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On quadratic forms of height two and a theorem of Wadsworth. (English) Zbl 0867.11024

For quadratic forms \(\varphi\) and \(\psi\) over a field \(F\) of characteristic different from two, the function fields \(F(\varphi)\) and \(F(\psi)\) are equivalent (i.e. there are \(F\)-places from each function field to the other) if and only if \(\varphi\) is isotropic over \(F(\psi)\) and \(\psi\) is isotropic over \(F(\varphi)\). This was proved by M. Knebusch in 1976. Equivalence of function fields of quadratic forms is, in general, weaker than their isomorphism, and the cases where the two coincide are of special interest. A third property involved is the similarity of the quadratic forms in question. Here a pioneering work was done by A. R. Wadsworth [Trans. Am. Math. Soc. 208, 352-358 (1975; Zbl 0336.15013)], who proved that for forms of dimension 4 and discriminant 1 the isomorphism of function fields of the forms implies similarity of the forms.
Combining the results of several authors on the interdependence of the equivalence and isomorphism of function fields of quadratic forms and of similarity of quadratic forms (A. R. Wadsworth, D. W. Leep, and the author himself) the author obtains a list of forms \(\varphi\) for which the three properties are equivalent for \(\varphi\) and any quadratic form \(\psi\) with \(\dim\psi=\dim\varphi\). This list consists of Pfister neighbors of codimension 0 or 1, and of forms of dimension at most 6 satisfying some additional conditions. This is the starting point for the author’s first main result.
It is shown that if an anisotropic form \(\varphi\) of dimension \(2^n\), \(n\geq 2\), can be written as the product of an \((n-2)\)-fold Pfister form and a four-dimensional form, then for any quadratic form \(\psi\) of dimension \(2^n\) the following are equivalent: (1) \(\varphi\) is similar to \(\psi\). (2) The function fields \(F(\varphi)\) and \(F(\psi)\) are isomorphic. (3) The function fields \(F(\varphi)\) and \(F(\psi)\) are equivalent.
The second main result asserts that (2) and (3) are equivalent when \(\varphi\) is an anisotropic form of height 2 and degree 1 or 2, \(\psi\) is an anisotropic form, and \(\dim\varphi=\dim\psi\).

MSC:

11E04 Quadratic forms over general fields
12F20 Transcendental field extensions
11E81 Algebraic theory of quadratic forms; Witt groups and rings

Citations:

Zbl 0336.15013
Full Text: DOI

References:

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