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1
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0028304539
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J. Faist, F. Capasso, D. L. Sivco, C. Sirtori, A. L. Hutchinson, and A. Y. Cho, Science 264, 553 (1994).
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Faist, J.1
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Hutchinson, A.L.5
Cho, A.Y.6
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2
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0039374658
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F. Capasso, C. Gmachl, A. Tredicucci, A. L. Hutchinson, D. L. Sivco, and A. Y. Cho, Opt. Photonics News 10, 31 (1999).
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Capasso, F.1
Gmachl, C.2
Tredicucci, A.3
Hutchinson, A.L.4
Sivco, D.L.5
Cho, A.Y.6
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3
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0032517715
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C. Sirtori, P. Kruck, S. Barbieri, P. Collot, J. Nagle, M. Beck, J. Faist, and U. Oesterle, Appl. Phys. Lett. 73, 3486 (1998).
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Appl. Phys. Lett.
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Sirtori, C.1
Kruck, P.2
Barbieri, S.3
Collot, P.4
Nagle, J.5
Beck, M.6
Faist, J.7
Oesterle, U.8
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4
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0032614402
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G. Strasser, S. Gianordoli, L. Hvozdara, W. Schrenk, K. Unterrainer, and E. Gornik, Appl. Phys. Lett. 75, 1345 (1999).
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Strasser, G.1
Gianordoli, S.2
Hvozdara, L.3
Schrenk, W.4
Unterrainer, K.5
Gornik, E.6
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5
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0001610981
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C. Sirtori, P. Kruck, S. Barbieri, H. Page, J. Nagle, M. Beck, J. Faist and U. Oesterle, Appl. Phys. Lett. 75, 3911 (1999).
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Sirtori, C.1
Kruck, P.2
Barbieri, S.3
Page, H.4
Nagle, J.5
Beck, M.6
Faist, J.7
Oesterle, U.8
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6
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85037502682
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unpublished results: photocurrent measurements and calculations show that for I = 0 all carriers present by doping populate level 1 in the QCS, i.e., level 2 is empty
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S. Barbieri and C. Sirtori, unpublished results: photocurrent measurements and calculations show that for I = 0 all carriers present by doping populate level 1 in the QCS, i.e., level 2 is empty.
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Barbieri, S.1
Sirtori, C.2
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7
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0002515987
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R. A. Kaindl, D. C. Smith, M. Joschko, M. P. Hasselbeck, M. Woerner, and T. Elsaesser, Opt. Lett. 23, 861 (1998).
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Kaindl, R.A.1
Smith, D.C.2
Joschko, M.3
Hasselbeck, M.P.4
Woerner, M.5
Elsaesser, T.6
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8
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0000004252
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R. A. Kaindl, F. Eickemeyer, M. Woerner, and T. Elsaesser, Appl. Phys. Lett. 75, 1060 (1999).
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Kaindl, R.A.1
Eickemeyer, F.2
Woerner, M.3
Elsaesser, T.4
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9
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85037493914
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note
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The gain coefficient g of the bare active region characterizes the gain for light propagating in the plane of the quantum wells polarized parallel to the stack axis of the QCS.
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11
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36149007117
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The complex dielectric function of the n-type contacts was modeled by the Drude formula with plasma frequency and scattering rate accounting correctly for the free carrier absorption observed experimentally by, e.g., W. G. Spitzer and J. M. Whelan, Phys. Rev. 114, 59 (1959).
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(1959)
Phys. Rev.
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, pp. 59
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Spitzer, W.G.1
Whelan, J.M.2
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