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The oriented volume form epsilon and the permutation symbols of an inertial frame

Definition

Let (A,V,η,C+) be an oriented time-oriented affine Minkowski space and let (o;e0,e1,e2,e3) be an inertial frame with its inertial chart (Inertial frames and inertial charts of the affine Minkowski model). Every v∈V has a unique coordinate vector (v0,v1,v2,v3) with v=∑avaea. For an ordered 4-tuple (v0,v1,v2,v3) of vectors of V let

[vja]:=(v00v10v20v30v01v11v21v31v02v12v22v32v03v13v23v33)

be the 4×4 real matrix whose j-th column lists the coordinates of vj in the ordered basis (e0,e1,e2,e3), and define

ϵ(v0,v1,v2,v3):=det⁡([vja])

by the determinant of a square matrix (For n≥1, the determinant over a commutative ring by the Leibniz formula, and ∣det⁡A∣ for a real matrix). Then ϵ is an alternating 4-linear form on V (Alternating k-linear maps): the determinant is multilinear and alternating in the columns, so replacing one vj by λvj+μw replaces the j-th column correspondingly and ϵ is linear in each argument, and ϵ(v0,…,v3)=0 whenever two arguments coincide, since then two columns coincide (The determinant is the unique normalized alternating multilinear function on the columns). The form ϵ is the oriented volume form of the model. Its well-definedness as a form of the model, independent of the inertial frame used in the display, is proved in The oriented volume form is independent of the positively oriented inertial frame ↗.

Components. Write ϵabcd:=ϵ(ea,eb,ec,ed) for the components of ϵ in the inertial frame. Evaluating the determinant on the coordinate matrix of (ea,eb,ec,ed), which is the permutation matrix of the tuple, gives

ϵ0123=+1,ϵabcd=sgn⁡(σ)  if (a,b,c,d)=(σ(0),σ(1),σ(2),σ(3))  for a permutation σ,

and ϵabcd=0 whenever two of the indices coincide; these are the permutation symbols of the frame. Indeed the coordinate vector of ea is the a-th standard basis vector, so the coordinate matrix of (ea,eb,ec,ed) is the permutation matrix of the tuple and its determinant is +1 on the identity tuple, the sign of the permutation otherwise, and 0 when two indices repeat.

Raised components. The inverse metric ηab is the inverse of the matrix ηab:=η(ea,eb)=diag⁡(−1,1,1,1)ab, which exists because η is nondegenerate (Lorentz forms of inertia (3,1,0) on a 4-dimensional real vector space); it is again ηab=diag⁡(−1,1,1,1)ab. The raised components of the volume form are

ϵabcd:=ηaa′ηbb′ηcc′ηdd′ϵa′b′c′d′

(summation over repeated primed indices). Since the inverse metric is diagonal with diagonal entries −1,1,1,1, only one term contributes to ϵ0123 and

ϵ0123=η00η11η22η33ϵ0123=(−1)(+1)(+1)(+1)(+1)=−1.

Spatial symbol. The spatial permutation symbol ϵijk for i,j,k∈{1,2,3} is defined by ϵ123=+1 together with alternation in the three indices; explicitly ϵijk=+1 for even permutations of (1,2,3), ϵijk=−1 for odd permutations, and ϵijk=0 whenever two of i,j,k coincide.

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