TY - JOUR
T1 - Average eigenstate entanglement entropy of the XY chain in a transverse field and its universality for translationally invariant quadratic fermionic models
AU - Hackl, Lucas
AU - Vidmar, Lev
AU - Rigol, Marcos
AU - Bianchi, Eugenio
N1 - Funding Information:
We thank J. Eisert and I. Roth for discussions. We acknowledge support from a Mebus Fellowship (L.H.), the Max Planck Harvard Research Center for Quantum Optics (L.H.), the Slovenian Research Agency research core Funding No. P1-0044 (L.V.), and the National Science Foundation Grants No. PHY-1707482 (M.R.) and No. PHY-1806428 (E.B.). The computations were done at the Institute for CyberScience at Penn State.
Publisher Copyright:
© 2019 American Physical Society.
PY - 2019/2/11
Y1 - 2019/2/11
N2 - We recently showed [Phys. Rev. Lett. 121, 220602 (2018)PRLTAO0031-900710.1103/PhysRevLett.121.220602] that the average bipartite entanglement entropy of all energy eigenstates of the quantum Ising chain exhibits a universal (for translationally invariant quadratic fermionic models) leading term that scales linearly with the subsystem's volume, while in the thermodynamic limit the first subleading correction does not vanish at the critical field (it only depends on the ratio f between the volume of the subsystem and volume of the system) and vanishes otherwise. Here we show, analytically for bounds and numerically for averages, that the same remains true for the spin-1/2 XY chain in a transverse magnetic field. We then tighten the bounds for the coefficient of the universal volume-law term, which is a concave function of f. We develop a systematic approach to compute upper and lower bounds, and we provide explicit analytic expressions for up to the fourth-order bounds.
AB - We recently showed [Phys. Rev. Lett. 121, 220602 (2018)PRLTAO0031-900710.1103/PhysRevLett.121.220602] that the average bipartite entanglement entropy of all energy eigenstates of the quantum Ising chain exhibits a universal (for translationally invariant quadratic fermionic models) leading term that scales linearly with the subsystem's volume, while in the thermodynamic limit the first subleading correction does not vanish at the critical field (it only depends on the ratio f between the volume of the subsystem and volume of the system) and vanishes otherwise. Here we show, analytically for bounds and numerically for averages, that the same remains true for the spin-1/2 XY chain in a transverse magnetic field. We then tighten the bounds for the coefficient of the universal volume-law term, which is a concave function of f. We develop a systematic approach to compute upper and lower bounds, and we provide explicit analytic expressions for up to the fourth-order bounds.
UR - http://www.scopus.com/inward/record.url?scp=85061972327&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=85061972327&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.99.075123
DO - 10.1103/PhysRevB.99.075123
M3 - Article
AN - SCOPUS:85061972327
SN - 2469-9950
VL - 99
JO - Physical Review B-Condensed Matter
JF - Physical Review B-Condensed Matter
IS - 7
M1 - 075123
ER -