Spin 1 Particle in a time dependant magnetic field

In summary, the student is trying to find the hamiltonian and the time-dependent Schrodinger equation for a system of three particles. However, they are not sure how to start solving the equation. They are also lost on how to calculate the hamiltonian or the coefficients c_1, c_2, and c_3.
  • #1
richyw
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Homework Statement



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Homework Equations



[tex]\left|\psi ,t\right\rangle=\sum_i c_i(t)e^{-\frac{i E_n t}{\hbar}}\left|n\right\rangle[/tex]

The Attempt at a Solution



I'm quite lost on how to even start this. I can work out that the hamiltonian is[tex]H(t)=\gamma S_z B(t)[/tex]Then I tried to put that into the time-dependant shrodinger equation. [tex]-i\hbar \frac{d}{dt}\left|\psi(t)\right\rangle=H(t)\left|\psi(t)\right\rangle[/tex]but I am not really sure if this is correct or even how to begin solving this.
 
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  • #2
richyw said:
I'm quite lost on how to even start this. I can work out that the hamiltonian is[tex]H(t)=\gamma S_z B(t)[/tex]Then I tried to put that into the time-dependant shrodinger equation. [tex]-i\hbar \frac{d}{dt}\left|\psi(t)\right\rangle=H(t)\left|\psi(t)\right\rangle[/tex]but I am not really sure if this is correct or even how to begin solving this.

I think you're on the right track. After substituting the given expression for |ψ(t)> into the Schrodinger equation, you should be able to get a differential equation for each coefficient ci(t).
 
  • #3
I'm still stuck on this one actually. I don't think I am substituting [itex]\left|\psi ,t \right\rangle[/itex] into the equation properly. How to I get [itex]\psi (t)[/itex] from [itex]\left|\psi ,t \right\rangle[/itex]?
 
  • #4
wait, can I say[tex]\left| \psi ,t \right\rangle=c_1(t)\left| 1,1 \right\rangle+c_2(t)\left| 1,0 \right\rangle+c_3(t)\left| 1,-1 \right\rangle[/tex][tex]\left| \psi ,t \right\rangle=c_1(t)\left(\begin{matrix}1 \\ 0 \\ 0\end{matrix}\right)+c_2(t)\left(\begin{matrix}0 \\ 1 \\ 0\end{matrix}\right)+c_3(t)\left(\begin{matrix}0 \\ 0 \\ 1\end{matrix}\right)[/tex][tex]\left| \psi ,t \right\rangle=\left(\begin{matrix} c_1(t) \\ c_2(t) \\ c_3(t)\end{matrix}\right)[/tex]
 
  • #5
and then [tex]i\hbar\frac{d}{dt}\left| \psi ,t \right\rangle=\gamma B(t) S_z\left| \psi ,t \right\rangle[/tex]
 
  • #6
[tex]i\hbar \left(\begin{matrix} c'_1(t) \\ c'_2(t) \\ c'_3(t)\end{matrix}\right)=\hbar\gamma B(t)\left(\begin{matrix}1 & 0&0\\0&0&0\\0&0&-1\\\end{matrix}\right)\left(\begin{matrix} c_1(t) \\ c_2(t) \\ c_3(t)\end{matrix}\right)[/tex]
 
  • #7
and then get [tex]c'_1(t)=-i\gamma B(t) c_1(t)[/tex][tex]c'_2(t)=0[/tex][tex]c'_3(t)=i\gamma B(t) c_3(t)[/tex]
 
  • #8
Yes, that looks good. Just have to solve each of these equations.
 
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FAQ: Spin 1 Particle in a time dependant magnetic field

What is a spin 1 particle?

A spin 1 particle is a type of elementary particle that has a spin quantum number of 1. This means that it has angular momentum and behaves like a tiny spinning top.

How does a time dependent magnetic field affect a spin 1 particle?

A time dependent magnetic field can change the orientation of a spin 1 particle's spin axis, causing it to precess or rotate in a specific direction. This phenomenon is known as Larmor precession.

What is the relationship between the magnetic field and the precession frequency of a spin 1 particle?

The precession frequency of a spin 1 particle is directly proportional to the strength of the magnetic field. This means that a stronger magnetic field will cause the particle to precess at a higher frequency.

Can a spin 1 particle exist in a time independent magnetic field?

Yes, a spin 1 particle can exist in a time independent magnetic field. However, its spin axis will remain constant and will not precess unless the magnetic field becomes time dependent.

What are the applications of studying spin 1 particles in time dependent magnetic fields?

Studying spin 1 particles in time dependent magnetic fields can help us understand the behavior of particles in quantum mechanics and can also have applications in technologies such as magnetic resonance imaging (MRI) and quantum computing.

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