1992
DOI: 10.1016/0030-4018(92)90430-y
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Trochoson

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Cited by 88 publications
(22 citation statements)
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“…Using the identity J:xpLtneJexp(tkrp/z)cos(e)Jde = 2Tr(-tfexp(tn&J(krp/z) (4) we can represent the diffraction integral in the following form: U(p,,z) = t)fl+1exp(tn)CJexP(tkr(r)÷r2/2z1;J(krp/z)rdr (5) The axial amplitude distribution, for n=O is given by U(O,z) = _i)fl+1exP(tn)CJexp(tk[(r)+r2/2zJ)rdr (6) and for is equal to 0.…”
Section: Discussionmentioning
confidence: 99%
“…Using the identity J:xpLtneJexp(tkrp/z)cos(e)Jde = 2Tr(-tfexp(tn&J(krp/z) (4) we can represent the diffraction integral in the following form: U(p,,z) = t)fl+1exp(tn)CJexP(tkr(r)÷r2/2z1;J(krp/z)rdr (5) The axial amplitude distribution, for n=O is given by U(O,z) = _i)fl+1exP(tn)CJexp(tk[(r)+r2/2zJ)rdr (6) and for is equal to 0.…”
Section: Discussionmentioning
confidence: 99%
“…the OAM projection onto the z axis takes the form: Expression (51) coincides, up to a constant, with the first term in equation (19) derived in [13].…”
Section: The Orbital Angular Momentum Of the Bbmentioning
confidence: 97%
“…Thus, an optical axis segment, at which the BB formed by a finite phase DOE, preserves its modal character, starts from some z min , needed to form the beam, and ends at <2z max , with z max given by equation (52). In [19,32] it was proposed that the multi-mode BB should be formed by use of a DOE whose transmission function is a linear combination of an axicon and an angular harmonic:…”
Section: Doe Synthesismentioning
confidence: 99%
“…As a rule vortical beams are created by inserting vortex phase singularity into initial plane beam using diffractive optical elements. Particularly, spiral phase plates, vortical axicons, vortical zone plates, binary forked gratings are used to create vortical beams [4][5][6] .…”
Section: Introductionmentioning
confidence: 99%