| 11. | A fundamental difference between classical and quantum mechanics concerns the concept of indistinguishability of identical particles.
|
| 12. | The permutations of identical particles constitute the symmetric group "'S " '.
|
| 13. | With identical particles, the state described by ought to be indistinguishable from the state described by.
|
| 14. | Fermi Dirac ( F D ) statistics apply to identical particles with half-integer energy states.
|
| 15. | Depending on the value of the spin, identical particles split into two different classes, fermions and bosons.
|
| 16. | When there are external lines, the amplitudes are antisymmetric when two Fermi insertions for identical particles are interchanged.
|
| 17. | In other words, in an antisymmetric state two identical particles cannot occupy the same single-particle states.
|
| 18. | Read Gibbs paradox, and Identical particles . talk ) 18 : 00, 29 May 2013 ( UTC)
|
| 19. | It appears to be a fact of nature that identical particles do not occupy states of a mixed symmetry, such as
|
| 20. | For non-interacting identical particles, the potential is a sum but the wavefunction is a sum over permutations of products.
|
