suvendu said:
Thanks for the reply fluidistic.
But I did not get this point. Can you elaborate it a bit please?
"In 1 dimension, the bound states, if they exist, are between the infimum value of the potential and the lesser of the assymptotes (assuming they exist) for when x tends to positive infinity and negative infinity."...
Thanks
Yes, I should have said "the eigenvalues (energies) corresponding to the bound states" instead of bound states.
If you plot V(x) in function of x and if you assume that \lim _{x \to \pm \infty} V(x) =V_{\pm} exist (##V_+## and ##V_-## could be worth + and - infinity), then the energy(ies) of the bound states can exist only in the interval ## (V_0, V_{min}]## where ##V_0## is the infimum of V(x) and ##V_{min}## is the minimum between ##V_+## and ##V_-##.
Example 1: The quadratic potential (harmonic oscillator). In that case ##V_+=V_-=+\infty##. ##V_0=0## and ##V_{min}=+\infty##. So the energies corresponding to the bound states, if they exist, are in the interval ##(0, \infty )##.
Example 2: The non-inverted Gaussian potential. In that case ##V_0=0##, ##V_\pm = 0=V_{min}## so there are no energy possible. Hence no possible bound state.
Example 3:The inverted Gaussian potential. In that case ##V_0=-C## where C>0, ##V_{min}=0##. So the energies corresponding to bound states, if they exist, are between ##(-C,0]##. To ensure that they exist one would have to check whether the potential satisfies 2 criteria that I don't remember, plus that the condition ##\int _{-\infty} ^\infty V(x)dx <0##. This will always be satisfied with such an inverted Gaussian so there is at least 1 bound state with an energy between (-C,0].