Superposition Equation solution

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SUMMARY

The discussion centers on the superposition equation in quantum mechanics, specifically the equation |\psi\rangle = {3\over 5} i |A\rangle + {4\over 5} |B\rangle. Participants clarify that |A\rangle and |B\rangle are abstract representations of quantum states and do not require specific values to be plugged in. The probabilities of measuring the system in states A and B are given by P_A = |N_A|^2 and P_B = |N_B|^2, where N_A and N_B are the coefficients in the superposition.

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  • Understanding of quantum mechanics concepts, specifically superposition.
  • Familiarity with linear operators in quantum mechanics.
  • Knowledge of probability amplitudes in quantum state measurements.
  • Basic grasp of complex numbers and their representation in quantum equations.
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Students and researchers in quantum mechanics, particularly those studying superposition and measurement theory. This discussion is beneficial for anyone looking to deepen their understanding of quantum states and their mathematical representations.

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Homework Statement



Hi everyone,
This is my first time posting, and I really need some help. I'm doing a project on Schrödinger's cat, concentrating on superposition and the linearity of operators.
I have this equation: |\psi\rangle = {3\over 5} i |A\rangle + {4\over 5} |B\rangle
but I don't know what amounts to plug in for A and B, as well as what amount the imaginary number represents, if anything.



Homework Equations


|\psi\rangle = {3\over 5} i |A\rangle + {4\over 5} |B\rangle

The Attempt at a Solution


I think I understand what the equation is saying, that if a particle can be at A and B, it can also be 3/5i in position A and 4/5 in position B. But beyond that, I don't know what step to take next.

Any input would be extremely helpful
thanks!
 
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Hi asechman,
|A> and |B> are abstract representations of quantum states. You don't plug in anything for A and B. They are just labels used to distinguish the states.

Let's say you're making a measurement, and |A> and |B> represent two possible states resulting from that measurement. Then the formula

[tex] |\psi\rangle = N_A |A\rangle + N_B |B\rangle[/tex]

means that the probability of finding the system in state A is

[tex]P_A = |N_A|^2 = {N_A}^*N_A[/tex]

and the probability for finding the system in the other state is

[tex]P_B = |N_B|^2 = {N_B}^*N_B[/tex]
 
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