Understanding the Difference Between |z>, |+z>, and |-z> in Quantum Mechanics

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SUMMARY

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.

PREREQUISITES
  • Understanding of quantum state vectors and notation
  • Familiarity with Hilbert space concepts
  • Knowledge of quantum mechanics probability amplitudes
  • Basic skills in calculating inner products of quantum states
NEXT STEPS
  • Study Griffiths' Quantum Mechanics for foundational concepts
  • Learn about normalization of quantum state vectors
  • Explore Nielsen and Chuang's Quantum Computation for advanced topics
  • Research the implications of linear independence in quantum states
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Students in introductory quantum mechanics courses, quantum physicists, and anyone interested in the mathematical foundations of quantum state representation and calculations.

Agnostic
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does |z> = |+z> + |-z> ?
 
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No, |+z> + |-z> = |z> - |z> = 0.
 
Logarythmic said:
No, |+z> + |-z> = |z> - |z> = 0.

umm..., no.
 
What is | z \rangle?
 
Last edited:
Hargoth said:
What is | z \rangle?

In quantum mechanics, |z> is a state vector read at "ket z".

It describes the state a particle is in.
 
Yeah, but if | z_+ \rangle, | z_- \rangle are basekets of the Hilbert space you consider, your equation would be a definition of | 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

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.
 
Agnostic said:
does |z> = |+z> + |-z> ?

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
 
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

|z> is not equal to |+z>

I thought |+z>=(1,0)
 
  • #10
Agnostic 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.
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".
 
  • #11
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".

<-z|-z> = 1

<-z|-z> means what is the "probability" amplitude that a particle in state |-z> will be in state |-z>
 
  • #12
Yeah, I just wanted to say that your probability of finding z in state z from the equation above would be 2^2=4, so you have to normalize.
 
  • #13
you don't have to write the plus explicity. |z>=|+z>=(1,0) which is not equal to -|-z>=(0,-1). The negatives are part of the nomenclature and do not have algebraic significance.
 

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