Agnostic
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does |z> = |+z> + |-z> ?
The discussion clarifies the distinctions between the quantum states |z>, |+z>, and |-z>. It establishes that |z> is not equal to |+z> + |-z> and emphasizes that |z> represents a state vector in the z basis, specifically |z> = (1,0) and |-z> = (0,1). The conversation also highlights the importance of normalization in quantum mechanics, stating that the inner product must equal one, and discusses the calculation of probabilities related to these states. Recommended resources for further understanding include Griffiths' Quantum Mechanics and Nielsen and Chuang's Quantum Computation.
PREREQUISITESStudents in introductory quantum mechanics courses, quantum physicists, and anyone interested in the mathematical foundations of quantum state representation and calculations.
Logarythmic said:No, |+z> + |-z> = |z> - |z> = 0.
Hargoth said:What is | z \rangle?
Hargoth said:Yeah, but if | z_+ \rangle, | z_- \rangle are basekets of the Hilbert space you consider, your equation would be a definition of | z \rangle
Agnostic said:does |z> = |+z> + |-z> ?
jonestr said:No since |z>=(1,0) in the z basis and |-z>= (0,1) in the z basis you could a. never get a scalar under addition and you could not get an answer of the zero vector since these vectors are linearly independent and form a complete basis. For your previous post you need to calculate what |-z> is in the x basis or what |x> is in the z basis to compute the inner product. Griffiths QM or Liboff are good sources for this. As is Nielsen and Chuang
Hope that helps
For a QM-Interpretation you have to normalize the statevector, so thatAgnostic said:is it a valid/correct definition?
I'm in an intro quantum class and I need to calculate:
so far, we have just been calculating things like: <+or-phi|+or-psi>
Now we are asked to calculate things like:
<-z|x>
Which i read as that is the amplitude of something in either the +x or -x state being in the -z state.
Hargoth said:For a QM-Interpretation you have to normalize the statevector, so that
\langle z | z \rangle = 1. If \langle z_+ | z_+ \rangle = 1 and \langle z_- | z_- \rangle = 1-, this not the case here.
I wouldn't say "amplitude" but "probability": |\langle -z | x \rangle|^2 is the probability to measure "z-spin-down" on a particle of which you know it is in state "x-spin-up".