A How to interpret this equation in Szabo & Ostlund's book

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The discussion centers on interpreting equation 1.48a from Szabo & Ostlund's "Modern Quantum Chemistry," specifically regarding the role of the index j. Participants clarify that j represents components in the same basis as i, with j acting as an index over the basis vectors. The relationship between bras and kets is likened to linear algebra, where bras correspond to row vectors of kets. The importance of understanding the orthogonality property and the representation of vectors in complex vector spaces is emphasized. Overall, the conversation highlights the need for clarity in mathematical notation and understanding the underlying principles of linear algebra.
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Szabo & Ostlund
I am trying to interpret equation 1.48a on page 11 in Szabo & Ostlund's "Modern Quantum Chemistry".

What purpose does the index j serve? Is j another basis? Why do we need j?Reference:
Szabo, A., & Ostlund, N. S. (1996). Modern quantum chemistry: Introduction to advanced electronic structure theory. Mineola, N.Y: Dover Publications.
 
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it uses eq 1.47 the orthogonality property.
If you know linear algebra, you can think of these indices as you would do for basis vectors in say R3

The <j|a> is similar as you would do in linear algebra, for a vector a, what its compnents are in a certain basis
 
yes, but where does j even come from? if we are trying to find the components of |a> with respect to the basis {|i>}, why do we need j? I do not understand
 
was |a> in the basis {| j >} to begin with?
 
or perhaps the better question is, are i and j two separate bases? Is j just another index over the basis i ?
 
oh wait, is aj just the jth component of ket | a > ?
 
compchemrulez said:
or perhaps the better question is, are i and j two separate bases? Is j just another index over the basis i ?
You can use any letter you want, you will get the kronecker delta anyway.
Yes they are in the same basis, well ##\langle i | ## is the dual-basis of ##| i \rangle ##. If this was "regular vectors" ##\langle i | ## would be the "row vector" of ## | i \rangle## so to say.

Review the linear algebra chapter again. Bras and kets at this point are just representations of vectors in a complex vector space. Eq. 1.48a is the "same" as eq 1.8 but you write ##|a\rangle## instead of ##\vec a## and ##\sum |i\rangle a_i## instead of ##\vec a = a_1 \hat e_1 + a_2 \hat e_2 + a_3 \hat e_3## and ##|i \rangle ## instead of ##\hat e_i## and ##\langle i | ## would be ##(\hat e_i)^T## (the row vector form of ##\hat e_i##)
 
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ok I think this is making more sense now

Thank you Malawi_glenn, you will see me posting many more questions in this forum : )
 
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compchemrulez said:
Thank you Malawi_glenn, you will see me posting many more questions in this forum : )
You need to post the relevant equations here, and your own effort in trying to understand.
For this, I recommend that you learn some basic LaTeX, there is a nice guide here https://www.physicsforums.com/help/latexhelp/

A good title is also needed "help with an equation in book X" is not very useful.

A question like this, I would have reported, but I decided to cut some slack here since you are new and I have the book pretty close to me in my little library.
 
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How should I cite an equation from a book?
 

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