Heralded magnetism in non-Hermitian atomic systems

207Citations
Citations of this article
77Readers
Mendeley users who have this article in their library.

Abstract

Quantum phase transitions are usually studied in terms of Hermitian Hamiltonians. However, cold-atom experiments are intrinsically non-Hermitian because of spontaneous decay. Here, we show that non- Hermitian systems exhibit quantum phase transitions that are beyond the paradigm of Hermitian physics. We consider the non-Hermitian XY model, which can be implemented using three-level atoms with spontaneous decay. We exactly solve the model in one dimension and show that there is a quantum phase transition from short-range order to quasi-long-range order despite the absence of a continuous symmetry in the Hamiltonian. The ordered phase has a frustrated spin pattern. The critical exponent ν can be 1 or 1=2. Our results can be seen experimentally with trapped ions, cavity QED, and atoms in optical lattices.

Figures

  • FIG. 1. (a) Experimental setup with a chain of atoms. The population in the auxiliary state jai is measured by scattering photons off of it. (b) The non-Hermitian model is heralded by the absence of population in jai, i.e., the absence of fluorescence. (c) j↑i decays into the auxiliary state jai. (d) The population of jai is measured by exciting it with a laser and detecting the fluorescence (red arrows). (e) Level scheme for a 171Ybþ ion, showing optical pumping (black arrows) and detection (red arrows).
  • FIG. 2. Population in the six slowest-decaying eigenstates of Heff during the non-Hermitian evolution (a) without normalization and (b) with normalization. This is from exact diagonalization of N ¼ 10 atoms with open boundary conditions, the initial condition j↓↓ ↓i, J0 ¼ 0.12γ, and J ¼ 0. The thick red line denotes the steady state.
  • FIG. 3. hσzni for (a) two atoms and (b) an infinite chain with J ¼ 0 (blue solid line) and J ¼ 0.1γ (red dashed line). The critical point is J0 ¼ γ=8 for all cases. Panel (a) is independent of J.
  • FIG. 5. Real part of ϵðkÞ for the same parameters as in Fig. 4.
  • FIG. 4. Imaginary part of ϵðkÞ for J0 ¼ 0.1γ (black solid line), J0 ¼ 0.125γ (red dashed line), and J0 ¼ 0.15γ (blue dash-dotted line). (a) J ¼ 0.1γ. (b) J ¼ 0.
  • FIG. 8. Correlation length ξðJ0Þ for J ¼ 0.1γ, found by fitting the exponential decay of hσxmσxni. At the phase transition, ξ diverges with critical exponent ν ¼ 1.
  • FIG. 6. Ordered-phase correlation functions: hσxmσxni (blue solid line) and hσymσyni (red dashed line) for J0 ¼ 0.13γ with (a) J ¼ 0.1γ and (b) J ¼ 0.
  • FIG. 7. Correlation functions for J0 ¼ 0.13γ (solid line) and J0 ¼ 0.12γ (dashed line) for (a) J ¼ 0.1γ and (b) J ¼ 0. Panel (b) shows only even distances for J0 ¼ 0.12γ.

References Powered by Scopus

Quantum Phase Transitions

6563Citations
432Readers
Get full text
Get full text
4464Citations
727Readers
Get full text

Cited by Powered by Scopus

Get full text
1233Citations
472Readers
1060Citations
399Readers

Register to see more suggestions

Mendeley helps you to discover research relevant for your work.

Already have an account?

Cite

CITATION STYLE

APA

Lee, T. E., & Chan, C. K. (2014). Heralded magnetism in non-Hermitian atomic systems. Physical Review X, 4(4). https://doi.org/10.1103/PhysRevX.4.041001

Readers over time

‘14‘15‘16‘17‘18‘19‘20‘21‘22‘23‘240481216

Readers' Seniority

Tooltip

PhD / Post grad / Masters / Doc 32

62%

Professor / Associate Prof. 12

23%

Researcher 7

13%

Lecturer / Post doc 1

2%

Readers' Discipline

Tooltip

Physics and Astronomy 50

89%

Engineering 3

5%

Materials Science 2

4%

Philosophy 1

2%

Article Metrics

Tooltip
Mentions
News Mentions: 1

Save time finding and organizing research with Mendeley

Sign up for free
0