Hi,In Mandl&Shaw, when we calculate the covaiant commutation

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The discussion centers on the covariant commutation relations for a scalar field as presented in Mandl & Shaw. The relation [\phi(x),\phi(y)]= i\Delta(x-y)=0 holds true when x-y represents a space-like interval. The participants clarify that a Lorentz transformation cannot convert a time-like interval into a space-like interval due to the invariance of the Minkowski norm, which distinguishes between positive and negative norms. This understanding is crucial for grasping the implications of commutation relations in quantum field theory.

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Hi,

In Mandl&Shaw, when we calculate the covaiant commutation relations for a scalar field we obtain :
[\phi(x),\phi(y)]= i\Delta(x-y)=0
and the last equality stands if x-y is a space-like interval. But I don't understand why. We know that it is zero if the time component is zero and we also know that delta is invariant under proper Lorentz transformation. I don't see why we can't do the correct lorentz transformation (which bring time to zero) with a time-like interval so that it is also zero.

Thank you!
 
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You can't Lorentz transform a time-like interval into a space-like interval. The Minkowski norm
<br /> t^2 - x^2 - y^2 - z^2<br />
is invariant under Lorentz transformations, so a time-like interval (positive norm) cannot be mapped into a space-like interval (negative norm).
 


I got it, thank you!
 

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