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Volumn 81, Issue 15, 2010, Pages

Optical injection and control in germanium: Thirty-band kp theory

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EID: 77955350052     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.81.155215     Document Type: Article
Times cited : (63)

References (56)
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    • By symmetry of the diamond structure, the nonzero momentum matrix elements are given by: S | p x | X = S | p y | Y = S | p z | Z, X | p y | z = Y | p z | x = Z | p x | y = X | p z | y = Y | p x | z = Z | p y | x, D z | p x | X = D z | p y | Y = - 1 2 D z | p z | Z = - 1 √ 3 D x | p x | X = 1 √ 3 D x | p y | Y, and complex conjugates of these relations.
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    • For details of the germanium band structure, see Fig. 4 of Ref..
    • For details of the germanium band structure, see Fig. 4 of Ref..
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    • This is the simplest orientation. For the same crystal cut, one can get a slightly larger current injection with beams polarized along 110 ; the largest current injection is achieved with beams polarized along 111 (Ref.). We choose to present 100 polarization results to keep the expressions simple
    • This is the simplest orientation. For the same crystal cut, one can get a slightly larger current injection with beams polarized along 110 ; the largest current injection is achieved with beams polarized along 111 (Ref.). We choose to present 100 polarization results to keep the expressions simple.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.