Back to Search
Start Over
Entropic fluctuations in XY chains and reflectionless Jacobi matrices
- Source :
- Annales Henri Poincaré, Annales Henri Poincaré, 2013, 14, pp.1775-1800. ⟨10.1007/s00023-013-0231-2⟩, Annales Henri Poincaré, Springer Verlag, 2013, 14, pp.1775-1800. ⟨10.1007/s00023-013-0231-2⟩
- Publication Year :
- 2012
-
Abstract
- We study entropic functionals/fluctuations of the XY chain with Hamiltonian $$\begin{array}{ll} \frac{1}{2} \sum\limits_{x \in \mathbb{Z}}J_x( \sigma_x^{(1)} \sigma_{x+1}^{(1)} +\sigma_x^{(2)} \sigma_{x+1}^{(2)}) + \lambda_x \sigma_x^{(3)}\end{array}$$ where initially the left (x ≤ 0)/right (x > 0) part of the chain is in thermal equilibrium at inverse temperature β l /β r . The temperature differential results in a non-trivial energy/entropy flux across the chain. The Evans–Searles (ES) entropic functional describes fluctuations of the flux observable with respect to the initial state while the Gallavotti–Cohen (GC) functional describes these fluctuations with respect to the steady state (NESS) the chain reaches in the large time limit. We also consider the full counting statistics (FCS) of the energy/entropy flux associated with a repeated measurement protocol, the variational entropic functional (VAR) that arises as the quantization of the variational characterization of the classical Evans–Searles functional and a natural class of entropic functionals that interpolate between FCS and VAR. We compute these functionals in closed form in terms of the scattering data of the Jacobi matrix hu x = J x u x+1 + λ x u x + J x−1 u x−1 canonically associated with the XY chain. We show that all these functionals are identical if and only if h is reflectionless (we call this phenomenon entropic identity). If h is not reflectionless, then the ES and GC functionals remain equal but differ from the FCS, VAR and interpolating functionals. Furthermore, in the non-reflectionless case, the ES/GC functional does not vanish at α = 1 (i.e., the Kawasaki identity fails) and does not have the celebrated α ↔ 1 − α symmetry. The FCS, VAR and interpolating functionals always have this symmetry. In the Schrodinger case, where J x = J for all x, the entropic identity leads to some unexpected open problems in the spectral theory of one-dimensional discrete Schrodinger operators.
- Subjects :
- Nuclear and High Energy Physics
Spectral theory
Gallavotti-Cohen fluctuation theorem
[PHYS.MPHY]Physics [physics]/Mathematical Physics [math-ph]
FOS: Physical sciences
Lambda
entropy production
01 natural sciences
Mathematics - Spectral Theory
symbols.namesake
Open quantum system
[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]
0103 physical sciences
FOS: Mathematics
[PHYS.COND.CM-SM]Physics [physics]/Condensed Matter [cond-mat]/Statistical Mechanics [cond-mat.stat-mech]
0101 mathematics
010306 general physics
Spectral Theory (math.SP)
Mathematical Physics
nonequilibrium statistical mechanics
Mathematical physics
Thermal equilibrium
Physics
Quantum Physics
Evans-Searless fluctuation relation
1D discrete Schrödinger operators
Entropy production
010102 general mathematics
Sigma
Statistical and Nonlinear Physics
Observable
Mathematical Physics (math-ph)
reflectionless Jacobi matrices
XY spin chain
symbols
Quantum Physics (quant-ph)
Hamiltonian (quantum mechanics)
Subjects
Details
- Language :
- English
- ISSN :
- 14240637 and 14240661
- Database :
- OpenAIRE
- Journal :
- Annales Henri Poincaré, Annales Henri Poincaré, 2013, 14, pp.1775-1800. ⟨10.1007/s00023-013-0231-2⟩, Annales Henri Poincaré, Springer Verlag, 2013, 14, pp.1775-1800. ⟨10.1007/s00023-013-0231-2⟩
- Accession number :
- edsair.doi.dedup.....4092a0971a90458d82e7415c65532d33
- Full Text :
- https://doi.org/10.1007/s00023-013-0231-2⟩