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Stream: learning: questions

Topic: Derived bilinear and quadratic forms


view this post on Zulip Damien Robert (Mar 18 2026 at 13:21):

Hi everyone, this is my first time posting here!

I have some elementary questions about derived (non additive) functors between categories of sheaf modules, seen as functors between stable or prestable \infty-categories, and I hope I am in the correct channel to ask them. (Disclaimer: I have been trying to learn more about \infty-categories but currently I am just a beginner on this topic.)

First some context. Warning, wall of text incoming, you can skip this part and go directly in my questions below.

view this post on Zulip Damien Robert (Mar 18 2026 at 13:22):

I work in algorithmic number theory, and lately I have taken an interest in the arithmetic associated to biextensions and cubical torsor structures on abelian varieties. Biextensions were introduced by Mumford, and thoroughly developed by Grothendieck in SGA7. Later, Lawrence Breen in his book Fonctions thêta et théorème du cube introduces the notions of a symmetric biextension and of a "structure du cube sur un torseur LL" which I'll translate as a cubical (or cubic?) torsor structure. The first Chapter of the book by Moret-Bailly Pinceaux de variétés Abéliennes gives also a nice introduction to this concept (and of hypercube torsor structures).

For now let Sh(X,τ)Sh(X,\tau) be an arbitrary topos, and F,G,HF,G,H be abelian sheaves over XX. Then Grothendieck shows in SGA7 that the stack of biextensions of F×GF \times G by HH corresponds to τ0RHom(FLG,H[1])\tau_{\leq 0} R\mathcal{Hom}(F \otimes^L G, H[1]) (using cohomogical grading). Then Breen shows that a symmetric biextension by HH over F×FF \times F corresponds to τ0RHom(LSym2F,H[1])\tau_{\leq 0} R\mathcal{Hom}(L Sym^2 F, H[1]), and a cubical HH-torsor structure over FF corresponds to τ0RHom(LP2+F,H[1])\tau_{\leq 0} R\mathcal{Hom}(L P^+_2 F, H[1]), where P2+FP^+_2 F represents the universal quadratic form qq on FF, normalised by q(0)=0q(0)=0 (by quadratic form I mean an application of degree 2\leq 2, not necessarily homogeneous; since qq is normalised, this is equivalent to requiring q(x+y+z)q(x+y)q(y+z)q(x+z)+q(x)+q(y)+q(z)=0q(x+y+z)-q(x+y)-q(y+z)-q(x+z)+q(x)+q(y)+q(z)=0 internally in the topos).

They then specialize the theory to the case of (degenerations) of abelian schemes over some base SS, with F,GF, G the fppf sheafs associated to abelian schemes A,B/SA,B/S, and HH the fppf sheaf associated to Gm\mathbb{G}_m. For simplicity I'll stick to the case of abelian varieties A,B/kA,B/k over some field kk here.

Reformulating the cohomological definitions above (which I will call the "intrinsic definitions"), we obtain that:

Notice that in each case the derived bilinear/quadratic structure induces a map to BGmB\mathbb{G}_m, hence a Gm\mathbb{G}_m-torsor (i.e. a line bundle) over A×BA \times B, resp. AA; torsor which is further endowed with a "bilinear", resp. "quadratic" structure. Taking simplicial resolutions, Grothendieck and Breen give concrete description of what this extra structure means in practice (I will call this the "external description").

For instance, a cubical structure on a Gm\mathbb{G}_m-torsor LL should consist in a trivialisation σ\sigma of θ3(L)=m123Lm12L1m23L1m13L1m1Lm2Lm3L\theta_3(L) = m_{123}^{\ast} L \otimes m_{12}^{\ast} L^{-1} \otimes m_{23}^{\ast} L^{-1} \otimes m_{13}^{\ast} L^{-1} \otimes m_{1}^{\ast} L \otimes m_{2}^{\ast} L \otimes m_{3}^{\ast} L (using the notations of Moret-Bailly), where m123:A3A,(P1,P2,P3)P1+P2+P3m_{123}: A^3 \to A, (P_1, P_2, P_3) \mapsto P_1+P_2+P_3, m12:A3A,(P1,P2,P3)P1+P2m_{12}: A^3 \to A, (P_1, P_2, P_3) \mapsto P_1+P_2, and so on. Furthermore, this trivialisation σ\sigma should satisfy some appropriate cocycle conditions (one elegant way to state them, as explained in Moret-Bailly's book, is that up to replacing AA by an fppf cover AA', and Gm\mathbb{G}_m by some injective group GG, we obtain an induced trivialisation σ\sigma' associated to Θ3(L)\Theta_3(L') where LL' is the GG-torsor on AA' associated to LL, and this σ\sigma' should be of the form Θ3(s)\Theta_3(s) for ss a trivialisation of LL' over AA', i.e. LL' should be endowed with a "trivial cubical structure"). Similar external descriptions hold for biextensions and symmetric biextensions.

Now the remarkable thing is that due to the rigidity of abelian varieties, given a line bundle LL on AA, it is automatically endowed with a unique cubical structure. Likewise we have a bijection between morphisms ABA \to B^{\vee} and biextensions over A×BA \times B (via pullback of the Poincare biextension over B×BB \times B^{\vee}), and symmetric biextensions over A×AA \times A correspond to polarisations λ:AA\lambda: A \to A^{\vee}.

This is pretty cool, because this means that we can think of polarisations and line bundles on an abelian variety AA as derived symmetric bilinear form and derived quadratic forms with values in BGmB\mathbb{G}_m respectively. And this explains many constructions we do with them: e.g., the Mumford construction that associates a polarisation λL\lambda_L on AA from a line bundle LL mirrors the way we associate a symmetric bilinear form b(x,y)=q(x+y)q(x)q(y)b(x,y)=q(x+y)-q(x)-q(y) from a (normalised) quadratic form qq; this also "explains" why having a rational line bundle LL is stronger than having a rational polarisation (because a quadratic form is a stronger arithmetic data than a symmetric bilinear form). More generally every elementary statement on quadratic/bilinear form seems to translate to a "categorical version" (I'll come back to this later).

For another example: a quadratic form qq on XX degenerates (i.e. becomes linear) over XXX' \subset X when the associated bilinear form bb is 00 over X×XX' \times X'. Well if LL is a line bundle on AA, the associated biextension is trivial over K(L)×K(L)K(L) \times K(L) where K(L)K(L) is the kernel of the polarisation λL\lambda_L, so the cubical structure on LL degenerates to a squared structure on LK(L)L \mid K(L), i.e. we have a "derived linear form" with values in BGmB\mathbb{G}_m, i.e. an element of Ext1(K(L),Gm)Ext^1(K(L), \mathbb{G}_m), i.e. a group extension G(L)G(L) of K(L)K(L) by Gm\mathbb{G}_m. We recover Mumford's theta group G(L)G(L). In fact, the biextension associated to λL\lambda_L is trivial over K(L)×AK(L) \times A, this gives the usual action of G(L)G(L) on the sections of LL. We also recover the standard Weil pairing as a degeneration of the biextension structure.

Yet another (related) example: a quadratic form qq on XX descends through a morphism ϕ:XY\phi: X \to Y with kernel XX' when q(X)=0q(X')=0, but also the associated bilinear form bb is trivial over X×XX' \times X. There is a corresponding statement for descending a cubical structure over AA through a morphism ϕ:AB\phi: A \to B with kernel AA': there should be a trivialisation of the cubical structure over AA' and of the biextension over A×AA' \times A, trivialisations compatible with each other over A×AA' \times A'. Applying this to a complex abelian variety A=Cg/ΛA=\mathbb{C}^g/\Lambda, and because cube structures over Cg\mathbb{C}^g are necessarily trivial, we get that cube structures over AA can be described as suitable descent of the trivial cube structure over Cg\mathbb{C}^g through Λ\Lambda. As explained by Breen in his book this gives an alternative algebraic theory of theta functions.

A last comment on this: we can think of a cube structure on a line bundle LL over AA as some sort of "quadratic arithmetic" on LL which lifts the group arithmetic (i.e. a "linear arithmetic") on AA. It turns out that instantiating this arithmetic explicitly gives surprisingly efficient formulas. This is what I have been working on: even in the very special case of an elliptic curve E/FqE/\mathbb{F}_q over a finite field, it turns out that using this "cubical arithmetic" (on the torsor associated to (0E)(0_E)) to compute e.g. pairings beat in certain cases the state of the art.

Ok, that's it for the context, apologies that was longer than I expected. Now for my questions.

view this post on Zulip Damien Robert (Mar 18 2026 at 13:22):

Question 1

As we saw above, the stack of "derived symmetric bilinear form" is given by τ0RHom(LSym2A,Gm[1])\tau_{\leq 0} R\mathcal{Hom}(L Sym^2 A, \mathbb{G}_m[1]), and a "derived quadratic form" is given by τ0RHom(LP2+A,Gm[1])\tau_{\leq 0} R\mathcal{Hom}(L P^+_2 A, \mathbb{G}_m[1]) (using cohomological grading).

In both cases we need to derive a quadratic functor GG (in particular not additive), like G=Sym2G=Sym^2, on abelian sheaves in a topos. For this, Breen takes simplicial resolutions. I expect that the modern point of view of derived categories as stable \infty-categories clarifies the construction of LGLG.

More precisely (this is essentially a copy/paste of this question I asked on mathoverflow):

First we consider the case of a topos over a point, and of an additive functor. So let G:AbAbG:Ab→Ab be a right exact functor on the abelian category of abelian groups.

Since AbAb has enough projectives, we can build the left derived functor LG:D(Ab)DAb)LG:D_−(Ab)→D_Ab) (Lurie, Higher Algebra, Example 1.3.3.4.), which we can extend to LG:D(Ab)D(Ab)LG:D(Ab)→D(Ab) using the fact that D(Ab)D(Ab) (using the construction of Higher Algebra, Definition 1.3.5.8. for Grothendieck abelian categories) is left complete.

More generally, I also want to consider functors GG which are not necessarily additive, but at least preserve 1-sifted colimits. In which case, I think that we can also define LG:D(Ab)D(Ab)LG:D(Ab)→D(Ab) as the stabilisation of Ani(G):D(Ab)0D(Ab)0Ani(G):D(Ab)_{≥0}→D(Ab)_{≥0} (using homological grading).

Now let (X,τ)(X,τ) be a 1-site, then we can consider the 1-topos Sh(X,Ab)Sh(X,Ab). Then, if I understand correctly "Lurie, Spectral Algebraic Geometry, Corollary 2.1.2.3", we have that D(Sh(X,Ab))D(Sh(X,Ab)) is the hypercompletion of the topos of hZh\mathbb{Z}-sheaf of spectras Sh(X,D(Ab))Sh(X,D(Ab)).

On the one hand we can extend GG to a functor G\mathcal{G} on Sh(X,Ab)Sh(X,Ab) by sheafification. On the other hand we can also extend LGLG to a functor LG\mathcal{LG} on D(Sh(X,Ab))D(Sh(X,Ab)) by (hyper)sheafification.

Now I would expect LG\mathcal{LG} to be a left derived functor LGL\mathcal{G} of G\mathcal{G}. Is it true?

N.B.: for my applications, I am interested in τ0Hom(LG,BGm)\tau_{\ge 0} \mathcal{Hom}(\mathcal{LG}, B \mathbb{G}_m) (in homological grading this time). Since I am truncating to the connective part, I guess that hypercompleting does not really change the result, and I could take the sheafification of LGLG rather than the hypersheafification. Is that correct? (I am not really confortable with hypercompletion subtleties).

view this post on Zulip Damien Robert (Mar 18 2026 at 13:22):

Question 2

So we have seen that we have an intrinsic definition of biextensions, symmetric biextensions and cubical torsor structures as derived bilinear form, derived symmetric bilinear forms and derived quadratic forms with values in BGmB\mathbb{G}_m.

But translating this definition into an external statement is quite painful, see e.g. $8 of Breen's book. Now in a standard 1-topos, I am fairly confortable translating/compiling an internal statement in the internal logic into an external statement.

Here we are in the derived world, so in an \infty-topos, but from what I understand HoTT gives us precisely an internal logic of this \infty-topos, and a way to "compile" internal statements into external statements. (Disclaimer: I know even less about HoTT than about \infty-categories.)

So the question is whether compiling the internal statement "we have a quadratic form with values in BGmB\mathbb{G}_m" gives back the external characterisation of cubical torsor structures, without having to jump through the hoop of computing explicit simplicial resolutions as Breen does in his book?

To be fair, since I am looking at 1-truncations of Hom spaces/anima, HoTT is probably overkill and I probably just need to look at 1-stack semantics, rather than a fully fledged \infty-topos semantic (let alone the univalence principle).

Still, from the few thing I learned about HoTT, is that from afar it seems that it would work. The very rough idea I get from HoTT is that the equality type should be a fully fledged type/Anima, not just as a Proposition. And so an equality should be 'witnessed' by some sort of extra data, maybe subject to some sort of coherence condition, and recursively so.

If I apply this guiding principle to what should be a "derived quadratic form with values in BGmB\mathbb{G}_m, I get that if qq corresponds to the torsor LL, the statement q(x+y+z)q(x+y)q(y+z)q(x+z)+q(x)+q(y)+q(z)=0q(x+y+z)-q(x+y)-q(y+z)-q(x+z)+q(x)+q(y)+q(z)=0 corresponds to a choice trivialisation σ\sigma of θ3(L)=m123Lm12L1m23L1m13L1m1Lm2Lm3L\theta_3(L) = m_{123}^{\ast} L \otimes m_{12}^{\ast} L^{-1} \otimes m_{23}^{\ast} L^{-1} \otimes m_{13}^{\ast} L^{-1} \otimes m_{1}^{\ast} L \otimes m_{2}^{\ast} L \otimes m_{3}^{\ast} L. But now this choice σ\sigma is subject to some coherence conditions.
Except that I have moved one categorical level up, from the delooping BGmB \mathbb{G}_m to Gm\mathbb{G}_m; and if σ\sigma does give a cubical structure, I can tweak it by an actual quadratic form σ\sigma' with values in Gm\mathbb{G}_m to get a potentially non isomorphic cube structure σσ\sigma \sigma'. (And I can stop the recursion here, because the πi\pi_i are trivial for i>1i>1.) Which is precisely what happens in practice from the explicit description of the cubical torsor structure. (One needs to be a bit careful about moving one level up from BGmB \mathbb{G}_m to Gm\mathbb{G}_m: for instance if we have σ\sigma inducing a trivial symmetric biextension, then we have to tweak σ\sigma by σ\sigma' an alternate bilinear form rather than a symmetric bilinear form to get another symmetric biextension.)

view this post on Zulip Damien Robert (Mar 18 2026 at 15:50):

Damien Robert said:

This is pretty cool, because this means that we can think of polarisations and line bundles on an abelian variety AA as derived symmetric bilinear form and derived quadratic forms with values in BGmB\mathbb{G}_m respectively.

Of course, retrospectively, I should have understood this a lot sooner. Already to define the dual abelian variety AA^{\vee}, we cannot use Hom(A,Gm)\mathcal{Hom}(A, \mathbb{G}_m) because it is trivial, so we instead go through τ0RHom(A,Gm[1])\tau_{\leq 0} R\mathcal{Hom}(A, \mathbb{G}_m[1]), whose' π1\pi_1' is trivial, and whose 'π0\pi_0' is Ext1(A,Gm)\mathcal{Ext}^1(A, \mathbb{G}_m); which we can also reinterpret as Hom(A,BGm)Hom(A, B\mathbb{G}_m) where here in the Hom we want morphisms that respects the group structure, i.e. "morphisms of Picard stacks". In other words the dual abelian variety is described by "1-truncated derived linear forms" already.

(One might naively expect that RHom(A,Gm)R \mathcal{Hom}(A, \mathbb{G}_m) would be concentrated in degree [0,1][0,1], but although Ext2(A,Gm)=0\mathcal{Ext}^2(A, \mathbb{G}_m)=0, Breen has examples of abelian varieties in characteristic 2 where Ext3(A,Gm)0\mathcal{Ext}^3(A, \mathbb{G}_m) \ne 0, so that's why we need to truncate to have something sane.)

And as a bilinear form b:X×YZb: X \times Y \to Z may be thought as a linear map ϕ:XY\phi: X \to Y^{\vee} where Y=Hom(Y,Z)Y^{\vee}=Hom(Y, Z) is the "dual" of YY (and, in the case Y=XY=X with XXX \simeq {X^{\vee}}^{\vee} is "bidual", then bb is symmetric precisely when ϕ\phi is autodual), it indeed is the case that a biextension, i.e. a derived bilinear form on A×BA \times B, is the same as a linear map ABA \to B^{\vee}, where BB^{\vee} is the "derived dual" of BB (and in the case A=BA=B, the biextension is symmetric precisely when ϕ\phi is symmetric, i.e. equal to its dual). So it makes sense that polarisations are a way to encode (1-truncated) derived bilinear forms on abelian varieties.

view this post on Zulip Kevin Carlson (Mar 18 2026 at 15:58):

Hi Damien, welcome! This is really an awfully, awfully long, very technical post. I think you’d have a lot better luck getting a conversation started if you could pick somewhere to start where an expert would have at least a decent chance of being able to say something quickly.

view this post on Zulip Damien Robert (Mar 18 2026 at 16:09):

Hi Kevin, thanks! Yes I wanted to add some context to my questions, but maybe that was a bad idea... I am mostly interested in Question 1 which should be self contained: basically to what extent can we expect sheafification to commute with derivation. Or more precisely, given a functor G:AbAbG: Ab \to Ab (say which preserves 1-sifted colimits), if we sheafify and then derive it, is it the same thing as sheafifying the derivation of GG (up to hypercompletion subtleties)?

view this post on Zulip Kevin Carlson (Mar 18 2026 at 16:16):

Thanks for clarifying that. As far as I can tell you have a sequence of two questions, even in that: first, about deriving sifted colimit-preserving functors, and then about how this hypothetical operation interacts with sheafification. No?

view this post on Zulip Damien Robert (Mar 18 2026 at 16:38):

Indeed, but I am fairly sure that for GG a 1-sifted colimit preserving functor, then under the identification of Ani(Ab)Ani(Ab) with D0(Ab)D_{\geq 0}(Ab), Ani(G)Ani(G) coincides with LGLG. Here Ani(G)Ani(G) is the unique functor Ani(Ab)Ani(Ab)Ani(Ab) \to Ani(Ab) that commutes with \infty-sifted limit and whose value on projective f.t. Z\mathbb{Z}-modules (or even just free f.t. Z\mathbb{Z}-modules) MM is given by G(M)G(M).

On the other hand there is indeed also an implicit question about whether stabilisation also commutes with sheafification, because I need to have BGmB \mathbb{G}_m, the delooping of Gm\mathbb{G}_m, in my sheaf topos, but that's less important.

So forgetting about stabilisation, I guess my main question is, given (X,τ)(X,\tau) a 11-site and denoting G:Sh(X,Ab)Sh(X,Ab)\mathcal{G}: Sh(X, Ab) \to Sh(X, Ab) the sheafification of GG, then is the hypersheafification of Ani(G)Ani(G) a derived functor of G\mathcal{G} under the identification of D0(Shτ(X,Ab))D_{\geq 0}(Sh_{\tau}(X,Ab)) as the hypercompletion of Shτ(X,D0(Ab))Sh_{\tau}(X, D_{\geq 0} (Ab))?

view this post on Zulip John Baez (Mar 18 2026 at 17:16):

I'm really interested in polarizations of abelian varieties, and curious about quantifying the way they contain less information than line bundles, but I'd have to overcome a laziness barrier to follow how it relates to all this more general abstract stuff. :cry: In short, I'm the guy who was interested in your intended application more than the techniques.

view this post on Zulip Damien Robert (Mar 18 2026 at 19:03):

John Baez said:

I'm really interested in polarizations of abelian varieties, and curious about quantifying the way they contain less information than line bundles

So that's a very good question, and IMHO a good rule of thumb to have an intuition about the difference between line bundles and polarisations is that it is exactly (a derived version of) the difference between a (normalised) quadratic form and a symmetric bilinear form.

To a (normalised) quadratic form q:XZq: X \to Z (where X,ZX, Z are say some abelian groups) we can associate a symmetric bilinear form b:X×XZb: X \times X \to Z via b(x,y)=q(x+y)q(x)q(y)b(x,y)=q(x+y)-q(x)-q(y). Conversely to a bilinear form bb, we can associate a quadratic form Q(x)=b(x,x)Q(x)=b(x,x). Crucially, these are not inverse operations!

A few remarks on this:

All of this generalizes to abelian varieties, replacing XX by AA and ZZ by Gm\mathbb{G}_m, or rather by BGmB\mathbb{G}_m:

In particular, given a rational polarisation ϕ:AA\phi: A \to A^{\vee} over kk, ϕ\phi is induced by a line bundle only over an étale extension of kk in general (notice that although the multiplication by 22 is not surjective on Gm\mathbb{G}_m it is étale locally surjective, at least in characteristic different from 22). The set of such line bundles form a torsor AA' under AA^{\vee}, and we can find a rational line bundle on AA inducing ϕ\phi iff AA' is trivial, i.e. has a point over kk. If kk is a finite field, this is always the case by Lang's theorem, so there is no obstruction! Likewise, if we want a rational symmetric line bundle LL representing ϕ\phi, the obstruction is measured by an étale A[2]A[2]-torsor.

(to be continued later)

view this post on Zulip Damien Robert (Mar 18 2026 at 21:26):

As an aside, I would like to point out that the above statements on line bundles on abelian varieties are treated in pretty much every book about them, but they do require some work, unless the trivial corresponding statements about standard quadratic and biliear forms. Related to my Question 2, is the question of how much the general theory of (symmetric) biextensions and cubical structures could simply be seen as the specialisation of a general theory of quadratic and bilinear forms in an \infty-topos; which would give the statements above "for free". Of course we would still need to prove the specific feature of abelian varieties, which is that all line bundles over them have a unique cubical structure. By the way, a key insight of Grothendieck-Breen-Moret Bailly is that it is the later notion rather than the former which is the "correct" one when looking at deformations of abelian schemes.

view this post on Zulip Damien Robert (Mar 18 2026 at 21:26):

Anyway, going back to quadratic forms, if we have a XX-torsor XX' (i.e. a set XX' with a free and transitive action from XX), then we can still define a notion of quadratic form q:XZq: X' \to Z on XX'. Namely, q(w+x+y+z)q(w+x+y)q(w+y+z)q(w+z+x)+q(w+x)+q(w+y)+q(w+z)q(w)=0wX,x,y,zXq(w+x+y+z)-q(w+x+y)-q(w+y+z)-q(w+z+x)+\\q(w+x)+q(w+y)+q(w+z)-q(w) =0\quad \forall w \in X', x,y,z \in X (in fact it suffices to check this for one base point wXw \in X'). To this qq over XX', we can still associate a bilinear form b:X×XZb: X \times X \to Z via b(x,y)=q(w+x+y)+q(w)q(w+x)q(w+y)b(x,y)=q(w+x+y)+q(w)-q(w+x)-q(w+y).

view this post on Zulip Damien Robert (Mar 18 2026 at 21:26):

The same construction works for abelian varieties. If we have a AA-torsor AA' and a rational line bundle LL on AA', this LL still gives a rational polarisation ϕ:AA\phi: A \to A^{\vee} on AA.

The most important example is the case of Jacobians. If C/kC/k is a (proper smooth geometrically connected) curve, the theta divisor Θ\Theta (the locus of effective divisors of degree g1g-1) is rational and lives in Picg1(C)Pic^{g-1}(C), which is a torsor under the Jacobian J(C)=Pic0(C)J(C)=Pic^0(C). So the Jacobian always has a rational principal polarisation λ\lambda, but it may not have a rational line bundle associated to λ\lambda if Picg1(C)Pic^{g-1}(C) has no rational points.

view this post on Zulip Damien Robert (Mar 18 2026 at 21:26):

There is a famous article by Poonen and Stoll about this situation. When A/kA/k is a principally polarised abelian variety over a number field kk, the Cassel-Tate pairing ш(A)×ш(A)Q/Zш(A) \times ш(A) \to \mathbb{Q}/\mathbb{Z} is non degenerate and antisymmetric (assuming the Tate-Shafarevich group is finite). If furthermore λ\lambda is represented by a rational line bundle, then the Cassel-Tate pairing is even alternate, so the Tate-Shafarevich group has cardinal a square. But Poonen and Stoll construct explicit examples of curves where the Tate-Shafarevich group of the Jacobian is twice a square; hence their Jacobian cannot admit a rational line bundle representing the canonical principal polarisation!

view this post on Zulip John Baez (Mar 18 2026 at 22:01):

Damien Robert said:

John Baez said:

I'm really interested in polarizations of abelian varieties, and curious about quantifying the way they contain less information than line bundles

So that's a very good question, and IMHO a good rule of thumb to have an intuition about the difference between line bundles and polarisations is that it is exactly (a derived version of) the difference between a (normalised) quadratic form and a symmetric bilinear form.

To a (normalised) quadratic form q:XZq: X \to Z (where X,ZX, Z are say some abelian groups) we can associate a symmetric bilinear form b:X×XZb: X \times X \to Z via b(x,y)=q(x+y)q(x)q(y)b(x,y)=q(x+y)-q(x)-q(y). Conversely to a bilinear form bb, we can associate a quadratic form Q(x)=b(x,x)Q(x)=b(x,x). Crucially, these are not inverse operations!

I've mainly thought about this in two contexts, which you might be interested in. Maybe you know all about this, and I'm not really an expert on it, but anyway:

  1. The classification of finite simple groups includes those of 'Lie type' like the special orthogonal groups SO(n,F) and symplectic groups Sp(n,F) for finite fields F, but this becomes tricky when F has characteristic two, because the difference between symmetric and antisymmetric bilinear forms evaporates, but also the difference between bilinear forms and quadratic forms becomes very significant. (There's also the added complication that the classification of nondegenerate quadratic forms over finite fields is unfamiliar to physicists such as myself who are used to working over R\mathbb{R} or C\mathbb{C}.)

  2. Mac Lane classified homotopy 2-types of double loop spaces in terms of 'quadratic functions' from an abelian group GG to an abelian group AA. Joyal and Street realized that Mac Lane was secretly classifying braided 2-groups XX: braided monoidal groupoids where every object has an inverse under tensor product. GG is the group of isomorphism classes of objects of XX (aka π0\pi_0) while AA is the group of automorphisms of the unit object (aka π1)\pi_1)). The quadratic function comes from the 'self-braiding' of objects xx, namely Bx,x:xxxx B_{x,x} : x \otimes x \to x \otimes x , together with a standard trick for turning an endomorphism of xxx \otimes x into an endomorphism of the unit object.

I feel the second one might even be relevant to what you're saying, though you're probably dealing with (derived versions of) symmetric 2-groups rather than braided ones.

view this post on Zulip Damien Robert (Mar 19 2026 at 22:08):

John Baez said:

I've mainly thought about this in two contexts, which you might be interested in. Maybe you know all about this,

On the contrary, I am quite out of my depth on all this higher category / derived stuff.

  1. The classification of finite simple groups includes those of 'Lie type' like the special orthogonal groups SO(n,F) and symplectic groups Sp(n,F) for finite fields F, but this becomes tricky when F has characteristic two, because the difference between symmetric and antisymmetric bilinear forms evaporates, but also the difference between bilinear forms and quadratic forms becomes very significant. (There's also the added complication that the classification of nondegenerate quadratic forms over finite fields is unfamiliar to physicists such as myself who are used to working over R\mathbb{R} or C\mathbb{C}.)

I tend to avoid characteristic 2 in my work because I use symmetric theta structures on ppavs a lot, and things get a bit weird when the 22-torsion is not étale.
So apart from the Arf invariant, which is of course very important to classify even and odd theta characteristics, I don't know much about quadratic forms in char 2.

You might be interested in the following paper by Breen: Biextensions alternées. He defines a notion of antisymmetric and alternate biextension (in an analog way of his earlier definition of a symmetric biextension in his book); show that this is the 'correct' derived generalisation of a antisymmetric, resp. alternate bilinear form; and that being alternate is a stronger property than being antisymmetric, as expected.

view this post on Zulip Damien Robert (Mar 19 2026 at 22:09):

(For some reason most of the litterature on biextensions/cube structure seem to be in french)

view this post on Zulip Damien Robert (Mar 19 2026 at 22:34):

John Baez said:

  1. Mac Lane classified homotopy 2-types of double loop spaces in terms of 'quadratic functions' from an abelian group GG to an abelian group AA. Joyal and Street realized that Mac Lane was secretly classifying braided 2-groups XX: braided monoidal groupoids where every object has an inverse under tensor product. GG is the group of isomorphism classes of objects of XX (aka π0\pi_0) while AA is the group of automorphisms of the unit object (aka π1)\pi_1)). The quadratic function comes from the 'self-braiding' of objects xx, namely Bx,x:xxxx B_{x,x} : x \otimes x \to x \otimes x , together with a standard trick for turning an endomorphism of xxx \otimes x into an endomorphism of the unit object.

This seems very interesting, do you have a reference for this?

More generally, it has been quite a surprise to me to learn that the polarisations/line bundles on abelian varieties I had been working with were actually (1-truncated) derived bilinear forms and quadratic forms in disguise, and I'd be very interested in other examples of this kind in nature. Notably:

1) Going up in degree/dimension: of course biextension can be generalised to n-multi-extension (the derived version of multilinear forms), and cube structures to $n+1$-hypercube structure (the derived version of a form of degree n\leq n; there is an unfortunate shift on the nn here), and an n+1n+1-hypercube structure on AA gives a symmetric nn-multiextension on AnA^n in exactly the same way a form of degree $\leq n$$ gives a nn-multilinear form.

However, triextensions (and more) of an abelian variety by GmG_m are trivial, and so are the n+1n+1-hypercube structures. It seems that the interesting arithmetic on abelian varieties is inherently quadratic.

Apparently, if π:XS\pi: X \to S is a proper flat morphism of schemes of relative dimension nn, then the determinant functor RdetπR det \pi_{\ast} has a (n+2)(n+2)-hypercube structure.

2) Going up in categorical level. I would also be curious to see some "natural examples" of a derived quadratic or bilinear form with value in B2GmB^2 \mathbb{G}_m, i.e. in gerbes rather than in torsors.

view this post on Zulip John Baez (Mar 20 2026 at 02:16):

Damien Robert said:

John Baez said:

  1. Mac Lane classified homotopy 2-types of double loop spaces in terms of 'quadratic functions' from an abelian group GG to an abelian group AA. Joyal and Street realized that Mac Lane was secretly classifying braided 2-groups XX: braided monoidal groupoids where every object has an inverse under tensor product.

This seems very interesting, do you have a reference for this?

Sorry, I forgot to include a link: this is available in the unpublished version of their paper "Braided monoidal categories", which contains more than the published version! It's in section 7, "Cohomology of abelian groups", though you should also look at section 6, "Cohomology of groups".