Since Chapter 9 the book has looked at one operator
at a time, or at a family whose members commute. But
operators rarely arrive alone. The polynomials in a
fixed operator, the circulants of Chapter 12 §09, the
matrices commuting with a given matrix, the linear
symmetries of a figure: each of these is a whole set of
operators, closed under addition, under scalars, and
under composition. This section makes such a system a
single object of study. It fixes the vocabulary —
subalgebra, homomorphism, generated algebra, commutant —
and builds the two examples the rest of the chapter runs
on, the matrix algebra and the group algebra.
What an
algebra is, and what we assume about it
The definition is already in the book. Chapter 14 §12
introduced an algebra over (Definition 14.12.1) as a
vector space over
with a
multiplication that is bilinear (A1), associative (A2)
and has an identity (A3). It also fixed
the notion of a homomorphism of -algebras. We build on
that definition; the homomorphism clause is restated
below only so that later sections have a label to
cite.
Three standing conventions, stated once and used
everywhere in this chapter.
- Associative and unital. Every
algebra satisfies (A1), (A2) and (A3). Lie algebras and
the cross product, which fail (A2) and (A3), are outside
the chapter.
- Finite-dimensional. Unless a
statement says otherwise, . The
one standing exception is , which we keep as a
source of counterexamples and always name as
infinite-dimensional when we use it that way.
- Not commutative, not invertible.
Nothing requires , and nothing requires a non-zero element to
have an inverse. An algebra has an addition and a
multiplication with all the usual laws except
commutativity and division; it is not a group.
The examples are the ones Chapter 14 listed, and it
is worth seeing why each satisfies the axioms. In , matrix
multiplication is bilinear and associative with identity
(Theorem 0.9.4), so
is an -algebra of dimension
. In for a vector space
over , composition is
bilinear, associative and has the identity (Theorem 2.4.2), so
is an -algebra; when it has
dimension (Theorem 4.1.4).
The polynomial ring is an algebra of
infinite dimension. The quaternions form a real algebra
of dimension (Definition 14.12.3). The
field itself is
an algebra of dimension , the degenerate case,
and it matters: it is the smallest algebra that is not
the zero space, and every non-zero algebra contains a
copy of it.
Subalgebras
After an object come its subobjects. We already know
several sets of matrices that are closed under the three
operations: the diagonal matrices, the upper triangular
matrices, the circulants (Corollary 12.9.5),
the polynomials in a fixed matrix. In each case we
checked closure by hand. The right move is to name the
condition once.
A subalgebra is a subspace that is closed under
multiplication and contains the identity.
Definition
23.1.1 (Subalgebra)
Let be an
algebra over . A
subset is a subalgebra of if
- (SA1) is a
subspace of ;
- (SA2) for
all ;
- (SA3) .
Clause by clause. (SA1) is the linear condition:
is closed under
addition and under scalars, so it is a vector space in
its own right. (SA2) says the multiplication of restricts to a map
.
(SA3) asks for the identity of , not merely for some
element of that
acts as an identity on ; the difference is
real, and the warning below shows a set that satisfies
(SA1) and (SA2), has its own identity, and is not a
subalgebra.
Well-definedness. A subalgebra is an
algebra. Bilinearity, associativity and the identity law
are equations among elements of , and they hold there
because they hold in . So nothing needs to be
re-checked once (SA1)–(SA3) are known — which is exactly
the labor that naming the condition saves.
Throughout, denotes the
matrix unit with a in position and zeros
elsewhere; the
of them are a basis of (Example (Standard Bases)).
Example
(Six subalgebras)
Decide which of the following are subalgebras, and of
which algebra.
- (a) The scalars
inside any algebra .
- (b) The diagonal
matrices and the upper triangular matrices inside . We write for the second of
these, since it returns below and in the next
section.
- (c) The circulants
inside (Chapter 12
§09).
- (d) The quaternions
inside , as an algebra
over .
- (e) The
strictly upper triangular matrices
inside .
- (f) The matrices of
trace inside
.
Solution.
(a) A subalgebra.
It is the image of the linear map , hence a
subspace; by bilinearity; and . Its
dimension is
unless :
if , then
for
every . This is
the degenerate example, and every subalgebra contains
it.
(b) Both are
subalgebras. Sums and scalar multiples of diagonal
(respectively upper triangular) matrices are again such,
the product of two upper triangular matrices is upper
triangular because vanishes when — every term has
or — and is diagonal. The
diagonal matrices have dimension , with basis the , and has dimension , with basis the
for .
(c) A subalgebra,
of dimension :
this is exactly Corollary 12.9.5
(a), (b), together with the fact that is the circulant whose
first row is .
(d) A subalgebra
of
over , of real
dimension , as Definition 14.12.3 records:
the real span of is closed under multiplication by the
quaternion relations, and it contains . It is
not a subalgebra over , since it is not
closed under multiplication by : has both diagonal
entries equal to ,
while every element of has diagonal entries
and , forcing and and at once.
(e)
Not a subalgebra. It is a subspace and
it is closed under products, by the computation in (b)
with strict inequalities. But is not strictly
upper triangular for , so (SA3) fails. This is the non-example by
minimal change: drop the diagonal from (b) and exactly
one clause breaks.
(f)
Not a subalgebra.
has trace ,
so (SA2) fails. Clause (SA3) fails too, except in
characteristic ,
where .
Warning. (SA3) is not a formality.
In , the set
is a subspace, is closed under products,
and even has an identity of its own, namely , since . It is still not a subalgebra of , because . Subspaces
that are closed under multiplication but miss the
identity are the shape of the ideals of the
next section — though this particular one is not an
ideal either, as Section 2 checks. They are a different
kind of object, and no theorem about subalgebras applies
to them.
Quick check. In , is the set of
matrices of trace
closed under multiplication? Does it contain the
identity?
Solution. It contains , because in
, so (SA3)
holds here. But it is still not a subalgebra: and have trace and
has trace ,
so (SA2) fails. One clause can hold over one field and
fail over another; the other clause fails over every
field.
Homomorphisms, isomorphisms, and the algebra generated
by a set
Definition 14.12.1 already
says what a homomorphism of -algebras is: an -linear map
with and . We
name it, so that later sections can cite it, and add the
two subsets it produces.
Definition
23.1.2 (Algebra Homomorphism, Kernel and
Image)
Let and be algebras over . An algebra
homomorphism is
an -linear map
with as in Definition 14.12.1. Its
kernel is and its image
is , the kernel and image of as a linear
map.
The unital clause does
not follow from the other two. The zero map is
linear and multiplicative and sends to , so it is
not an algebra homomorphism. We will
never call it one.
Definition
23.1.3 (Isomorphic Algebras)
An algebra isomorphism is a
bijective algebra homomorphism. Algebras and are
isomorphic, written , if there is an
algebra isomorphism .
The inverse of an algebra isomorphism is again one: it
is linear (Theorem 2.5.1), it
satisfies — apply the
injective map to both sides —
and . So is symmetric, and
it is reflexive and transitive for the same reasons as
in Theorem 2.5.3.
Two homomorphisms to keep in mind. First, taking
matrices: for a finite-dimensional with ordered basis
, the map is an algebra isomorphism
,
being a linear bijection (Theorem 4.1.4)
that turns composition into matrix multiplication (Theorem 4.1.2)
and sends to
. Second, a
non-example: transposition on is a linear
bijection fixing , but ,
so it reverses products. For it is not a
homomorphism, since while .
Now the construction we need constantly: the smallest
subalgebra containing a given set of operators.
Definition
23.1.4 (The Subalgebra Generated by a
Set)
Let be an
algebra over and
. The
subalgebra generated by , written , is the
intersection of all subalgebras of containing .
The letter in
records that scalars are allowed; the next section
writes , without the , for the
ideal generated by , which is a different
and usually larger set. The intersection of any
collection of subalgebras is a subalgebra — each clause
of Definition 23.1.1 is
preserved by intersections — and itself is one of them,
so is a subalgebra containing , and it is contained in
every other one. That is what “generated” means. It also
has a concrete description.
Proposition
23.1.1 (What the Generated Subalgebra
Contains)
Let be an
algebra over and
. Then
is the span of
together with all finite products with
and .
Proof. Let be that span. Every
subalgebra containing contains each product
by
(SA2) and induction on , contains by (SA3), and is a
subspace by (SA1); hence it contains . In particular .
Conversely is
itself a subalgebra: it is a span, hence a subspace; it
contains ; and a
product of two spanning elements is either , or a product , or a
concatenation , which is again such a
product by associativity. By bilinearity, a product of
two elements of
is a combination of such products, so it lies in . Since , minimality
gives . This proves the proposition.
For a single operator the products are just the
powers, and the minimal polynomial says how many of them
are independent.
Proposition
23.1.2 (The Algebra Generated by One
Operator)
Let
be finite-dimensional over and let have minimal
polynomial , of
degree . Then
is a commutative subalgebra
of , it
equals , and
is a basis of it. In particular .
Idea. Division with remainder cuts
every power of
down to degree less than , which gives spanning;
and a shorter relation among the powers would be an
annihilating polynomial of degree less than , which is what
minimality forbids.
Proof. By Theorem 6.7.1 the map
is
linear and multiplicative, so is a subspace closed
under products, and it contains ; it is
therefore a subalgebra. Any two of its elements commute,
since . By Proposition 23.1.1, is
the span of
and the powers
with , which
is .
Since is
finite-dimensional, exists (Theorem 6.7.3 (b),
(c)); and ,
because the only monic polynomial of degree is , whose value at is since .
Spanning. Let . Dividing by (Theorem 6.1.1) gives
with
, and
, a combination of .
Independence. Suppose with the not all zero. Then
is a non-zero polynomial with
and ,
contradicting the fact that has least degree
among the non-zero annihilating polynomials (Theorem 6.7.3
(b)).
So the listed
operators are a basis, and . This
proves the proposition.
Example
(Two polynomial algebras)
Compute for and for
over .
Solution. For : and , so annihilates and no polynomial of
degree does (if
,
reading the
and entries
gives ).
Hence
and , with basis . Note that is much
smaller than .
For :
annihilates ,
since the product of the three diagonal matrices is . No polynomial of degree at most does, unless : would give three distinct roots.
So has
degree and , with
basis .
The group
algebra
Here is the object that turns a group of symmetries
into linear algebra. Suppose a finite group acts on a space by
invertible operators . Then every -combination is
again an operator, and the products of such combinations
are governed entirely by the multiplication table of
. It is worth
building, once and for all, the algebra in which those
formal combinations live.
The group algebra is the set of formal -combinations of group
elements, multiplied by the group law.
Definition
23.1.5 (Group Algebra)
Let be a
finite group with identity , and let be a field. The
group algebra is the free vector
space on
the set (Definition 15.2.3), with
basis , equipped with the unique bilinear
multiplication satisfying We write for and for , so that a
general element is a formal sum
with all ,
two such sums are equal exactly when all their
coefficients agree, and
Well-definedness. Choose an ordering
of
, so that is an ordered basis of (Lemma 15.2.2 (a)). By Theorem 15.1.1 with , there is
exactly one bilinear map
taking the prescribed values on basis
pairs. The displayed formula for the product is that
bilinear map written out: expanding and
collecting the terms with , which means , gives the stated coefficient of
.
The axioms hold. Bilinearity is (A1) by construction.
For associativity (A2), both and are trilinear in
, so by Theorem 15.1.1 it is
enough to compare them on basis triples, where by the associativity
axiom (G1) of Definition 0.10.1. For
(A3), on
basis elements, hence everywhere by bilinearity. So
is an -algebra, of dimension
.
In words: an element of is a bookkeeping
device, a list of scalars indexed by the group, and
multiplying two of them convolves the lists along the
group law. The group sits inside : the map is
injective (distinct basis vectors) and multiplicative,
and each
is invertible with inverse .
Example
(Three group algebras)
- (a) .
- (b) , written
multiplicatively as with .
- (c) .
In each case give the dimension and decide whether
is
commutative.
Solution.
(a) , of dimension , and commutative. This
is the degenerate case.
(b) , and is commutative
because on basis elements and multiplication is
bilinear. Moreover the map sending to is an
algebra homomorphism: it is linear by construction, it
sends to , and for and
,
where the middle equality is bilinearity
together with . It is surjective because the powers
are a basis. Its kernel is exactly
: dividing by (Theorem 6.1.1) gives
with ,
and since we get , which vanishes only when all
coefficients of
vanish, the
being a basis. The next section turns this into an
isomorphism .
(c) , and
is
not commutative: with and we have
in , so are distinct basis
vectors. In general is commutative if
and only if is
abelian: the displayed argument gives one direction, and
if is
commutative then , and distinct group elements give
distinct basis vectors, so .
Warning. The elements of are formal sums, not
group elements, and most of them are
not invertible. In with , the
element
satisfies , so is a
non-zero element equal to its own square and different
from . Multiplying
it by gives
, so neither
factor has an inverse. Passing from to buys linearity at
the price of invertibility.
Every
finite-dimensional algebra is an algebra of
matrices
Matrices look like a special case of an algebra. They
are not: every finite-dimensional algebra is one, and
the embedding is the most economical thing imaginable —
let the algebra act on itself.
Theorem
23.1.3 (Left Multiplication Embeds an Algebra
in Its Own Operators)
Let be an
algebra over . For
define
by .
Then is an injective algebra
homomorphism. If , then is isomorphic to a
subalgebra of .
Idea. Each axiom of an algebra says
one thing about :
bilinearity in the second slot makes linear, bilinearity
in the first makes linear, associativity makes multiplicative, and the
identity makes
unital and — this is the point — injective, because an
operator that kills everything in particular kills , and .
Proof. Each is linear, because
multiplication is linear in its second argument (A1).
The map is
linear, because multiplication is linear in its first
argument: for all
.
is
multiplicative: for , associativity (A2) gives so . It is unital: , so
.
is injective:
if then,
evaluating at ,
. So and is injective (Theorem 2.2.3).
Suppose now . Then is a subalgebra of
: it is a
subspace, it is closed under products since , and it
contains . The map is a bijective algebra
homomorphism, hence an algebra isomorphism. Fixing an
ordered basis of
and taking matrices is an algebra isomorphism , as
recorded after Definition 23.1.3, and it
carries to a
subalgebra of isomorphic to
. This proves the
theorem.
The theorem is the reason the rest of the chapter may
think in matrices without loss. It is also a genuine
computation: to see an abstract algebra concretely,
write down the matrices of left multiplication in a
basis.
Example
(Left multiplication for the upper triangular
algebra)
Let ,
the upper triangular matrices in , with ordered
basis . Compute the matrix of for , and read off what the
embedding of Theorem 23.1.3 does.
Solution. Multiply each basis
element on the left by : Putting the coordinate vectors in as columns,
So ,
an algebra of matrices of dimension , is isomorphic to the
algebra of matrices of this shape. The embedding is
faithful but wasteful: already embeds in . Left
multiplication is the embedding that always exists, not
the smallest one.
Commutants
The last construction of the section is the one that
will carry Schur’s lemma later. Given a set of
operators, ask which operators commute with all of them.
Chapter 9 §09 asked this about a pair, Chapter 10 §04
about a Weyr matrix, Chapter 12 §07 about a normal
family. It is the same question each time.
The commutant of a set is everything that
commutes with all of it.
Definition
23.1.6 (Commutant and Center)
Let be an
algebra over and
let
be any subset. The
commutant of in is The center of is ,
the set of elements commuting with
every element of . We write for .
In words: to belong to , an element must
commute with each member of — one failure
disqualifies it. The members of need not commute with
each other, and
need not be a subspace or a subalgebra; the definition
asks nothing of .
Proposition
23.1.4 (Properties of the Commutant)
Let be an
algebra over and
.
- (a) is a subalgebra of
; in particular
is a
commutative subalgebra.
- (b) If , then .
- (c) .
- (d) .
Proof.
(a) Fix . The set is the
kernel of the linear map , hence a subspace (Theorem 2.2.1); is the
intersection of these subspaces over , hence a
subspace. If then , using
associativity at each step, so . And , so . Thus
is a
subalgebra. For the center, every element of commutes with every
element of , so in
particular any two of them commute.
(b) If commutes with every
element of and
, then
commutes with
every element of .
(c) Let . Every satisfies
, which is
the condition for
to lie in .
(d) Applying (c)
to gives
. Applying (b) to the inclusion
of (c) gives , that is, .
Three commutants, computed. Each is a short exercise
in comparing entries, and the pattern they show is the
one Schur’s lemma will explain.
Example
(Commutants of three matrices)
Compute the commutant inside the stated
algebra for
- (a) inside , where
has
distinct;
- (b) inside , where is the
nilpotent Jordan block;
- (c) inside .
Solution.
(a) Distinct
diagonal. Comparing the entries,
and , so says for all . Since the are distinct, whenever . So is the
algebra of diagonal matrices in , of dimension
. Here has degree , since annihilates while no non-zero
polynomial of degree at most does, such a polynomial
having the three distinct roots ; so by Proposition 23.1.2 as well.
Every polynomial in commutes with , so , and equal dimensions give .
(b) Jordan
block. Write . Then
(read as when
) and
(read as when ). Setting
these equal for all : the entries with give , the
entries with
give , and the four remaining equations give , , and . So of dimension , since are exactly
the three matrices of this shape with one of equal to and the others . Again , so this
is by Proposition 23.1.2.
(c) The whole
algebra. Let . Commuting with forces
diagonal by the
first computation, say ; and then
while , so , and similarly . Hence is a scalar matrix.
Conversely scalar matrices commute with everything. So
, of dimension . The argument used that
are
distinct scalars; over a field of characteristic or they are not, which is
why the general statement below is proved with matrix
units instead.
The last computation deserves a clean statement over
every field, because later sections use it.
Proposition
23.1.5 (The Center of the Matrix Algebra Is the
Scalars)
Let be
any field and . Then .
Equivalently, for a finite-dimensional , the
operators commuting with every operator on are exactly the scalar
multiples of .
Proof. A scalar
matrix
satisfies by Theorem 0.9.4 (4).
For
the claim
reads ,
which is true, so assume . Let . Writing and expanding both
products with Theorem 0.9.2 (1),
Now fix
and choose any , which is possible because . Reading at
with gives
, so every off-diagonal entry in row of vanishes; and reading
it at gives . Letting run over all indices
makes diagonal,
and applying the second conclusion to every pair makes all its
diagonal entries equal. So .
The statement for operators follows by choosing a
basis and applying the algebra isomorphism
recorded after Definition 23.1.3, which
carries to
, and under
which an element of the center corresponds to an element
of the center. This proves the proposition.
Quick check. In , what is , and what
is ? Does
hold for ?
Solution. Everything commutes with
, so .
Then by Proposition 23.1.5. So
here: is the
one-dimensional space of scalar matrices, while is a single matrix. The
inclusion of Proposition 23.1.4 (c) is
genuinely an inclusion, and should be
read as “the smallest thing cannot be distinguished
from by commutation”.
Warning. An algebra is not a group,
and the theory of this chapter never assumes an inverse.
In the only
elements with a multiplicative inverse are the non-zero
constants, since ; in the invertible
elements are the non-singular matrices, a proper subset;
in the warning
above produced two non-zero elements with product . Every argument below
that wants to divide must first produce an inverse, and
most of them cannot.
Exercises
A. Check your
understanding
Exercise
(A1)
- (a) State the three
clauses in the definition of a subalgebra, and say which
one the strictly upper triangular matrices fail.
- (b) Give the
definition of the commutant of a subset of an algebra , and say why itself need not be a
subalgebra.
- (c) True or false,
with a reason: a linear bijection
with for all is an algebra
isomorphism.
- (d) What is , and what is
for an
operator on a
finite-dimensional space?
Solution.
(a) (SA1) a
subspace, (SA2) closed under products, (SA3) contains
. The strictly
upper triangular matrices fail (SA3), since has non-zero
diagonal.
(b) (Definition 23.1.6). The
definition quantifies over the elements of one at a time and asks
nothing of as a
set, so may be a
single element, a finite list, or any subset at
all.
(c) True — but
note that is a separate requirement in general, which
here follows from bijectivity: for every , writing , we get
and likewise on the other
side, so is an
identity of and
equals by
uniqueness of identities. The statement is true for
bijective ;
it is false without bijectivity, as the zero map
shows.
(d) (Definition 23.1.5) and
(Proposition 23.1.2).
B. Practice
Exercise
(B1: Determine which are subalgebras)
Determine which of the following are subalgebras of
the stated algebra. Justify your answer, naming the
exact clause that fails when one does.
- (a) inside .
- (b) inside .
- (c) inside .
- (d) inside , for .
Solution.
(a) A subalgebra:
this is ,
handled in Example (Six subalgebras)
(b).
(b)
Not a subalgebra. The set is the
symmetric matrices, a subspace containing , so (SA1) and (SA3)
hold. But (SA2) fails: , which is
not symmetric.
(c) A subalgebra.
It is the kernel of the linear functional ,
hence a subspace; it contains ; and if and then by Theorem 0.8.5.
(d)
Not a subalgebra, because it is not
even a subspace: (SA1) fails. Take and , both
squaring to .
Their sum has and , so is not of the listed
form: if with , then and , whose diagonal
entries in the standard basis are all ; so , and then with .
Exercise
(B2: A commutant)
Let . Compute and its
dimension, and compare it with . Hence show
that .
Solution. As in Example (Commutants of three matrices),
says
with . The coefficient vanishes
exactly for , so of dimension .
For : the
polynomial annihilates
, and no
polynomial of degree does, since would give
and , hence . So and
by
Proposition 23.1.2. Since
, the two
algebras differ; concretely
is not a polynomial in , because every such
polynomial is diagonal.
Exercise
(B3: Cayley for the quaternions)
Let be the
quaternions with ordered basis
over , where
denotes . Compute the
matrices of
and in , and verify that they
satisfy and .
Solution. By Definition 14.12.3, , , and . Writing the
coordinate vectors of these four images as columns,
Likewise , , , , so Squaring the first gives , and multiplying
the two in this order gives the matrix with columns
, which is the matrix of
computed the
same way from , , , . Both checks also follow from Theorem 23.1.3 without
computing: is
multiplicative, so and . This exhibits as a subalgebra of
.
C. Going deeper
Exercise
(C1: The center of a group algebra)
Let be a
finite group and
a field. For , the conjugacy class of
is , and the class sum is
.
- (a) Prove that lies in
if and only
if for all .
- (b) Deduce that the
distinct class sums form a basis of , so that is the
number of conjugacy classes of .
- (c) Compute .
Hint for (a): by bilinearity it is enough to test
commutation against the basis elements .
Solution.
(a) By
bilinearity, is
central if and only if for every , equivalently for every
(multiply by
, which
exists in ). Now
where the second equality substitutes , that is,
; this
is a bijection of , so it merely relabels
the sum. Comparing coefficients with , which
is legitimate because the are a basis, gives
for
all exactly when
for all .
(b) Being
conjugate is an equivalence relation on : ; if then
; and conjugating
twice is conjugating by the product. So is the disjoint union
of its distinct classes . By (a), a central element has a
constant coefficient on each class, so is exactly the
span of the class sums ; and these are independent, because
they are sums over disjoint non-empty
sets of basis vectors. Hence .
(c) Conjugate
elements satisfy the same equations : expanding and
canceling the inner pairs gives , which equals exactly when . Now splits into three
sets by this test: ; the three
transpositions, which are the elements with ; and the
two -cycles, which
are the elements with . No conjugacy class can meet two of
these sets. Each of them is a single class: and make the three
transpositions conjugate, and makes the two -cycles conjugate. So
and .
Exercise
(C2: Generated by two matrix units)
Work in .
- (a) Compute
and its dimension.
- (b) Compute and its dimension.
- (c) Deduce that
adding one generator can change the commutant from an
algebra of dimension to the scalars, and
compute both commutants.
Solution.
(a) , so by Proposition 23.1.1 the
generated algebra is , of
dimension . It is
, which
matches Proposition 23.1.2 since
.
(b) The words
include and ,
so the generated algebra contains all four matrix units
and is , of
dimension .
(c) : writing
,
has first
row and second row zero, while has second
column and first column zero. Equality forces
and
, so
, of dimension . By Proposition 23.1.4 (b),
, and it equals by part
(b) and Proposition 23.1.5. One
extra generator cuts the commutant from dimension to dimension .
Exercise
(C3: Is the group algebra ever a field?)
Let be a
finite group with and let be any field.
- (a) Pick in of order , meaning and for . (Such an
exists: the
powers cannot all be distinct in a finite group,
and canceling gives for some .) Show that and satisfy with and .
- (b) Deduce that
is never a
field, and never isomorphic to a subalgebra of a
field.
- (c) Is ever commutative for
? Give an example or a proof that it is
not.
Solution.
(a) The powers
are distinct elements of : if with
then
with , contradicting minimality of (cancellation is Theorem 0.10.1 (4)).
So and
, both being
non-zero combinations of distinct basis vectors.
Expanding,
(b) In a field,
and more generally in any subalgebra of a field, a
product of two non-zero elements is non-zero: if and then . Part
(a) produces a violation, so is not a field and
embeds in none. (An algebra with such a pair is said to have
zero divisors.)
(c) Yes, whenever
is abelian: then
on
basis elements, and bilinearity extends the identity to
all of . For
example
is commutative of dimension . Part (b) says it is
still not a field, which is consistent: , a commutative algebra with zero
divisors.