Suvarna Garge (Editor)

Levinson's Theorem

Updated on
Edit
Like
Comment
Share on FacebookTweet on TwitterShare on LinkedInShare on Reddit

Levinson's Theorem is an important theorem in non-relativistic quantum scattering theory. It relates the number of bound states of a potential to the difference in phase of a scattered wave at zero and infinite energies. It was published by Norman Levinson in 1949.

Statement of theorem

The difference in phase of a scattered wave at zero energy, ϕ l ( 0 ) , and infinite energy, ϕ l ( ) , for a spherically symmetric potential V ( r ) is related to the number of bound states n ¯ l by:

ϕ l ( 0 ) ϕ l ( ) = ( n + 1 2 N ) π  

where N = 1 for s -wave scattering, N = 2 for l 1 and N = 0 otherwise. Furthermore, the potential must satisfy the following asymptotic conditions:

r 2 | V ( r ) | 0  at  r 0 r 3 | V ( r ) | 0  at  r

References

Levinson's Theorem Wikipedia