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Volumn 35, Issue 15, 1987, Pages 7959-7965

Macroscopic physics of the silicon inversion layer

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Indexed keywords


EID: 0000776042     PISSN: 01631829     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevB.35.7959     Document Type: Article
Times cited : (279)

References (9)
  • 1
    • 84926597623 scopus 로고    scopus 로고
    • Note that a macroscopic description in which the strong inversion layer is considered to be part of the surface can still be formulated.
  • 4
    • 0001652537 scopus 로고
    • The treatment in Sec. II of the double force follows more general work of, The Appendix outlines a similar development from a variational principle following, 11, 385, The connections between the two approaches and their relative merits have been discussed by H. F. Tiersten and J. L. Bleustein, in R. D. Mindlin and Applied Mechanics, edited by G. Herrmann (Pergamon, New York, 1974) p. 67., R. A. Toupin, Arch. Ration. Mech. Anal.
    • (1962) Arch. Ration. Mech. Anal. , vol.16 , pp. 325
    • Green, A.E.1    Rivlin, R.S.2
  • 6
    • 84926568889 scopus 로고    scopus 로고
    • A linear gradient dependence in (3.3), which could arise only in crystals which can exhibit pyroelectricity, is readily shown to be unimportant since it leaves the differential equations unaffected. Its sole effect would be on the boundary condition (2.16a), the physical significance of which is unclear.
  • 8
    • 84926586290 scopus 로고    scopus 로고
    • The reason for this can be seen by inserting (3.4a) into (2.16a) and expressing the fact that the electron density must be non-negative by the change of variable ρe -> - S2. Condition (2.16a) then demands the continuity bS ^ dS/ dn which is satisfied for all dS /dn when S=0.
  • 9
    • 84926605350 scopus 로고    scopus 로고
    • In the case when b is a function of electron density the form of (4.10a) changes slightly, being replaced by 2 sqrt b d over dx left ( sqrt b dS over dx right ) + S ( φ + φ0e - φb e star ) = 0 ~.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.