Thermal Field Theory: Calculating Angular Distribution of CMB

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Discussion Overview

The discussion revolves around the basic concepts and applications of thermal field theory, particularly in relation to the calculation of the angular distribution of the Cosmic Microwave Background (CMB) temperature. Participants explore the relevance of thermal field theory in cosmological contexts and its connection to correlation functions.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant seeks a basic understanding of thermal field theory and its relevance to the CMB's angular temperature distribution.
  • Another participant explains that traditional quantum field theory calculations are typically performed at zero temperature, but finite temperature considerations are necessary for certain applications, including temperature-dependent observables.
  • A participant mentions encountering the concept of the two-point temperature function in a review paper on the CMB and requests clarification on its meaning.
  • A later reply defines the "two-point function" as a two-point cross-correlation function, providing a reference for further reading.

Areas of Agreement / Disagreement

The discussion does not appear to reach a consensus on the specific applications of thermal field theory to the CMB, and multiple viewpoints regarding its relevance and definitions remain present.

Contextual Notes

Participants express varying levels of familiarity with cosmology and thermal field theory, indicating potential gaps in understanding and assumptions about the applicability of certain concepts.

shahbaznihal
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What is the basic idea and purpose of the thermal field theory? I don't need a full in depth description of it, not at the moment at least. I am just trying to understand how it is relevant in the calculation of angular distribution of temperature of CMB(Comic Microwave Background) over the sky.
 
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"Usual" quantum field theory calculations are all done with respect to the ground state of the system; correlation functions are all taken with respect to the ground state. In other words, they are done at zero temperature, which is a perfectly valid approximation for many applications.

However, in some applications you are working at finite temperature, or maybe you explicitly want temperature-dependent observables like the specific heat. For example, if your system is in equilibrium with some temperature T, you need to sum over all excited states with each state weighted by a Boltzmann factor:
<br /> \langle A \rangle = \frac{1}{Z}\sum_n \langle n | A | n \rangle e^{-\beta E_n} = \frac{\mathrm{Tr}\left( A e^{- \beta H} \right)}{\mathrm{Tr}\left( e^{- \beta H} \right)}<br />
Computing these expectation values using perturbation theory/diagrams is done using the Matsubara formalism, which you can find in many textbooks.

I'm not familiar enough with cosmology to know the specific application to the CMB which you mentioned.
 
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Thanks for the introduction. I was studying a review paper on the Cosmic Microwave Background. The temperature is written as a sum of Spherical Harmonics. I stumbled upon the thermal field theory when they mentioned something called the two point temperature function and I did not know what that meant. May be you could shed some light on this as well (?).

Many thanks for your time.
 

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