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Annals of Physics

A microscopic theory of the lambda transition

Tadashi Toyoda

Published Jun 1, 1982• 43 citations
Publisher
DOI
10.1016/0003-4916(82)90277-9

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Abstract Phase transitions are both thermodynamically and quantum-mechanically ubiquitous in nature and laboratories, and their understanding remains one of the most active issues in modern physics and related disciplines. The Landau theory provides a general framework to describe phenomenologically phase transitions by introducing order parameters and associated symmetry breaking. This theory is also taken as a starting point to explore critical phenomena in connection with phase transitions in the renormalization group, which provides a complete theoretical description of behaviors close to critical points. In this context, the microscopic mechanism of phase transitions remains unclear. In this study, we explore the microscopic mechanism of the superradiant phase transition in the quantum Rabi model (QRM). First, we perform a diagonalization operation in an operator space to obtain three fundamental patterns, denoted as λ 1 , λ 2 , and λ 3 , involved in the QRM. Then, we explicitly analyze the energy evolutions of these patterns with increasing coupling strength. The observed characteristic behaviors reveal the microscopic mechanism of the superradiant phase transition as a consequence of competition between patterns due to different phase relations. In other words, with increasing coupling strength, the pattern λ 1 drives the phase transition, the pattern λ 2 exhibits a similar response speed but less energy compensation than the pattern λ 1 , and the pattern λ 3 exhibits a slow response speed but plays a key role in the balance between it and the pattern λ 1 , which stabilizes the new phase. This type of dissecting mechanism explains why and how the superradiant phase transition occurs in the QRM and paves the way for exploring the microscopic mechanism of phase transitions that occur frequently in nature.

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Physical review. B, Condensed matter•Aug 1, 1979•11 citations
Abstract Phase transitions are both thermodynamically and quantum-mechanically ubiquitous in nature and laboratories, and their understanding remains one of the most active issues in modern physics and related disciplines. The Landau theory provides a general framework to describe phenomenologically phase transitions by introducing order parameters and associated symmetry breaking. This theory is also taken as a starting point to explore critical phenomena in connection with phase transitions in the renormalization group, which provides a complete theoretical description of behaviors close to critical points. In this context, the microscopic mechanism of phase transitions remains unclear. In this study, we explore the microscopic mechanism of the superradiant phase transition in the quantum Rabi model (QRM). First, we perform a diagonalization operation in an operator space to obtain three fundamental patterns, denoted as λ 1 , λ 2 , and λ 3 , involved in the QRM. Then, we explicitly analyze the energy evolutions of these patterns with increasing coupling strength. The observed characteristic behaviors reveal the microscopic mechanism of the superradiant phase transition as a consequence of competition between patterns due to different phase relations. In other words, with increasing coupling strength, the pattern λ 1 drives the phase transition, the pattern λ 2 exhibits a similar response speed but less energy compensation than the pattern λ 1 , and the pattern λ 3 exhibits a slow response speed but plays a key role in the balance between it and the pattern λ 1 , which stabilizes the new phase. This type of dissecting mechanism explains why and how the superradiant phase transition occurs in the QRM and paves the way for exploring the microscopic mechanism of phase transitions that occur frequently in nature.
An effective Hamiltonian for the two-photon two-level model is derived form the microscopic Hamiltonian of a three-level atom in a \ensuremath{\Lambda} configuration, interacting through two-photon transitions with a light field. The effective Hamiltonian includes a term describing the optical Stark shift. With this effective Hamiltonian, we study the steady-state equation and the squeezing spectrum for a cavity-field mode interacting with an ensemble of three-level ``\ensuremath{\Lambda}-configuration'' atoms by a two-photon transition. It is shown that significant changes in the transmission characteristics and the squeezing spectrum for the output field result from the inclusion of the Stark shift.