Название | Quantum Mechanics, Volume 3 |
---|---|
Автор произведения | Claude Cohen-Tannoudji |
Жанр | Физика |
Серия | |
Издательство | Физика |
Год выпуска | 0 |
isbn | 9783527822751 |
(45)
We follow the same steps as in § 2-a of Complement EXV: we use the mean field approximation to replace the computation of the average value of a two-particle operator by that of average values for one-particle operators. We can, for example, use relation (43) of Complement BXV, which shows that:
(46)
We then get:
(47)
Which, according to (40), can also be written as:
where Pex is the exchange operator between particles 1 and 2. Since:
(49)
and as the operators (1) and
(2) are diagonal in the basis |θi〉, we can write the right-hand side of (48) as:
(50)
which is simply a (double) trace on two particles 1 and 2. This leads to:
As announced above, the average value of the two-particle operator Ĝ can be expressed, within the Hartree-Fock approximation, in terms of the one-particle reduced density operator (1); this relation is not linear.
Comment:
The analogy with the computations of Complement Exv becomes obvious if we regroup its equations (57) and (58) and write:
Replacing W2(1, 2) by G, we get a relation very similar to (51), except for the fact that the projectors PN must be replaced by the one-particle operators . In § 3-d, we shall come back to the correspondence between the zero and non-zero temperature results.
2-c. Variational grand potential
We now have to compute the grand potential written in (30). As the exponential form (28) for the trial operator makes it easy to compute ln
, we see that the terms in μ
cancel out, and we get:
(53)
We now have to compute the average energy, with the density operator , of the difference between the Hamiltonians Ĥ and
respectively defined by (1) and (25).
We first compute the trace:
(54)
starting with the kinetic energy contribution Ĥ0 in (1). We call K0 the individual kinetic energy operator:
(55)
(m is the particle mass). Equality (43) applied to Ĥ0 yields the average kinetic energy when the system is described by :
This result is easily interpreted; each individual state contributes its average kinetic energy, multiplied by its population.
The computation of the average value follows the same steps:
(as in Complement EXV, operator V1 is the one-particle external potential operator).
To complete the calculation of the average value of Ĥ, we now have to compute the trace , the average value of the interaction energy when the system is described by
. Using relation (51) we can write this average value as a double trace:
We now turn to the average value of . The calculation is simplified since
is, like Ĥ0,