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Comment: Added eftx concept question

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1) 

  

EFT Concepts:

1) Power counting not in the rest frame

What happens to this discussion and to the power counting rule 
Mathinline
body\partial_t \sim 1/m
 when we are doing HQET in a frame other than the rest frame, where the leading kinetic energy term is a single gradient term with no m suppression? It sounds like the problem you point out, that 

  

Mathinline
bodyp^2/2m
 is the first term inducing not trivial dynamics, would go away!


Yes, in HQET you do not count   

Mathinline
body\partial_t \sim 1/m
. That counting only arises because   
Mathinline
body\partial_t \sim E \sim p^2 / m \sim \nabla^2 / m
 
for  for a Non-Relativistic EFTs of two or more heavy particles. HQET, with a single heavy particle, has a homogeneous scaling for   
Mathinline
body\partial^\mu
 
in  in frames that are close to the rest frame. You can also look at the power counting of derivatives for HQET in a boosted frame (which is called bHQET). This gives you exactly what you'd expect by applying the boost. See this paper for a description and application of bHQET.