2001
DOI: 10.1134/1.1358450
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Diffraction of an ultrashort pulse by an aperture

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Cited by 15 publications
(12 citation statements)
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“…Application of this formula to the field behind the screen revealed [12,13,14] that it comprised only two components: V(P,t)= VG(P,t)+VB(P,t) -VG ('t) is the part of incident plane wave cut out of the initial one by the aperture; this part propagates in space without any change of its form, its transverse amplitude distribution is proportional to T(x, y); -VB ('t) is the wave excited by the edge of the aperture (or any other spatial heterogeneity of its transparency).…”
Section: Basic Relationsmentioning
confidence: 98%
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“…Application of this formula to the field behind the screen revealed [12,13,14] that it comprised only two components: V(P,t)= VG(P,t)+VB(P,t) -VG ('t) is the part of incident plane wave cut out of the initial one by the aperture; this part propagates in space without any change of its form, its transverse amplitude distribution is proportional to T(x, y); -VB ('t) is the wave excited by the edge of the aperture (or any other spatial heterogeneity of its transparency).…”
Section: Basic Relationsmentioning
confidence: 98%
“…The most popular diffraction problem of the elementary physical optics is that of the plane wave diffraction from the circular aperture of a radius. Solution of this problem using 8 -wave approach was given in [12,14] and contained only Position of observation points: P1 is before the screen, P2 is in the illuminated zone out of z-axis, P3 is at z-axis, P4 is in the shadow.…”
Section: Pulse Response Of the Circular Aperturementioning
confidence: 99%
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