1. Prove that the matrices are hermitian or
anti-hermitian.
2. Prove that in order for the Dirac equation to be covariant (i.e., form-invariant) under the Lorentz group of trans formations with the constraint that the gamma-matrices are unchanged, the following relation must hold:
,
where
is the Lorentz-transformation matrix for the 4- vectors (x'=Lx) and
S is a unitary matrix that transforms the spinor as


1. Prove that the matrices are hermitian or anti-hermitian. 2. Prove that in order for the...
Extra HW 1. Prove the following properties of the density matrix. (a) ? is a Hermitian operator, i.e. ?-? (b) (A)) is invariant under unitary transformation. (c) Quantum Liouville's equation ih Ot (d) For pure states ?-? and for mixed states ?2 < p.
(L43*) Spin can be represented by matrices. Show that all three spin matrices l 0 2 0 -1 0),"2=2 1 have eigenvalues of +1/2h and -1/2h. Calculate the corresponding eigenfunctions which we will denote as α-and β-eigenfunctions corresponding to spin l/2 particles. Show that Sj can be determined by the commutation of the other two matrices sn and sm, n, maj. Prove that the (2×2) matrix sz-s' +ss+s, commutes with all spin matrices, ie. s2s,-sis-. Calculate the eigenvalues of s2....
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3.1 Rotations and Angular-Momentum Commutation Relations 159 We are particularly interested in an infinitesimal form of Ry: (3.1.4) where terms of order & and higher are ignored. Likewise, we have R0= ° :- R(E) = 1 (3.1.5) and (3.1.5b) - E01 which may be read from (3.1.4) by cyclic permutations of x, y, zthat is, x y , y → 2,2 → x....