Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

Yang-Lee Quantum Criticality in Various Dimensions

Erick Arguello Cruz1, Igor R. Klebanov2,3, Grigory Tarnopolsky1, and Yuan Xin1

Phys. Rev. X 16, 011022 – Published 9 February, 2026

DOI: https://doi.org/10.1103/w4qg-2xwn

Abstract

The Yang-Lee universality class arises when an imaginary magnetic field is tuned to its critical value in the paramagnetic phase of the d<6 Ising model. In d=2, this nonunitary conformal field theory (CFT) is exactly solvable via the M(2,5) minimal model. As found long ago by von Gehlen using exact diagonalization, the corresponding real-time, quantum critical behavior arises in the periodic Ising spin chain when the imaginary longitudinal magnetic field is tuned to its critical value from below. Even though the Hamiltonian is not Hermitian, the energy levels are real due to the PT symmetry. In this paper, we explore the analogous quantum critical behavior in higher-dimensional non-Hermitian Hamiltonians on regularized spheres Sd−1. For d=3, we use the recently invented, powerful fuzzy sphere method, as well as discretization by the platonic solids cube, icosahedron, and dodecahedron. The low-lying energy levels and structure constants we find are in agreement with expectations from the conformal symmetry. The energy levels are in good quantitative agreement with the high-temperature expansions and with Padé extrapolations of the 6−ε expansions in Fisher’s iϕ3 Euclidean field theory for the Yang-Lee criticality. In the course of this work, we clarify some aspects of matching between operators in this field theory and quasiprimary fields in the M(2,5) minimal model. For d=4, we obtain new results by replacing S3 with the self-dual polytope called the 24-cell.

View figure in article

Physics Subject Headings (PhySH)

Popular Summary

Article Text

References (115)

  1. E. Ising, Contribution to the theory of ferromagnetism, Z. Phys. 31, 253 (1925).
  2. L. Onsager, Crystal statistics. 1. A two-dimensional model with an order disorder transition, Phys. Rev. 65, 117 (1944).
  3. A. Belavin, A. M. Polyakov, and A. Zamolodchikov, Infinite conformal symmetry in two-dimensional quantum field theory, Nucl. Phys. B241, 333 (1984).
  4. K. G. Wilson and M. E. Fisher, Critical exponents in 3.99 dimensions, Phys. Rev. Lett. 28, 240 (1972).
  5. R. Rattazzi, V. S. Rychkov, E. Tonni, and A. Vichi, Bounding scalar operator dimensions in 4D CFT, J. High Energy Phys. 12 (2008) 031.
  6. S. El-Showk, M. F. Paulos, D. Poland, S. Rychkov, D. Simmons-Duffin, and A. Vichi, Solving the 3D Ising model with the conformal bootstrap, Phys. Rev. D 86, 025022 (2012).
  7. A. M. Polyakov, Conformal symmetry of critical fluctuations, JETP Lett. 12, 381 (1970).
  8. D. Poland, S. Rychkov, and A. Vichi, The conformal bootstrap: Theory, numerical techniques, and applications, Rev. Mod. Phys. 91, 015002 (2019).
  9. D. Simmons-Duffin, The conformal bootstrap, in New Frontiers in Fields and Strings (World Scientific, Singapore, 2017), pp. 1–74.
  10. S. Rychkov, EPFL Lectures on Conformal Field Theory in D>=3 Dimensions, SpringerBriefs in Physics (Springer, Geneva, 2016), 1.
  11. S. M. Chester, Weizmann lectures on the numerical conformal bootstrap, Phys. Rep. 1045, 1 (2023).
  12. A. Cappelli, L. Maffi, and S. Okuda, Critical Ising model in varying dimension by conformal bootstrap, J. High Energy Phys. 01 (2019) 161.
  13. J. Henriksson, S. R. Kousvos, and M. Reehorst, Spectrum continuity and level repulsion: The Ising CFT from infinitesimal to finite ϵ, J. High Energy Phys. 02 (2023) 218.
  14. W. Zhu, C. Han, E. Huffman, J. S. Hofmann, and Y.-C. He, Uncovering conformal symmetry in the 3D Ising transition: State-operator correspondence from a quantum fuzzy sphere regularization, Phys. Rev. X 13, 021009 (2023).
  15. L. Hu, Y.-C. He, and W. Zhu, Operator product expansion coefficients of the 3D Ising criticality via quantum fuzzy spheres, Phys. Rev. Lett. 131, 031601 (2023).
  16. L. Hu, W. Zhu, and Y.-C. He, Entropic F-function of 3D Ising conformal field theory via the fuzzy sphere regularization, Phys. Rev. B 111, 155151 (2025).
  17. B.-X. Lao and S. Rychkov, 3D Ising CFT and exact diagonalization on icosahedron: The power of conformal perturbation theory, SciPost Phys. 15, 243 (2023).
  18. A. M. Läuchli, L. Herviou, P. H. Wilhelm, and S. Rychkov, Exact diagonalization, matrix product states and conformal perturbation theory study of a 3D Ising fuzzy sphere model, SciPost Phys. 19, 076 (2025).
  19. C. Han, L. Hu, W. Zhu, and Y.-C. He, Conformal four-point correlators of the three-dimensional Ising transition via the quantum fuzzy sphere, Phys. Rev. B 108, 235123 (2023).
  20. F. D. M. Haldane, Fractional quantization of the Hall effect: A hierarchy of incompressible quantum fluid states, Phys. Rev. Lett. 51, 605 (1983).
  21. J. Madore, The fuzzy sphere, Classical Quantum Gravity 9, 69 (1992).
  22. G. Fardelli, A. L. Fitzpatrick, and E. Katz, Constructing the infrared conformal generators on the fuzzy sphere, SciPost Phys. 18, 086 (2025).
  23. R. Fan, Note on explicit construction of conformal generators on the fuzzy sphere, arXiv:2409.08257.
  24. D. Przetakiewicz, S. Wessel, and F. P. Toldin, Boundary operator product expansion coefficients of the three-dimensional Ising universality class, Phys. Rev. Res. 7, L032051 (2025).
  25. Z. Zhou and Y.-C. He, A new series of 3D CFTs with Sp(N) global symmetry on fuzzy sphere, Phys. Rev. Lett. 135, 026504 (2025).
  26. M. Dedushenko, Ising BCFT from fuzzy hemisphere, arXiv:2407.15948.
  27. B.-B. Chen, X. Zhang, and Z. Yang Meng, Emergent conformal symmetry at the multicritical point of (2+1)D SO(5) model with Wess-Zumino-Witten term on a sphere, Phys. Rev. B 110, 125153 (2024).
  28. B.-B. Chen, X. Zhang, Y. Wang, K. Sun, and Z. Y. Meng, Phases of (2+1)D SO(5) nonlinear sigma model with a topological term on a sphere: Multicritical point and disorder phase, Phys. Rev. Lett. 132, 246503 (2024).
  29. Z. Zhou, L. Hu, W. Zhu, and Y.-C. He, SO(5) deconfined phase transition under the fuzzy-sphere microscope: Approximate conformal symmetry, pseudo-criticality, and operator spectrum, Phys. Rev. X 14, 021044 (2024).
  30. C. Han, L. Hu, and W. Zhu, Conformal operator content of the Wilson-Fisher transition on fuzzy sphere bilayers, Phys. Rev. B 110, 115113 (2024).
  31. D. L. Jafferis, I. R. Klebanov, S. S. Pufu, and B. R. Safdi, Towards the F-theorem: N=2 field theories on the three- sphere, J. High Energy Phys. 06 (2011) 102.
  32. I. R. Klebanov, S. S. Pufu, and B. R. Safdi, F-Theorem without supersymmetry, J. High Energy Phys. 10 (2011) 038.
  33. H. Casini and M. Huerta, On the RG running of the entanglement entropy of a circle, Phys. Rev. D 85, 125016 (2012).
  34. L. Fei, S. Giombi, I. R. Klebanov, and G. Tarnopolsky, Generalized F-theorem and the ε expansion, J. High Energy Phys. 12 (2015) 155.
  35. C.-N. Yang and T. D. Lee, Statistical theory of equations of state and phase transitions. 1. Theory of condensation, Phys. Rev. 87, 404 (1952).
  36. T. D. Lee and C.-N. Yang, Statistical theory of equations of state and phase transitions. 2. Lattice gas and Ising model, Phys. Rev. 87, 410 (1952).
  37. P. J. Kortman and R. B. Griffiths, Density of zeros on the Lee-Yang circle for two Ising ferromagnets, Phys. Rev. Lett. 27, 1439 (1971).
  38. M. Fisher, Yang-Lee edge singularity and ϕ3 field theory, Phys. Rev. Lett. 40, 1610 (1978).
  39. J. L. Cardy, Conformal invariance and the Yang-Lee edge singularity in two-dimensions, Phys. Rev. Lett. 54, 1354 (1985).
  40. J. Cardy, The Yang-Lee edge singularity and related problems, arXiv:2305.13288.
  41. M. Borinsky, J. A. Gracey, M. V. Kompaniets, and O. Schnetz, Five-loop renormalization of ϕ3 theory with applications to the Lee-Yang edge singularity and percolation theory, Phys. Rev. D 103, 116024 (2021).
  42. M. Kompaniets and A. Pikelner, Critical exponents from five-loop scalar theory renormalization near six-dimensions, Phys. Lett. B 817, 136331 (2021).
  43. After the original version of this paper appeared, the six-loop beta function and anomalous dimension became available [44], which determine the O(ε6) terms in Δϕ and Δϕ3.

  44. O. Schnetz, ϕ3 theory at six loops, Phys. Rev. D 112, 016028 (2025).
  45. F. Gliozzi, More constraining conformal bootstrap, Phys. Rev. Lett. 111, 161602 (2013).
  46. F. Gliozzi and A. Rago, Critical exponents of the 3D Ising and related models from conformal bootstrap, J. High Energy Phys. 10 (2014) 042.
  47. S. Hikami, Conformal bootstrap analysis for the Yang–Lee edge singularity, Prog. Theor. Exp. Phys. 2018, 053I01 (2018).
  48. The icosahedron has also been used to discretize the 2D classical Ising model on a sphere [49, 50].

  49. R. C. Brower and E. K. Owen, The Ising model on S2, arXiv:2407.00459.
  50. R. C. Brower, G. T. Fleming, N. Matsumoto, and R. Misra, Ising on S2–The Affine Conjecture, in 41st International Symposium on Lattice Field Theory (2025), 3, arXiv:2503.05621.
  51. G. von Gehlen, Critical and off critical conformal analysis of the Ising quantum chain in an imaginary field, J. Phys. A 24, 5371 (1991).
  52. G. von Gehlen, NonHermitian tricriticality in the Blume-Capel model with imaginary field, arXiv:hep-th/9402143.
  53. O. A. Castro-Alvaredo and A. Fring, A spin chain model with non-Hermitian interaction: The Ising quantum spin chain in an imaginary field, J. Phys. A 42, 465211 (2009).
  54. More recent studies of non-Hermitian spin chain Hamiltonians were carried out in the context of Q-state Potts models with Q=5 [55, 56]. Let us also note that the YL universality class is related to the Q→∞ limit of the Potts model [57].

  55. Y. Tang, H. Ma, Q. Tang, Y.-C. He, and W. Zhu, Reclaiming the lost conformality in a non-Hermitian quantum 5-state Potts model, Phys. Rev. Lett. 133, 076504 (2024).
  56. J. L. Jacobsen and K. J. Wiese, Lattice realization of complex conformal field theories: Two-dimensional Potts model with Q>4 states, Phys. Rev. Lett. 133, 077101 (2024).
  57. K. J. Wiese and J. L. Jacobsen, The two upper critical dimensions of the Ising and Potts models, J. High Energy Phys. 05 (2024) 092.
  58. K. Uzelac and R. Jullien, The Yang-Lee edge singularity by the phenomenological renormalisation group, J. Phys. A 14, L151 (1981).
  59. E. Arguello Cruz, G. Tarnopolsky, and Y. Xin, Precision study of the massive Schwinger model near quantum criticality, Phys. Rev. D 112, 034023 (2025).
  60. P. Butera and M. Pernici, Yang-Lee edge singularities from extended activity expansions of the dimer density for bipartite lattices of dimensionality 2<=d<=7, Phys. Rev. E 86, 011104 (2012).
  61. V. P. Yurov and A. B. Zamolodchikov, Truncated conformal space approach to scaling Lee-Yang model, Int. J. Mod. Phys. A 05, 3221 (1990).
  62. H.-L. Xu and A. Zamolodchikov, 2D Ising field theory in a magnetic field: The Yang-Lee singularity, J. High Energy Phys. 08 (2022) 057.
  63. M. Leitner, The (2,5) minimal model on genus two surfaces, arXiv:1801.08387.
  64. A. Katsevich, The spectrum of perturbed (3, 10) minimal model, arXiv:2410.18069.
  65. C. M. Bender, N. Hassanpour, S. P. Klevansky, and S. Sarkar, PT-symmetric quantum field theory in D dimensions, Phys. Rev. D 98, 125003 (2018).
  66. O. de Alcantara Bonfim, J. Kirkham, and A. McKane, Critical exponents to order ε3 for ϕ3 models of critical phenomena in 6−ε dimensions, J. Phys. A 13, L247 (1980).
  67. O. de Alcantara Bonfim, J. Kirkham, and A. McKane, Critical exponents for the percolation problem and the Yang-Lee edge singularity, J. Phys. A 14, 2391 (1981).
  68. L. Fei, S. Giombi, I. R. Klebanov, and G. Tarnopolsky, Three loop analysis of the critical O(N) models in 6−ϵ dimensions, Phys. Rev. D 91, 045011 (2015).
  69. This approach is analogous to the identification of L−3L¯−3ϕ in the 2D Ising model M(3,4) with the operator ϕ5 in the massless ϕ4 field theory [46].

  70. I. R. Klebanov, V. Narovlansky, Z. Sun, and G. Tarnopolsky, Ginzburg-Landau description and emergent supersymmetry of the (3, 8) minimal model, J. High Energy Phys. 02 (2023) 066.
  71. S. Giombi and V. Kirilin, Anomalous dimensions in CFT with weakly broken higher spin symmetry, J. High Energy Phys. 11 (2016) 068.
  72. R. Gopakumar, A. Kaviraj, K. Sen, and A. Sinha, Conformal bootstrap in Mellin space, Phys. Rev. Lett. 118, 081601 (2017).
  73. P. Dey and A. Kaviraj, Towards a bootstrap approach to higher orders of epsilon expansion, J. High Energy Phys. 02 (2018) 153.
  74. V. Goncalves, Skeleton expansion and large spin bootstrap for ϕ3 theory, arXiv:1809.09572.
  75. In the Ising model, the dimension of Tμν′ as a function of d was calculated using the numerical bootstrap methods [12]. It equals 6 in 4D and 2D, while in 3D it is approximately 5.5.

  76. S. Nixon and J. Yang, Nonlinear wave dynamics near phase transition in PT-symmetric localized potentials, Physica (Amsterdam) 331D, 48 (2016).
  77. A. Chernyavsky and D. E. Pelinovsky, Krein signature for instability of PT-symmetric states, Physica (Amsterdam) 371D, 48 (2018).
  78. G. A. Starkov, M. V. Fistul, and I. M. Eremin, Formation of exceptional points in pseudo-Hermitian systems, Phys. Rev. A 108, 022206 (2023).
  79. Y.-J. Wei and Z.-C. Gu, Tensor network renormalization: Application to dynamic correlation functions and non-hermitian systems, arXiv:2311.18785.
  80. M. G. Yamada, T. Sanno, M. O. Takahashi, Y. Akagi, H. Suwa, S. Fujimoto, and M. Udagawa, Matrix product renormalization group: Potential universal quantum many-body solver, arXiv:2212.13267.
  81. W. D. Heiss, The physics of exceptional points, J. Phys. A 45, 444016 (2012).
  82. C. J. Hamer and M. N. Barber, Finite-size scaling in Hamiltonian field theory, J. Phys. A 13, L169 (1980).
  83. C. J. Hamer and M. N. Barber, Finite-lattice methods in quantum Hamiltonian field theory. I. The Ising model, J. Phys. A 14, 241 (1981).
  84. C. J. Hamer and M. N. Barber, Finite-lattice methods in quantum Hamiltonian field theory. I. O(2) and O(3) Heisenberg models, J. Phys. A, 14 259 (1981).
  85. G. Von Gehlen, Critical and off-critical conformal analysis of the Ising quantum chain in an imaginary field, J. Phys. A 24, 5371 (1991).
  86. G. V. Gehlen, Non-Hermitian tricriticality in the Blume-Capel model with imaginary field, Int. J. Mod. Phys. B 08, 3507 (1994).
  87. Although CPT predicts the convergence rate of ihz*(N) to ihzcrit at large N, we observe that, for small values of N, the points are fitted well by the 1/N linear fit.

  88. For the FSS criterion, we followed Ref. [82] and defined hz*(N) as the point where N+1E10(1)(N+1)=NE10(1)(N),where we used R∝N [89].

  89. Z. Zhou, FuzzifiED: Julia package for numerics on the fuzzy sphere, arXiv:2503.00100.
  90. J. L. Cardy, Operator content of two-dimensional conformally invariant theories, Nucl. Phys. B270, 186 (1986).
  91. A. B. Zamolodchikov, Renormalization group and perturbation theory near fixed points in two-dimensional field theory, Sov. J. Nucl. Phys. 46, 1090 (1987).
  92. J. L. Cardy, Conformal invariance and universality in finite-size scaling, J. Phys. A 17, L385 (1984).
  93. Y. Zou, A. Milsted, and G. Vidal, Conformal data and renormalization group flow in critical quantum spin chains using periodic uniform matrix product states, Phys. Rev. Lett. 121, 230402 (2018).
  94. Y. Zou, A. Milsted, and G. Vidal, Conformal fields and operator product expansion in critical quantum spin chains, Phys. Rev. Lett. 124, 040604 (2020).
  95. The error bars are determined by the difference between the linear and quadratic extrapolations. The purpose of these error bars is to show the scale of a possible fitting error but not to assert that the true value should lie within the error bar. Note that Cϕϕ3ϕ3 has nonoverlapping error bars.

  96. M. S. Costa, J. Penedones, D. Poland, and S. Rychkov, Spinning conformal correlators, J. High Energy Phys. 11 (2011) 071.
  97. D. Meltzer, Higher spin ANEC and the space of CFTs, J. High Energy Phys. 07 (2019) 001.
  98. T. Kondo, The characters of the Weyl group of type F4, J. Fac. Sci. Univ. Tokyo Sect. I 11, 1965 (1965).
  99. R. W. Carter, Conjugacy classes in the Weyl group, Compos. Math. 25, 1 (1972).
  100. R. Carter, Finite Groups of Lie Type: Conjugacy Classes and Complex Characters, Wiley Classics Library (Wiley, New York, 1993).
  101. G. Carleo and M. Troyer, Solving the quantum many-body problem with artificial neural networks, Science 355, 602 (2017).
  102. S. Giombi, E. Himwich, A. Katsevich, I. Klebanov, and Z. Sun, Sphere free energy of scalar field theories with cubic interactions, arXiv:2412.14086.
  103. A. Katsevich, I. R. Klebanov, and Z. Sun, Ginzburg-Landau description of a class of non-unitary minimal models, J. High Energy Phys. 03 (2025) 170.
  104. Y. Nakayama and T. Tanaka, Infinitely many new renormalization group flows between Virasoro minimal models from non-invertible symmetries, J. High Energy Phys. 11 (2024) 137.
  105. O. Delouche, J. Elias Miro, and J. Ingoldby, Testing the RG-flow M(3,10)+ϕ1,7→M(3,8) with Hamiltonian truncation, J. High Energy Phys. 04 (2025) 144.
  106. H. Kausch, G. Takacs, and G. Watts, On the relation between Phi(1,2) and Phi(1,5) perturbed minimal models, Nucl. Phys. B489, 557 (1997).
  107. T. Quella, I. Runkel, and G. M. Watts, Reflection and transmission for conformal defects, J. High Energy Phys. 04 (2007) 095.
  108. D. Poland, V. Prilepina, and P. Tadić, Improving the five-point bootstrap, J. High Energy Phys. 05 (2024) 299.
  109. D. Poland, V. Prilepina, and P. Tadić, The five-point bootstrap, J. High Energy Phys. 10 (2023) 153.
  110. C.-H. Chang, V. Dommes, R. S. Erramilli, A. Homrich, P. Kravchuk, A. Liu, M. S. Mitchell, D. Poland, and D. Simmons-Duffin, Bootstrapping the 3D Ising stress tensor, J. High Energy Phys. 03 (2025) 136.
  111. G. Tarnopolsky, Numerical analysis of the Yang-Lee critical point across different dimensions, Available from https://www.youtube.com/watch?v=zfw63uGGiDE.
  112. R. Fan, J. Dong, and A. Vishwanath, Simulating the non-unitary Yang-Lee conformal field theory on the fuzzy sphere, arXiv:2505.06342.
  113. J. E. Miro and O. Delouche, Flowing from the Ising model on the fuzzy sphere to the 3D Lee-Yang CFT, J. High Energy Phys. 10 (2025) 037.
  114. S. Mamone, G. Pileio, and M. H. Levitt, Orientational sampling schemes based on four dimensional polytopes, Symmetry 2, 1423 (2010).
  115. M. Geck and G. Pfeiffer, Characters of Finite Coxeter Groups and Iwahori-Hecke Algebras, London Mathematical Society Monographs New Series (Oxford University Press, New York, 2000).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation