Solving Quantum Rigid Rotator Problems - Sam

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SUMMARY

The discussion focuses on solving quantum rigid rotator problems, specifically a two-dimensional rigid rotator in the xy plane with angular momentum defined as Lz=-ih ∂/∂t. The key equations include hbar^2/(2I) d^2Φ(φ)/(dφ^2) = EΦ(φ) and dT(t)/(dt) = -iE(T(t))/hbar, where E represents the separation constant. The allowed energy values are derived as E=hbar^2m^2/(2I) for integer values of m, and the normalization of the wave function Φ(φ)=e^imφ is also discussed. The relationship between energy and the angular momentum operator L is established as E=L^2/(2mr^2).

PREREQUISITES
  • Understanding of quantum mechanics principles, specifically rigid rotators.
  • Familiarity with cylindrical coordinates in physics.
  • Knowledge of wave functions and normalization techniques.
  • Proficiency in solving differential equations related to quantum systems.
NEXT STEPS
  • Study the derivation of the Schrödinger equation for rigid rotators.
  • Learn about angular momentum operators in quantum mechanics.
  • Explore normalization techniques for wave functions in quantum systems.
  • Investigate the implications of single-valuedness in quantum mechanics.
USEFUL FOR

Students preparing for physics exams, particularly those focusing on quantum mechanics, as well as educators and researchers interested in quantum rigid rotator problems.

Sam Johnson
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Hi! I have been doing some problems to prepare for my physics final and came across this series which I have not been able to solve and was hoping someone here might be able to help me out with.

The problem is that of a two-dimensional rigid rotator which rotates in the xy plane and has angular momentum Lz=-ih ∂/∂t

It is in cylindrical coordinates.


Given:

- hbar^2/(2I) d^2Φ(φ)/(dφ^2) = EΦ(φ)

and

dT(t)/(dt) = -iE(T(t))/hbar

Here E is the separation constant; also, Φ(φ)T(t)=Ψ(φ,t)

First of all we must solve the equation for the time dependence of the wave function just listed.

Second show that the separation constant is the total energy.

------------------------------
One solution is Φ(φ)=e^imφ where m = sqrt[2IE]/hbar
------------------------------

Third apply the condition of single-valuedness.

------------------------------
The allowed values of energy are E=hbar^2m^2/(2I) when abs[m] = 0,1,2...
------------------------------

Fourth normalize the funcions Φ(φ)=e^imφ found previously.


I SINCERERLY appreciate any help!
Sam
 
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if Lz=(h/i)*(∂/∂φ), how can u write the energy in terms of the operator Lz?

E=-hbar/(2*I)d^2Φ(φ)/(dφ^2)=EΦ(φ)
 
All you have to do to find the energy in terms of L is:

E=.5Iω^2 +0potential = .5I(L/I)^2 = L^2/(2mr^2)

because L=Iω and I=mr^2.

Thanks,
Sam
 

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