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Physical Review A

Dual eigenkets of the Susskind-Glogower phase operator

Hong-Yi Fan, Min Xiao

Published Dec 1, 1996• 67 citations
Publisher

Abstract

By contour integration we show that the phase operator ${\mathit{e}\mathit{\^{}}}^{\mathrm{\ensuremath{-}}\mathit{i}\mathrm{\ensuremath{\varphi}}}$ (one of the pair of Susskind-Glogower operators) also possesses eigenkets |\ensuremath{\gamma}${\mathrm{〉}}_{\mathrm{*}}$, which are the dual vector of ${\mathit{e}\mathit{\^{}}}^{\mathit{i}\mathrm{\ensuremath{\varphi}}}$'s eigenkets. The properties of |\ensuremath{\gamma}${\mathrm{〉}}_{\mathrm{*}}$ are studied and we see that |\ensuremath{\gamma}${\mathrm{〉}}_{\mathrm{*}}$ and ${\mathit{e}\mathit{\^{}}}^{\mathit{i}\mathrm{\ensuremath{\varphi}}}$'s eigenkets can also make up a phase-state representation. \textcopyright{} 1996 The American Physical Society.

DOI
10.1103/physreva.54.5295

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By contour integration we show that the phase operator eˆ\ensuremath−i\ensuremathφ{\mathit{e}\mathit{\^{}}}^{\mathrm{\ensuremath{-}}\mathit{i}\mathrm{\ensuremath{\varphi}}}eˆ\ensuremath−i\ensuremathφ (one of the pair of Susskind-Glogower operators) also possesses eigenkets |\ensuremath{\gamma}〉∗{\mathrm{〉}}_{\mathrm{*}}〉∗​, which are the dual vector of eˆi\ensuremathφ{\mathit{e}\mathit{\^{}}}^{\mathit{i}\mathrm{\ensuremath{\varphi}}}eˆi\ensuremathφ's eigenkets. The properties of |\ensuremath{\gamma}〉∗{\mathrm{〉}}_{\mathrm{*}}〉∗​ are studied and we see that |\ensuremath{\gamma}〉∗{\mathrm{〉}}_{\mathrm{*}}〉∗​ and eˆi\ensuremathφ{\mathit{e}\mathit{\^{}}}^{\mathit{i}\mathrm{\ensuremath{\varphi}}}eˆi\ensuremathφ's eigenkets can also make up a phase-state representation. \textcopyright{} 1996 The American Physical Society.
We define a unitary phase operator for photons in a single momentum mode. The operator acts on a Hilbert space with basis consisting of all number states in both polarizations. The Susskind Glogower operator, E^=eiϕ^{\hat{E}} = e^{i \hatϕ}E^=eiϕ^​, thus defined is unitary and acts as a true ladder operator over all the states. It satisfies the commutation relation [E^,n^]=E^[{\hat{E}}, {\hat{n}}] = {\hat{E}}[E^,n^]=E^; consequently, the phase ϕ^\hatϕϕ^​ satisfies the canonical commutation relation [n^,ϕ^]=i[{\hat{n}}, {\hatϕ}] = i[n^,ϕ^​]=i. The eigenstates of the Susskind Glogower operator are found. Our model is able to directly account for phase measurements when polarization changes cannot be neglected and at the same time gives a well defined phase operator.