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Volumn 54, Issue 4 SUPPL. B, 1996, Pages 4256-4265

Light diffusion with gain and random lasers

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EID: 4243485552     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/physreve.54.4256     Document Type: Article
Times cited : (523)

References (26)
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    • (1990) Classical Wave Localization
    • Sheng, P.1
  • 2
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    • For recent reviews, see Classical Wave Localization, edited by P. Sheng (World Scientific, Singapore, 1990); Analogies in Optics and Micro Electronics, edited by W. van Haeringen and D. Lenstra (Kluwer, Dordrecht, 1990); P. Sheng, Introduction to Wave Scattering, Localization, and Mesoscopic Phenomena (Academic, San Diego, 1995).
    • (1990) Analogies in Optics and Micro Electronics
    • Van Haeringen, W.1    Lenstra, D.2
  • 3
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    • Academic, San Diego
    • For recent reviews, see Classical Wave Localization, edited by P. Sheng (World Scientific, Singapore, 1990); Analogies in Optics and Micro Electronics, edited by W. van Haeringen and D. Lenstra (Kluwer, Dordrecht, 1990); P. Sheng, Introduction to Wave Scattering, Localization, and Mesoscopic Phenomena (Academic, San Diego, 1995).
    • (1995) Introduction to Wave Scattering, Localization, and Mesoscopic Phenomena
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    • Y. Kuga and A. Ishimaru, J. Opt. Soc. Am. A 8, 831 (1984); M.P. van Albada and A. Lagendijk, Phys. Rev. Lett. 55, 2692 (1985); P.E. Wolf and G. Maret, ibid. 55, 2696 (1985).
    • (1984) J. Opt. Soc. Am. A , vol.8 , pp. 831
    • Kuga, Y.1    Ishimaru, A.2
  • 5
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    • Y. Kuga and A. Ishimaru, J. Opt. Soc. Am. A 8, 831 (1984); M.P. van Albada and A. Lagendijk, Phys. Rev. Lett. 55, 2692 (1985); P.E. Wolf and G. Maret, ibid. 55, 2696 (1985).
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  • 6
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    • Y. Kuga and A. Ishimaru, J. Opt. Soc. Am. A 8, 831 (1984); M.P. van Albada and A. Lagendijk, Phys. Rev. Lett. 55, 2692 (1985); P.E. Wolf and G. Maret, ibid. 55, 2696 (1985).
    • (1985) Phys. Rev. Lett. , vol.55 , pp. 2696
    • Wolf, P.E.1    Maret, G.2
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    • V.S. Letokhov, Zh. Éksp. Teor. Fiz. 53, 1442 (1967) [Sov. Phys. JETP 26, 835 (1968)].
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  • 15
    • 5644289869 scopus 로고    scopus 로고
    • note
    • Note that direct absorption and stimulated emission of pump, respectively, probe without scattering is not taken into account. This is justified due to the fact that in our case the scattering is always much stronger than the absorption and stimulated emission. Taking direct absorption and stimulated emission into account requires adding (two) appropriate terms to Eq. (6), and allowing the extinction coefficient in Eqs. (8) and (9) to become place and time dependent.
  • 18
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    • 0. In other words, for the stability criterion the relevant system size is the physical thickness plus the extrapolation length
    • 0. In other words, for the stability criterion the relevant system size is the physical thickness plus the extrapolation length.
  • 19
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    • At large sample thicknesses, the spatial profile of the pump energy density starts to play a role, which makes the relation between the obtained excitation level and the sample thickness more complex
    • At large sample thicknesses, the spatial profile of the pump energy density starts to play a role, which makes the relation between the obtained excitation level and the sample thickness more complex.
  • 20
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    • Oxford University Press, New York
    • See, for instance, A.E. Siegman, Lasers (Oxford University Press, New York, 1986).
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    • i, which would result in more efficient pumping
    • i, which would result in more efficient pumping.
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    • P. Pradhan and N. Kumar, Phys. Rev. B 50, 9644 (1994); Z. Zhang, ibid. 52, 7960 (1995).
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