| |
The Number of Particles and the Phase as Canonically
Conjugate Variables |
We first look at the root mean square (rms) fluctuation, , in the number of particles in the BCS condensate before proceeding to show
that the number of particles operator and the phase are canonically conjugate dynamical variables. The rms in the BCS state is
found to be |
 |
(1) |
| (2) |
| Since |
 |
(3) |
 |
(4) |
| (5) |
|
|
|