2013
DOI: 10.1088/1367-2630/15/7/073014
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Nondeterministic noiseless amplification via non-symplectic phase space transformations

Abstract: We analyse the action of an ideal noiseless linear amplifier operator, gˆa †â , using the Wigner function phase space representation. In this setting we are able to clarify the gain g for which a physical output is produced when this operator is acted upon inputs other than coherent states. We derive compact closed form expressions for the action of N local amplifiers, with potentially different gains, on arbitrary N -mode Gaussian states and provide several examples of the utility of this formalism for determ… Show more

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Cited by 28 publications
(26 citation statements)
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References 54 publications
(91 reference statements)
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“…For a loss channel, the effective parameters {χ e , τ e , ε e } have been computed in Refs. [51,52], but can also be found in the Appendix B. Before we apply this technique, let us give a brief description on how NLA works.…”
Section: B Thermal Channelsmentioning
confidence: 99%
See 1 more Smart Citation
“…For a loss channel, the effective parameters {χ e , τ e , ε e } have been computed in Refs. [51,52], but can also be found in the Appendix B. Before we apply this technique, let us give a brief description on how NLA works.…”
Section: B Thermal Channelsmentioning
confidence: 99%
“…The effective parameters for a thermal loss channel {χ e , τ e , ε e } have been computed in Refs. [51,52], and are given by…”
Section: Effective Parameters Of the Nlamentioning
confidence: 99%
“…Further discussion of this point can be found in Ref. [15]. More intuitively, we can see the extra noise as being due to our incomplete knowledge of the target state.…”
Section: And the Converse As The Reverse Inference (Ementioning
confidence: 90%
“…For Gaussian states, an NLA can, in principle, probabilistically increase the signal-to-noise ratio by increasing the mean values of the quadratures while keeping their variances at the initial level [38,[45][46][47][48]. The amplification can be described by an operatorĈ = gn, wheren is the number operator in the Fock basis.…”
Section: Noiseless Linear Amplifiermentioning
confidence: 99%