For subfields E⊆F∩LE \subseteq F \cap L of C\mathbb{C}, Broudy and Eterović (Ramanujan J. 62:781–795, 2023) define FF to be G(E)G(E)-disjoint from LL, written F⊥EGLF \perp_E^G L, where G=GL2G = \mathrm{GL}_2 acts by Möbius transformations: every finite subset of LL whose elements lie in distinct G(E)G(E)-orbits also has its elements in distinct G(F)G(F)-orbits. Unlike linear disjointness and freeness of fields, which are symmetric relations, it is unknown whether GG-disjointness is symmetric: does F⊥EGLF \perp_E^G L imply L⊥EGFL \perp_E^G F? The authors prove symmetry only in the special case E=F∩LE = F \cap L with FF and LL linearly disjoint over EE (their Lemma 2.2). The question, posed as open in their Remark 2.1, remains open.

Background

A standard notion in field theory is linear disjointness: extension fields FF and LL of a common base field EE are linearly disjoint over EE if every finite EE-linearly independent tuple from one remains linearly independent over the other; a companion notion, freeness (EE-algebraically independent tuples staying algebraically independent over the other field) is defined analogously with algebraic independence in place of linear independence. Both relations are symmetric, a classical fact recorded for instance in Lang's Algebra and recalled by Broudy and Eterović in their study of Schanuel-type conjectures.

The motivation comes from transcendence theory. Schanuel's conjecture predicts that for complex numbers x1,…,xnx_1,\dots,x_n linearly independent over Q\mathbb{Q}, the field Q(x1,…,xn,ex1,…,exn)\mathbb{Q}(x_1,\dots,x_n,e^{x_1},\dots,e^{x_n}) has transcendence degree at least nn over Q\mathbb{Q}. Work quoted in Broudy and Eterović (their reference [CDH+09]) shows that, assuming Schanuel's conjecture, the field generated by all iterated exponentials of algebraic numbers and the field generated by all iterated logarithms are linearly disjoint over Q‾\overline{\mathbb{Q}}, the field of algebraic numbers. Broudy and Eterović extend this to towers built over more general base fields FF, and, crucially, to the modular jj-function (the holomorphic function on the upper half-plane H\mathbb{H} whose value at zz classifies the complex elliptic curve C/(Z+Zz)\mathbb{C}/(\mathbb{Z} + \mathbb{Z}z)) under a modular Schanuel conjecture. Because the jj-function is not a group homomorphism, linear disjointness is no longer the correct notion there; the replacement, introduced earlier by the second author in his 'A Schanuel property for jj' (Bull. Lond. Math. Soc. 50, 2018, DOI: 10.1112/blms.12135), is GG-disjointness, defined as follows.

Let G=GL2G = \mathrm{GL}_2 (the group of invertible 2×22 \times 2 matrices) act on the Riemann sphere P1(C)=C∪{∞}\mathbb{P}^1(\mathbb{C}) = \mathbb{C} \cup \{\infty\} by Möbius transformations: a matrix (abcd)\left(\begin{smallmatrix} a & b \\ c & d \end{smallmatrix}\right) with coefficients in a subfield K⊆CK \subseteq \mathbb{C} sends xx to (ax+b)/(cx+d)(ax+b)/(cx+d). For a subfield K⊆CK \subseteq \mathbb{C} and a finite set A⊂CA \subset \mathbb{C}, write dim⁡G(K)(A)\dim_{G(K)}(A) for the number of distinct G(K)G(K)-orbits (under this action) meeting AA; a set is G(K)G(K)-independent if each of its elements lies in a different G(K)G(K)-orbit. Given subfields E⊆F∩LE \subseteq F \cap L of C\mathbb{C}, one says that FF is G(E)G(E)-disjoint from LL, denoted F⊥EGLF \perp_E^G L, if every finite subset of LL that is G(E)G(E)-independent is also G(F)G(F)-independent; equivalently, whenever two elements ℓ1,ℓ2∈L\ell_1, \ell_2 \in L are related by some matrix in G(F)=GL2(F)G(F) = \mathrm{GL}_2(F), they are already related by a matrix in G(E)=GL2(E)G(E) = \mathrm{GL}_2(E). This notion is what lets Broudy–Eterović prove (under a modular Schanuel conjecture) that the tower of fields generated by iterated jj-values and the tower generated by their iterated jj-preimages are disjoint over the base in the orbit sense; the related closure-operator machinery for jj appears in Aslanyan–Eterović–Kirby's 'A closure operator respecting the modular jj-function'.

The definition of ⊥EG\perp_E^G quantifies only over tuples from one side (LL), just as linear disjointness is classically defined; but for linear disjointness and freeness the symmetry can be recovered, while for GG-disjointness the usual exchange/dimension arguments are unavailable, since orbit structure under Möbius transformations is not a matroid-like dimension (a matroid is the abstract independence structure with an exchange law that makes basis-and-dimension counting work for linear and algebraic independence). Broudy and Eterović note two structural facts. Their Lemma 2.3: F⊥EGLF \perp_E^G L forces F∩L=EF \cap L = E. Their Lemma 2.2: if E=F∩LE = F \cap L and FF is linearly disjoint from LL over EE, then both F⊥EGLF \perp_E^G L and L⊥EGFL \perp_E^G F hold — this is the only general source of symmetry currently known, and it is how the authors convert the freeness obtained from Schanuel-type inequalities into GG-disjointness of the two jj-towers in both directions.

Problem Statement

Let G=GL2G = \mathrm{GL}_2 act on the Riemann sphere P1(C)=C∪{∞}\mathbb{P}^1(\mathbb{C}) = \mathbb{C} \cup \{\infty\} by Möbius transformations, (abcd)⋅x=(ax+b)/(cx+d)\left(\begin{smallmatrix} a & b \\ c & d \end{smallmatrix}\right) \cdot x = (ax+b)/(cx+d). For subfields K⊆CK \subseteq \mathbb{C}, say a finite subset of C\mathbb{C} is G(K)G(K)-independent if no two of its elements lie in a common G(K)G(K)-orbit. For subfields E,F,L⊆CE, F, L \subseteq \mathbb{C} with E⊆F∩LE \subseteq F \cap L, define F⊥EGLF \perp_E^G L to mean: every finite subset of LL that is G(E)G(E)-independent is also G(F)G(F)-independent (equivalently, any two elements of LL related by a matrix in GL2(F)\mathrm{GL}_2(F) are already related by a matrix in GL2(E)\mathrm{GL}_2(E)).

Question (Broudy–Eterović, Remark 2.1, Ramanujan J. 62, 2023; posed as open): is GG-disjointness a symmetric relation? That is, is it true for all subfields E,F,L⊆CE, F, L \subseteq \mathbb{C} with E⊆F∩LE \subseteq F \cap L that

F⊥EGL  ⟺  L⊥EGF?F \perp_E^G L \iff L \perp_E^G F?

Symmetry fails exactly when there are subfields E⊆F∩L⊆CE \subseteq F \cap L \subseteq \mathbb{C} with F⊥EGLF \perp_E^G L but L̸⊥EGFL \not\perp_E^G F; by Lemmas 2.2 and 2.3 of the source, any such triple must satisfy E=F∩LE = F \cap L, with FF and LL not linearly disjoint over EE.

References

  1. Isaac A. Broudy, Sebastian Eterović, Schanuel type conjectures and disjointness, The Ramanujan Journal 62(3):781–795, 2023. DOI: 10.1007/s11139-023-00707-3, https://doi.org/10.1007/s11139-023-00707-3 (preprint arXiv:2211.09556, https://arxiv.org/abs/2211.09556)
  2. Sebastian Eterović, A Schanuel property for j, Bulletin of the London Mathematical Society 50(2):293–315, 2018. DOI: 10.1112/blms.12135, https://doi.org/10.1112/blms.12135 (preprint arXiv:1701.05841, https://arxiv.org/abs/1701.05841)
  3. Vahagn Aslanyan, Sebastian Eterović, Jonathan Kirby, A closure operator respecting the modular j-function, Israel Journal of Mathematics 253(1):321–357, 2023. DOI: 10.1007/s11856-022-2362-y, https://doi.org/10.1007/s11856-022-2362-y (preprint arXiv:2010.00102, https://arxiv.org/abs/2010.00102)