Every finite division ring is a field: Difference between revisions
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| 2 || <math>L</math> is a field under the operations induced from <math>K</math>, and the multiplicative group <math>L^*</math> (the nonzero elements of <math>L</math>) is the center of <math>K^*</math>. || || <math>K</math> is a division ring || || <toggledisplay><math>L</math> is an additive subgroup of <math>K</math> because of the distributivity laws relating addition and multiplication. By definition, the nonzero elements of <math>L</math> are the center of the multiplicative group <math>K^*</math>. The center of a group is an abelian subgroup, so the nonzero elements of <math>L</math> form a commutative subgroup of <math>K^*</math>, hence <math>L</math> is a field under the induced operations.</toggledisplay> || Creation of base field (<math>L</math>) for which many of the additive structures of interest are vector spaces | | 2 || <math>L</math> is a field under the operations induced from <math>K</math>, and the multiplicative group <math>L^*</math> (the nonzero elements of <math>L</math>) is the center of <math>K^*</math>. || || <math>K</math> is a division ring || || <toggledisplay><math>L</math> is an additive subgroup of <math>K</math> because of the distributivity laws relating addition and multiplication. By definition, the nonzero elements of <math>L</math> are the center of the multiplicative group <math>K^*</math>. The center of a group is an abelian subgroup, so the nonzero elements of <math>L</math> form a commutative subgroup of <math>K^*</math>, hence <math>L</math> is a field under the induced operations.</toggledisplay> || Creation of base field (<math>L</math>) for which many of the additive structures of interest are vector spaces | ||
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| 3 || <math>K</math> is a vector space over <math>L</math> where the additive structure is the same as that for <math>K</math> as a | | 3 || <math>K</math> is a vector space over <math>L</math> where the additive structure is the same as that for <math>K</math> as a division ring and where the action of elements of <math>L</math> is by left multiplication. || || || Step (2) || <toggledisplay>The linearity follows from distributivity of multiplication.</toggledisplay> || Linear consolidation over <math>L</math> | ||
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| 4 || If <math>L</math> has size <math>q > 1</math>, <math>K</math> has size <math>q^d</math> for some positive integer <math>d</math>, where <math>d</math> is the dimension of <math>K</math> as a vector space over <math>L</math>. || || <math>K</math> is finite || Step (3) || <toggledisplay>Since <math>K</math> is finite, so is <math>L</math>, so <math>L</math> has some size <math>q > 1</math> (since there is no field with one element). Next, since <math>K</math> is finite, it must be finite-dimensional as a vector space over <math>L</math>. If its dimension is <math>d</math>, it is in bijection with the vector space <math>L^d</math> obtained by taking a direct sum of <math>d</math> copies of <math>L</math>. Hence its size must be <math>q^d</math>.</toggledisplay> || Linear consolidation over <math>L</math>, introducing numerical constraints. Note that <math>q</math> must in fact be a prime power, but we only use here that <math>q > 1</math>. | | 4 || If <math>L</math> has size <math>q > 1</math>, <math>K</math> has size <math>q^d</math> for some positive integer <math>d</math>, where <math>d</math> is the dimension of <math>K</math> as a vector space over <math>L</math>. || || <math>K</math> is finite || Step (3) || <toggledisplay>Since <math>K</math> is finite, so is <math>L</math>, so <math>L</math> has some size <math>q > 1</math> (since there is no field with one element). Next, since <math>K</math> is finite, it must be finite-dimensional as a vector space over <math>L</math>. If its dimension is <math>d</math>, it is in bijection with the vector space <math>L^d</math> obtained by taking a direct sum of <math>d</math> copies of <math>L</math>. Hence its size must be <math>q^d</math>.</toggledisplay> || Linear consolidation over <math>L</math>, introducing numerical constraints. Note that <math>q</math> must in fact be a prime power, but we only use here that <math>q > 1</math>. | ||
Revision as of 05:49, 29 August 2026
History
This result was first proved by Wedderburn.
Statement
Every finite division ring is a field, and hence, a finite field. Here, by division ring, we mean associative division ring.
Related facts
Stronger facts
- Bruck-Kleinfeld theorem states that every alternative division ring is either associative (and hence a division ring in the usual sense) or is a Cayley-Dickson algebra.
- In particular, this shows that every finite alternative division ring is a field.
Facts used
Proof
This proof uses a tabular format for presentation. Provide feedback on tabular proof formats in a survey (opens in new window/tab) | Learn more about tabular proof formats|View all pages on facts with proofs in tabular format
Given: A division ring of finite size.
To prove: is a field.
Proof': We denote by the multiplicative group of nonzero elements of .
The key idea behind the proof is to switch between the additive/linear structure and the multiplicative structure. For the additive structure, we use the key fact that the size of a vector space over a field is a power of the size of the field. For the multiplicative structure, we use Lagrange's theorem (a multiplicative constraint) and the class equation (a combinatorial constraint on how things should add up). Finally, we show that the number theory does not work out.
| Step no. | Assertion/construction | Facts used | Given data used | Previous steps used | Explanation | Commentary |
|---|---|---|---|---|---|---|
| 1 | Let be the center of , i.e., the subset of comprising those elements that commute multiplicatively with every element of . | |||||
| 2 | is a field under the operations induced from , and the multiplicative group (the nonzero elements of ) is the center of . | is a division ring | [SHOW MORE] | Creation of base field () for which many of the additive structures of interest are vector spaces | ||
| 3 | is a vector space over where the additive structure is the same as that for as a division ring and where the action of elements of is by left multiplication. | Step (2) | [SHOW MORE] | Linear consolidation over | ||
| 4 | If has size , has size for some positive integer , where is the dimension of as a vector space over . | is finite | Step (3) | [SHOW MORE] | Linear consolidation over , introducing numerical constraints. Note that must in fact be a prime power, but we only use here that . | |
| 5 | For an element , define to be the set of elements of that commute with . Then, is a subspace of as a -vector space. It contains and has dimension and size for . Further, if , then ( depends on ). | Step (4) | [SHOW MORE] | Linear consolidation over | ||
| 6 | For , the centralizer of in the multiplicative group has size for ( depends on ). | Step (5) | For the multiplicative group, we need to throw out the zero element. | Conversion of linear/additive constraint to constraint on multiplicative group | ||
| 7 | The class equation of is: where are dimensions over of the centralizers in of representatives of conjugacy classes in of non-central elements. For each , we have . | Fact (2) | Steps (2) -- (6) | This is a direct application of the construction of the class equation. | Combinatorial constraint on multiplicative group | |
| 8 | Each divides . | Fact (1) | Steps (2), (3), (6) | [SHOW MORE] | Combination of linearly arising multiplicative constraints with basic number theory to get further constraints | |
| 9 | Let where is the cyclotomic polynomial with parameter . Then, as an integer, divides as well as each of the quotient appearing in step (7). | Steps (7), (8) | [SHOW MORE] | Pure cyclotomic polynomial theory (number theory/algebra) | ||
| 10 | If , then does not divide . | [SHOW MORE] | Pure cyclotomic polynomial theory (number theory/algebra) | |||
| 11 | We can conclude , so and is a field. | Steps (7), (9), (10) | [SHOW MORE] | Demonstration of irreconcilability of constraints derived from linear structure and constraints arising from cyclotomic polynomial theory |