Graduate Thermal Field Theory: Calculating Angular Distribution of CMB

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Thermal field theory is essential for calculating the angular distribution of the Cosmic Microwave Background (CMB) temperature by incorporating finite temperature effects into quantum field theory. Unlike standard quantum field theory, which operates at zero temperature and focuses on the ground state, thermal field theory accounts for excited states weighted by a Boltzmann factor, allowing for temperature-dependent observables. The two-point temperature function, a key concept in this context, represents a two-point cross-correlation function that helps analyze temperature fluctuations across the sky. This approach is particularly relevant when studying the CMB, as it provides insights into the underlying physics at different temperatures. Understanding these principles is crucial for interpreting the CMB's angular distribution accurately.
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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.
 
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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