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    The commutator [x2,px2] is equal to [x: position operator, px: momentum operator]\text{The comm
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    The commutator [x2,px2] is equal to [x: position operator, px: momentum operator]\text{The commutator } [x^2, p_x^2] \text{ is equal to } [x: \text{ position operator, } p_x: \text{ momentum operator}]


    A.

    2xi2x i \hbar

    B.

    2i2 i \hbar

    C.

    4i4 i \hbar​​

    D.

    2i(xpx+pxx)2 i \hbar (x p_x + p_x x)

    Correct option is D

    If two observables  A and  B have linear operators 

    , the commutator is defined by,

    The commutator is itself a (composite) operator. Acting the commutator on  ψ gives:

    If  ψ is an eigenfunction with eigenvalues  a and  b for observables  A and  B respectively, and if the operators commute:

    then the observables  A and  B can be measured simultaneously with infinite precision, i.e., uncertainties ΔA=0

    , ΔB=0simultaneously.  ψ is then said to be the simultaneous eigenfunction of A and B. To illustrate this:


    It shows that measurement of A and B does not cause any shift of state, i.e., initial and final states are same (no disturbance due to measurement). Suppose we measure A to get value a. We then measure B to get the value b. We measure A again. We still get the same value a. Clearly the state ( ψ) of the system is not destroyed and so we are able to measure A and B simultaneously with infinite precision.
    If the operators do not commute:

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