For a number field FF, Burns, de Jeu, Gangl, Rahm and Yasaki (Forum Math. Sigma 9 (2021) e40) constructed a 'modified Bloch group' B‾(F)\overline{\mathcal{B}}(F) from symbols [x][x], x∈F∖{0,1}x\in F\setminus\{0,1\}, together with a natural homomorphism ψF:B‾(F)→K3(F)tfind\psi_F:\overline{\mathcal{B}}(F)\to K_3(F)^{\mathrm{ind}}_{\mathrm{tf}} into the torsion-free part of the indecomposable third algebraic KK-group of FF. Injectivity of ψF,tf\psi_{F,\mathrm{tf}} is proven for every number field, and the conjecture (their Conjecture 3.33) is that ψF,tf\psi_{F,\mathrm{tf}} is an isomorphism for every number field FF; it has been verified computationally for all imaginary quadratic fields of discriminant >−1000>-1000. The problem is to prove surjectivity for all number fields, or to exhibit a number field for which the image has index strictly greater than 11.

Background

Algebraic KK-theory attaches to any field FF a sequence of abelian groups Kn(F)K_n(F) introduced by Quillen. For n=3n=3 there is a canonical map from Milnor KK-theory K3M(F)K_3^{M}(F) (the degree-33 part of the graded ring built from F×=F∖{0}F^{\times}=F\setminus\{0\} modulo the Steinberg relation x⊗(1−x)x\otimes(1-x)), and the cokernel K3(F)indK_3(F)^{\mathrm{ind}} is the indecomposable K3K_3. A theorem of Borel computes K3(F)indK_3(F)^{\mathrm{ind}} for a number field FF (a finite extension of Q\mathbb{Q}) rationally: its torsion-free part K3(F)tfindK_3(F)^{\mathrm{ind}}_{\mathrm{tf}} is a free abelian group of rank r2(F)r_2(F), the number of conjugate pairs of complex embeddings, and it is measured by the regulator, obtained by evaluating the Bloch–Wigner dilogarithm DD (the single-valued real-analytic function on C∖{0,1}\mathbb{C}\setminus\{0,1\} defined by integrating log⁡∣w∣ darg⁡(1−w)−log⁡∣1−w∣ darg⁡(w)\log|w|\,d\arg(1-w)-\log|1-w|\,d\arg(w), which satisfies the five-term functional equation) under each embedding σ:F→C\sigma:F\to\mathbb{C}. Borel's result further identifies the size of the regulator lattice with the leading term ζF∗(−1)\zeta_F^{*}(-1) at −1-1 of the Dedekind zeta function of FF (the analogue for FF of the Riemann zeta function: the Dirichlet series ∑aN(a)−s\sum_{\mathfrak{a}}N(\mathfrak{a})^{-s} over the non-zero ideals a\mathfrak{a} of OFO_F, with N(a)N(\mathfrak{a}) the norm); the Lichtenbaum conjecture refines this to an integral formula ζF∗(−1)=±2r2+t2(F)∣K2(OF)∣/∣K3(OF)tor∣⋅R2(F)\zeta_F^{*}(-1)=\pm 2^{r_2+t_2(F)}|K_2(O_F)|/|K_3(O_F)_{\mathrm{tor}}|\cdot R_2(F), where OFO_F is the ring of integers of FF, R2(F)R_2(F) is the covolume of the regulator image, and the power of 22 was pinned down conditionally in the same paper. The classical bridge between dilogarithms and K3K_3 is the Bloch group. The pre-Bloch group of FF is the free abelian group Z[F♭]\mathbb{Z}[F^{\flat}] on F♭=F∖{0,1}F^{\flat}=F\setminus\{0,1\} modulo the five-term relations [x]−[y]+[y/x]−[(1−y)/(1−x)]+[(1−y−1)/(1−x−1)]=0[x]-[y]+[y/x]-[(1-y)/(1-x)]+[(1-y^{-1})/(1-x^{-1})]=0; Suslin's Bloch group B(F)B(F) is the kernel of the boundary map [x]↦(1−x)∧x[x]\mapsto (1-x)\wedge x into an exterior-square group of F×F^{\times}. Suslin proved that for every infinite field B(F)tf≅K3(F)tfindB(F)_{\mathrm{tf}}\cong K_3(F)^{\mathrm{ind}}_{\mathrm{tf}}, which for number fields re-interprets Borel's theorem through the dilogarithm. Burns, de Jeu, Gangl, Rahm and Yasaki introduced a modified version designed to avoid the factor-of-22 losses in Goncharov's original GL2\mathrm{GL}_2-equivariant construction. They define

∧~2F×=(F×⊗ZF×)/⟨(−x)⊗x⟩,\widetilde{\wedge}^{2}F^{\times}=(F^{\times}\otimes_{\mathbb{Z}}F^{\times})/\langle(-x)\otimes x\rangle,

with class written a ∧~ ba\,\tilde{\wedge}\,b, and the boundary δ2,F:Z[F♭]→∧~2F×\delta_{2,F}:\mathbb{Z}[F^{\flat}]\to\widetilde{\wedge}^{2}F^{\times}, [x]↦(1−x) ∧~ x[x]\mapsto(1-x)\,\tilde{\wedge}\,x. The modified pre-Bloch group is p(F)=Z[F♭]\mathfrak{p}(F)=\mathbb{Z}[F^{\flat}] modulo the five-term relations above and the additional inversion relations [x]+[x−1]=0[x]+[x^{-1}]=0 and [x]+[1−x]=0[x]+[1-x]=0, and the modified Bloch group is B‾(F)=ker⁡(δ2,F:p(F)→∧~2F×)\overline{\mathcal{B}}(F)=\ker(\delta_{2,F}:\mathfrak{p}(F)\to\widetilde{\wedge}^{2}F^{\times}). A theorem of Burns–de Jeu–Gangl (2012) gives a homomorphism φF:ker⁡(δ2,F)→K3(F)tfind\varphi_F:\ker(\delta_{2,F})\to K_3(F)^{\mathrm{ind}}_{\mathrm{tf}}, natural up to a universal sign, characterized by the fact that, after fixing the sign, composing with the regulator induced by an embedding σ\sigma sends each [x][x] to iD(σ(x))iD(\sigma(x)). Theorem 3.25 of the paper shows φF\varphi_F descends to a homomorphism ψF:B‾(F)→K3(F)tfind\psi_F:\overline{\mathcal{B}}(F)\to K_3(F)^{\mathrm{ind}}_{\mathrm{tf}}. For a number field FF, the kernel of ψF\psi_F is exactly the torsion subgroup of B‾(F)\overline{\mathcal{B}}(F), so the induced ψF,tf:B‾(F)tf→K3(F)tfind\psi_{F,\mathrm{tf}}:\overline{\mathcal{B}}(F)_{\mathrm{tf}}\to K_3(F)^{\mathrm{ind}}_{\mathrm{tf}} is injective and its cokernel is finite; combining with Suslin's isomorphism and the paper's Theorem 3.23 (B‾(F)tf≅B(F)tf\overline{\mathcal{B}}(F)_{\mathrm{tf}}\cong B(F)_{\mathrm{tf}}) yields an injective endomorphism of the free abelian group K3(F)tfindK_3(F)^{\mathrm{ind}}_{\mathrm{tf}} of rank r2(F)r_2(F), whose index is finite and computable in examples. The conjecture is supported by explicit geometry and computation. For an imaginary quadratic field kk (with ring of integers OkO_k), the group GL2(Ok)\mathrm{GL}_2(O_k) acts on hyperbolic 33-space H3\mathbb{H}^{3}, and the Voronoi tessellation of the cone of positive-definite binary Hermitian forms over OkO_k gives an explicit finite cell decomposition of a quotient of H3\mathbb{H}^{3}. From the cells, their finite stabiliser subgroups, and the cross-ratios of their ideal vertices, the authors construct a 'geometric' element βgeo∈B‾(k)\beta_{\mathrm{geo}}\in\overline{\mathcal{B}}(k) with reg2(ψk(βgeo))/(2πi)=−12ζk′(−1)\mathrm{reg}_2(\psi_k(\beta_{\mathrm{geo}}))/(2\pi i)=-12\zeta'_k(-1), generating a subgroup of index ∣K2(Ok)∣|K_2(O_k)| in K3(k)tfindK_3(k)^{\mathrm{ind}}_{\mathrm{tf}}; dividing by ∣K2(Ok)∣|K_2(O_k)| using 'exceptional SS-units' (an SS-unit, for a finite set SS of primes of OkO_k, is an element of kk that is a unit at every prime outside SS; it is exceptional when 1−x1-x is also an SS-unit) produces generators whenever the division is possible in B‾(k)\overline{\mathcal{B}}(k). In this way the conjecture was verified for all imaginary quadratic fields of discriminant >−1000>-1000, the first proven explicit generators, modulo torsion, of an infinite KK-group of a number field.

Problem Statement

Prove or refute Conjecture 3.33 of Burns–de Jeu–Gangl–Rahm–Yasaki (2021). Let FF be a number field, F♭=F∖{0,1}F^{\flat}=F\setminus\{0,1\}, ∧~2F×=(F×⊗ZF×)/⟨(−x)⊗x:x∈F×⟩\widetilde{\wedge}^{2}F^{\times}=(F^{\times}\otimes_{\mathbb{Z}}F^{\times})/\langle(-x)\otimes x:x\in F^{\times}\rangle, and δ2,F:Z[F♭]→∧~2F×\delta_{2,F}:\mathbb{Z}[F^{\flat}]\to\widetilde{\wedge}^{2}F^{\times} the homomorphism [x]↦(1−x) ∧~ x[x]\mapsto(1-x)\,\tilde{\wedge}\,x. Let p(F)\mathfrak{p}(F) be Z[F♭]\mathbb{Z}[F^{\flat}] modulo the five-term relations [x]−[y]+[y/x]−[(1−y)/(1−x)]+[(1−y−1)/(1−x−1)]=0[x]-[y]+[y/x]-[(1-y)/(1-x)]+[(1-y^{-1})/(1-x^{-1})]=0 (x≠yx\neq y in F♭F^{\flat}) and the inversion relations [x]+[x−1]=0[x]+[x^{-1}]=0, [x]+[1−x]=0[x]+[1-x]=0; let B‾(F)=ker⁡(δ2,F:p(F)→∧~2F×)\overline{\mathcal{B}}(F)=\ker(\delta_{2,F}:\mathfrak{p}(F)\to\widetilde{\wedge}^{2}F^{\times}) be the modified Bloch group, and let ψF:B‾(F)→K3(F)tfind\psi_F:\overline{\mathcal{B}}(F)\to K_3(F)^{\mathrm{ind}}_{\mathrm{tf}} be the homomorphism of Theorem 3.25 of that paper (induced by the sign-normalized map φF\varphi_F of Burns–de Jeu–Gangl, under which the regulator composed with an embedding σ\sigma sends [x][x] to iD(σ(x))iD(\sigma(x))).

Since ψF,tf\psi_{F,\mathrm{tf}} is known to be injective for every number field and both sides are free abelian of rank r2(F)r_2(F), the conjecture is exactly the assertion that

im⁡(ψF,tf)=K3(F)tfindfor every number field F,\operatorname{im}(\psi_{F,\mathrm{tf}})=K_3(F)^{\mathrm{ind}}_{\mathrm{tf}}\quad\text{for every number field }F,

equivalently [K3(F)tfind:im⁡(ψF,tf)]=1[K_3(F)^{\mathrm{ind}}_{\mathrm{tf}}:\operatorname{im}(\psi_{F,\mathrm{tf}})]=1 for every number field FF, equivalently the composite endomorphism of K3(F)tfindK_3(F)^{\mathrm{ind}}_{\mathrm{tf}} obtained from Suslin's isomorphism K3(F)tfind≅B(F)tfK_3(F)^{\mathrm{ind}}_{\mathrm{tf}}\cong B(F)_{\mathrm{tf}}, Theorem 3.23, and ψF,tf\psi_{F,\mathrm{tf}} is an isomorphism (conjecturally multiplication by ±1\pm1).

References

  1. David Burns, Rob de Jeu, Herbert Gangl, Alexander D. Rahm, and Dan Yasaki, Hyperbolic tessellations and generators of K3K_3 for imaginary quadratic fields, Forum of Mathematics Sigma 9 (2021), e40. DOI 10.1017/fms.2021.9; arXiv:1909.09091; https://arxiv.org/abs/1909.09091
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