Simultaneous higher-order Hong-Mandel's squeezing and higher-order sub-Poissonian photon statistics in superposed coherent states
详细信息    查看全文
文摘
We study maximum simultaneous 2n  th-order Hong and Mandel's squeezing of the most general the Hermitian operator, pan id="mmlsi7" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0030402616001753&_mathId=si7.gif&_user=111111111&_pii=S0030402616001753&_rdoc=1&_issn=00304026&md5=97ba718de8fe46885ba343998d0b74ca" title="Click to view the MathML source">Xθ≡X1cosθ+X2sinθpan>pan class="mathContainer hidden">pan class="mathCode">XθX1cosθ+X2sinθpan>pan>pan>, and nth-order sub-Poissonian photon statistics (connected with expectation value of 2n  th power of number fluctuation), in the most general superposition state, pan id="mmlsi8" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0030402616001753&_mathId=si8.gif&_user=111111111&_pii=S0030402616001753&_rdoc=1&_issn=00304026&md5=516dbd7f4155825dd408740c55370368" title="Click to view the MathML source">|ψ〉=Z1|α〉+Z2|β〉pan>pan class="mathContainer hidden">pan class="mathCode">pen="|" close="〉">ψ=Z1pen="|" close="〉">α+Z2pen="|" close="〉">βpan>pan>pan> of two coherent states pan id="mmlsi9" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0030402616001753&_mathId=si9.gif&_user=111111111&_pii=S0030402616001753&_rdoc=1&_issn=00304026&md5=37704d747f77555b1873b51a81e1d7b8" title="Click to view the MathML source">|α〉pan>pan class="mathContainer hidden">pan class="mathCode">pen="|" close="〉">αpan>pan>pan> and pan id="mmlsi10" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0030402616001753&_mathId=si10.gif&_user=111111111&_pii=S0030402616001753&_rdoc=1&_issn=00304026&md5=2da87ad17eed5595898092ed50ad0408" title="Click to view the MathML source">|β〉pan>pan class="mathContainer hidden">pan class="mathCode">pen="|" close="〉">βpan>pan>pan>. 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 pan id="mmlsi11" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0030402616001753&_mathId=si11.gif&_user=111111111&_pii=S0030402616001753&_rdoc=1&_issn=00304026&md5=0cc42085cdb1faead8fb4b70d58d9d23" title="Click to view the MathML source">|α+β|≫|α−β|pan>pan class="mathContainer hidden">pan class="mathCode">pen="|" close="|">α+βpen="|" close="|">αβpan>pan>pan>. 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 pan id="mmlsi12" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0030402616001753&_mathId=si12.gif&_user=111111111&_pii=S0030402616001753&_rdoc=1&_issn=00304026&md5=49670f289120eec61a0347780c832576" title="Click to view the MathML source">α−β=A2nexp[±i(1/2)π+iθ]pan>pan class="mathContainer hidden">pan class="mathCode">αβ=A2nexppen="[" close="]">±ipen="(" close=")">1/2π+iθpan>pan>pan>; pan id="mmlsi13" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0030402616001753&_mathId=si13.gif&_user=111111111&_pii=S0030402616001753&_rdoc=1&_issn=00304026&md5=a7128869b7ab27ce37b7109e7fa18c22" title="Click to view the MathML source">A2npan>pan class="mathContainer hidden">pan class="mathCode">A2npan>pan>pan> is a constant which depends on the order of squeezing, pan id="mmlsi14" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0030402616001753&_mathId=si14.gif&_user=111111111&_pii=S0030402616001753&_rdoc=1&_issn=00304026&md5=2b86c8a911265b67dfaef35add214408" title="Click to view the MathML source">Z2/Z1=exp[(1/2)(βα*−β*α)]pan>pan class="mathContainer hidden">pan class="mathCode">Z2/Z1=exppen="[" close="]">pen="(" close=")">1/2(βα*β*α)pan>pan>pan> and with θ = arg(α + β  ) and pan id="mmlsi11" class="mathmlsrc">pan class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0030402616001753&_mathId=si11.gif&_user=111111111&_pii=S0030402616001753&_rdoc=1&_issn=00304026&md5=0cc42085cdb1faead8fb4b70d58d9d23" title="Click to view the MathML source">|α+β|≫|α−β|pan>pan class="mathContainer hidden">pan class="mathCode">pen="|" close="|">α+βpen="|" close="|">αβpan>pan>pan>. 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.

© 2004-2018 中国地质图书馆版权所有 京ICP备05064691号 京公网安备11010802017129号

地址:北京市海淀区学院路29号 邮编:100083

电话:办公室:(+86 10)66554848;文献借阅、咨询服务、科技查新:66554700