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Sheng, P.1
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Van Haeringen, W.1
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3
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0003532234
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Academic, San Diego
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15
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5644289869
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note
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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.
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17
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0003433960
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Cambridge University Press, New York
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85087249701
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0. In other words, for the stability criterion the relevant system size is the physical thickness plus the extrapolation length
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0. In other words, for the stability criterion the relevant system size is the physical thickness plus the extrapolation length.
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19
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5644286600
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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
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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.
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20
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0003434416
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Oxford University Press, New York
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See, for instance, A.E. Siegman, Lasers (Oxford University Press, New York, 1986).
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Lasers
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Siegman, A.E.1
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5644244696
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Ph.D. thesis, University of Amsterdam
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D.S. Wiersma, Ph.D. thesis, University of Amsterdam, 1995.
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Wiersma, D.S.1
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22
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85087250536
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i, which would result in more efficient pumping
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i, which would result in more efficient pumping.
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24
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0000613407
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D.S. Wiersma, M.P. van Albada, B.A. van Tiggelen, and A. Lagendijk, Phys. Rev. Lett. 74, 4193 (1995).
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26
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0000096004
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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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Zhang, Z.1
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