Evidence map›Paper›PMID 41429810›Full record

ArticleScientific reports2025

Dynamical phase diagram of the quantum Ising model with cluster interaction under noiseless and noisy driven field.

S Kheiri, R Jafari, S Mahdavifar, Seyed Ehsan Nedaaee Oskoee, Alireza Akbari

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Article in Scientific reports, 2025. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Not yet cited in PubMed.

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4 · The record

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5 · Who and what money

Authors and funding

5 authors.

S KheiriDepartment of Physics, Institute for Advanced Studies in Basic Sciences (IASBS), Zanjan, 45137-66731, Iran.
R JafariDepartment of Physics, Institute for Advanced Studies in Basic Sciences (IASBS), Zanjan, 45137-66731, Iran. raadmehr.jafari@gmail.com.
S MahdavifarDepartment of Physics, University of Guilan, Rasht, 41335-1914, Iran.
Seyed Ehsan Nedaaee OskoeeDepartment of Physics, Institute for Advanced Studies in Basic Sciences (IASBS), Zanjan, 45137-66731, Iran.
Alireza AkbariBeijing Institute of Mathematical Sciences and Applications (BIMSA), Huairou District, Beijing, 101408, China.

Funding

No grant is acknowledged in the PubMed record.

6 · The paper itself

Abstract

In most lattice models, gap closing typically occurs at high-symmetry points in the Brillouin zone. In the transverse field Ising model with cluster interaction, the gap closes at high-symmetry points, as well as at the phase transition between paramagnetic and cluster phases, where the gap-closing mode can be moved by tuning the strength of the cluster interaction. We take advantage of this property to examine the nonequilibrium dynamics of the model in the framework of dynamical quantum phase transitions (DQPTs) after a noiseless and noisy ramp of the transverse magnetic field. The numerical results show that DQPTs always happen if the starting or ending point of the quench field is restricted between two critical points. In other ways, there is always critical sweep velocity above which DQPTs disappear. Our finding reveals that noise modifies drastically the dynamical phase diagram of the model. We find that the critical sweep velocity decreases by enhancing the noise intensity and scales linearly with the square of noise intensity for weak and strong noise. Moreover, the region with multi-critical modes (MCMs) induced in the dynamical phase diagram by noise. The sweep velocity under which the system enters the MCMs region increases by enhancing the noise and scales linearly with the square of noise intensity.

Identifiers

PMID41429810
PMCPMC12727827

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