2021
DOI: 10.48550/arxiv.2112.05886
|View full text |Cite
Preprint
|
Sign up to set email alerts
|

Relating entanglement spectra and energy spectra via path-integral on replica manifold

Abstract: Low-lying entanglement spectrum provide the quintessential fingerprint to identify the highly entangled quantum matter with topological and conformal field-theoretical properties. However, when the entangling region acquires long boundary with the environment, such as that between long coupled chains or in two or higher dimensions, there unfortunately exists no universal yet practical method to compute the entanglement spectra with affordable computational cost. Here we develop a new algorithm to overcome such… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
3
0

Year Published

2021
2021
2022
2022

Publication Types

Select...
3

Relationship

3
0

Authors

Journals

citations
Cited by 3 publications
(3 citation statements)
references
References 61 publications
0
3
0
Order By: Relevance
“…, where 𝑛 0 is the particle density, which is 1/2 at low-temperature and 𝑁 = k 1 ,𝑚 1 𝑑 † k 1 ,𝑚 1 𝑑 k 1 ,𝑚 1 is the particle number operator. We also compute the temperature dependence of the spetral functions from the stochastic analytic continuation (SAC) of the imaginary time Green's function from QMC [36,51,[61][62][63] and perform the finite size scaling of the order parameter for the QAH phase and find a good agreement with Ising universality. The topological aspect of the QAH phase can be also seen from the computed Berry curvature below the transition temperature, and from which the Chern numbe can then be calculated as 𝐶 = 𝐹 , where 𝐹 is the Berry curvature in the finite size mBZ obtained from the Green's function in the QMC simulations [64,65].…”
mentioning
confidence: 88%
“…, where 𝑛 0 is the particle density, which is 1/2 at low-temperature and 𝑁 = k 1 ,𝑚 1 𝑑 † k 1 ,𝑚 1 𝑑 k 1 ,𝑚 1 is the particle number operator. We also compute the temperature dependence of the spetral functions from the stochastic analytic continuation (SAC) of the imaginary time Green's function from QMC [36,51,[61][62][63] and perform the finite size scaling of the order parameter for the QAH phase and find a good agreement with Ising universality. The topological aspect of the QAH phase can be also seen from the computed Berry curvature below the transition temperature, and from which the Chern numbe can then be calculated as 𝐶 = 𝐹 , where 𝐹 is the Berry curvature in the finite size mBZ obtained from the Green's function in the QMC simulations [64,65].…”
mentioning
confidence: 88%
“…We note a similar geometry has been used in the computation of entanglement spectrum in (2+1)d quantum many-body systems [58]. The disorder parameter is then given by…”
Section: Acknowledgementmentioning
confidence: 99%
“…Such topological unit provides a stable and efficient way of carrying out the computation both conceptually and technically. Beyond the 2-leg geometry, a general n-leg Qiu Ku manifold can even give rise to the low-lying entanglement spectrum for quantum manybody systems [33].…”
Section: Introductionmentioning
confidence: 99%