What is the Interaction Hamiltonian in Quantum Mechanics?

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SUMMARY

The discussion focuses on the Interaction Hamiltonian in Quantum Mechanics, specifically the Hamiltonian \( H_{SE} \) defined as \( H_{SE}=\sum_{\alpha,j}\gamma(\alpha,j)P^{(\alpha)}\otimes\left|e_{j}\right\rangle\left\langle e_{j}\right| \). Participants analyze the expressions \( H_{SE}(\left|\beta,i_{\beta}\rangle\otimes\left|e_{j}\rangle) \) and \( \exp(-iH_{SE}t)(\left|\beta,i_{\beta}\rangle\otimes\left|e_{j}\rangle) \). The correct approach involves applying the Taylor expansion for the exponential and computing \( H_{SE}^2 \) before generalizing to \( H_{SE}^n \). Clarifications are made regarding the summation over indices and the use of Dirac notation.

PREREQUISITES
  • Understanding of Dirac notation in Quantum Mechanics
  • Familiarity with Hamiltonians and their role in quantum systems
  • Knowledge of Taylor series expansions
  • Basic concepts of quantum states and operators
NEXT STEPS
  • Study the derivation of the Interaction Hamiltonian in Quantum Mechanics
  • Learn about the application of Taylor series in quantum mechanics
  • Explore the properties of quantum operators and their commutation relations
  • Investigate the implications of different bases in quantum state representations
USEFUL FOR

Students and researchers in Quantum Mechanics, particularly those focusing on Hamiltonians and their applications in quantum systems. This discussion is beneficial for anyone learning Dirac notation and the mathematical foundations of quantum mechanics.

The thinker
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Homework Statement



Write out:

H_{SE}(\left|\right\beta,i_{\beta}\rangle\otimes\left|\right e_{j}\rangle)

and

exp(-iH_{SE}t)(\left|\right\beta,i_{\beta}\rangle\otimes\left|\right e_{j}\rangle)


Where:

H_{SE}=\sum_{\alpha,j}\gamma(\alpha,j)P^{(\alpha)}\otimes\left|e_{j}\right\rangle\left\langle e_{j}\right|

and

P^{(\alpha)}=\sum_{i_{\alpha}}\left|i_{\alpha}\right\rangle\left\langle i_{\alpha}\right|


(\left|i_{\alpha}\right\rangle can be written \left|\right\alpha,i_{\alpha}\rangle where alpha is a quantum number indexed by i_{\alpha} )

The Attempt at a Solution



For the first part I'm fairly sure it comes out as:

\sum_{\beta,j}\gamma(\beta,j)\left|\right\beta,i_{\beta}\rangle\otimes\left|\right e_{j}\rangle


But the second part I am not sure of, is it something like:

(Cos(t)-i\gamma(\alpha,j)Sin(t))(\left|\right\beta,i_{\beta}\rangle\otimes\left|\right e_{j}\rangle)


Thanks!
 
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In the first you should not summate over j (and you need to explain why ;))

For the second you first apply the Taylor expansion for the exponential. After that, compute:

H_{SE}^2 followed by generalizing this to H_{SE}^n.
 
Thanks for that.

I'll have a bash at that.. although I honestly can't see why you wouldn't sum over j
 
Oh wait... is it because the e_{j} basis correspond to different alpha's but not i's?

Edit: Actually on second thought that doesn't make sense because we are summing over alpha(beta).
 
Can anyone else offer some more help?

-I've been teaching myself dirac notation as part of my project this year. This is the first time I've looked at interaction Hamiltonians.
 

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