The text computed and quoted the other commutators of the Lorentz algebra

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Relativity & Gravitation · Special relativity: spacetime and kinematics

Invariance, Ch Lie groups and Lie algebras: rotations, SU(2) and the double cover

Problem

The text computed [Kx,Ky][K_x,K_y] and quoted the other commutators of the Lorentz algebra. Work in the coordinates (ct,x,y,z)(ct,x,y,z) with the active boosts Λx(ϕ)=e−iϕKx\Lambda_x(\phi)=e^{-i\phi K_x} and Λy(ϕ)=e−iϕKy\Lambda_y(\phi)=e^{-i\phi K_y}, where KyK_y has ii in the (ct,y)(ct,y) and (y,ct)(y,ct) entries and zeros elsewhere, and let JxJ_x be the 3×33\times3 rotation generator placed in the spatial block. ((a)) Multiply the 4×44\times4 matrices to find [Jx,Ky][J_x,K_y], and show that it equals iKziK_z. ((b)) Let A=−iαKxA=-i\alpha K_x and B=−iβKyB=-i\beta K_y, with rapidities α\alpha and β\beta. Use eAeB=eA+B+12[A,B]+⋯e^Ae^B=e^{A+B+\frac12[A,B]+\cdots} to write Λx(α)Λy(β)\Lambda_x(\alpha)\Lambda_y(\beta) and Λy(β)Λx(α)\Lambda_y(\beta)\Lambda_x(\alpha) each as a single exponential, correct to second order in the rapidities. Show that the two exponents differ only by a multiple of JzJ_z, and find it. ((c)) Take as given that e−i(αKx+βKy)e^{-i(\alpha K_x+\beta K_y)} is a single boost, and that eX+Y=eXeYe^{X+Y}=e^Xe^Y to second order when XX is of first order and YY of second order in the rapidities. What does Λx(α)Λy(β)\Lambda_x(\alpha)\Lambda_y(\beta) do to a particle at rest, besides setting it moving? Give the angle and sense of the effect for α=β=0.20\alpha=\beta=0.20.

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