Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:1108.3406 · The European Physical Journal B

Quantum phases and dynamics of geometric phase in a quantum spin chain under linear quench

S. Sarkar, B. Basu

Published Dec 1, 2012• 1 citation
arXivHTMLPDF
DOI
10.1140/epjb/e2012-30428-0

Related papers

Dynamics of the geometric phase in the adiabatic limit of a quench induced quantum phase transition

Banasri Basu

arXiv:0908.3299•Physics Letters A•Jan 7, 2010•7 citations

Thermodynamical and dynamical properties of quenched quantum spin chains

Oleg Derzhko, Taras Krokhmalskii, Taras Verkholyak

Materials Science and Engineering A•Jun 1, 1997•1 citation

Dynamics of the geometric phase in inhomogeneous quantum spin chains

Kaiyuan Cao, Shuxiang Yang, Yayun Hu +1 more

The dynamics of the geometric phase are studied in inhomogeneous quantum spin chains after a quench. Analytic expressions of the Pancharatnam geometric phase (PGP) are derived for both the period-2 quantum Ising chain (QIC) and the disordered QIC. In the period-2 QIC, due to the periodic modulation, the phase difference between the boundaries of the half Brillouin zone $(0,\ensuremath{\pi}]$ changes with time, and consequently, the winding number ${\ensuremath{\nu}}_{D}(t)$ of the PGP is not quantized and thus is not topological anymore. Nevertheless, the PGP and its winding number show nonanalytic singularities at the critical times of the dynamical quantum phase transitions (DQPTs). This relation between the PGP and the DQPT is further confirmed in the disordered QIC. It is found that the critical time of the DQPT inherited from the homogeneous system and the additional one induced by weak disorder are also accompanied by the nonanalytic singularity of the PGP by decomposing the PGP into each quasiparticle mode. The connection between the nonanalytic behavior of the PGP at the critical time and the DQPT, regardless of whether the winding number is topological, can be explained by the fact that they both arise when the Loschmidt amplitude vanishes.

arXiv:2211.15976•Physical review. B./Physical review. B•Jul 5, 2023•9 citations

Quantum renormalization group approach to geometric phases in spin chains

Rouhollah Jafari

arXiv:1206.2047•Physics Letters A•Oct 26, 2013•17 citations

Quantum Spin Chains: Phase Behaviour and Dynamic Excitations

Jill C. Bonner, John B. Parkinson

Springer series in solid-state sciences•Jan 1, 1984•0 citations

Geometric quenches in quasidisordered lattice systems

Ravi Kumar, Ranjan Modak

While global quantum quench has been extensively used in the literature to understand the localization-delocalization transition for the one-dimensional quantum spin chain, the effect of geometric quench (which corresponds to a sudden change of the geometry of the chain) in the context of such transitions is yet to be well understood. In this work, we investigate the effect of geometric quench in the Aubry-Andr\'e model, which supports localization-delocalization transition even in one dimension. We study the spreading of the entanglement and the site occupation with time and find many interesting features that can be used to characterize localization-delocalization transition. We observe that geometric quench causes a power-law type growth of the entanglement entropy in the delocalized phase in contrast to the linear growth which is found in the global quench studies. We also find that the saturation values in the many-body localized (MBL) phase obey area law in contrast to the usual volume law, which is a signature feature of the MBL phase in the context of global quench. This area law can also be understood from the long time site-occupation profile in the MBL phase.

arXiv:2201.06813•Physical review. B./Physical review. B•Jun 9, 2022•1 citation
The dynamics of the geometric phase are studied in inhomogeneous quantum spin chains after a quench. Analytic expressions of the Pancharatnam geometric phase (PGP) are derived for both the period-2 quantum Ising chain (QIC) and the disordered QIC. In the period-2 QIC, due to the periodic modulation, the phase difference between the boundaries of the half Brillouin zone $(0,\ensuremath{\pi}]$ changes with time, and consequently, the winding number ${\ensuremath{\nu}}_{D}(t)$ of the PGP is not quantized and thus is not topological anymore. Nevertheless, the PGP and its winding number show nonanalytic singularities at the critical times of the dynamical quantum phase transitions (DQPTs). This relation between the PGP and the DQPT is further confirmed in the disordered QIC. It is found that the critical time of the DQPT inherited from the homogeneous system and the additional one induced by weak disorder are also accompanied by the nonanalytic singularity of the PGP by decomposing the PGP into each quasiparticle mode. The connection between the nonanalytic behavior of the PGP at the critical time and the DQPT, regardless of whether the winding number is topological, can be explained by the fact that they both arise when the Loschmidt amplitude vanishes.
While global quantum quench has been extensively used in the literature to understand the localization-delocalization transition for the one-dimensional quantum spin chain, the effect of geometric quench (which corresponds to a sudden change of the geometry of the chain) in the context of such transitions is yet to be well understood. In this work, we investigate the effect of geometric quench in the Aubry-Andr\'e model, which supports localization-delocalization transition even in one dimension. We study the spreading of the entanglement and the site occupation with time and find many interesting features that can be used to characterize localization-delocalization transition. We observe that geometric quench causes a power-law type growth of the entanglement entropy in the delocalized phase in contrast to the linear growth which is found in the global quench studies. We also find that the saturation values in the many-body localized (MBL) phase obey area law in contrast to the usual volume law, which is a signature feature of the MBL phase in the context of global quench. This area law can also be understood from the long time site-occupation profile in the MBL phase.