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Zeros, chaotic ratios and the computational complexity of approximating the independence polynomial

Published online by Cambridge University Press:  24 November 2023

DAVID DE BOER
Affiliation:
Korteweg de Vries Institute for Mathematics, University of Amsterdam, P.O. Box 94248 1090 GE Amsterdam, The Netherlands. e-mails: fdaviddeboer2795@gmail.com, pjotr.buys@gmail.com, lorenzo.guerini92@gmail.com, hanpeters77@gmail.com, guusregtsg@gmail.com
PJOTR BUYS
Affiliation:
Korteweg de Vries Institute for Mathematics, University of Amsterdam, P.O. Box 94248 1090 GE Amsterdam, The Netherlands. e-mails: fdaviddeboer2795@gmail.com, pjotr.buys@gmail.com, lorenzo.guerini92@gmail.com, hanpeters77@gmail.com, guusregtsg@gmail.com
LORENZO GUERINI
Affiliation:
Korteweg de Vries Institute for Mathematics, University of Amsterdam, P.O. Box 94248 1090 GE Amsterdam, The Netherlands. e-mails: fdaviddeboer2795@gmail.com, pjotr.buys@gmail.com, lorenzo.guerini92@gmail.com, hanpeters77@gmail.com, guusregtsg@gmail.com
HAN PETERS
Affiliation:
Korteweg de Vries Institute for Mathematics, University of Amsterdam, P.O. Box 94248 1090 GE Amsterdam, The Netherlands. e-mails: fdaviddeboer2795@gmail.com, pjotr.buys@gmail.com, lorenzo.guerini92@gmail.com, hanpeters77@gmail.com, guusregtsg@gmail.com
GUUS REGTS
Affiliation:
Korteweg de Vries Institute for Mathematics, University of Amsterdam, P.O. Box 94248 1090 GE Amsterdam, The Netherlands. e-mails: fdaviddeboer2795@gmail.com, pjotr.buys@gmail.com, lorenzo.guerini92@gmail.com, hanpeters77@gmail.com, guusregtsg@gmail.com
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Abstract

The independence polynomial originates in statistical physics as the partition function of the hard-core model. The location of the complex zeros of the polynomial is related to phase transitions, and plays an important role in the design of efficient algorithms to approximately compute evaluations of the polynomial.

In this paper we directly relate the location of the complex zeros of the independence polynomial to computational hardness of approximating evaluations of the independence polynomial. We do this by moreover relating the location of zeros to chaotic behaviour of a naturally associated family of rational functions; the occupation ratios.

Information

Type
Research Article
Copyright
© The Author(s), 2023. Published by Cambridge University Press on behalf of Cambridge Philosophical Society
Figure 0

Fig. 1. The cardioid $\Lambda_3$.

Figure 1

Fig. 2. The graph $\widetilde{P}_n$ in Lemma 2·6.

Figure 2

Fig 3. The rooted graph $\widetilde G_n$ in the proof of Theorem 5·1.

Figure 3

Fig 4. The graph $(\widetilde{G}_n, v_n)$ in the proof of the claim.

Figure 4

Fig 5. The generalised circles $\lambda_1 \cdot \hat{\mathbb{R}}$ and $\hat{\mathbb{R}}$ intersect in the points 0 and $\infty$. A region around 0 is drawn. The open set U is shaded in gray. Examples of generalised circles $C_w$ that intersect $\lambda_1 \cdot \hat{\mathbb{R}}$ transversely are drawn with dashed lines, while examples of circles that do not intersect $\lambda_1 \cdot \hat{\mathbb{R}}$ are drawn with dotted lines.

Figure 5

Fig. 6. An example of two orbits with the same initial value converging to $z_i$ under iteration of two different maps. For the dark gray orbit converging horizontally to $z_i$ the derivative at $z_i$ is real. For the light gray orbit the derivative at $z_i$ has the same magnitude, while its argument is a little less than $2\pi /3$.

Figure 6

Fig 7. An illustration of the disk A and B such that the arc along B between $S_2$ and $S_1$ is contained in A and the arc along A between $S_1$ and $S_2$ is contained in B in the proof of Lemma 6·9.

Figure 7

Fig 8. An illustration of how the disk D sits inside $\textrm{Sec}_A(Q_1,Q_2)$ in situation (i), on the left and situation (ii), on the right.

Figure 8

Fig 9. The activity-locus of Cayley trees for down-degrees 2, 3 and 4. For each pixel the spherical derivative of the occupation ratio is computed for the Cayley tree of depth 120. Pixels for which this derivative is sufficiently large are depicted in white, suggesting that the corresponding parameter $\lambda$ lies approximately on the activity locus.