Quantum mechanics vol 2

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Quantum mechanics vol 2

TEXTBOOK PHYSICSClaude Cohen-Tannoudji<$WILEY-VCHQuantum MechanicsUseful Identitiesc : scalar field: A. B. ... : vector fields.V X (VC) - 0V. (Vx A) =

Quantum mechanics vol 2 = 0V. (VC) = ACV X (Vx A) = V(V. A) - A AL = 7 r X Vil_£*-LÌr fir2ỉt:r2A X (B X C) = (A.C)B - (A . B)CA X (B X C) + B x (C X A) + c X (A X Bi = 0(A X

B). (C X l>) « (A . C)(B . D) - (A . r>)(B . C)(A X B)x (C X D) = T(A X B|. D]c - [(A X B). C]D = i(C X D). A]B - i(C X D). BJAV(CT)-cv^+rvcA (VH ưAr Quantum mechanics vol 2

+ 2(W). (V*z) I I A//V.(L’A)=-. ƠV.A+A.VƠVX ((/A)« Ơ VxA + (VC ) X AV.(AxB) « B.(VxA)— A.(VxB)V(A.B) = A X (Vx B) + B X (Vx A) 4- B.v AíA.V B Vx (A x

Quantum mechanics vol 2

B) = A (V. B) - B (V. A) + B. V A -A.v BN.B. :B .V A vector field whose components arc :(B VA;(i = X. V. c)www.pdfgrip.comAn elementary approach to th

TEXTBOOK PHYSICSClaude Cohen-Tannoudji<$WILEY-VCHQuantum MechanicsUseful Identitiesc : scalar field: A. B. ... : vector fields.V X (VC) - 0V. (Vx A) =

Quantum mechanics vol 2 a potential3.Definition of the scattering cross section4.Organization of this chapter

TEXTBOOK PHYSICSClaude Cohen-Tannoudji<$WILEY-VCHQuantum MechanicsUseful Identitiesc : scalar field: A. B. ... : vector fields.V X (VC) - 0V. (Vx A) =