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 Consider the Schrödinger equation and the complex conjugate equation: 
If   is normalized to unity at the initial instant, it remains normalized at any later time. The mean value of a given observable   is equal at every instant to the scalar product 
and one has 
The last term of the right-hand side, 
 , is zero if   does not depend upon the time explicitly. 
Taking into account the Schrödinger equation and the hermiticity of the hamiltonian, one has 
Hence we obtain the general equation giving the time-dependence of the mean value of  : 
![$\displaystyle i\hbar\frac{d}{dt}<A>=<[A,H]> + i\hbar\left<\frac{\partial A}{\partial t} \right>$ $\displaystyle i\hbar\frac{d}{dt}<A>=<[A,H]> + i\hbar\left<\frac{\partial A}{\partial t} \right>$](https://images.physicslibrary.org/cache/objects/819/l2h/img11.png)  | 
(1) | 
 
 
 
When we replace  by the operator 
 , we obtain an analogous equation for the time-dependence of the characterisic function of the statistical distribution of  . 
In particular, for any variable   which commutes with the Hamiltonian 
and which does not depend explicitly upon the time, one has the result 
The mean value of   remains constant in time. More generally, if   commutes with  , the function 
  also commues with  , and, consequently 
The characteristic function, and hence the statistical distribution of the observable  , remain constant in time. 
By analogy with Classical Analytical mechanics,   is called a constant of the motion. In particular, if at the initial instant the wave function is an eigenfunction of   corresponding to a give eigenvalue  , this property continues to hold in the course of time. One says that   is a "good quantum number". If, in particular,   does not explicitly depend upon the time, and if the dynamical state of the system is represented at time   by an eigenfunction common to   and  , the wave function remains unchanged in the course of time, to within a phase factor. The energy and the variable   remain well defined and constant in time. 
[1] Messiah, Albert. "Quantum mechanics: volume I." Amsterdam, North-Holland Pub. Co.; New York, Interscience Publishers, 1961-62. 
This entry is a derivative of the Public domain work [1]. 
  
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