Graduate Extra terms in the Action in Zee chapter 1.3?

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The tau and sigma terms in the expression are arbitrary coupling constants that originate from the self-interaction energy V of the field φ, as expressed in equation (2). They represent the self-interaction part of the arbitrary function V in a series of φ. Additionally, there is confusion regarding the transition from 3-momentum to 4-momentum in the Sidney Coleman lectures, specifically why the operator on the right side is dropped. This transition typically involves simplifying the expression under certain assumptions about the momentum operators. Understanding these concepts is crucial for grasping the underlying physics in the context of quantum field theory.
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Hi, could someone please explain where the tau and sigma terms come from in this expression:

Screen Shot 2019-09-20 at 10.47.53 PM.png

I see the kinetic energy and quadratic "mattress" potential terms, but the tau and sigma kinda come out of nowhere. Where are they from?
 
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These are just arbitrary coupling constants. They originate from the self interaction energy V of the field ##\varphi## with itself in equation (2). It is a way of expressing the self interaction part of the arbitrary function V in a series of ##\varphi##.
 
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Hans de Vries said:
These are just arbitrary coupling constants. They originate from the self interaction energy V of the field ##\varphi## with itself in equation (2). It is a way of expressing the self interaction part of the arbitrary function V in a series of ##\varphi##.

Thanks that makes sense.

I was wondering if anyone could address another question I had?
This one is from the Sidney Coleman lectures (2.72)

##e^{i P . x}\alpha(p)e^{-i P . x} = e^{-i p . x}\alpha(p)##

i'm confused why we drop the operator on the right side when we go from 3-momentum to 4-momentum?
 
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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