TY - JOUR
T1 - Lattice ℂP N−1 model with ℤ N twisted boundary condition
T2 - bions, adiabatic continuity and pseudo-entropy
AU - Fujimori, Toshiaki
AU - Itou, Etsuko
AU - Misumi, Tatsuhiro
AU - Nitta, Muneto
AU - Sakai, Norisuke
N1 - Publisher Copyright:
© 2020, The Author(s).
PY - 2020/8/1
Y1 - 2020/8/1
N2 - We investigate the lattice ℂPN−1 sigma model on Ss1(large) ×Sτ1(small) with the ℤN symmetric twisted boundary condition, where a sufficiently large ratio of the circumferences (Ls ≫ Lτ) is taken to approximate ℝ × S1. We find that the expectation value of the Polyakov loop, which is an order parameter of the ℤN symmetry, remains consistent with zero (|〈P〉| ∼ 0) from small to relatively large inverse coupling β (from large to small Lτ). As β increases, the distribution of the Polyakov loop on the complex plane, which concentrates around the origin for small β, isotropically spreads and forms a regular N-sided-polygon shape (e.g. pentagon for N = 5), leading to |〈P〉| ∼ 0. By investigating the dependence of the Polyakov loop on Ss1 direction, we also verify the existence of fractional instantons and bions, which cause tunneling transition between the classical N vacua and stabilize the ℤN symmetry. Even for quite high β, we find that a regular-polygon shape of the Polyakov-loop distribution, even if it is broken, tends to be restored and |〈P〉| gets smaller as the number of samples increases. To discuss the adiabatic continuity of the vacuum structure from another viewpoint, we calculate the β dependence of “pseudo-entropy” density ∝ 〈Txx − Tττ〉. The result is consistent with the absence of a phase transition between large and small β regions.
AB - We investigate the lattice ℂPN−1 sigma model on Ss1(large) ×Sτ1(small) with the ℤN symmetric twisted boundary condition, where a sufficiently large ratio of the circumferences (Ls ≫ Lτ) is taken to approximate ℝ × S1. We find that the expectation value of the Polyakov loop, which is an order parameter of the ℤN symmetry, remains consistent with zero (|〈P〉| ∼ 0) from small to relatively large inverse coupling β (from large to small Lτ). As β increases, the distribution of the Polyakov loop on the complex plane, which concentrates around the origin for small β, isotropically spreads and forms a regular N-sided-polygon shape (e.g. pentagon for N = 5), leading to |〈P〉| ∼ 0. By investigating the dependence of the Polyakov loop on Ss1 direction, we also verify the existence of fractional instantons and bions, which cause tunneling transition between the classical N vacua and stabilize the ℤN symmetry. Even for quite high β, we find that a regular-polygon shape of the Polyakov-loop distribution, even if it is broken, tends to be restored and |〈P〉| gets smaller as the number of samples increases. To discuss the adiabatic continuity of the vacuum structure from another viewpoint, we calculate the β dependence of “pseudo-entropy” density ∝ 〈Txx − Tττ〉. The result is consistent with the absence of a phase transition between large and small β regions.
KW - Lattice Quantum Field Theory
KW - Sigma Models
KW - Solitons Monopoles and Instantons
KW - Wilson
KW - ’t Hooft and Polyakov loops
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U2 - 10.1007/JHEP08(2020)011
DO - 10.1007/JHEP08(2020)011
M3 - Article
AN - SCOPUS:85089134765
SN - 1126-6708
VL - 2020
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 8
M1 - 11
ER -