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Undeformed Lefschetz and Hodge-Riemann restrict to the next Soergel summand

Facts & Assumptions

Given: x,s with xs>x, the tensor product M=BxRBsR with its induced form and the operators Lζ (The deformed Lefschetz operator L_zeta on B_x B_s), and the assumption that Bxs occurs as the top bimodule summand of M with multiplicity one.

[F1]

The normalized summand BxsR⊆M is a direct summand as a graded bimodule; under S(<xs) the comparison lemma gives the unshifted decomposition M=BxsR⊕⨁y<xsByR,ay, and then ch⁡(M)=H‾xH‾s and ch⁡(Bxs)=H‾xs after S(xs) (Indecomposable labels, characters and filtration ranks agree after real scalar extension).

[F2]

If the ambient space satisfies hL and HR and V is an L0-stable graded subspace with dim⁡V−i=dim⁡Vi for every i, then V inherits hL and HR with the ambient signs, and its restricted form is non-degenerate (Signature constancy in a Lefschetz family, the L-stable subspace lemma and the weak-Lefschetz substitute).

[F3]

Under S(xs) the nonzero invariant forms on BxsR are unique up to a nonzero real scalar, and the restriction of the intersection form of M along any reduced-word embedding of xs is a positive multiple of the normalized intrinsic form; consequently HR(xs) and HRbar(xs) are equivalent and no sign changes (Invariant forms on an indecomposable Soergel bimodule are unique up to scalar, non-degenerate, and agree with the restricted Bott-Samelson form).

Statement

Let xs>x. The normalized indecomposable BxsR occurs as a bimodule summand of BxRBsR.

(a) If hL(x,s)0 holds, then hL(xs) holds.

(b) If S(<xs) and hL(y) for every y<xs hold, then hL(x,s)0 is equivalent to hL(xs).

(c) If HRbar(x,s)0 holds, then the restriction to the chosen BxsR summand satisfies the Hodge-Riemann relations for its induced form; once S(xs) has been established, positive comparison of invariant forms gives HR(xs) and HRbar(xs) with the standard sign.

(d) More generally an L0-stable graded subspace with symmetric Betti numbers inherits HR with the ambient signs, and a graded direct summand whose subspace and complement are both L0-stable inherits hL from an ambient hL operator. These conclusions apply to a positive deformation only if the chosen subspace, and for the direct-sum argument its complement, are preserved by that operator; they make no identification of the restricted positive operator with left multiplication by ρ.

Proof

technique · direct; block decomposition of the operator along the summand and the stable-subspace lemma
1.1givenF1algebra

Restriction of hard Lefschetz (a). The inclusion i:BxsR→M and the projection π:M→BxsR of the summand are degree-zero bimodule maps, and they commute with left multiplication by ρ, since left multiplication by a central element is a bimodule endomorphism; after right reduction they remain a split inclusion and projection of the finite-dimensional real spaces. Hence the operator L0i on M‾ is block diagonal with respect to the decomposition of M‾ into the summand and its complement, and each block is the corresponding power of the restricted operator. If L0i is an isomorphism, then its inverse commutes with the block decomposition, so each diagonal block is invertible; in particular the block BxsR‾−i→BxsR‾i is an isomorphism. This holds for every i≥0, which is hL(xs).

2.1step 1.1F1

The converse under the character hypotheses (b). Assume S(<xs) and hL(y) for all y<xs. By [F1] the decomposition M=BxsR⊕⨁y<xsByR,ay has no shifts, and every lower label y<xs satisfies S(y); the module BxsR is self-dual with symmetric Betti numbers, and by the comparison lemma the same holds for every lower summand. If hL(xs) holds, the block of L0i on BxsR is invertible; by hypothesis each lower block ByR is invertible (hL(y)), and no other summands occur; therefore every diagonal block is invertible, so L0i is invertible, which is hL(x,s)0. This proves the equivalence.

3.1step 2.1F2F3

Restriction of HR (c). Assume HRbar(x,s)0, that is, HR for the restriction of the intersection form over a fixed reduced-word embedding of x‾ and a fixed induced form of M; the summand BxsR has symmetric Betti numbers by self-duality, and the inclusion is L0-stable. Applying the stable-subspace lemma [F2] to V=BxsR‾ inside M‾ gives that the restricted operator and form satisfy hL and HR with the ambient signs; since the lowest degree of BxsR equals the lowest degree −ℓ(xs) of M, the ambient standard sign is the standard sign of BxsR. Once S(xs) is known, [F3] identifies the restricted form with a positive multiple of the normalized intrinsic form, and HR(xs) and HRbar(xs) follow with no change of signs.

4.1step 1.1step 3.1F2∎

General stable subspaces (d). For an L0-stable graded subspace with symmetric Betti numbers, [F2] gives hL and HR with the ambient signs. If instead a graded decomposition H=V⊕W has both V and W L0-stable and H satisfies hL, then each L0i:H−i→Hi is block diagonal. Its injectivity and surjectivity give injectivity and surjectivity on each block separately, hence hL on V, as in step 1.1. Merely being a graded direct summand is insufficient: in a length-one Lefschetz string, the stable top line has zero degree −1 part and a nonzero degree 1 part. A positive deformation Lζ with ζ>0 preserves a summand only when the summand's projector commutes with the middle-position operator, which is not automatic; when it does not, the restriction of Lζ to the summand is not defined as an operator on the reduced summand, so no positive-parameter restriction statement is made. In particular no step identifies the restriction of Lζ with left multiplication by ρ. This proves (d) and completes the lemma.

Remarks

  • The equivalence in (b) is the point where the induction closes downward: hL for the tensor product is recovered from hL for the top summand and the already-established hL of the strictly lower summands, with the unshifted decomposition supplied by S(<xs).
  • The last sentence of (d) is a genuine caveat: middle multiplication does not commute with an arbitrary summand projector, so positive-parameter restriction is never used on this page; the positive parameters are handled by the deformation principle and the signature-constancy lemma instead.

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