4.6 Article

Generating high-order quantum exceptional points in synthetic dimensions

期刊

PHYSICAL REVIEW A
卷 104, 期 1, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevA.104.012205

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资金

  1. Grant Agency of the Czech Republic [18-08874S, CZ.02.1.01 0.0 0.0 16_019 0000754]
  2. Ministry of Education, Youth and Sports of the Czech Republic
  3. Polish National Science Centre (NCN) under Maestro Grant [DEC-2019/34/A/ST2/00081]
  4. Nippon Telegraph and Telephone Corporation (NTT) Research, the Japan Science and Technology Agency (JST) [JPMJMS2061]
  5. Centers of Research Excellence in Science and Technology (CREST) [JPMJCR1676]
  6. Japan Society for the Promotion of Science (JSPS) [JP20H00134]
  7. JSPSRFBR [JPJSBP120194828]
  8. Army Research Office (ARO) [W911NF-18-1-0358]
  9. Asian Office of Aerospace Research and Development (AOARD) [FA2386-20-1-4069]
  10. Foundational Questions Institute Fund (FQXi) [FQXi-IAF19-06]

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Intense research has been conducted on constructing high-order exceptional points in dissipative systems. Previous methods mainly focused on spatial networks of coupled modes or utilization of synthetic dimensions. A recent simple and effective method has been introduced for engineering non-Hermitian Hamiltonians with high-order quantum EPs.
Recently, there has been intense research in proposing and developing various methods for constructing high-order exceptional points (EPs) in dissipative systems. These EPs can possess a number of intriguing properties related to, e.g., chiral transport and enhanced sensitivity. Previous proposals to realize non-Hermitian Hamiltonians (NHHs) with high-order EPs have been mainly based on either direct construction of spatial networks of coupled modes or utilization of synthetic dimensions, e.g., mapping of spatial lattices to time or photon-number space. Both methods rely on the construction of effective NHHs describing classical or postselected quantum fields, which neglect the effects of quantum jumps and which, thus, suffer from a scalability problem in the quantum regime, when the probability of quantum jumps increases with the number of excitations and dissipation rate. Here, by considering the full quantum dynamics of a quadratic Liouvillian superoperator, we introduce a simple and effective method for engineering NHHs with high-order quantum EPs, derived from evolution matrices of system operator moments. That is, by quantizing higher-order moments of system operators, e.g., of a quadratic two-mode system, the resulting evolution matrices can be interpreted as alternative NHHs describing, e.g., a spatial lattice of coupled resonators, where spatial sites are represented by high-order field moments in the synthetic space of field moments. Notably, such a mapping allows correct reproduction of the results of the Liouvillian dynamics, including quantum jumps. As an example, we consider a U(1)-symmetric quadratic Liouvillian describing a bimodal cavity with incoherent mode coupling, which can also possess anti-PT symmetry, whose field moment dynamics can be mapped to an NHH governing a spatial network of coupled resonators with high-order EPs.

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