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Holonomy and discrete geometric interfaces — flat local transport with global holonomy

Statement

Let M=S1×R3, write (x,y) for the standard embedding coordinates on S1, and set α=x dy−y dx. With real coordinates t,z1,z2 on R3, define

g=−dt⊗dt+α⊗α+dz1⊗dz1+dz2⊗dz2.

The global frame E0=∂t, E1=−y∂x+x∂y, E2=∂z1, E3=∂z2 is an orthonormal tetrad for g with signature (−,+,+,+). Here E1 is the restriction of the indicated ambient vector field to S1, where it is tangent because it is orthogonal to (x,y). Orient M by this ordered frame and time-orient it by E0. Let J be the constant matrix with JE2=E3, JE3=−E2, and JE0=JE1=0. Assume the ACω convention in Local Lorentz tetrad and connection. Define ω=14Jα and the affine connection on this frame by

∇X(∑JvJEJ):=∑I(X(vI)+∑JωIJ(X)vJ)EI.

For a real 4×4 matrix A, exp⁡(A) denotes the matrix series ∑m=0∞Am/m!, which converges absolutely in any fixed submultiplicative matrix norm.

This is a flat Lorentz connection. On any coordinate arc of S1 with angular coordinate θ, transport between endpoints is exp⁡(−14J(θ1−θ0)), independent of the chosen path inside that arc. Around the once-around loop it is exp⁡(−π2J)≠I4, although the curvature is zero; the loop is not thin-contractible.

Facts & Assumptions

Given: The manifold, metric, tetrad, and matrix-valued one-form in the statement; use the connection and transport conventions of the linked A-page items.

[A1]

Assume ACω as required by Local Lorentz tetrad and connection.

[F1]

Local Lorentz tetrad and connection: a Lorentz connection matrix is η-skew, has curvature F=dω+ω∧ω, and in this signature uses η=diag⁡(−1,1,1,1).

[F2]

Connection path transport: transport solves U′=−ω(γ˙)U with initial value I4.

[F3]

The once-around circle path is not thin-contractible: the once-around loop in S1 is not the identity class in the thin path groupoid.

[F4]

A smooth differential k-form: a smooth one-form is a smooth section of the cotangent bundle.

[F5]

A regular level set is an embedded submanifold: a nonempty regular level set of a smooth real-valued function is a smooth embedded submanifold of codimension one.

[F6]

The exterior derivative by the invariant vector-field formula: for a one-form β, dβ(X,Y)=X(β(Y))−Y(β(X))−β([X,Y]).

[F7]

The pullback of a differential form: the pullback evaluates the ambient form on tangent vectors after applying the differential of the embedding.

[F8]

Pullback of forms is smooth functorial and preserves wedges: pullback along a smooth map sends smooth differential forms to smooth differential forms.

[F9]

The invariant exterior-derivative formula is C∞-multilinear: the invariant exterior-derivative formula is alternating and C∞(M)-multilinear and defines a smooth form. In particular dα is a two-form, determined by its values on pairs from a tangent frame.

Proof

technique · direct construction
1.1givenA1F1F4F5F6F7F8F9algebra

The function f(x,y)=x2+y2 has derivative (2x,2y)≠0 on S1=f−1(1), so [F5] gives its usual smooth one-dimensional submanifold structure. Let j:M↪R2×R3 be the product inclusion, put α~=x dy−y dx on R2×R3, and interpret the stated form as α=j∗α~, defined by [F7] and smooth by [F8], hence a smooth cotangent section by [F4]. On the global frame, α(E1)=1 and α(E0)=α(E2)=α(E3)=0; the frame fields commute pairwise. By [F9], dα is a smooth two-form. Thus [F6] gives dα(EI,EJ)=EI(α(EJ))−EJ(α(EI))−α([EI,EJ])=0 for every I,J, so dα=0 intrinsically on M. Also α(E1)=1 and it vanishes on the other frame vectors, so the displayed frame is orthonormal for g; it is smooth and E0 is future-directed. In the E2,E3 plane the matrix J is the standard skew rotation generator, so JTη+ηJ=0. The displayed formula for ∇ is linear over smooth functions in X, additive in the vector field argument, and satisfies ∇X(fV)=X(f)V+f∇XV by the ordinary product rule; hence it defines a smooth affine connection with tetrad matrix ω. Its curvature is F=dω+ω∧ω=14Jdα+116J2α∧α=0, since dα=0 and α∧α=0. It is η-skew and flat, so it is a Lorentz connection under [F1].

2.1givenF2F3step 1.1algebra∎

On an angular arc, α=dθ. The matrix U(t)=exp⁡(−14J(θ(t)−θ(0))) starts at I4; termwise differentiation of the defining series, whose derivative series converges uniformly on compact parameter intervals, gives U˙(t)=−14Jθ˙(t)U(t). By [F2] it is the transport by uniqueness, and it depends only on the endpoints on that arc. For the path θ(t)=2πt, its endpoint is exp⁡(−π2J). Since J2=−I on span⁡(E2,E3), separating the even and odd terms of the series gives exp⁡(−π2J)=cos⁡(π2)I−sin⁡(π2)J=−J on that plane, so it is not the identity. If the once-around loop in M were thin-contractible, composing that homotopy with the smooth projection M→S1 would preserve fixed endpoints, the finite smooth-triangle subdivision, and rank at most one, and would contract the once-around circle loop, contrary to [F3]. Thus its loop class is nontrivial despite F=0.

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