Delta written as Minkowski metric ?

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SUMMARY

The discussion centers on the relationship between the Minkowski metric and the delta function in the context of quantum mechanics and field theory. Specifically, the user questions how the delta function, represented as ##\delta^{(4)v}_y##, can be expressed in terms of the Minkowski metric ##\eta_{\nu \mu}##. The equivalence is established through the commutation relations of position and momentum operators, where ##[p_\mu, x^\nu] = -i \hbar \delta^\nu_\mu## and ##[p_\mu, x_\nu] = -i \hbar \eta_{\nu \mu}##, indicating that the Minkowski metric serves as a generalization of the delta function in this framework.

PREREQUISITES
  • Understanding of quantum mechanics, particularly commutation relations.
  • Familiarity with the Minkowski metric and its notation.
  • Basic knowledge of tensor calculus and indices.
  • Concept of partial derivatives in the context of scalar fields.
NEXT STEPS
  • Study the properties of the Minkowski metric in special relativity.
  • Explore the implications of commutation relations in quantum mechanics.
  • Learn about tensor notation and operations in physics.
  • Investigate the role of delta functions in quantum field theory.
USEFUL FOR

Students and professionals in theoretical physics, particularly those focusing on quantum mechanics and general relativity, will benefit from this discussion. It is also relevant for anyone studying the mathematical foundations of field theories.

binbagsss
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Homework Statement


IMG_0871.jpg


Hi, I am just stuck in why / how we can write minkowski metric where I would usually write delta.

I see that the product rule is used in the first term to cancel the terms in the second term since partials commute for a scalar and so we are left with the d rivative acting on a x terms.

I would usually write ##\frac{\partial x^v}{\partial x ^y} = \delta ^{(4)v} _y ##

How is this equivalent to the minkowski metric ?

Homework Equations



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The Attempt at a Solution



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Many thanks [/B]
 

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binbagsss said:
Hi, I am just stuck in why / how we can write minkowski metric where I would usually write delta.

The metric comes into play because:

##[p_\mu, x^\nu] = -i \hbar \delta^\nu_\mu## as you would expect, but

##[p_\mu, x_\nu] = -i \hbar \eta_{\nu \mu}##

The ##\eta_{\nu \mu}## is part of the definition of ##x_\nu##: ##x_\nu = \eta_{\nu \lambda} x^\lambda##
 

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