Simultaneous higher-order Hong-Mandel's squeezing and higher-order sub-Poissonian photon statistics in superposed coherent states
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We study maximum simultaneous 2n  th-order Hong and Mandel's squeezing of the most general the Hermitian operator, issn=00304026&md5=97ba718de8fe46885ba343998d0b74ca" title="Click to view the MathML source">Xθ≡X1cosθ+X2sinθ, and nth-order sub-Poissonian photon statistics (connected with expectation value of 2n  th power of number fluctuation), in the most general superposition state, issn=00304026&md5=516dbd7f4155825dd408740c55370368" title="Click to view the MathML source">|ψ〉=Z1|α〉+Z2|β〉 of two coherent states issn=00304026&md5=37704d747f77555b1873b51a81e1d7b8" title="Click to view the MathML source">|α〉 and issn=00304026&md5=2da87ad17eed5595898092ed50ad0408" title="Click to view the MathML source">|β〉. Here Hermitian operators X1,2 are defined by X1 + iX2 = a, the annihilation operator, complex numbers Z1,2, α, β are all arbitrary and the only restriction on these is the normalization condition of the state. We find a linear relationship between these two non-classical effects when the angle θ = arg(α + β  ) and issn=00304026&md5=0cc42085cdb1faead8fb4b70d58d9d23" title="Click to view the MathML source">|α+β|≫|α−β|. We show that maximum simultaneous 2nth-order Hong and Mandel's squeezing for the operator Xθ and n  th-order sub-Poissonian photon statistics in the state occur for an infinite combinations with issn=00304026&md5=49670f289120eec61a0347780c832576" title="Click to view the MathML source">α−β=A2nexp[±i(1/2)π+iθ]; issn=00304026&md5=a7128869b7ab27ce37b7109e7fa18c22" title="Click to view the MathML source">A2n is a constant which depends on the order of squeezing, issn=00304026&md5=2b86c8a911265b67dfaef35add214408" title="Click to view the MathML source">Z2/Z1=exp[(1/2)(βα*−β*α)] and with θ = arg(α + β  ) and issn=00304026&md5=0cc42085cdb1faead8fb4b70d58d9d23" title="Click to view the MathML source">|α+β|≫|α−β|. We also illustrate analytically and numerically by an example that both effects occur simultaneously for high-intensity field but for observation of such effects, sensitive settings of the parameters are required.

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