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Volumn 13, Issue 1, 1996, Pages 96-100

Comparison of quasi-classical and quasi-static quantum approaches to the ionization of helium by a circularly polarized laser field

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EID: 0030553305     PISSN: 07403224     EISSN: None     Source Type: Journal    
DOI: 10.1364/JOSAB.13.000096     Document Type: Review
Times cited : (11)

References (26)
  • 5
    • 0000397342 scopus 로고
    • L. Wilets, Nucl. Phys. A 282, 341 (1977); 301, 250 (1979); 367, 459 (1981).
    • (1977) Nucl. Phys. A , vol.282 , pp. 341
    • Wilets, L.1
  • 6
    • 0000397342 scopus 로고
    • L. Wilets, Nucl. Phys. A 282, 341 (1977); 301, 250 (1979); 367, 459 (1981).
    • (1979) Nucl. Phys. A , vol.301 , pp. 250
  • 7
    • 4243061610 scopus 로고
    • L. Wilets, Nucl. Phys. A 282, 341 (1977); 301, 250 (1979); 367, 459 (1981).
    • (1981) Nucl. Phys. A , vol.367 , pp. 459
  • 12
    • 4243061609 scopus 로고
    • Shortwavelength V, P. B. Corkum and M. D. Perry, eds., Optical Society of America, Washington, D.C.
    • P. B. Corkum, in Shortwavelength V, P. B. Corkum and M. D. Perry, eds., Vol. 17 of OSA Proceedings Series (Optical Society of America, Washington, D.C., 1993), p. 83.
    • (1993) OSA Proceedings Series , vol.17 , pp. 83
    • Corkum, P.B.1
  • 17
    • 4243111684 scopus 로고    scopus 로고
    • We use atomic units throughout
    • We use atomic units throughout.
  • 18
    • 0001208558 scopus 로고
    • We use an analytic expression for the energy gain, Eq. (5), which is adequate for circular polarization and, consequently, an unaveraged formula for the tunneling rate, Eq. (2). Corkum's simulations use the formula for ionization given by M. V. Ammosov, N. B. Delone, and V. P. Krainov, Zh. Eksp. Teor. Fiz. 91, 2008 (1986) [Sov. Phys. JETP 64, 1191 (1986)], i.e., the quasi-static tunneling formula averaged by the radiation cycle and, consistently, the rotating-wave approximation for the electron motion.
    • (1986) Zh. Eksp. Teor. Fiz. , vol.91 , pp. 2008
    • Ammosov, M.V.1    Delone, N.B.2    Krainov, V.P.3
  • 19
    • 0001467967 scopus 로고
    • We use an analytic expression for the energy gain, Eq. (5), which is adequate for circular polarization and, consequently, an unaveraged formula for the tunneling rate, Eq. (2). Corkum's simulations use the formula for ionization given by M. V. Ammosov, N. B. Delone, and V. P. Krainov, Zh. Eksp. Teor. Fiz. 91, 2008 (1986) [Sov. Phys. JETP 64, 1191 (1986)], i.e., the quasi-static tunneling formula averaged by the radiation cycle and, consistently, the rotating-wave approximation for the electron motion.
    • (1986) Sov. Phys. JETP , vol.64 , pp. 1191
  • 20
    • 35949014495 scopus 로고
    • th for the final stage of ionization; however, the intermediate intensities can differ substantially. Our FMD simulations are closer to the second formula; however, the accuracy of the experiment is insufficient to permit us to distinguish between these versions of the OBI threshold.
    • (1989) Phys. Rev. Lett. , vol.63 , pp. 2212
    • Augst, S.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.