thelonious
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Homework Statement
A particle of mass m is constrained to a circular loop of radius R in the x-y plane. The particle's position is given by the angle [itex]\varphi[/itex], measured with respect to the x axis. Given [itex]\Psi[/itex]([itex]\varphi[/itex],0), what is the probability that a measurement of the z-component of the angular momentum will yield +[itex]\hbar[/itex] at t=0?
Homework Equations
The classical Hamiltonian: H=Lz2 / 2mR2
The wave function: [itex]\Psi[/itex]([itex]\varphi[/itex],0)=(1/√2[itex]\pi[/itex])(cos[itex]\varphi[/itex]-sin[itex]\varphi[/itex])
The Attempt at a Solution
I need to find the eigenfunction of Lz with eigenvalue +[itex]\hbar[/itex].
Once I have this eigenfunction, the probability is given by P=|<+[itex]\hbar[/itex]|[itex]\Psi[/itex]>|2
My question: how do I begin to solve for this eigenfunction of Lz?