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**Unformatted text preview: **Physics 216 Solutions to Problem Set 2 Spring 2010 1. We wish to determine the correct form of the Schrodinger equation for a spin- 1 2 particle in an external electromagnetic field. The wavefunction for a spin- 1 2 particle is a two-component spinor wave function, where each component is an independent function of vectorx and t . Thus, the Hamiltonian must be a 2 2 matrix, whose elements are also operators on the Hilbert space of square integrable functions. (a) First consider a free spin- 1 2 particle. We demand that H is rotationally invari- ant. Two candidate Hamiltonians are: ( i ) H 1 = vector p 2 2 m I , ( ii ) H 2 = ( vector vector p ) 2 2 m . where I is the 2 2 identity matrix. Show that H 1 and H 2 are in fact identical. The Pauli matrices, i satisfy the identity, i j = ij I + i ijk k , (1) where there is an implicit sum over the repeated index k . Note that if we multiply eq. (1) by A i B j and sum over i and j , we recover eq. (14.3.39) on p. 382 of Shankar. Moreover, if A = B = p , then the resulting identity is ( vector vector p ) 2 = vector p 2 I , since ijk p i p j = 0 follows from the fact that ijk is antisymmetric under the interchange of i and j whereas p i p j is symmetric under the interchange of i and j . Hence, if follows that the two candidate Hamiltonians H 1 and H 2 are identical. (b) Consider now a spin- 1 2 particle with charge q in an external electromagnetic field. Using the principle of minimal coupling, deduce the Hamiltonians corresponding to (i) and (ii) above, which include the dependence on the scalar potential ( vectorx , t ) and the vector potential vector A ( vectorx , t ) [do not choose a specific gauge]. Show that the two resulting Hamiltonians differ. In particular, in case (ii) above, a term in the Hamiltonian arises of the form ge 2 mc vector S vector B , where g is called the gfactor and vector S 1 2 planckover2pi1 vector is the spin operator. Using the fact that the electron has q = e , what value of g is predicted by this approach? Applying the principle of minimal substitution to H 1 , we obtain a spin-independent Hamiltonian, H = 1 2 m parenleftBigg vector p q vector A c parenrightBigg 2 I + q I , (2) 1 for a particle in an external electromagnetic field that derives from a scalar potential and a vector potential vector A . In contrast, if we apply the principle of minimal substitution to H 2 , we obtain H = 1 2 m vector parenleftBigg vector p q vector A c parenrightBigg vector parenleftBigg vector p q vector A c parenrightBigg + q I . We can simplify the first term above by writing: vector parenleftBigg vector p q vector A c parenrightBigg vector parenleftBigg vector p q vector A c parenrightBigg = summationdisplay ij i j parenleftbigg p i qA i c parenrightbiggparenleftbigg p j qA j c parenrightbigg = summationdisplay ijk ( ij I + i ijk k ) parenleftbigg p i...

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