1.) Any Hermitian operator that commutes with the Hamiltonian is a generator of some symmetry (with a conserved quantity). Consider operator  = ( ) and Hamiltonian Ĥ (* ). Note [ ‚Ĥ] = 0. What is corresponding %3D symmetry operation? (Hint: compute exp(-i0Â).)
1.) Any Hermitian operator that commutes with the Hamiltonian is a generator of some symmetry (with a conserved quantity). Consider operator  = ( ) and Hamiltonian Ĥ (* ). Note [ ‚Ĥ] = 0. What is corresponding %3D symmetry operation? (Hint: compute exp(-i0Â).)
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![1.) Any Hermitian operator that commutes with the Hamiltonian is a generator of some
symmetry (with a conserved quantity). Consider operator  = ( )
and
Hamiltonian Ĥ
(* ). Note [Â ‚Ĥ] = 0. What is corresponding
%3D
symmetry operation? (Hint: compute exp(-i0Â).)](/v2/_next/image?url=https%3A%2F%2Fcontent.bartleby.com%2Fqna-images%2Fquestion%2F8313d306-6761-472a-88fa-c4e571fde3ad%2Fd71c8b3a-929e-4612-9e73-b00378e721f3%2F8dsdhc8_processed.png&w=3840&q=75)
Transcribed Image Text:1.) Any Hermitian operator that commutes with the Hamiltonian is a generator of some
symmetry (with a conserved quantity). Consider operator  = ( )
and
Hamiltonian Ĥ
(* ). Note [Â ‚Ĥ] = 0. What is corresponding
%3D
symmetry operation? (Hint: compute exp(-i0Â).)
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