KNOWPIA
WELCOME TO KNOWPIA

In special relativity, electromagnetism and wave theory, the **d'Alembert operator** (denoted by a box: ), also called the **d'Alembertian**, **wave operator**, **box operator** or sometimes **quabla operator**^{[1]} (*cf*. nabla symbol) is the Laplace operator of Minkowski space. The operator is named after French mathematician and physicist Jean le Rond d'Alembert.

In Minkowski space, in standard coordinates (*t*, *x*, *y*, *z*), it has the form

Here is the 3-dimensional Laplacian and *η ^{μν}* is the inverse Minkowski metric with

- , , for .

Note that the *μ* and *ν* summation indices range from 0 to 3: see Einstein notation. We have assumed units such that the speed of light c = 1.

(Some authors alternatively use the negative metric signature of (− + + +), with .)

Lorentz transformations leave the Minkowski metric invariant, so the d'Alembertian yields a Lorentz scalar. The above coordinate expressions remain valid for the standard coordinates in every inertial frame.

There are a variety of notations for the d'Alembertian. The most common are the *box* symbol (Unicode: U+2610 ☐ BALLOT BOX) whose four sides represent the four dimensions of space-time and the *box-squared* symbol which emphasizes the scalar property through the squared term (much like the Laplacian). In keeping with the triangular notation for the Laplacian, sometimes is used.

Another way to write the d'Alembertian in flat standard coordinates is . This notation is used extensively in quantum field theory, where partial derivatives are usually indexed, so the lack of an index with the squared partial derivative signals the presence of the d'Alembertian.

Sometimes the box symbol is used to represent the four-dimensional Levi-Civita covariant derivative. The symbol is then used to represent the space derivatives, but this is coordinate chart dependent.

The wave equation for small vibrations is of the form

where *u*(*x*, *t*) is the displacement.

The wave equation for the electromagnetic field in vacuum is

where *A ^{μ}* is the electromagnetic four-potential in Lorenz gauge.

The Klein–Gordon equation has the form

The Green's function, , for the d'Alembertian is defined by the equation

where is the multidimensional Dirac delta function and and are two points in Minkowski space.

A special solution is given by the *retarded Green's function* which corresponds to signal propagation only forward in time^{[2]}

where is the Heaviside step function.

**^**Bartelmann, Matthias; Feuerbacher, Björn; Krüger, Timm; Lüst, Dieter; Rebhan, Anton; Wipf, Andreas (2015).*Theoretische Physik*(Aufl. 2015 ed.). Berlin, Heidelberg. ISBN 978-3-642-54618-1. OCLC 899608232.`{{cite book}}`

: CS1 maint: location missing publisher (link)**^**S. Siklos. "The causal Green's function for the wave equation" (PDF). Retrieved 2 January 2013.

- "D'Alembert operator",
*Encyclopedia of Mathematics*, EMS Press, 2001 [1994] - Poincaré, Henri (1906). Wikisource., originally printed in Rendiconti del Circolo Matematico di Palermo. – via
- Weisstein, Eric W. "d'Alembertian".
*MathWorld*.