groups and physics coadjoint action momentum

En résumé (grâce à un LLM libre auto-hébergé)

  • The text discusses Poincaré groups and their application in physics.
  • It explains the concept of momentum and duality in the context of these groups.
  • Matrix calculations are performed to demonstrate the invariance of physical quantities.

A Poincaré group element gp in the group Gp is defined by a sequence of parameters {pi}, the number of which, as we have already said, represents the dimension of the group. The matrix dg (g = e) is built from the quantities {dpi}. The above mapping is therefore of the type:
(81)

In other words, to a set of scalars dpi we associate an equal number of scalars dpi'. Duality consists of postulating the invariance of a scalar, according to:

(82)

where n is the dimension of the group (ten, for the Poincaré group). The scalars Ji represent the components of the momentum, in the same number.

We will decide to decompose this momentum J into two objects. The first will be an antisymmetric matrix M of size (4,4), thus having six components, and the second a "four-vector" P, a matrix of size (4,1):

(83)

(84) J = { M , p , E} = { M , P } We will write the scalar product in the form:

(85)

Tr meaning "trace of", and we will also have:

(86)

a linear form whose invariance ensures the duality.

with:

(87) (87b)

(87c)

but GG = 1 therefore this equals:

(88)

Identify the terms in y (89)

That is to say:

(90)

----> Here again follow details of matrix calculations. If you wish, clicking here you can go directly to the result.

In the trace, we can perform a cyclic permutation of the terms.
(90a)

(90b)

(90c)

the second term of the right-hand side is equal to the product of a row matrix by a column matrix.

This is equal to the trace of the reversed product (below, schematically, the product of a row matrix by a column matrix):
(90d)

In this trace, I can perform a cyclic permutation:
(90e)

Hence:
(90f)

(90g)

Here we will apply again the theorem on the traces of matrices which are the product of another matrix by a symmetric matrix.

Any matrix can be symmetrized or antisymmetrized. Moreover, the trace of the product of a matrix by a symmetric matrix is zero.
(90h)

I can apply this to the matrix (90i) since we take the trace
(90j)

(90k) = sym ( ) + antisym ( )

but:
(90l)

hence
(90m) (90n)
(90o)
(90p)

and:
(90q)

finally:
(90r)

By grouping and changing the primes on one side I obtain my group action: