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An operator that commutes with the Hamiltonian is called a conserved quantity or a constant of motion. When an operator ( A ) satisfies the commutation relation ([A, H] = 0), where ( H ) is the Hamiltonian, it indicates that the observable associated with ( A ) is conserved over time in a quantum system. This means that the expectation value of the observable does not change as the system evolves. Examples include total momentum and total angular momentum in isolated systems.

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