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Smithey, D.T.1
Beck, M.2
Raymer, M.G.3
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2
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0027757441
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D. T. Smithey, M. Beck, J. Cooper, M. G. Raymer, and A. Faridani, Phys. Scr. T48, 35 (1993).
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Phys. Scr.
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Smithey, D.T.1
Beck, M.2
Cooper, J.3
Raymer, M.G.4
Faridani, A.5
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4
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85037193668
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For a review of homodyne tomography, cf. U. Leonhardt, Measuring the Quantum State of Light (Cambridge University Press, Cambridge, 1997)
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For a review of homodyne tomography, cf. U. Leonhardt, Measuring the Quantum State of Light (Cambridge University Press, Cambridge, 1997).
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5
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85037243571
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For a review of quantum-state reconstruction of light and matter, cf. D.-G. Welsch, W. Vogel, and T. Opatrný, Prog. Opt. (to be published)
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For a review of quantum-state reconstruction of light and matter, cf. D.-G. Welsch, W. Vogel, and T. Opatrný, Prog. Opt. (to be published).
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7
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0001372442
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A. Zucchetti, W. Vogel, M. Tasche, and D.-G. Welsch, Phys. Rev. A 54, 1678 (1996).
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Phys. Rev. A
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Zucchetti, A.1
Vogel, W.2
Tasche, M.3
Welsch, D.-G.4
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10
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U. Leonhardt, M. Munroe, T. Kiss, M. G. Raymer, and Th. Richter, Opt. Commun. 127, 144 (1996).
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Opt. Commun.
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Leonhardt, U.1
Munroe, M.2
Kiss, T.3
Raymer, M.G.4
Richter, T.5
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11
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0001096907
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S. Schiller, G. Breitenbach, S. F. Pereira, T. Müller, and J. Mlynek, Phys. Rev. Lett. 77, 2933 (1996)
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Schiller, S.1
Breitenbach, G.2
Pereira, S.F.3
Müller, T.4
Mlynek, J.5
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16
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0001339272
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T. Opatrný, D.-G. Welsch, S. Wallentowitz, and W. Vogel, J. Mod. Opt. 44, 2405 (1997).
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17
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5344249162
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M. Munroe, D. Boggavarapu, M. E. Anderson, and M. G. Raymer, Phys. Rev. A 52, R924 (1995).
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Munroe, M.1
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Raymer, M.G.4
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18
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85037227136
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We use the recursion relations (Formula presented) and (Formula presented) for the regular and irregular harmonic-oscillator eigenfunctions (Formula presented)
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We use the recursion relations (Formula presented) and (Formula presented) for the regular and irregular harmonic-oscillator eigenfunctions (Formula presented)
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19
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85037204958
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(Formula presented) since in Eq. (11) (Formula presented) because for all (Formula presented) either the regular or the irregular eigenfunctions are antisymmetric in (Formula presented) i.e., (Formula presented) or (Formula presented)
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(Formula presented) since in Eq. (11) (Formula presented) because for all (Formula presented) either the regular or the irregular eigenfunctions are antisymmetric in (Formula presented) i.e., (Formula presented) or (Formula presented)
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20
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85037201614
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The regular and irregular ground states read (Formula presented) and (Formula presented) with (Formula presented) being Dawson’s integral
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The regular and irregular ground states read (Formula presented) and (Formula presented) with (Formula presented) being Dawson’s integral 18.
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21
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85037225362
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Note that in this way we derived also the generating function (Formula presented) of the pattern functions, (Formula presented) as (Formula presented)
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Note that in this way we derived also the generating function (Formula presented) of the pattern functions, (Formula presented) as (Formula presented)
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22
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85037197246
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For an efficient numerical calculation of Dawson’s integral, (Formula presented) see Chap. 6.10 of W. H. Press, S. A. Teukolsky, W. T. Vetterling, and B. P. Flannery, Numerical Recipes in C (Cambridge University Press, Cambridge, 1995)
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For an efficient numerical calculation of Dawson’s integral, (Formula presented) see Chap. 6.10 of W. H. Press, S. A. Teukolsky, W. T. Vetterling, and B. P. Flannery, Numerical Recipes in C (Cambridge University Press, Cambridge, 1995).
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