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Hanbury Brown-Twiss interferometer

Let us stress that the operational definition of the quantum phase of radiation [47] is also based on the use of bilinear forms in the photon operators. In the simplest form, the idea of the operational approach to the phase difference can be illustrated with the aid of the two-port interferometer shown in Fig. 11 (see Refs. 14 and 47 for more detailed discussion). The two incident monochromatic (or quasimonochromatic) light beams are combined by a symmetric beamsplitter oriented at 45° to each beam. The resultant intensities emerging from each output port are measured by the two photodetectors connected with a comparator (computer) as in the Hanbury-Brown-Twiss interferometer [85] (also see Refs. 14, 15, and 86). Following Noh et al. [47], we denote by a and 2 the photon annihilation operators, describing the field at the two input ports, and by a and 04 the corresponding operators at the two output ports. Then... [Pg.445]

A famous example for the application of intensity-correlation interferometry in astronomy is the Hanbury Brown-Twiss interferometer sketched in Fig. 7.33. In its original form it was intended to measure the degree of spatial coherence of starlight (Vol. 1, Sect. 2.8) [945] from which diameters of stars could be determined. In its modern version it measures the degree of coherence and the photon statistics of laser radiation in the vicinity of the laser threshold [946]. [Pg.420]

Fig. 7.33 (a) Basic principle of the Hanbury Brown-Twiss intensity-correlation interferometer in astronomy (b) its application to measurements of spectral characteristics and statistics of laser radiation... [Pg.420]


See other pages where Hanbury Brown-Twiss interferometer is mentioned: [Pg.367]    [Pg.16]    [Pg.373]    [Pg.489]    [Pg.56]    [Pg.272]   
See also in sourсe #XX -- [ Pg.420 ]

See also in sourсe #XX -- [ Pg.721 ]




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Interferometer

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