Distortion of femtosecond pulses due to chromatic aberration in lenses
We study the pulse propagation through the singlet lens, by solving the diffraction integrals. Several peculiar features around the focal plane are shown, which the geometrical optics approximation cannot predict. Two conceptually different types of time distorsion are clearly distinguished: the gro...
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1992
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| Acceso en línea: | Registro en Scopus DOI Handle Registro en la Biblioteca Digital |
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| LEADER | 03552caa a22004457a 4500 | ||
|---|---|---|---|
| 001 | PAPER-19237 | ||
| 003 | AR-BaUEN | ||
| 005 | 20230518205035.0 | ||
| 008 | 190411s1992 xx ||||fo|||| 00| 0 eng|d | ||
| 024 | 7 | |2 scopus |a 2-s2.0-0038582309 | |
| 040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
| 030 | |a OPCOB | ||
| 100 | 1 | |a Federico, A. | |
| 245 | 1 | 0 | |a Distortion of femtosecond pulses due to chromatic aberration in lenses |
| 260 | |c 1992 | ||
| 270 | 1 | 0 | |m Federico, A.; Departamento de Fisica y Metrología, Instituto Nacional de Technología Industrial, Parque Miguletes, San Martin, CP 1650 Buenos Aires, Argentina |
| 506 | |2 openaire |e Política editorial | ||
| 504 | |a Szatmári, Kuhnle, Jasny, Schafer, (1989) Appl. Phys. B, 49, p. 239 | ||
| 504 | |a Szatmári, Kuhnle, Pulse front and pulse duration distortion in refractive optics, and its compensation (1988) Optics Communications, 69, p. 60 | ||
| 504 | |a Bor, (1988) J. Mod. Optics, 35, p. 1907 | ||
| 504 | |a Bor, Distortion of femtosecond laser pulses in lenses (1989) Optics Letters, 14, p. 119 | ||
| 504 | |a Bor, Gogolak, Szabo, Femtosecond-resolution pulse-front distortion measurement by time-of-flight interferometry (1989) Optics Letters, 14, p. 862 | ||
| 504 | |a Siegman, (1986) Laser, , University Science Books, Mill Valley | ||
| 504 | |a Martinez, (1988) IEEE J. Quantum Electron., 24, p. 2530 | ||
| 504 | |a Weisner, (1947) Introduction to the theory of equation, p. 134. , Macmillan, New York | ||
| 520 | 3 | |a We study the pulse propagation through the singlet lens, by solving the diffraction integrals. Several peculiar features around the focal plane are shown, which the geometrical optics approximation cannot predict. Two conceptually different types of time distorsion are clearly distinguished: the group dispersion that gives rise to a pulse broadening, and the concavity of the pulse that introduces a time delay across the beam section. Both of them result to be of the same order of magnitude, but appear at different locations. Analytical expressions are obtained for the maxima of the distortions and their position along the axis is discussed. © 1992. |l eng | |
| 536 | |a Detalles de la financiación: Consejo Nacional de Investigaciones Científicas y Técnicas | ||
| 536 | |a Detalles de la financiación: The authors wish to acknowledge partial support from grant OPID 31278001/88 from the CONICET. | ||
| 593 | |a Departamento de Fisica y Metrología, Instituto Nacional de Technología Industrial, Parque Miguletes, San Martin, CP 1650 Buenos Aires, Argentina | ||
| 593 | |a División Fisica del Sónido, Comisión Nacional de Energía Atómica, Libertador 8250, CP 1429 Buenos Aires, Argentina | ||
| 700 | 1 | |a Martinez, O. | |
| 773 | 0 | |d 1992 |g v. 91 |h pp. 104-110 |k n. 1-2 |p Opt Commun |x 00304018 |w (AR-BaUEN)CENRE-276 |t Optics Communications | |
| 856 | 4 | 1 | |u https://www.scopus.com/inward/record.uri?eid=2-s2.0-0038582309&doi=10.1016%2f0030-4018%2892%2990110-D&partnerID=40&md5=8d1ee9226d0e60214d88bdd6c8014a0f |y Registro en Scopus |
| 856 | 4 | 0 | |u https://doi.org/10.1016/0030-4018(92)90110-D |y DOI |
| 856 | 4 | 0 | |u https://hdl.handle.net/20.500.12110/paper_00304018_v91_n1-2_p104_Federico |y Handle |
| 856 | 4 | 0 | |u https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_00304018_v91_n1-2_p104_Federico |y Registro en la Biblioteca Digital |
| 961 | |a paper_00304018_v91_n1-2_p104_Federico |b paper |c PE | ||
| 962 | |a info:eu-repo/semantics/article |a info:ar-repo/semantics/artículo |b info:eu-repo/semantics/publishedVersion | ||
| 963 | |a VARI | ||
| 999 | |c 80190 | ||