QFT Index Notation: A Beginner's Guide

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Index notation in Quantum Field Theory (QFT) can be confusing for beginners, especially after studying relativity, as the conventions may differ. It's common to see the i-index on matrices like M inappropriately placed, but this is often due to the simplicity of flat space in Cartesian coordinates where covariant and contravariant components appear identical. Precision in notation is crucial for clarity in calculations, and older literature may use varied conventions that can lead to misunderstandings. Recommended resources for a clearer understanding include texts by Ryder, Bailin and Love, Brown, and Peskin and Schroeder, with caution advised for typos in the latter. Weinberg's comprehensive volumes are highly regarded but are better suited for advanced study rather than as an introductory text.
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Hi. I'm just starting QFT for the first time. I've just finished a course in relativity but I'm confused about the index notation I've found in QFT. Here are 2 examples yi = Σ Mij xj and yj = δij yi . These examples don't seem right after what I have learned in relativity unless the index notation changes in QFT ?
 
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The i-index on M should indeed be upstairs, but people are sometimes sloppy when considering flat space in Cartesian coordinates; there, covariant and contravariant components are numerically the same because the metric is given by the identity matrix. You'll encounter this often, but a good habit is to be precise when doing your own calculations. In older papers you can also encounter this notation for curved indices in general.
 
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Where does this come from? I'd look for a more carefully written source on the subject. QFT is difficult enough to understand. You don't need unnecessary sloppyness in notation. Good starting points are

L. H. Ryder. Quantum Field Theory. Cambridge University Press, Cambridge, New York, Melbourne, 2 edition, 1996.
D. Bailin and A. Love. Introduction to Gauge Field Theory. Adam Hilger, Bristol and Boston, 1986.
Lowell S. Brown. Quantum Field Theory. Cambridge University Press, 1992.
M.E. Peskin and D. V. Schroeder. An Introduction to Quantum Field Theory. Addison-Wesley Publ. Comp., 1995.

The last one has to be read with great care, because it has pretty many typos (and sometimes even quite annoying inprecisions), but overall it's didactically well written.

The non-plus-ultra are of course the 3 volumes by Weinberg

S. Weinberg, Quantum Theory of Fields, Cambridge University Press, 3 Vols.

I'd, however, not take them as a first text.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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