Help particel in spherical delta potential well

valtorEN
Messages
36
Reaction score
0

Homework Statement



A particle with mass M is moving in a spherical delta-potential well, V(r)=-Vo*delta(r-a); Vo>0, a>0
Find the minimum Vo value so that there is at least 1 bounded eigenstate for the particle.

Homework Equations



looking through my quantum book (griffiths of course), i found a similar problem (4.9) i assume i put the potential into the 3d schrodinger eqn and solve from there

The Attempt at a Solution



solve Schrödinger's eq in 3d
i assume l=0
i "plug" -Vo*delta(r-a) into the radial equation, -h^2/2m*d^2/dr^2+[-Vo*delta(r-a)]u=Eu

after plug n chug, i get
d^2u/dr^2=-k^2u k=SQRT(2m(E+Vo)/h^2)u

so is the solution just sines and cosines? i am confused
what is the minimal value for a bound state(E<0)?

any and all feedback is much appreciated
cheers
nate
 
Physics news on Phys.org
ok i will solve myself as u all r morons
i will post solution here
 
Thanks for your txt insult. I'm sure you'll be well received next time you post. FYI I have been thinking about your problem. Your radial part of the schrodinger equation didn't look right and I wanted to wait till I had access to materials and was away from work before I answered. It's only a second derivative, not some other stuff I would expect in a 3d laplacian. In general you should be aware that the delta function is zero except at r=a. So the solutions away from r=a are the same as with no potential, hence some form of damped exponential which I don't feel motivated to look up right now, u moron. And the presence of the delta function is generally a clue to look for a discontinuity in the first derivative. In a way in which I'm sure you can find yourself. Don't bother to post. I doubt anyone is interested.
 
hey dick at least u replied to my post!
thank u! i apologize but i am frustrated with this problem
i found a solution on the internet in a published paper that showed the 1D and 3D delta potential "attractive" well, but i am reluctant not to derive it myself
blah blah...
 
That's ok, but sometimes a question simply doesn't find someone who has the expertise to handle it. You want to splice two solutions corresponding to the same negative value of E together at r=a in such a way the there is a jump in the derivative at r=a corresponding to the size of V0. What is the form of solutions of SE corresponding to -E?
 
Last edited:
the solutions are of the form Ae^ikr+Be^ikr if E<Vo
 
Even if you weren't in three dimensions with spherical symmetry that should still be A*e^(-kr)*B*e^(kr) since it's a bound state (negative energy solution). But you are in 3d and so it's even more wrong. You looked up a solution for a 3d spherical 'square well' potential, right? Review it. You need the laplacian in spherical coordinates and the solutions are spherical bessel and hankel functions.
 
ah, i see, i see the solutions as
u(r)=A*r*jl(kr)+B*r*nl(kr)
where jl(kr) is the spherical Bessel function of order l
and nl(kr) is the spherical Neumann function or order l
is this correct?
 
I think you are getting there. My book calls it Hankel instead of Neumann, but I presume they are the same thing. You can set l=0 since you are looking for a lowest energy bound state. Now in the square well case you match the derivatives at the boundary. In this case the delta function tells you the derivatives don't match - but it does let you determine the difference of the derivatives as a function of V0.
 
  • #10
in my book they say that B= zero, sol u(r)=A*sin(kr)

now do i take that solution and use boundary conditions to solve for the minimum Vo

uin(a)=uout(a) and u'in(a)=u'out(a)?

do i use the radial equation to solve for Vo?
 
  • #11
Ok, but what's the exterior solution like? As I keep SHOUTING u'in(a)=u'out(a) is WRONG for this case. uin(a)=uout(a) is fine. Once you know u'in(a) you can figure out u'out(a) because their difference is controlled by the size of the delta function.
 
  • #12
the exterior has no potential, so i assume that V=0, so there is no wavefunction that exists outside the well.
 
  • #13
No potential doesn't mean no wavefunction. I've already agreed with you that uin(a)=uout(a). If that common value is non-zero its going to be difficult to claim there is no exterior wavefunction. The exterior solutions look exactly like they do for the square well. The only difference is the matching conditions between interior and exterior.
 
  • #14
so unlike the inf square well, the delta well does NOT meet the u'in(a)≠u'out(a)
boundary condition?
 
  • #15
so for r≥a the solutions are called modified spherical Bessel Functions (lol)

kl(kr) k^2=(2m|E|)/hbar^2

for boundary conditions (l=0)

r=a

(djl(Kr)/dr)/jl(Kr)|r=a- = (dkl(kr)/dr)/kl(kr)|r=a+

now since l=0, and j0(x)=sin(x)/x and k0(x)=e^-x/x (these are the solutions

that join together at the r=a condition right?!)

Kcot(Ka)=-k (l=0)

is this correct?

i found in a published article but did not derive as i do not have the math
 
  • #16
You have the outer solution right. But the inner solution also needs to be a negative energy V=0 solution. That makes it j0(ikr) not j0(kr). That comes out easy on the eye if you write it in exponentials, (e^(kr)-e^(-kr))/(2kr). So now you've got A*uin and B*uout to match. A*uin(ka)=B*uout(ka) and B*uout'(ka)-A*uin'(ka)=-2mV0*A*uin(ka)/(hbar^2). The latter is the term coming from the delta function. Use the first equation to eliminate A or B in the second one. Now you will notice if V0=0 there are no solutions! You can't match. What's the minimum V0 that will give a solution? I solved for V0 and took the limit as k->0 to find out. That's a LOT of hints.
 
  • #17
u'in(a)≠u'out(a)

uout(a)=C*e^-(l*a) (simple enough)

since l=0, the Neumann function nl(ka)=-B*a*(cos(a)/a)

uin(a)=-B(cos(a)) ?

u'in(a)B*sin(a)

u'out(a)=-l*a*C*e^(-l*a)

now i use u'in(a)≠u'out(a) to solve for Vo?

can i get away with setting A=0 and D=0 like in the finite spherical well (griffiths problem 4.9)?
 
  • #18
You didn't read my last post, did you? I actually TOLD you what uin was.
 
Back
Top