Ket and Bra with the momentum j,m

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Discussion Overview

The discussion revolves around the graphical method in the theory of angular momentum, specifically focusing on the permutation of Ket and Bra vectors with momentum quantum numbers j and m. Participants explore the implications of the formula for both integer and semi-integer values of j, particularly j = 1/2.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • Antony Gorkh expresses confusion about the application of the permutation formula for semi-integer j values, particularly j = 1/2, and seeks clarification.
  • One participant notes that j-m is always an integer and suggests evaluating it for all possible m values when j = 3/2.
  • Another participant emphasizes that for integer j, each state |jm> corresponds to spherical functions, while for semi-integer j, |jm> is represented as a two-element column vector, raising questions about the validity of the formula in this context.
  • A participant challenges the notion that Kets and Bras can be equal up to a minus sign, suggesting a misunderstanding in the original formulation.
  • Antony acknowledges the confusion stemming from the authors' terminology in the referenced book and clarifies that the quantity (-1)^(j-m) |j, -m> should not be considered a Bra.

Areas of Agreement / Disagreement

Participants express differing views on the validity of the permutation formula for semi-integer j values, with some agreeing on the confusion caused by terminology while others challenge the underlying assumptions. The discussion remains unresolved regarding the application of the formula in the context of semi-integer j.

Contextual Notes

There are limitations regarding the clarity of notation and terminology used in the referenced literature, which may contribute to misunderstandings about the relationship between Kets and Bras in this context.

brombenzol123
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Hi there!

I try to understand and to use graphical method in the theory of angular momentum. It is not very difficult to master is fundamentals excepting a few things. The most fundamental is the following.

In literature there is used the fact that Kat and Bra vectors with momentum j,m can be mutually permutated using
<jm| = (-1)j-m |j, -m>. It is clear for integer j. But how to understand this fact, for example, in the case j = 1/2 ?

I would be glad if somebody could give me advice.

I'm absolutely novice at forums where scientific questions are discussed. So, first of all, I would be glad to see a few words about where else I can discuss such questions. What cites / forums are the most popular for these purposes?With Best Regards,
Antony Gorkh.
 
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j-m in the exponential is always an integer. If you take j=3/2, then m has 4 possible values: -3/2, -1/2, 1/2 and 3/2. Evaluate j-m for all 4 possible cases.
 
dextercioby said:
j-m in the exponential is always an integer. If you take j=3/2, then m has 4 possible values: -3/2, -1/2, 1/2 and 3/2. Evaluate j-m for all 4 possible cases.

Yes, it's obvious true. But the deal is in the other thing.

In the case of integer j every state |jm> is represented by spherical function, and the formula above is just a property of spherical functions. But in the case of semi-integer j we have the other picture. For example in the case of 1/2 |jm> is a column of 2 elements in the basis (1,0)T, (0,1)T, and it's hard to understand how that formula can still hold. But it is so (in some magic way) and it is used widely in literature.

I used the book "Graphical method of spin algebras" by E. Elbaz and B. Castel. The formula (1.2.5) chapter 1, paragraph 2. I use Russian edition, so there may be some shift.
 
Last edited:
Thinking about it, the bra's and the kets don't live in the same vector space, hence they can't be equal up to a minus 1. There's something wrong with what you wrote.
 
You're absolutely right and there are no doubts that Kets and Bras can't be equal up to minus 1. That formula was written originally not by me but by the authors of the book I mentioned above. Being not accurate with notations and terminilogy they confused me so that I had nothing to do but ask people on forums. I hope all people that ever read that book had mastered this problem.

The authors calls the quantity (-1)j-m |j, -m> as covector in the respect to the vector |jm> in the sense that Σm(-1)j-m |j, -m> |j,m> gives the total momentum with j=0, i.e. scalar (here (-1)j-m plays the role of Clebsh-Gordan coefficient). It was the authors' mistake to denote it as <jm| and it was my mistake to call it Bra. It has nothing common with Bra.
 

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