From the definition
"[A, B] = AB - BA \\neq 0"i.e. there exists such state
"A(B|\\psi\\rangle) \\neq B(A|\\psi\\rangle)"Moreover, if A is hermitian, there must exists an eigenstate of A, that is not an eigenstate of B. Proof by contradiction: let any eigenstate of A with the eigenvalue a is an eigenstate of B with the eigenvalue b. Then
and due to the fullness of the set of eigenvectors of a hermitian operator this equality is true for any state - wrong.
Hence there exists a state, in which both quantities A and B cannot be determined simultaneously.
Heisenberg's uncertainty principle: consider displacement
"\\Delta A = A - \\langle A \\rangle""\\langle\\Delta A^2 \\rangle= \\langle (A - \\langle A \\rangle)^2\\rangle = \\langle A^2 \\rangle - \\langle A \\rangle^2"
Then in any state
where we define
"i C \\equiv [A,B]"Hence C is hermitian:
Proof: consider
"\\langle (A -i\\alpha B)\\psi | (A - i\\alpha B) \\psi \\rangle = \\langle \\psi | (A +i\\alpha B) (A -i\\alpha B) |\\psi \\rangle \\geq 0""\\langle \\Delta A^2 - i \\alpha [\\Delta A, \\Delta B] +\\alpha^2\\Delta B^2 \\rangle \\geq 0"using
"[\\Delta A, \\Delta B] = [A,B] = iC"and the condition that the discriminant of the inequality with respect to alpha is non-negative:
"\\langle C \\rangle ^2 - 4 \\langle \\Delta A^2 \\rangle \\langle \\Delta B^2 \\rangle \\geq 0""\\langle \\Delta A^2 \\rangle \\langle \\Delta B^2 \\rangle \\geq\\frac{\\langle C \\rangle^2}{4}"For example, it quantum mechanics
"[x, p] = i\\hbar"Here A = x, B = p and C = h, hence
"\\langle \\Delta x^2 \\rangle \\langle \\Delta p^2 \\rangle \\geq\\frac{\\hbar^2}{4}"in any state.
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