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Quantum Mechanics I

Kate E W&M Physics Qualifying Exam Graduate English 19 cards

Quantum Mechanics I

Cards in this deck (19)

  1. 1Time Independent Schrodinger Equation\[-\frac{\hbar^2}{2m}\frac{\partial^2\psi}{\partial x^2}+V\psi=E\psi\]
    \[\varphi(t)=e^{-iEt/\hbar}\]
  2. 2Energy Eigenvalues of the Infinite Square Well of Width \(a\)\[E_n=\frac{n^2\pi^2\hbar^2}{2ma^2}\]
  3. 3Eigenfunctions of the Infinite Square Well of Width \(a\)\[\psi_n(x)=\sqrt{\frac{2}{a}}\sin{\Big(\frac{n\pi}{a}x\Big)}\]
  4. 4Energy Eigenvalues of a Simple Harmonic Oscillator\[E_n=(n+1/2)\hbar\omega\]
  5. 5Eigenfunctions of a Simple Harmonic Oscillator\[\psi_n(x)=\Big(\frac{m\omega}{\pi\hbar}\Big)^{1/4}(a_+)^ne^{-(m\omega/2\hbar)x^2}\]
  6. 6Energy Eigenvalues of a Delta-Function Potential \(V(x)=-\alpha\delta(x)\)\[E=-\frac{m\alpha^2}{2\hbar^2}\]
  7. 7Eigenfunctions of a Delta-Function Potential \(V(x)=-\alpha\delta(x)\)\[\psi(x)=\frac{\sqrt{m\alpha}}{\hbar}e^{-m\alpha|x|/\hbar^2}\]
  8. 8\[[S_i,S_j]\]\[i\sum_k\epsilon_{ijk}\hbar S_k\]
  9. 9\[[x_i,p_j]\]\[i\hbar\delta_{ij}\]
  10. 10\[L_i,L_j\]\[i\hbar\sum_k\epsilon_{ijk}L_k\]
  11. 11\[[J_i,J_j]\]\[i\hbar\epsilon_{ijk}J_k\]
  12. 12Heisenberg Equation of Motion\[\frac{dA_H(t)}{dt}=\frac{1}{i\hbar}[A_H,H]\]
    \[[x_i,F(p)]=i\hbar\frac{\partial F}{\partial p_i}\]
    \[[p_i,G(x)]=-i\hbar\frac{\partial G}{\partial x_i}\]
  13. 13The Raising Operator\[a^{\dagger}=\sqrt{\frac{m\omega}{2\hbar}}\Big(x+\frac{ip}{m\omega}\Big)\]
    \[a^{\dagger}|n>=\sqrt{n+1}|n+1>\]
  14. 14The Lowering Operator\[a=\sqrt{\frac{m\omega}{2\hbar}}\Big(x-\frac{ip}{m\omega}\Big)\]
    \[a|n>=\sqrt{n}|n-1>\]
  15. 15\[J^2|j,m>\] \[J_z|j,m>\]\[j(j+1)\hbar^2|j,m>\]
    \[m\hbar|j,m>\]
  16. 16Spin Operator in Terms of the Pauli Operators\[S=\frac{\hbar}{2}\sigma\]
  17. 17Pauli MatricesPauli Matrices
  18. 18Orthogonality of Spherical Harmonics\[\int_0^{2\pi}d\phi\int_{-1}^1 d(\cos{\theta})Y_{l'}^{m'^*}(\theta,\phi)Y_{l}^{m}(\theta,\phi)=\delta_{ll'}\delta_{mm'}\]
  19. 19\[\boldsymbol{S}^2\]\[\boldsymbol{S_1}^2+\boldsymbol{S_2}^2+2\boldsymbol{S_1}\cdot\boldsymbol{S_2}\]

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Fall 2019 Krakauer
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Kate E
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