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

Springer theses

Investigated Models

Stefan Flörchinger

Published Jan 1, 2010• 0 citations
Publisher
DOI
10.1007/978-3-642-14113-3_6

Related papers

Related Models

Sei Suzuki, Jun‐ichi Inoue, Bikas K. Chakrabarti

Lecture notes in physics•Dec 12, 2012•0 citations

Effective Interactions of the One-Dimensionald-pModel Based on the Luttinger Liquid Theory

Kazuhiro Sano, Yoshiaki Ōno

We examine effective interactions of the 1D d-p model mapped to a typical one-dimensional(1D) model such as the Hubbard model or the t-J model by the numerical diagonalization method combined with the Luttinger liquid theory. Analysis of the effective coupling constants of the mapped model gives the relationship between these models without ambiguity. We find that the renormalized interaction is relatively weak, though the repulsion of the d-p model at Cu-sites is very strong. We also find that the d-p model corresponds to not the t-J model but the Hubbard model for wide range of the parameters. It suggests that the Hubbard model is more favorable than the t-J model as a effective model of the d-p model in the low energy limit.

Journal of the Physical Society of Japan•Jan 1, 2002•2 citations

Clock model interpolation and symmetry breaking in O(2) models

Leon Hostetler, Jin Zhang, Ryo Sakai +3 more

The $q$-state clock model is a classical spin model that corresponds to the Ising model when $q=2$ and to the $XY$ model when $q\to\infty$. The integer-$q$ clock model has been studied extensively and has been shown to have a single phase transition when $q=2$,$3$,$4$ and two phase transitions when $q>4$.We define an extended $q$-state clock model that reduces to the ordinary $q$-state clock model when $q$ is an integer and otherwise is a continuous interpolation of the clock model to noninteger $q$. We investigate this class of clock models in 2D using Monte Carlo (MC) and tensor renormalization group (TRG) methods, and we find that the model with noninteger $q$ has a crossover and a second-order phase transition. We also define an extended-$O(2)$ model (with a parameter $\gamma$) that reduces to the $XY$ model when $\gamma=0$ and to the extended $q$-state clock model when $\gamma\to\infty$, and we begin to outline the phase diagram of this model. These models with noninteger $q$ serve as a testbed to study symmetry breaking in situations corresponding to quantum simulators where experimental parameters can be tuned continuously.

International Symposium on Lattice Field Theory (LATTICE)•May 16, 2022•4 citations

Related Models

Lecture notes in physics. M, Monographs•Jan 1, 1996•0 citations

Clock model interpolation and symmetry breaking in O(2) models

Leon Hostetler, Jin Zhang, Ryo Sakai +3 more

The $q$-state clock model is a classical spin model that corresponds to the Ising model when $q=2$ and to the $XY$ model when $q\to\infty$. The integer-$q$ clock model has been studied extensively and has been shown to have a single phase transition when $q=2$,$3$,$4$ and two phase transitions when $q>4$.We define an extended $q$-state clock model that reduces to the ordinary $q$-state clock model when $q$ is an integer and otherwise is a continuous interpolation of the clock model to noninteger $q$. We investigate this class of clock models in 2D using Monte Carlo (MC) and tensor renormalization group (TRG) methods, and we find that the model with noninteger $q$ has a crossover and a second-order phase transition. We also define an extended-$O(2)$ model (with a parameter $γ$) that reduces to the $XY$ model when $γ=0$ and to the extended $q$-state clock model when $γ\to\infty$, and we begin to outline the phase diagram of this model. These models with noninteger $q$ serve as a testbed to study symmetry breaking in situations corresponding to quantum simulators where experimental parameters can be tuned continuously.

arXiv:2110.05527•Oct 11, 2021•0 citations

Future Research

Cecilia Flori

Lecture notes in physics•Jan 1, 2013•0 citations
We examine effective interactions of the 1D d-p model mapped to a typical one-dimensional(1D) model such as the Hubbard model or the t-J model by the numerical diagonalization method combined with the Luttinger liquid theory. Analysis of the effective coupling constants of the mapped model gives the relationship between these models without ambiguity. We find that the renormalized interaction is relatively weak, though the repulsion of the d-p model at Cu-sites is very strong. We also find that the d-p model corresponds to not the t-J model but the Hubbard model for wide range of the parameters. It suggests that the Hubbard model is more favorable than the t-J model as a effective model of the d-p model in the low energy limit.
The qqq-state clock model is a classical spin model that corresponds to the Ising model when q=2q=2q=2 and to the XYXYXY model when q→∞q\to\inftyq→∞. The integer-qqq clock model has been studied extensively and has been shown to have a single phase transition when q=2q=2q=2,333,444 and two phase transitions when q>4q>4q>4.We define an extended qqq-state clock model that reduces to the ordinary qqq-state clock model when qqq is an integer and otherwise is a continuous interpolation of the clock model to noninteger qqq. We investigate this class of clock models in 2D using Monte Carlo (MC) and tensor renormalization group (TRG) methods, and we find that the model with noninteger qqq has a crossover and a second-order phase transition. We also define an extended-O(2)O(2)O(2) model (with a parameter γ\gammaγ) that reduces to the XYXYXY model when γ=0\gamma=0γ=0 and to the extended qqq-state clock model when γ→∞\gamma\to\inftyγ→∞, and we begin to outline the phase diagram of this model. These models with noninteger qqq serve as a testbed to study symmetry breaking in situations corresponding to quantum simulators where experimental parameters can be tuned continuously.
The qqq-state clock model is a classical spin model that corresponds to the Ising model when q=2q=2q=2 and to the XYXYXY model when q→∞q\to\inftyq→∞. The integer-qqq clock model has been studied extensively and has been shown to have a single phase transition when q=2q=2q=2,333,444 and two phase transitions when q>4q>4q>4.We define an extended qqq-state clock model that reduces to the ordinary qqq-state clock model when qqq is an integer and otherwise is a continuous interpolation of the clock model to noninteger qqq. We investigate this class of clock models in 2D using Monte Carlo (MC) and tensor renormalization group (TRG) methods, and we find that the model with noninteger qqq has a crossover and a second-order phase transition. We also define an extended-O(2)O(2)O(2) model (with a parameter γγγ) that reduces to the XYXYXY model when γ=0γ=0γ=0 and to the extended qqq-state clock model when γ→∞γ\to\inftyγ→∞, and we begin to outline the phase diagram of this model. These models with noninteger qqq serve as a testbed to study symmetry breaking in situations corresponding to quantum simulators where experimental parameters can be tuned continuously.