1996Journal of Modern OpticsRequires access

Finite number of measurements in optical homodyne tomography

Päivi Törmä

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Abstract

For infinite dimensional quantum systems, no general theory exists of the effect of using a finite size ensemble in quantum state measurements. We approach this topic by considering one particular measurement scheme, optical homodyne tomography. We define a measure which tells us how well a quantum state, belonging to a pre-set state space, is determined after N measurements. We illustrate the method by considering, as an example, a state space which includes all coherent and squeezed states as well as certain superpositions of these.

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What this paper is about

For infinite dimensional quantum systems, no general theory exists of the effect of using a finite size ensemble in quantum state measurements. We approach this topic by considering one particular measurement scheme, optical homodyne tomography. We define a measure which tells us how well a quantum state, belonging to a pre-set state space, is determined after N measurements. We illustrate the method by considering, as an example, a state space which includes all coherent and squeezed states as well as certain superpositions of these.

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Available abstract

For infinite dimensional quantum systems, no general theory exists of the effect of using a finite size ensemble in quantum state measurements. We approach this topic by considering one particular measurement scheme, optical homodyne tomography. We define a measure which tells us how well a quantum state, belonging to a pre-set state space, is determined after N measurements. We illustrate the method by considering, as an example, a state space which includes all coherent and squeezed states as well as certain superpositions of these.

Key concepts: Quantum tomography, Direct-conversion receiver, Homodyne detection, Measure (data warehouse), Quantum state, Physics, Quantum optics, Coherent states

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