Abstract
For quadratic forms in 4 variables defined over the rational function field in one variable over \(\mathbb C(\!(t)\!)\), the validity of the local-global principle for isotropy with respect to different sets of discrete valuations is examined.
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1 Introduction
Let E be a field of characteristic different from 2 and let E(X) denote the rational function field in one variable over E.
For \( E = \mathbb C(\!(t)\!)\), the field of Laurent series in one variable over the complex numbers, the quadratic form
in the variables \(Y_1, Y_2,Y_3,Y_4\) over E(X) has no non-trivial zero, but it has a non-trivial zero over the completion of E(X) with respect to any non-trivial valuation on E(X) that is trivial on E. This is in contrast to the situation when E is a finite field, by the Hasse-Minkowski theorem (see [6, Chapter VI, Theorem 66.1]). Note that, in both cases, the field E has a unique extension of each degree in a fixed algebraic closure.
By a \(\mathbb Z\)-valuation we mean a valuation with value group \(\mathbb Z\). A quadratic form is isotropic if it has a non-trivial zero, otherwise it is anisotropic. Without any restrictions on the base field E other than \(\mathsf {char}(E) \ne 2\), any anisotropic quadratic form over E(X) of dimension at most 3 remains anisotropic over the completion of E(X) with respect to some \(\mathbb Z\)-valuation on E(X) that is trivial on E; this follows for example from Milnor’s exact sequence [4, Theorem IX.3.1]. The case of 4-dimensional quadratic forms is the first case over E(X) where the validity of such a local-global principle for isotropy depends on the base field E.
When E is a non-dyadic local field, using a result of Lichtenbaum [5], one obtains that a 4-dimensional anisotropic quadratic form over E(X) remains anisotropic over the completion of E(X) with respect to some \(\mathbb Z\)-valuation on E(X) that is trivial on E (see [1, Remark 3.8]). This resembles the case where E is a finite field.
In contrast to the situations where E is a finite field or a local field, for \(E=\mathbb C(\!(t)\!)\), the example of the quadratic form above shows that the local-global principle for isotropy of 4-dimensional quadratic forms over E(X) fails with respect to \(\mathbb Z\)-valuations that are trivial on E. However, anisotropy of this quadratic form can be detected over the larger field \(\mathbb C(X)(\!(t)\!)\) by using Springer’s theorem (see [4, Proposition VI.1.9]).
Consider the more general situation where the field E is complete with respect to a non-dyadic \(\mathbb Z\)-valuation v. In this case, a local-global principle for isotropy was obtained in [1] using a geometric setup. Let \(\mathcal {O}_v\) denote the valuation ring of v. By a model for E(X) over \(\mathcal {O}_v\) we mean a two-dimensional integral normal projective flat \(\mathcal {O}_v\)-scheme \(\mathscr {X}\) whose function field is isomorphic to E(X). Codimension-one points on a model of E(X) over \(\mathcal {O}_v\) correspond to certain \(\mathbb Z\)-valuations on E(X). For a model \(\mathscr {X}\) of E(X) over \(\mathcal {O}_v\), let \(\Omega _\mathscr {X}\) denote the set of \(\mathbb Z\)-valuations given by codimension-one points of \(\mathscr {X}\). Consider the set \(\Omega = \bigcup _{\mathscr {X} } \Omega _\mathscr {X}\) where the union is taken over all models \(\mathscr {X}\) of E(X) over \(\mathcal {O}_v\). It follows from [1, Theorem 3.1 and Remark 3.2] that an anisotropic quadratic form over E(X) remains anisotropic over the completion of E(X) with respect to some \(\mathbb Z\)-valuation in \(\Omega \). One may ask whether this remains true if one replaces \(\Omega \) by \(\Omega _{\mathscr {X}}\) for some well-chosen model \(\mathscr {X}\) of E(X) over \(\mathcal {O}_v\).
The aim of this note is to show that this is not the case: if the residue field of v is separably closed, then, for any model \(\mathscr {X}\) of E(X) over \(\mathcal {O}_v\), there exists an anisotropic 4-dimensional quadratic form over E(X) which is isotropic over the completion of E(X) with respect to any \(w\in \Omega _{\mathscr {X}}\) (Corollary 2). Let \(\pi \in \mathcal {O}_v\) be a uniformiser of v. For any model \(\mathscr {X}\) of E(X) over \(\mathcal {O}_v\), the set \(\{w(\pi ) \mid w \in \Omega _{\mathscr {X}} \}\) is finite and hence it has an upper bound. However, for any positive integer r, the quadratic form
is anisotropic over E(X), but it is isotropic over the completion of E(X) with respect to any \(\mathbb Z\)-valuation w on E(X) with \(w(\pi ) <r\) (Theorem). The construction of \(\varphi _r\) is inspired by the example in [1, Remark 3.6] of an anisotropic 6-dimensional quadratic form over \(\mathbb Q_p(X)\) where p is an odd prime.
2 Results
We assume some familiarity with basic quadratic form theory over fields, for which we refer to [4]. We first fix some notation and recall some results.
By a quadratic form or simply a form we mean a regular quadratic form. Let E always be a field of characteristic different from 2 and let \({E}^{\times }\) denote its multiplicative group. For \(a_1, \ldots , a_n \in {E}^{\times }\), the diagonal form \(a_1X_1^2+\dots +a_nX_n^2\) is denoted by \(\langle a_1, \ldots ,a_n\rangle \).
Let v be a \(\mathbb Z\)-valuation on E. We denote the corresponding valuation ring, its maximal ideal, and its residue field respectively by \(\mathcal {O}_v, \mathfrak {m}_v\), and \(\kappa _v\). For an element \(a\in \mathcal {O}_v\), let \(\overline{a}\) denote the residue class \(a+\mathfrak {m}_v\) in \(\kappa _v\). The completion of E with respect to v is denoted by \(E_v\). We say that v is henselian if it extends uniquely to every finite field extension of E. Complete discretely valued fields are henselian (see [2, Theorem 1.3.1 and Theorem 4.1.3]). We recall a consequence of Hensel’s lemma:
Lemma
Let v be a henselian \(\mathbb Z\)-valuation on E such that \(v(2) =0\). Then:
-
(a)
For \(u_1,u_2\in {\mathcal {O}}^{\times }_v\), the quadratic form \(\langle u_1, u_2 \rangle \) over E is isotropic if and only if \(\overline{u_1u_2} \in -{\kappa }^{\times 2}_v\).
-
(b)
If \(\kappa _v\) is separably closed, then every 3-dimensional form over E is isotropic.
Proof
(a) For \(u_1,u_2\in {\mathcal {O}}^{\times }_v\), since v is henselian and \(v(2)=0\), it follows by [2, Theorem 4.1.3(4)] that \(u_1u_2 \in -{E}^{\times 2}\) if and only if \(\overline{u_1u_2} \in -{\kappa }^{\times 2}_v\).
(b) Every 3-dimensional form over E contains a 2-dimensional form isometric to \(\lambda \langle 1 ,u\rangle \) for some \(u \in {\mathcal {O}}^{\times }_v\) and \(\lambda \in {E}^{\times }\). If \(\kappa _v\) is separably closed, then \(\overline{u} \in -{\kappa }^{\times 2}_v\) and hence \(\langle 1, u\rangle \) is isotropic by (a). \(\square \)
The set of all \(\mathbb Z\)-valuations on E(X) is denoted by \(\Omega _{E(X)}\). For \(r\in \mathbb {N}\), we define
With this notation, \(\Omega _0\) is the set of all E-trivial \(\mathbb Z\)-valuations on E(X). We recall that any monic irreducible polynomial \(p \in E[X]\) determines a unique \(\mathbb Z\)-valuation \(v_p\) on E(X) which is trivial on E and such that \(v_p(p)=1\). There is further a unique \(\mathbb Z\)-valuation \(v_\infty \) on E(X) such that \(v_\infty (f)=-\deg (f)\) for any \(f\in E[X]\setminus \{0\}\). Moreover, every \(\mathbb Z\)-valuation w on E(X) trivial on E is either equal to \(v_\infty \) or to \(v_p\) for some monic irreducible polynomial \(p \in E[X]\) (see [2, Theorem 2.1.4]), and in either of the two cases the residue field is a finite field extension of E.
Theorem
Let v be a henselian \(\mathbb Z\)-valuation on E such that \(v(2) =0\). Assume that \(\kappa _v\) is separably closed. Let \(\pi \in {E}^{\times }\) be such that \(v(\pi ) =1\) and let \(r \in \mathbb {N}\). Then the quadratic form
is isotropic over \(E(X)_w\) for every \(\mathbb Z\)-valuation \(w \in \Omega _{r-1}\), but anisotropic over \(E(X)_w\) for some \(w\in \Omega _r\).
Proof
Set \(F=E(X)\). We first show that \(\varphi _r\) is isotropic over \(F_w\) for all \(w\in \Omega _{r-1}\). Consider \(w\in \Omega _{r-1}\).
Case 1: \(w(\pi ) =0 = w(X)\). Then \(\kappa _w\) is a finite extension of E. Since v is henselian, there is a unique extension \(v'\) of v to \(\kappa _w\), and \(v'\) is again henselian. Furthermore, it follows by [2, Theorem 3.3.4] that \(v'({\kappa }^{\times }_w)\) is isomorphic to \(\mathbb Z\) and \(\kappa _{v'}\) is separably closed. It follows by part (b) of the Lemma that every 3-dimensional quadratic form over \(\kappa _w\) is isotropic. We have that \(w =v_p\) for some monic irreducible polynomial \(p \in E[X]\) such that \(p \ne X\). Note that, in this case, at least three diagonal coefficients of \(\varphi _r\) are units in \(\mathcal {O}_w\). It follows by Springer’s theorem [4, Proposition VI.1.9] that \(\varphi _r\) is isotropic over \(F_w\).
Case 2: \(0 \le w (\pi )< r\) and \(1\le w(X)\). Let \( u = (X^r\pi ^{-1}-1)(X^{(r+1)}\pi ^{-1}+1)\). Then \(w(u) =0\) and \(\overline{u} =-1 \in - {\kappa }^{\times 2}_w\). It follows by part (a) of the Lemma that the form \(\pi ^{-1} \langle X^r-\pi , X^{r+1}+\pi \rangle \) is isotropic over \(F_w\). Thus \(\varphi _r\) is isotropic over \({F}_w\).
Case 3: \(w(X)< 0 \le w (\pi )< r\). Note that, if \(w(\pi ) =0\), then \(w =v_\infty \) and \(\kappa _w =E\), and otherwise \(w|_E\) is equivalent to v and \(\kappa _v \subseteq \kappa _w\); since \(-1\in {\kappa }^{\times 2}_v\), we get in either case that \(-1 \in {\kappa }^{\times 2}_w\). Consider \( u = (1+ \pi X^{-{(r+1)}})(1+\pi X^{-r})\). We have that \(w(u) =0\) and \(\overline{ u } = 1 \in {\kappa }^{\times 2}_w = -{\kappa }^{\times 2}_w\). It follows by part (a) of the Lemma that the form \(X^{-(r+1)} \langle X^{r+1}+\pi , X(X^{r}+\pi )\rangle \) is isotropic over \(F_w\). Thus \(\varphi _r\) is isotropic over \(F_w\).
We have thus shown that \(\varphi _r\) is isotropic over \(F_w\) for every \(w \in \Omega _{r-1}\). Now we show that \(\varphi _r\) is anisotropic over \(F_w\) for some \(w\in \Omega _F\).
Let \(E' = E(s)\), where \(s =\root r \of {\pi }\). Then v extends uniquely to a valuation on \(E'\) which we again denote by v. Note that \(s^r = \pi \) in \(E'\) and hence \(v (\pi ) = rv(s)\). Then \(v' = rv\) is a \(\mathbb Z\)-valuation on \(E'\).
Let \(L= E'(X)\) and let \(Y =\frac{X}{s}\). Note that \(L =E'(Y)\). By [2, Corollary 2.2.2], there exists a unique extension of \(v'\) to L such that \(v(Y) =0\) and \(\overline{Y}\) is transcendental of \(\kappa _{v'}\); we further have that \(\kappa _w = \kappa _{v'}(\overline{Y})\) and \(w({L}^{\times }) = v'({E'}^{\times }) = \mathbb Z\). Since \(w(Y) =0\), we have that \(w(X) =w(s) =1\). We get that
Consider the forms \(\varphi _1 = \langle Y^r-1,~ sY+1\rangle \) and \(\varphi _2 = \langle Y,~ Y(Y^r+1) \rangle \).
Since \( \overline{Y}^r-1, \overline{Y}^{r} +1 \notin - {\kappa }^{\times 2}_w\), it follows by Springer’s theorem [4, Proposition VI.1.9] that the quadratic form \(s^{-r}\varphi _r\) is anisotropic over \(L_w\). Hence \(\varphi _r\) is anisotropic over \(L_w\). We obtain that \(\varphi _r\) is anisotropic over \(F_{w|_F}\). Note that \(w(\pi ) = w(s^r) =rw(s) =r\), thus \(w\in \Omega _r\). \(\square \)
We now provide a different perspective to the above theorem. For a subset \(\Omega \subseteq \Omega _{E(X)}\), we say that \(\Omega \) has the finite support property if for every \(f \in {E(X)}^{\times }\), the set \(\{w\in \Omega \mid w(f) \ne 0\}\) is finite. It is well-known that \(\Omega _{0}\) has the finite support property. When E carries a discrete valuation, the set \(\Omega _{E(X)}\) does not have the finite support property. However, for any model \(\mathscr {X}\) of E(X) over \(\mathcal {O}_v\), the set \(\Omega _\mathscr {X}\) contains \(\Omega _0\) and has the finite support property. We show the following:
Corollary 1
Let v be a henselian \(\mathbb Z\)-valuation on E with \(v(2) =0\). Assume that \(\kappa _v\) is separably closed. Let \(\Omega \subseteq \Omega _{E(X)}\) be a subset with the finite support property. Then there exists an anisotropic 4-dimensional quadratic form over E(X) which is isotropic over \(E(X)_w\) for every \(w\in \Omega \).
Proof
Let \(\pi \in {E}^{\times }\) be such that \(v(\pi ) =1\). Since \(\Omega \) has the finite support property, the set \(\{w\in \Omega \mid w(\pi ) \ne 0 \}\) is finite. Set \(r= 1+\max \{w(\pi ) \mid w\in \Omega \}\). Clearly \(\Omega \subseteq \Omega _{r-1} \). Then the form \(\varphi _r\) in the Theorem is isotropic over \(E(X)_w\) for every \(w\in \Omega \), but anisotropic over E(X). \(\square \)
Corollary 2
Let v be a henselian \(\mathbb Z\)-valuation on E with \(v(2) =0\). Assume that \(\kappa _v\) is separably closed. Let \(\mathscr {X}\) be a regular model of E(X) over \(\mathcal {O}_v\). Then there exists an anisotropic 4-dimensional quadratic form over E(X) which is isotropic over \(E(X)_w\) for every \(w\in \Omega _{\mathscr {X}}\).
Proof
By [3, Chapter II, Lemma 6.1], for every element \(f\in {E(X)}^{\times }\), the set \(\{w \in \Omega _{\mathscr {X}} \mid w(f) \ne 0 \}\) is finite, hence the statement follows by Corollary 1.
\(\square \)
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Acknowledgements
The author wishes to thank David Leep, Suresh Venapally, Karim Johannes Becher, Gonzalo Manzano Flores, and Marco Zaninelli for many inspiring discussions and comments related to this article. This article is based on the author’s PhD-thesis, prepared under the supervision of Karim Johannes Becher (Universiteit Antwerpen) and Arno Fehm (Technische Universität Dresden) in the framework of a joint PhD at Universiteit Antwerpen and Universität Konstanz.
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This work was supported by the Fonds Wetenschappelijk Onderzoek – Vlaanderen (FWO) in the FWO Odysseus Programme (project ‘Explicit Methods in Quadratic Form Theory’), the Bijzonder Onderzoeksfonds (BOF), University of Antwerp (project BOF-DOCPRO-4, 2865), and the Science and Engineering Research Board (SERB), India (Grant CRG/2019/000271).
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Gupta, P. Four-dimensional quadratic forms over \(\mathbb C(\!(t)\!)(X)\). Arch. Math. 117, 369–374 (2021). https://doi.org/10.1007/s00013-021-01626-9
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DOI: https://doi.org/10.1007/s00013-021-01626-9