Question about d'Alembert operator

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    D'alembert Operator
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Discussion Overview

The discussion revolves around the properties of the d'Alembert operator and the expression \(\partial_{\mu}\partial^{\nu}\phi\), particularly in the context of whether this operator equals zero when the indices \(\mu\) and \(\nu\) are not equal. The scope includes theoretical considerations in the context of tensor calculus and differential equations.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant suggests that \(\partial_{\mu}\partial^{\nu}\phi\) equals \(\Box \phi\) when \(\mu = \nu\) and questions whether it is zero when \(\mu \neq \nu\.
  • Another participant argues that \(\partial_{\mu}\partial^{\nu}\phi\) is a second rank tensor and asserts that there is no reason for it to be identically zero.
  • A third participant notes that the Minkowski metric is typically used in these calculations and mentions that the expression simplifies in four dimensions.
  • A later reply asks if \(\partial_{\mu}\partial^{\nu}\phi\) is equal to \(\partial^{\nu}\partial_{\mu}\phi\), implying a consideration of symmetry in the operator.

Areas of Agreement / Disagreement

Participants express differing views on whether \(\partial_{\mu}\partial^{\nu}\phi\) is zero when \(\mu \neq \nu\), indicating that the discussion remains unresolved regarding this aspect.

Contextual Notes

The discussion does not clarify the assumptions regarding the nature of the field \(\phi\) or the specific conditions under which the operators are being evaluated.

Dixanadu
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Hey guys,

The expression [itex]\partial_{\mu}\partial^{\nu}\phi[/itex] is equal to [itex]\Box \phi[/itex] when [itex]\mu = \nu[/itex]. However when they are not equal, is this operator 0?

I'm just curious cos this sort of thing has turned up in a calculation of mine...if its 0 I'd be a very happy boy
 
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That thing is in fact a second rank tensor which in 1+1 dimensions becomes:

[itex] \partial_\mu \partial^\nu \phi=\eta^{\nu \lambda}\partial_\mu\partial_\lambda \phi=\left( \begin{array}{cc} \eta^{00}\frac{\partial^2 \phi}{\partial x^0 \partial x^0}+\eta^{01}\frac{\partial^2 \phi}{\partial x^0 \partial x^1} \ \ \ \ \ \ \eta^{00}\frac{\partial^2 \phi}{\partial x^1 \partial x^0}+\eta^{01}\frac{\partial^2 \phi}{\partial x^1 \partial x^1} \\ \\ \eta^{10}\frac{\partial^2 \phi}{\partial x^0 \partial x^0}+\eta^{11}\frac{\partial^2 \phi}{\partial x^0 \partial x^1} \ \ \ \ \ \ \eta^{10}\frac{\partial^2 \phi}{\partial x^1 \partial x^0}+\eta^{11}\frac{\partial^2 \phi}{\partial x^1 \partial x^1} \end{array} \right)[/itex]

I think its obvious that there is no reason for it to be identically zero.
 
Usually ##\eta## is used for the Minkowski metric in Cartesian coordinates. Shyan wrote you a general expression for a general metric, in 2 dimensions. Usually we work in 4-dimensions, but by using the Minkowski metric, the expression is much simpler.

It is perhaps easier to deal with ##\partial_\mu\partial_\nu\phi## in which case, this is just the Hessian matrix: http://en.wikipedia.org/wiki/Hessian_matrix (replace f with ##\phi##)
 
Okay thank you. so would you say that [itex]\partial_{\mu}\partial^{\nu}\phi=\partial^{\nu}\partial_{\mu}\phi[/itex]?
 

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