PhysLean Documentation

PhysLean.Relativity.LorentzAlgebra.ExponentialMap

Exponential map from the Lorentz algebra to the restricted Lorentz group #

In 1+3 Minkowski space with metric η, the Lie algebra lorentzAlgebra exponentiates onto the proper orthochronous Lorentz group (LorentzGroup.restricted 3). We prove:

A key property of a Lorentz algebra element A is that its transpose is related to its conjugation by the Minkowski metric η.

The exponential of the transpose of a Lorentz algebra element. This connects exp(Aᵀ) to a conjugation of exp(-A).

The exponential of an element of the Lorentz algebra is a member of the Lorentz group.

theorem lorentzAlgebra.trace_eq_sum_diagonal (A : Matrix (Fin 1 Fin 3) (Fin 1 Fin 3) ) :
A.trace = i : Fin 1 Fin 3, A i i

The trace of a matrix equals the sum of its diagonal elements.

The trace of any element of the Lorentz algebra is zero.

@[simp]
theorem lorentzAlgebra.Matrix.trace_reindex {n : Type u_1} {R : Type u_2} {ι : Type u_3} [Fintype n] [Semiring R] [Fintype ι] (e : n ι) (A : Matrix n n R) :
(A.submatrix e.symm e.symm).trace = A.trace
@[simp]
theorem lorentzAlgebra.Matrix.exp_reindex {n : Type u_4} {ι : Type u_6} [Fintype n] [DecidableEq n] {k : Type u_7} [RCLike k] [Fintype ι] [DecidableEq ι] (e : n ι) (A : Matrix n n k) :

The exponential of an element of the Lorentz algebra is proper (has determinant 1).

The exponential of an element of the Lorentz algebra is orthochronous.

The exponential of an element of the Lorentz algebra is a member of the restricted Lorentz group.