A tutorial introduction to quantum stochastic master equations based on the qubit/photon system
From the key composite quantum system made of a two-level system (qubit) and a harmonic oscillator (photon) with resonant or dispersive interactions, one derives the corresponding quantum Stochastic Master Equations (SME) when either the qubits or the photons are measured. Starting with an elementar...
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Main Author | |
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Format | Journal Article |
Language | English |
Published |
15.08.2022
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Subjects | |
Online Access | Get full text |
DOI | 10.48550/arxiv.2208.07416 |
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Summary: | From the key composite quantum system made of a two-level system (qubit) and
a harmonic oscillator (photon) with resonant or dispersive interactions, one
derives the corresponding quantum Stochastic Master Equations (SME) when either
the qubits or the photons are measured. Starting with an elementary
discrete-time formulation based on explicit formulae for the interaction
propagators, one shows how to include measurement imperfections and
decoherence. This qubit/photon quantum system illustrates the Kraus-map
structure of general discrete-time SME governing the dynamics of an open
quantum system subject to measurement back-action and decoherence induced by
the environment. Then, on the qubit/photon system, one explains the passage to
a continuous-time mathematical model where the measurement signal is either a
continuous real-value signal (typically homodyne or heterodyne signal) or a
discontinuous and integer-value signal obtained from a counter. During this
derivation, the Kraus map formulation is preserved in an infinitesimal way.
Such a derivation provides also an equivalent Kraus-map formulation to the
continuous-time SME usually expressed as stochastic differential equations
driven either by Wiener or Poisson processes. From such Kraus-map formulation,
simple linear numerical integration schemes are derived that preserve the
positivity and the trace of the density operator, i.e. of the quantum state. |
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DOI: | 10.48550/arxiv.2208.07416 |