Multiplication of Operators in Quantum Mechanics

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SUMMARY

The discussion focuses on the multiplication of operators in quantum mechanics, specifically using the states |1⟩ and |2⟩ represented as vectors in a two-dimensional space. The user successfully formed a matrix representation of the operators but initially struggled with the multiplication process. Key to resolving the confusion was the application of the inner product rule ⟨i|j⟩ = δij, which simplifies the evaluation of operator products. The user expressed gratitude for the clarification, indicating that understanding the expression of states significantly eased the problem-solving process.

PREREQUISITES
  • Understanding of quantum states represented as vectors, specifically |1⟩ and |2⟩.
  • Familiarity with matrix representation of quantum operators.
  • Knowledge of inner product notation and the Kronecker delta function (δij).
  • Basic principles of operator multiplication in quantum mechanics.
NEXT STEPS
  • Study the properties of quantum operators and their matrix representations.
  • Learn about the Kronecker delta function and its applications in quantum mechanics.
  • Explore the concept of operator multiplication in more complex quantum systems.
  • Investigate additional resources such as textbooks or online lectures on quantum mechanics operator theory.
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Quantum mechanics students, physicists, and researchers interested in operator theory and its applications in quantum systems.

Penny57
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Homework Statement
Operators can also be multiplied just like matrices. Physically, this represents applying two operations in succession. To compute in the abstract setting, we just need the rule ⟨i|j⟩ = δij .

(d) Compute the operator product of |1⟩⟨1| and |1⟩⟨1| + |2⟩⟨2|.
(e) Compute the operator product of |1⟩⟨2| + |2⟩⟨1| and |2⟩⟨2|.
Relevant Equations
O = O[SUB]ij[/SUB] |i⟩⟨j| = O[SUB]11[/SUB] * |1⟩⟨1| + O[SUB]12[/SUB] * |1⟩⟨2| + O[SUB]21[/SUB]|2⟩⟨1| + O[SUB]22[/SUB]|2⟩⟨2|.
For the first part of the problem, I managed to form this matrix;

<1|O|1><1|O|2>
<2|O|1><2|O|2>

=
10
00

However, that was because I was following this image;

MUuW2cj.png


I'm not entirely sure how this was obtained, and I'm not really sure what to do to continue forward with part e. I apologize for my lack of knowledge - I've attempted to search for any youtube videos to help and go through online textbooks, but I'm unable to find what I am looking for.
 
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Why don't you investigate it with the expression of the states
<br /> |1&gt;=<br /> \begin{pmatrix}<br /> 1 \\<br /> 0 \\<br /> \end{pmatrix}<br />
<br /> |2&gt;=<br /> \begin{pmatrix}<br /> 0 \\<br /> 1 \\<br /> \end{pmatrix}<br />
 
Last edited:
penny_ss said:
To compute in the abstract setting, we just need the rule ⟨i|j⟩ = δij .
For example, the operator ##| 2 \rangle \langle 1|## multiplied by the operator ##| 1 \rangle \langle 1|## would be $$| 2 \rangle \langle 1| \cdot | 1 \rangle \langle 1| = | 2 \rangle \langle 1|| 1 \rangle \langle 1| = | 2 \rangle \langle 1| 1 \rangle \langle 1|$$ The middle part ##\langle 1| 1 \rangle## of the expression on the far right can be evaluated using the rule ##\langle i| j \rangle = \delta_{ij}##.
 
Thank you so much for the help! I've managed to work through it with the advice given. I forgot to account for the expression of the states - once I did, the problem became much easier. Thank you for the help! And that rule makes a lot more sense now. Thank you again!
 

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