by the denominator in the integrand is the radical of the ideal generated by the product of Grassmann necklace minors.

MSC classification

Information

Type
Article
Copyright
© Canadian Mathematical Society 2021
Figure 0

Figure 1: The Wilson loop diagram $W = \big (\{(1,4), (2,4), (5,7), (5,8)\},[8]\big )$, which has four propagators and eight vertices.

Figure 1

Figure 2: Row and column numbering for a Young diagram with $k = 3$, $n = 7$ (left), and $k = 3$, $n = 8$ (right). The top-left box has coordinates $(1,7)$ in the left diagram, and $(2,8)$ in the right diagram.

Figure 2

Figure 3: The two configurations described in Lemma 3.3; every weakly admissible Wilson loop diagram with no nonsupporting vertices admits at least one example of at least one of these configurations.

Figure 3

Figure 4: The base case of the induction in Lemma 3.3.

Figure 4

Figure 5: We can replace $q_r$ with $q^{\prime }_r$ as long as $q_r$ and $p_{r+1}$ are on opposite sides of $q^{\prime }_r$.

Figure 5

Figure 6: $W'$ and $V'$ are locally the same between j and $l+1$, so we will have $I_i^W\cap [j,l] = I_m^V\cap [j,l]$ even though $p \neq s$ and $q \neq t$. Note that propagators such as r which have both ends inside the region of interest must be identical in both diagrams.

Figure 6

Figure 7: The two types of configuration that would (in theory) allow the propagator p to contribute its $<_i$-maximal support vertex to $I_i$.

Figure 7

Figure 8: Four cases for admissible Wilson loop diagrams with no nonsupporting vertices. The gray half-propagators illustrate where propagators may occur, but are not required to exist.

Figure 8

Figure 9: Diagram V is W with p removed; there are no propagators inside $q = (i,j)$, though there may be up to 4 non-supporting vertices labeled $l, l+1, \ldots , l+3$.

Figure 9

Figure 10: If q is counterclockwise of $p_r$ and the other end of $p_r$ lies on an edge between $a_r$ and $j_m$, then $V(q) \subseteq [a_{r-1},j_m]$. The vertex $a_r$ lies somewhere within the (blue) highlighted region.

Figure 10

Figure 11: If the other end of $p_r$ does not lie on an edge between $a_r$ and $j_m$, then we must have a propagator $p_s \in Q_{l-2}$ in one of the depicted configurations. The (blue) highlighted regions indicate the approximate position of a vertex whose precise position is unknown. Cutoff propagators indicate that the location of the propagator’s other end is unknown; in particular, no meaning should be ascribed to the angle at which these propagators are drawn.

Figure 11

Figure 12: The two cases for W and p following Lemma 4.3. No other propagators can end in the bolded (red) sections. Other segments may have additional propagators ending in them.

Figure 12

Figure 13: Le diagrams for V (left) and W (right).

Figure 13

Figure 14: The Le diagrams for V and W in the setting of Theorem 4.12. The shaded regions indicate where the plusses match up perfectly from V to W, the bold (red) plusses exist if and only if $n-2 \in I_{n-2}^V$, and the (blue) plusses in the bottom row of the Le diagrams of W diagrams are the three new plusses coming from the induction step.

Figure 14

Figure 15: Example Wilson loop diagram for illustrating Algorithm 5.1 and bijections between propagators and vertices for each Grassmann necklace element.

Figure 15

Figure 16: The two cases in the proof that no factors of $\Delta _{I_i}$ have degree 3 or more.

Figure 16

Figure 17: In order to obtain $I_{i-1}(s) = a$, propagators s and p must each have an end on edge $(i-2)$.