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The middle-boundary Maslov correction composes for Lagrangian relations

Statement

Use the Wall-form Maslov convention of The four-Lagrangian Maslov cocycle identity. Let B⊆V‾⊕W be a finite-dimensional real Lagrangian relation, where the product symplectic form is −ωV⊕ωW. Write B(L)={w:∃v∈L,(v,w)∈B} and Bt(Q)={v:∃w∈Q,(v,w)∈B}. For Lagrangians L,P⊆V and Q,R⊆W,

μV(L,P,Bt(Q))+μW(B(L),Q,R)=μW(B(P),Q,R)+μV(L,P,Bt(R)).

Consequently, for composable Lagrangian relations A:V0→V1, B:V1→V2, C:V2→V3 and specified Lagrangians λi⊆Vi, the integer correction m(B,A)=μV1(A(λ0),λ1,Bt(λ2)) satisfies

m(B,A)+m(C,BA)=m(C,B)+m(CB,A).

It vanishes when either relation is the identity of a specified object (V,λ) (so the source and target specified Lagrangians agree), is additive on direct sums, and for graphs of symplectic isomorphisms f1,f2 equals μ(f2f1λ0,f2λ1,λ2). No injectivity, transversality or equal-dimension hypothesis on a general relation is imposed.

Facts & Assumptions

Given: The finite-dimensional symplectic spaces, Lagrangian relations and Lagrangians in the Statement.

[F1]

The Wall form on L1∩(L2+L3)/((L1∩L2)+(L1∩L3)) is ψ([a],[a′])=ω(a,b′) with a+b+c=0; its signature μ satisfies the four-Lagrangian cocycle (The four-Lagrangian Maslov cocycle identity).

[F2]

Images of Lagrangians under Lagrangian relations are Lagrangian (A linear Lagrangian relation sends a Lagrangian subspace to a Lagrangian subspace).

[F3]

Lagrangians equal their symplectic orthogonal complements, and finite-dimensional rank-nullity and subspace dimension formulas apply (Isotropic, coisotropic, symplectic, and Lagrangian subspaces, Rank-nullity: dim⁡FV=nullity⁡T+rank⁡T).

Proof

1.1F1F3algebra

The Wall form in [F1] is unchanged by a symplectic isomorphism: the isomorphism carries its numerator and denominator to the corresponding subspaces and preserves ω(a,b′). The cyclic map [a]↦[b], with a+b+c=0, is a well-defined isomorphism between the cyclic Wall quotients: changing a decomposition adds an adjacent intersection, and its inverse is obtained by solving the same sum-zero equation. It preserves the form because ω(b,c′)=−ω(b,a′)=ω(a′,b)=ω(a,b′). Hence μ is cyclically invariant. If the first two Lagrangians agree, its numerator and denominator are both that Lagrangian, so the quotient is zero. Cyclic invariance therefore shows that μ vanishes whenever any two arguments agree. Orthogonal direct sums give orthogonal direct sums of Wall quotients and forms, so their signatures add.

1.2F3algebraconstruct

Set K={v:(v,0)∈B} and K′={w:(0,w)∈B}. Both are isotropic. A vector x annihilates πVB exactly when (x,0) annihilates B, hence belongs to B=B⊥. Thus (πVB)⊥=K and πVB=K⊥; likewise πWB=K′⊥. A pair (v,w)∈B defines an isomorphism ϕ:K⊥/K→K′⊥/K′. Changing w adds precisely K′, and changing v adds K; the two projections are onto and these are their kernels. Isotropy of B gives ωW(w,w′)=ωV(v,v′), so ϕ is symplectic.

1.3F3construct

Choose a Lagrangian N0 containing K. This finite construction needs no transversality: extend a basis ei of K to hyperbolic pairs by choosing vectors fj with ω(ei,fj)=δij, possible by nondegeneracy. Replace fi by fi−12∑jω(fi,fj)ej to make their pairings zero. Their span is symplectic. In its symplectic orthogonal complement, repeatedly choose a nonzero vector and a vector pairing to 1, splitting off a symplectic plane each time. Adjoining one vector from each such plane to the ei spans the required Lagrangian. The construction ends by finite dimension.

2.1F2F3step 1.2algebra

For a Lagrangian L⊆V, put LK=((L∩K⊥)+K)/K. It is Lagrangian in K⊥/K: the inverse image PL=(L∩K⊥)+K is isotropic, and PL⊥=(L+K)∩K⊥=(L∩K⊥)+K=PL. The last equality follows by writing x=l+k and observing that x,k∈K⊥ force l∈K⊥. Here (U∩T)⊥=U⊥+T⊥ follows from inclusion and equal dimensions by [F3]. The relation normal form in step 1.2 gives B(L)/K′=ϕ(LK) and Bt(Q)/K=ϕ−1(QK′). These are equalities of the actual subspaces containing K′ or K, not an assumption that relation images are injective.

3.1F1F3step 1.1step 2.1algebra

Suppose N0,N⊆V both contain K. We prove μV(L,N0,N)=μK⊥/K(LK,N0/K,N/K) by identifying their complete Wall forms. The left numerator L∩(N0+N) lies in K⊥. It projects onto the right numerator: if a representative l+k, with l∈L∩K⊥, lies in the sum of the two reduced spaces, then l∈N0+N, since that sum contains K. The image of (L∩N0)+(L∩N) is precisely the right denominator: l+k∈N0 is equivalent to l∈N0, and likewise for N. The projection kernel L∩K is already in this denominator. Hence the Wall quotient spaces are isomorphic. A decomposition a+b+c=0 projects to the corresponding decomposition, and ω(a,b′) descends to the quotient form because both entries lie in K⊥. The isomorphism is an isometry, proving equality of signatures. By step 1.1 the same reduction holds when any two arguments contain K.

4.1F1step 3.1step 1.3algebra

For arbitrary L,P and N containing K, the four-Lagrangian identity gives μ(L,P,N)−μ(L,P,N0)=μ(L,N0,N)−μ(P,N0,N). Reduce the two right-hand terms by step 3.1 and apply that same identity in K⊥/K. Thus μV(L,P,N)=μK⊥/K(LK,PK,N/K)+ηK(L,P), where ηK(L,P)=μV(L,P,N0)−μK⊥/K(LK,PK,N0/K). In particular the defect is independent of N. The auxiliary N0 disappears from the differences used below.

5.1F1step 1.1step 2.1step 3.1step 4.1algebra

In step 4.1 take N=Bt(Q). By step 2.1 and symplectic invariance, its reduced triple transports by ϕ to (B(L)/K′,B(P)/K′,QK′). Since B(L) and B(P) both contain K′, step 3.1 applied in W identifies this reduced signature with μW(B(L),B(P),Q). Therefore μV(L,P,Bt(Q))−μW(B(L),B(P),Q)=ηK(L,P), independent of Q. Subtract the equations for Q and R and use the four-Lagrangian identity on (B(L),B(P),Q,R) in W. This yields exactly the first identity in the Statement.

6.1F2step 5.1algebra

Relational composition obeys (BA)(λ0)=B(A(λ0)) and (CB)t(λ3)=Bt(Ct(λ3)) by the defining existential equations. Substitute L=A(λ0), P=λ1, Q=λ2, R=Ct(λ3) into step 5.1. All these spaces are Lagrangian by [F2], including inverse images by applying it to transposed relations. The resulting equality is precisely m(B,A)+m(C,BA)=m(C,B)+m(CB,A). Thus adding these integer corrections gives associative weights.

7.1step 1.1step 6.1algebra∎

For the identity of a specified object (V,λ) on either side, its source and target Lagrangians are the same λ, so its image or inverse image is the specified middle Lagrangian, so two arguments of μ agree and the correction is zero by step 1.1. Direct sums add corrections by that same step, including the zero-dimensional empty space. For graphs of symplectic isomorphisms the correction is μ(f1λ0,λ1,f2−1λ2). Transporting all three arguments by f2 gives μ(f2f1λ0,f2λ1,λ2) with precisely the stated sign and order. These prove the remaining conclusions.

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