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Volumn 89, Issue 2, 2001, Pages 1232-1250

Long-range Coulomb interactions in small Si devices. Part II. Effective electron mobility in thin-oxide structures

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EID: 0000805232     PISSN: 00218979     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.1332424     Document Type: Article
Times cited : (134)

References (53)
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    • I. I. Boiko and Yu. N. Sirenko, Zh. Tekh. Fiz. 58, 967 (1988) [ Sov. Phys. Tech. Phys. 33, 586 (1988)].
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    • for additional references
    • See also the review article by A. G. Rojo, J. Phys.: Condens. Matter 11, R31 (1999) for additional references.
    • (1999) J. Phys.: Condens. Matter , vol.11
    • Rojo, A.G.1
  • 21
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    • note
    • This is indeed what we found in the semiclassical work presented in Ref. 1: At least at high drain-to-source bias, short-range electron-electron collisions do not alter the characteristics of the devices, even at the smallest oxide thickness considered.
  • 30
    • 0003448505 scopus 로고
    • McGraw-Hill, New York
    • A. L. Fetter and J. D. Walecka, Quantum Theory of Many-Particle Systems (McGraw-Hill, New York, 1971), p. 305. See also Eqs. (73) and (74) of Ref. 20 and Eqs. (A5) and (A6) in Appendix A of M. V. Fischetti, S. E. Laux, and E. Crabbé, J. Appl. Phys. 78, 1058 (1995;) for the explicit expressions we have used in the two-and three-dimensional cases, respectively.
    • (1971) Quantum Theory of Many-Particle Systems , pp. 305
    • Fetter, A.L.1    Walecka, J.D.2
  • 31
    • 0001553399 scopus 로고
    • A. L. Fetter and J. D. Walecka, Quantum Theory of Many-Particle Systems (McGraw-Hill, New York, 1971), p. 305. See also Eqs. (73) and (74) of Ref. 20 and Eqs. (A5) and (A6) in Appendix A of M. V. Fischetti, S. E. Laux, and E. Crabbé, J. Appl. Phys. 78, 1058 (1995;) for the explicit expressions we have used in the two-and three-dimensional cases, respectively.
    • (1995) J. Appl. Phys. , vol.78 , pp. 1058
    • Fischetti, V.1    Laux, S.E.2    Crabbé, E.3
  • 37
    • 0346857458 scopus 로고    scopus 로고
    • note
    • Q≠0, Eq. (77) is the "plasmon-pole approximation" of the exact result.
  • 38
    • 0000891665 scopus 로고
    • For thicker oxides, as the coupling between gate and substrate weakens, the effect of the finite thickness of the inversion layer on the optical mode disappears, while its effect on the acoustic mode has the opposite trend of reducing its frequency. In the limit of infinitely thick oxides this has been shown by D. E. Beck and P. Kumar, Phys. Rev. B 13, 2859 (1976); 14, 5127(E) (1976). This work, as well as the work by A. K. Rajagopal, Phys. Rev. B 15, 4264 (1977) and by M. Jonson, J. Phys. C 9, 3055 (1977), also accounts for exchange-correlation effects, which we have ignored.
    • (1976) Phys. Rev. B , vol.13 , pp. 2859
    • Beck, D.E.1    Kumar, P.2
  • 39
    • 33744617156 scopus 로고
    • For thicker oxides, as the coupling between gate and substrate weakens, the effect of the finite thickness of the inversion layer on the optical mode disappears, while its effect on the acoustic mode has the opposite trend of reducing its frequency. In the limit of infinitely thick oxides this has been shown by D. E. Beck and P. Kumar, Phys. Rev. B 13, 2859 (1976); 14, 5127(E) (1976). This work, as well as the work by A. K. Rajagopal, Phys. Rev. B 15, 4264 (1977) and by M. Jonson, J. Phys. C 9, 3055 (1977), also accounts for exchange-correlation effects, which we have ignored.
    • (1976) Phys. Rev. B , vol.14
  • 40
    • 33744705816 scopus 로고
    • For thicker oxides, as the coupling between gate and substrate weakens, the effect of the finite thickness of the inversion layer on the optical mode disappears, while its effect on the acoustic mode has the opposite trend of reducing its frequency. In the limit of infinitely thick oxides this has been shown by D. E. Beck and P. Kumar, Phys. Rev. B 13, 2859 (1976); 14, 5127(E) (1976). This work, as well as the work by A. K. Rajagopal, Phys. Rev. B 15, 4264 (1977) and by M. Jonson, J. Phys. C 9, 3055 (1977), also accounts for exchange-correlation effects, which we have ignored.
    • (1977) Phys. Rev. B , vol.15 , pp. 4264
    • Rajagopal, A.K.1
  • 41
    • 0000891665 scopus 로고
    • For thicker oxides, as the coupling between gate and substrate weakens, the effect of the finite thickness of the inversion layer on the optical mode disappears, while its effect on the acoustic mode has the opposite trend of reducing its frequency. In the limit of infinitely thick oxides this has been shown by D. E. Beck and P. Kumar, Phys. Rev. B 13, 2859 (1976); 14, 5127(E) (1976). This work, as well as the work by A. K. Rajagopal, Phys. Rev. B 15, 4264 (1977) and by M. Jonson, J. Phys. C 9, 3055 (1977), also accounts for exchange-correlation effects, which we have ignored.
    • (1977) J. Phys. C , vol.9 , pp. 3055
    • Jonson, M.1


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