If and are random variables and is their joint probability distribution, the marginal distribution of is given by
(6.54) |
(6.55) |
(6.56) |
(6.57) |
Classically the definition of the local (marginal) expectation values of observables is not ambiguous due to the commutativity of all observables. However, quantum mechanically to each way of calculating the expectation value in 6.59 corresponds a definition for the local expectation value and in general these definitions give different results
(6.59) |
In general the operator is not selfadjoint, so the definitions using Dirac brackets above are different. We can rephrase this by using the explicit expression for the density operator for a pure state . For a single wave function we get two definitions for the local expectation
(6.60) |
A good way to define the local expectation is to symmetrize the definitions
This definition has the property that is again a selfadjoint operator, hence the local expectation is real. This is the way in which the current is conventionally defined.
A special case which is not treated in this way is the definition of local expectation for an energy-like operator where is selfadjoint. Then we can define
However, in the Wigner formalism one usually defines energy as the second -moment in the form
With this definition for the local expectation value the local energy can become negative, as was observed in Wigner function simulations.
To calculate the Wigner transformation of we use a suitable definition for the star product. We get
(6.64) |
The question of marginalization is also discussed in [Wlo99].
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