Graduate Pauli Villars for Quadratic Divergences

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The discussion centers on the use of Pauli-Villars regularization to address quadratic divergences in quantum field theory. A specific integral form is proposed for evaluation, involving momentum integrals and mass terms. There is a preference expressed for dimensional regularization over Pauli-Villars due to its complexity. The original poster seeks validation of their approach and further assistance. Overall, the conversation highlights the challenges and considerations in regularization techniques within theoretical physics.
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How would I do Pauli Villars Regularization for an integral of the form

$\frac{\int d^4k}{(2\pi)^4}\frac{k^2}{(k^2-m^2+i\epsilon)^2}$
My guess would be to do an integral of the form

$$\frac{\int d^4k}{(2\pi)^4}k^2(\frac{1}{(k^2-m^2+i\epsilon)}-\frac{1}{k^2-\Lambda_1^2+i\epsilon})(\frac{1}{(k^2-m^2+i\epsilon)}-\frac{1}{k^2-\Lambda_2^2+i\epsilon})$$

before Wick otating and integrating. Any help is appreciated. Thanks.
 
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This looks promising. What's your specific question? I never liked Pauli-Villars regularization much, because it's pretty complicated compared to dimensional regularization ;-)).
 
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Just wanted to check if I was on the right path. Thanks!
 
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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