Undergrad Help with integration conventions in "Spacetime and Geometry" by Sean Carroll

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In "Spacetime and Geometry" by Sean Carroll, the discussion focuses on the integration conventions used in classical field theory, particularly regarding the Lagrange density and action. The integral can be expressed in different forms, such as using ##d^4x## to simplify notation and avoid emphasizing the order of integration. It is noted that the equivalence of integrals over regions and iterated integrals depends on certain mathematical properties, like Fubini's theorem. The conversation confirms the use of ##dx\, dy\, dz\, dt## and appreciates the clarity provided. Overall, the integration conventions are important for understanding the formulation of field theories.
George Keeling
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I am reading Spacetime and Geometry by Sean Carroll. In section 1.10 on classical field theory, he uses this formula (1.132)
shortintegral.png

The curly L is a Lagrange density. S is an action, Φ is a vector potential.

Could the integral also be written as follows?
longintegral.png
 

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Yes, assuming you mean ##dx\, dy\, dz\, dt##. One reason for using ##d^4x## instead is to save space, and to not emphasize any particular order for the iterated integrals. (There is also a little matter of the fact that the integral over a region is only equivalent to iterated integration over a series of intervals when the region and function being integrated satisfy certain properties, such as Fubini's theorem, but this is not really a big deal most of the time.)
 
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I did indeed mean dx dy dz dt. Thank you, I liked your answer!
 
That's enough thanks!
 

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