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Conditional squeezing induced by a two-level system: a first-principles approach to QND readout

Phoenix M. M. Paing

TL;DR

The paper addresses the problem of capturing beyond-RWA light–matter dynamics in the Jaynes–Cummings framework. By applying a systematic Magnus expansion to the rotated Hamiltonian up to second order, it derives $\hat{\Omega}_1(t)$ and $\hat{\Omega}_2(t)$, uncovering time-dependent energy shifts and a conditional squeezing term proportional to $\hat{\sigma}_z$ and two-photon field operators with a squeezing coefficient $\zeta(t)$. The analysis exposes an underlying $SU(1,1)$ algebraic structure that permits exact disentangling of the second-order evolution into unitary factors, clarifying how squeezing emerges from a minimal two-level system. These insights provide a first-principles link between atom–field interactions and nonclassical light, with potential for quantum nondemolition, phase-sensitive readout via homodyne detection, and guidance for extending the approach to more complex, multi-level systems.

Abstract

We present a systematic Magnus expansion treatment of light-matter interaction beyond the Rotating Wave Approximation. We show that at the second order of Magnus series, the time-evolution operator acquires both energy-shifts and squeezing contributions. In addition to the energy shifts caused by vacuum and photon numbers, the second-order evolution operator contains a term that induces conditional squeezing of the field mode depending on the state of the atom. Such a term suggests a natural mechanism for phase-sensitive, quantum non-demolishing type measurements of squeezed light via homodyne detection. We also show that the second-order Magnus operator in a close SU(1,1) algebra, ensuring the exponentiation of the Magnus series yields a well-defined unitary evolution. By deriving squeezing directly from the Jaynes-Cummings Hamiltonian, our results clarify how energy shifts and $\hatσ$-dependent squeezing arise from an SU(1,1) structure, with direct implications for phase-sensitive and quantum nondemolition measurements.

Conditional squeezing induced by a two-level system: a first-principles approach to QND readout

TL;DR

The paper addresses the problem of capturing beyond-RWA light–matter dynamics in the Jaynes–Cummings framework. By applying a systematic Magnus expansion to the rotated Hamiltonian up to second order, it derives and , uncovering time-dependent energy shifts and a conditional squeezing term proportional to and two-photon field operators with a squeezing coefficient . The analysis exposes an underlying algebraic structure that permits exact disentangling of the second-order evolution into unitary factors, clarifying how squeezing emerges from a minimal two-level system. These insights provide a first-principles link between atom–field interactions and nonclassical light, with potential for quantum nondemolition, phase-sensitive readout via homodyne detection, and guidance for extending the approach to more complex, multi-level systems.

Abstract

We present a systematic Magnus expansion treatment of light-matter interaction beyond the Rotating Wave Approximation. We show that at the second order of Magnus series, the time-evolution operator acquires both energy-shifts and squeezing contributions. In addition to the energy shifts caused by vacuum and photon numbers, the second-order evolution operator contains a term that induces conditional squeezing of the field mode depending on the state of the atom. Such a term suggests a natural mechanism for phase-sensitive, quantum non-demolishing type measurements of squeezed light via homodyne detection. We also show that the second-order Magnus operator in a close SU(1,1) algebra, ensuring the exponentiation of the Magnus series yields a well-defined unitary evolution. By deriving squeezing directly from the Jaynes-Cummings Hamiltonian, our results clarify how energy shifts and -dependent squeezing arise from an SU(1,1) structure, with direct implications for phase-sensitive and quantum nondemolition measurements.

Paper Structure

This paper contains 9 sections, 19 equations.