What is the Interaction Hamiltonian in Quantum Mechanics?

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Homework Help Overview

The discussion revolves around the Interaction Hamiltonian in Quantum Mechanics, specifically focusing on the expression for the Hamiltonian \( H_{SE} \) and its application in a time evolution operator. Participants are examining the mathematical formulation and implications of these expressions.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the correct formulation of the Hamiltonian and whether to sum over certain indices. There is an attempt to understand the implications of the basis states involved and the application of Taylor expansion for the exponential operator.

Discussion Status

The conversation is active, with some participants questioning the need to sum over specific indices and others providing guidance on applying Taylor expansion. There is a mix of attempts to clarify concepts and explore the reasoning behind the mathematical steps.

Contextual Notes

One participant notes their self-study of Dirac notation and the context of their project, indicating a learning environment where foundational concepts are being explored.

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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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