The 10 Commandments of Index Expressions and Tensor Calculus - Comments

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Discussion Overview

The discussion revolves around the complexities and nuances of index expressions and tensor calculus, particularly in the context of quantum mechanics and the bra-ket notation. Participants explore various interpretations, applications, and potential confusions arising from these mathematical constructs.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification
  • Mathematical reasoning

Main Points Raised

  • Some participants express a preference for bra-ket notation in single systems but find it confusing when dealing with product states, raising questions about the correct representation of hermitian conjugates.
  • There is a discussion about using Einstein's notation for quantum states, with some proposing that states could be represented as components in a vector space.
  • One participant argues that the hermitian conjugate of a product state must be expressed as a Kronecker product, emphasizing the importance of vector spaces in this context.
  • Concerns are raised about the clarity of notation when performing partial contractions, with suggestions that Einstein indices might provide a clearer representation.
  • Participants note the distinction between indices that are summed over and abstract indices, with some suggesting that students may struggle with the former and may not need to learn the latter early on.
  • There is a clarification regarding the interpretation of "next-to-next commandment" in relation to the rules governing index expressions, indicating some confusion among participants.

Areas of Agreement / Disagreement

Participants express differing views on the clarity and utility of various notational systems, particularly regarding bra-ket notation and Einstein notation. Some agree on the challenges of notation, while others emphasize the importance of understanding vector spaces. The discussion remains unresolved on several points, particularly regarding the best practices for representing complex states.

Contextual Notes

Limitations include potential misunderstandings of notation and the varying levels of familiarity participants have with abstract index notation versus traditional index expressions. There is also a noted confusion regarding the phrasing used in the commandments, which may affect comprehension.

Orodruin
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Greg Bernhardt submitted a new PF Insights post

The 10 Commandments of Index Expressions and Tensor Calculus
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As made for me and my aversion against indices. Can I order another one for the bra - ket - "covariant" - "contravariant" - world? I mean their physical use, not their mathematical meaning.
 
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fresh_42 said:
As made for me and my aversion against indices. Can I order another one for the bra - ket - "covariant" - "contravariant" - world? I mean their physical use, not their mathematical meaning.

I've decided that the bra-ket notation is pretty wonderful if you're dealing with single systems, but gets messy and confusing if you have product states.

For example, should ##(|A\rangle |B\rangle)^\dagger## be written as ##\langle A| \langle B|## or ##\langle B| \langle A|##? Also, how do you write a "partial" contraction on just one component of a product state?

Has someone tried using Einstein's notation for quantum states? So you would write ##|A\rangle## as just ##A^\mu##, and you would write ##\langle A|## as ##A_\mu##? Then the corresponding "metric" would be ##g(A,B) = \langle A|B\rangle##.
 
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Well, in this case it's easy to answer, if you consider ##|A \rangle## to belong to a completely different vector space than ##|B \rangle##. Then, what physicists mean is a Kronecker product of vectors ##|AB \rangle=|A \rangle |B \rangle = |A \rangle \otimes B \rangle##. Then it's clear that the hermitean conjugate form of this, acting on ##V_1 \otimes V_2## can only be ##|AB \rangle^{\dagger}=\langle AB | = \langle A |\otimes \langle B|##, because you can apply it only on a vector ##|v_1 v_2 \rangle \in V_1 \otimes V_2## but not on a vector ##|v_2 v_1 \rangle \in V_2 \otimes V_1##, i.e., a correct expression is
$$\langle AB|v_1 v_2 \rangle=\langle A|v_1 \rangle \langle B |v_2 \rangle.$$
It doesn't make any sense to swap ##A## and ##B## in this expression, since ##\langle A|v_2\rangle## doesn't make any sense, because you cannot take a vector product of a vector with a vector belonging to a different vector space (e.g., think about ##V_1## being a spin-1 vector space (3D vector space) and ##V_2## a spin-2 vector space (5D vector space).
 
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vanhees71 said:
...$$\langle AB|v_1 v_2 \rangle=\langle A|v_1 \rangle \langle B |v_2 \rangle.$$.

But if you're writing ##\langle A| \langle B|## contracted with ## |C\rangle |D \rangle##, it looks like

##\langle A| \langle B | |C\rangle |D\rangle = \langle A| (\langle B|C\rangle) |D\rangle##, rather than what's supposed to be, ##\langle A|B\rangle \langle C|D\rangle##. Of course, you can disambiguate it, but the notation is pretty ugly.
 
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And as I said, partial contractions are really ugly. If you want to have ##\langle C|## act on the second component of ##|A\rangle |B\rangle##, you can't write it as:

##\langle C|A\rangle |B\rangle##

You could express it with Einstein indices, though:

##C_\mu A^\nu B^\mu##
 
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vanhees71 said:
$$\langle AB|v_1 v_2 \rangle=\langle A|v_1 \rangle \langle B |v_2 \rangle.$$
It doesn't make any sense to swap ##A## and ##B## in this expression, since ##\langle A|v_2\rangle## doesn't make any sense, because you cannot take a vector product of a vector with a vector belonging to a different vector space (e.g., think about ##V_1## being a spin-1 vector space (3D vector space) and ##V_2## a spin-2 vector space (5D vector space).

One would probably use different sets of indices, e.g.
$$A_a B_\mu {v_1}^a {v_2}^\mu$$
 
One thing that wasn't mentioned in the Insight is
the distinction between
 
robphy said:
One thing that wasn't mentioned in the Insight is
the distinction between
In my experience, students have enough problems with the first of these to delve into the abstract index notation early on and most of the time they do not need it (and the students that are interested enough to delve into it really do not need to be told anything).
 
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  • #10
robphy said:
One would probably use different sets of indices, e.g.
$$A_a B_\mu {v_1}^a {v_2}^\mu$$
Yes, if you define
$$A_a=A^{*a}, \quad B_{\mu} = B^{* \mu}.$$
 
  • #11
## (\vec{v}\times\vec{w})^i = \epsilon_{ijk}v^jw^k ## ##\ \ \ \vec{v}\times\vec{w} = \vec{e}_i\epsilon_{ijk}v^jw^k ##
(Note that this expression breaks the next-to-next commandment if taken literally! It is intended to hold only in Cartesian coordinates. See the caveat.)

5. You shall not have more than two of anyone index in an index expression
Reference https://www.physicsforums.com/insights/the-10-commandments-of-index-expressions-and-tensor-calculus/

Which expression is considered to have more than two instances of an index?
 
  • #12
Stephen Tashi said:
Which expression is considered to have more than two instances of an index?

Have you looked at the example given in the explanation of Commandment 5?
 
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  • #13
George Jones said:
Have you looked at the example given in the explanation of Commandment 5?

My question concerns the remarks before Commandment 5 and the examples before Commandment 5.

The examples after Commandment 5 are clear.

My confusion was due to the phrase "next-to-next commandment". I thought it referred to Commandment 5. I see now that it refers to Commandment 6.
 
  • #14
Stephen Tashi said:
My question concerns the remarks before Commandment 5 and the examples before Commandment 5.

I think by "next-to-next commandment", @Orodruin means Commandment 6. In the example you quoted, two "downstairs" indices are summed over, instead of one "downstairs" index and one "upstairs" index.
 
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  • #15
George Jones said:
I think by "next-to-next commandment", @Orodruin means Commandment 6. In the example you quoted, two "downstairs" indices are summed over, instead of one "downstairs" index and one "upstairs" index.
This is correct. However, it does not hurt to be specific so I will update the text when I get around to it.

Edit: Done.
 
Last edited:
  • #16
"You shall not have more than two of anyone index in an index expression.

Guilty as charged, your Honour.
 

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