Quaternion algebra

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In

extending scalars (equivalently, tensoring with a field extension
), i.e. for a suitable field extension K of F, is
isomorphic
to the 2 × 2 matrix algebra over K.

The notion of a quaternion algebra can be seen as a generalization of Hamilton's quaternions to an arbitrary base field. The Hamilton quaternions are a quaternion algebra (in the above sense) over , and indeed the only one over apart from the 2 × 2 real matrix algebra, up to isomorphism. When , then the biquaternions form the quaternion algebra over F.

Structure

Quaternion algebra here means something more general than the algebra of Hamilton's quaternions. When the coefficient field F does not have characteristic 2, every quaternion algebra over F can be described as a 4-dimensional F-vector space with basis , with the following multiplication rules:

where a and b are any given nonzero elements of F. From these rules we get:

The classical instances where are Hamilton's quaternions (a = b = −1) and split-quaternions (a = −1, b = +1). In split-quaternions, and , differing from Hamilton's equations.

The algebra defined in this way is denoted (a,b)F or simply (a,b).[3] When F has characteristic 2, a different explicit description in terms of a basis of 4 elements is also possible, but in any event the definition of a quaternion algebra over F as a 4-dimensional central simple algebra over F applies uniformly in all characteristics.

A quaternion algebra (a,b)F is either a

matrix algebra of 2 × 2 matrices over F; the latter case is termed split.[4]
The norm form

defines a structure of

anisotropic quadratic form, that is, zero only on the zero element. The conic
C(a,b) defined by

has a point (x,y,z) with coordinates in F in the split case.[5]

Application

Quaternion algebras are applied in

p-adic fields the construction of quaternion algebras can be viewed as the quadratic Hilbert symbol of local class field theory
.

Classification

It is a theorem of Frobenius that there are only two real quaternion algebras: 2 × 2 matrices over the reals and Hamilton's real quaternions.

In a similar way, over any local field F there are exactly two quaternion algebras: the 2 × 2 matrices over F and a division algebra. But the quaternion division algebra over a local field is usually not Hamilton's quaternions over the field. For example, over the p-adic numbers Hamilton's quaternions are a division algebra only when p is 2. For odd prime p, the p-adic Hamilton quaternions are isomorphic to the 2 × 2 matrices over the p-adics. To see the p-adic Hamilton quaternions are not a division algebra for odd prime p, observe that the congruence x2 + y2 = −1 mod p is solvable and therefore by Hensel's lemma — here is where p being odd is needed — the equation

x2 + y2 = −1

is solvable in the p-adic numbers. Therefore the quaternion

xi + yj + k

has norm 0 and hence doesn't have a multiplicative inverse.

One way to classify the F-algebra isomorphism classes of all quaternion algebras for a given field F is to use the one-to-one correspondence between isomorphism classes of quaternion algebras over F and isomorphism classes of their norm forms.

To every quaternion algebra A, one can associate a quadratic form N (called the norm form) on A such that

for all x and y in A. It turns out that the possible norm forms for quaternion F-algebras are exactly the Pfister 2-forms.

Quaternion algebras over the rational numbers

Quaternion algebras over the rational numbers have an arithmetic theory similar to, but more complicated than, that of quadratic extensions of .

Let be a quaternion algebra over and let be a

place
of , with completion (so it is either the p-adic numbers for some prime p or the real numbers ). Define , which is a quaternion algebra over . So there are two choices for : the 2 × 2 matrices over or a division algebra.

We say that is split (or unramified) at if is isomorphic to the 2 × 2 matrices over . We say that B is non-split (or ramified) at if is the quaternion division algebra over . For example, the rational Hamilton quaternions is non-split at 2 and at and split at all odd primes. The rational 2 × 2 matrices are split at all places.

A quaternion algebra over the rationals which splits at is analogous to a

real quadratic field
and one which is non-split at is analogous to an
unit groups
in an order of a rational quaternion algebra: it is infinite if the quaternion algebra splits at [citation needed] and it is finite otherwise[citation needed], just as the unit group of an order in a quadratic ring is infinite in the real quadratic case and finite otherwise.

The number of places where a quaternion algebra over the rationals ramifies is always even, and this is equivalent to the

quadratic reciprocity law
over the rationals. Moreover, the places where B ramifies determines B up to isomorphism as an algebra. (In other words, non-isomorphic quaternion algebras over the rationals do not share the same set of ramified places.) The product of the primes at which B ramifies is called the discriminant of B.

See also

Notes

  1. ^ See Pierce. Associative algebras. Springer. Lemma at page 14.
  2. ^ See Milies & Sehgal, An introduction to group rings, exercise 17, chapter 2.
  3. ^ Gille & Szamuely (2006) p.2
  4. ^ Gille & Szamuely (2006) p.3
  5. ^ Gille & Szamuely (2006) p.7
  6. ^ Lam (2005) p.139

References

  • Gille, Philippe; Szamuely, Tamás (2006). Central simple algebras and Galois cohomology. Cambridge Studies in Advanced Mathematics. Vol. 101. Cambridge: .
  • .

Further reading