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25
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84894395621
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Following the standard usage, we denote by J both the mutual intensity and the Bessel functions of the first kind. No confusion should arise since Bessel functions have a numerical index.
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Following the standard usage, we denote by J both the mutual intensity and the Bessel functions of the first kind. No confusion should arise since Bessel functions have a numerical index.
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26
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2042540050
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Shape invariance and a universal form for the Gouy phase
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27
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84942362507
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Actually, a different coherent limit in which the mutual intensity has the form Ja(φ12)=I0 exp(imφ12) with integer m could be considered. This corresponds to illuminating the annulus with a coherent field carrying a vortex of order m. In that case, the intensity of the propagated field would have a Jm2 structure.
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Actually, a different coherent limit in which the mutual intensity has the form Ja(φ12)=I0 exp(imφ12) with integer m could be considered. This corresponds to illuminating the annulus with a coherent field carrying a vortex of order m. In that case, the intensity of the propagated field would have a Jm2 structure.
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28
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84894393737
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Quadratic phase factors can be compensated for through the use of a suitable lens
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Quadratic phase factors can be compensated for through the use of a suitable lens.
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29
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84894396067
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Stability performances allowing such an approximation are often ensured by commercial lasers
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Stability performances allowing such an approximation are often ensured by commercial lasers.
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30
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33144487316
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Finite-elementary-source model for partially coherent radiation
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31
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84894392224
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In principle, each term could be multiplied by an arbitrary phase factor
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In principle, each term could be multiplied by an arbitrary phase factor.
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