The tensor algebra is free, and being free it is
useless on its own: it records the order of the slots
even when nothing in the problem cares about the order.
A symmetric bilinear form does not care (Definition 14.3.1); nor does
a quadratic form; nor does the monomial , which is the same
polynomial as . This section
forces to
forget the order, by dividing the tensor power by the span
of the differences .
The result, the symmetric power , turns out to
have a basis indexed by nondecreasing index tuples, and
the algebra assembled from all the turns out to be
the polynomial algebra of Chapter 0, one variable per
basis vector.
The construction repeats Section 02’s three moves for
the second time: universal property, uniqueness, then a
model built as a quotient. If the shape of the argument
below feels familiar, that is the intention.
Throughout, is
a field, is a
finite-dimensional vector space over with , and
unless
stated otherwise. The field is
arbitrary, and the single place where the
characteristic matters is isolated in the last part of
the section.
Symmetric
multilinear maps
Before asking for a space, we name the maps it is
supposed to linearize. Chapter 14 called a bilinear
form symmetric when swapping its two arguments
changed nothing (Definition 14.3.1). With
arguments there
are more ways to rearrange them, and we demand
invariance under all of them.
A symmetric map cannot tell in which order its
arguments were handed to it.
Definition
15.7.1 (Symmetric Multilinear Map)
Let be a
vector space over . A -linear map (Definition 15.1.1) is
symmetric if for every permutation and
for all .
At the
only nonidentity permutation is the swap, so this is
exactly Definition 14.3.1 with a
general target in
place of . At
the condition
is empty and every linear map is symmetric.
Three examples and one nonexample.
- A symmetric bilinear form, with . This is the case
, .
- Products of one fixed functional.
For , the map is
-linear, by the
third example after Definition 7.2.1, and
symmetric because multiplication in is commutative:
rearranging the factors does not change the
product.
- Multiplication in a commutative
algebra. If is a commutative -algebra and is
linear, then is symmetric, by commutativity of
.
- A nonexample by minimal change. On
, the map
is bilinear but not symmetric: it sends
to and
to . Only the
symmetry clause fails; bilinearity survives
untouched.
Note which permutations are allowed:
all of , not only the swaps
of adjacent slots. Nothing is lost by asking for all of
them, and asking for all of them spares us a lemma about
generating .
The
symmetric power
Now the object. The demand is Definition 15.6.1’s,
restricted to the symmetric maps.
The -th
symmetric power is the space in which symmetric -linear maps become
linear.
Definition
15.7.2 (-th Symmetric
Power)
A -th
symmetric power of is a pair
, where
is a vector space
over and is a
symmetric -linear map, such
that
- (S1)
(universal property) for
every vector space over and every
symmetric -linear map , there
is a unique linear map
with .
We write for
and denote the value by juxtaposition, calling it a symmetric
product. By convention .
The one difference from (T1) is the word
symmetric, in two places: the structure
map is required
to be symmetric, and only symmetric maps are required to factor.
Both changes are needed. If were not symmetric,
the notation would be false; if
nonsymmetric maps had to factor, no space could do the
job, since is symmetric whenever is.
Uniqueness is the template of Theorem 15.2.1 for the
third time, and we no longer write it out.
Theorem
15.7.1 (Uniqueness of the Symmetric
Power)
Let and
both be -th
symmetric powers of . Then there is a unique
linear isomorphism with .
Proof. Word for word the proof of
Theorem 15.6.1, with
“symmetric -linear” in place of
“-linear”
throughout: (S1) for applied to the
symmetric map gives , (S1) for applied to gives , the composite is a linear
self-map of with
, and the uniqueness clause of (S1) applied
to forces .
Symmetrically . This proves the theorem.
And now the model: the tensor power, divided by the
relations we want to impose.
Theorem
15.7.2 (Existence of the Symmetric
Power)
Let be the span of all the elements
and let be the
quotient map (Definition 4.4.3).
Then , together with is a -th
symmetric power of . At the subspace is the span of the
elements .
Idea. Two things to check, and both
are one line each once the right tool is named. That
is symmetric is
the definition of : permuting the
arguments changes the tensor by an element of , which kills. That symmetric
maps factor is Theorem 4.4.10:
turn into a
linear map on by (T1), observe that symmetry of makes it vanish on the
generators of ,
and let the quotient’s universal property do the rest.
This is the move the chapter uses three times: a
quotient kills exactly the relations you
want.
Proof. is a subspace, being
a span. The map
is -linear, being
the -linear of Theorem 15.6.2 followed by
the linear map .
It is symmetric: for , the difference lies in by definition, so the
two tensors have the same image under : .
Now let be symmetric -linear. By (T1) there
is a unique linear with . On a generator of , which is because is symmetric. A linear
map vanishing on a spanning set of vanishes on , so . By Theorem 4.4.10
(a) there is exactly one linear with , and then
For uniqueness, suppose is linear with . Since
is surjective and
is
spanned by its simple tensors (Theorem 15.6.2), the
elements span . So
and agree on a
spanning set, hence everywhere. This proves the
theorem.
Warning. is a quotient of
, not
a subspace of it. Its elements are cosets, and
the identity in says that
and
lie in the same coset. It does
not say in , which is
false for independent by Theorem 15.6.3. Confusing
the two is the commonest error here; the safe habit is
never to write an element of as a tensor.
A basis,
and the dimension
Sorting an index tuple is now legal, so the basis of
Theorem 15.6.3 collapses:
only the sorted tuples survive. Counting them is the
substance of the section.
Theorem
15.7.3 (Basis of a Symmetric Power)
Let be a basis of and . Then the
symmetric products one for each nondecreasing
tuple, form a basis of . Consequently
over every field .
Idea. Spanning is sorting: the
image of any index tuple equals the image of its sorted
version, so the sorted ones already span. Independence
needs one linear functional per nondecreasing tuple, and
it must be built without dividing by
anything, since we want the theorem over every
field. The functional that works is a sum over all ways
of dealing out the dual basis functionals
to the slots with
prescribed multiplicities: every coefficient in it is
. Counting the
tuples is then the stars-and-bars bijection, which turns
a nondecreasing tuple into a strictly increasing one by
adding to its entries.
Proof. Spanning. By Theorem 15.6.3 the tensors
,
over all tuples ,
form a basis of , and
is surjective, so their images
span .
Given any , let
sort
it, so that is nondecreasing. Since
is symmetric,
.
So the nondecreasing tuples already give a spanning
set.
Independence. Let be the dual basis of (Theorem 5.1.3). For a
nondecreasing tuple , let be its multiplicity vector,
so , and let be the set of
functions taking the value
exactly times, for each . Define Each summand is -linear, being a product
of one functional per slot, so is -linear.
It is symmetric. Let . Substituting and then reindexing the
product by , The map is a bijection of onto itself,
since composing with a permutation of the domain does
not change how often a value is taken. So the sum is
unchanged, and
is symmetric.
By (S1),
induces a linear . Evaluate it on a basis
candidate: for any tuple , A summand is exactly when for every
, and otherwise; so the whole
sum is if the
function belongs to , and if it does not. For
nondecreasing and
, that function
lies in
exactly when has
the same multiplicity vector as , which for
nondecreasing tuples means . Hence .
Now suppose , the sum over nondecreasing tuples.
Applying
leaves .
Since was
arbitrary, every coefficient is , and the list is
independent. So it is a basis.
The count. Send a nondecreasing tuple to
Consecutive entries satisfy because , so the image is
strictly increasing, and its entries
lie between and
.
Conversely, subtracting from a strictly increasing tuple
in returns a nondecreasing tuple in : the
differences become , and
, give
and . The two
assignments are mutually inverse, so the nondecreasing
-tuples from are in
bijection with the -element subsets of
, and there are of
those. This proves the theorem.
Nothing in the proof divided by an integer, which is
why the conclusion holds over as it does over
. Keep that in
view: the last part of this section shows that a
different and very common description of does not survive
over , and the
difference between the two is exactly one division.
Quick check. Let . Compute and , and
say which basis tensors of become
equal in .
Solution. and . The six surviving
basis elements are . The three pairs and with become equal, which removes from the count: .
Example
(A symmetric square, in coordinates)
Let .
Write down a basis of and expand in
it.
Solution. By Theorem 15.7.3 a basis is
, of size
.
Expanding one slot at a time and then using , Compare with expanding in ordinary algebra. That is not a
coincidence, and the next part of this section says
exactly what it is.
Warning. Not every element
of is a
product of
vectors. Take , , and . If
with and , then comparing coordinates in the
basis gives , , and . The first and
last force , and multiplying by gives ,
impossible in .
This is the same phenomenon as the nonsimple tensors of
Section 02, and it is why is much larger
than the set of products.
The
symmetric algebra is a polynomial algebra
Stacking the symmetric powers gives an algebra,
exactly as stacking the tensor powers did, and the
multiplication descends from concatenation.
Proposition
15.7.4 (The Symmetric Product of Two Symmetric
Tensors)
Let .
There is a unique bilinear map with
Proof. Concatenation carries
the relations into the relations. Let and . For
a generator
and a simple , the
product of
Proposition 15.6.4 is
again a generator of , for the
permutation acting as on the first slots and fixing the
last . Since
generators span , since is spanned
by its simple tensors, and since is bilinear, . Swapping the roles of the two blocks
gives .
Descending, one argument at a time. Let
denote the quotient maps. Fix . The
linear map kills by the first
inclusion, so Theorem 4.4.10
gives a unique linear with . The assignment is
linear, since and
agree on the spanning set ; and it kills , since gives and
hence .
By Theorem 4.4.10
again it descends to a linear map , and evaluating gives the required
bilinear map. It is unique because the products of
vectors span each factor. When or the product is
scalar multiplication, as in Section 06. This proves the
proposition.
Definition
15.7.3 (Symmetric Algebra)
The symmetric algebra of is the vector space
of sequences with finitely many nonzero
components, with the multiplication assembled from Proposition 15.7.4 by
.
Proposition
15.7.5 ( Is a Commutative
Algebra)
is an
associative, commutative, unital -algebra with identity
,
and .
Proof. Bilinearity, associativity,
and the identity are proved exactly as in Theorem 15.6.5: all three
are identities between multilinear expressions, so it
suffices to check them on products of vectors, which
span each ,
and there all three read “concatenate the strings”.
Commutativity is the new point. Both
and
equal the symmetric product of the same vectors in two
different orders, and is symmetric, so they
are equal. Two bilinear maps agreeing on spanning sets
of both arguments agree everywhere, so for all . This proves the
proposition.
To name what is, we need
polynomials in more than one variable. Chapter 0 built
; the
several-variable version is the same construction with
monomials indexed by exponent vectors.
Definition
15.7.4 (The Polynomial Algebra )
Let . The
polynomial algebra in variables over
is the vector
space with basis the monomials
with the unique bilinear multiplication
satisfying . The
degree of is , and denotes the span of the monomials
of degree .
The bilinear extension exists and is unique because a
bilinear map may be prescribed freely on a pair of
bases, by the argument used twice in the proof of Proposition 15.6.4. The
multiplication is associative, commutative, and unital,
with identity the monomial all of whose exponents are
, because exponent
addition in
is associative, commutative, and has an identity. For
the monomials
are and the rule is , so
is the ring
of Definition 0.8.2,
whose basis of monomials is Example (A Basis of ).
Everything Chapter 6 proved — division, greatest common
divisors, unique factorization — lives in that
one-variable case.
Theorem
15.7.6 (The Symmetric Algebra Is a Polynomial
Algebra)
Let be a basis of . Then there is an
isomorphism of -algebras and it carries onto . In
particular
Idea. Both sides have a basis
indexed by the same combinatorial object: a
nondecreasing -tuple on the left, a
degree- monomial
on the right, and each is determined by its multiplicity
vector with .
So match the bases, which gives a linear isomorphism for
free, and then check multiplicativity on basis elements,
where both products are “add the exponent vectors”.
Proof. Write for . Given with ,
let be
the nondecreasing tuple taking the value exactly times, and write
for the corresponding symmetric product .
The assignment is a bijection onto the
nondecreasing -tuples, since a
nondecreasing tuple is recovered from its multiplicity
vector and conversely. So by Theorem 15.7.3 the family
is a basis of , and hence is a basis of .
Define to
be the unique linear map with , which exists by Theorem 2.1.6. It
sends a basis of bijectively onto
the basis of monomials, so it is a linear isomorphism,
and it sends the degree- basis onto the
degree- monomials,
so .
Multiplicativity: the maps
and are bilinear, so it is enough to
compare them on the basis. By Proposition 15.7.4,
is the symmetric product of the vectors of the two
strings, which after sorting is ; and by Definition 15.7.4. Also
sends the
empty product to
the monomial with all exponents , which is . Hence is an algebra
isomorphism. Finally is the basis
element whose
has a
single in
position , so
.
The dimension formula follows from Theorem 15.7.3, since
restricts to
an isomorphism in each degree. This proves the
theorem.
So the symmetric algebra is nothing exotic: it is
the polynomial algebra, with one variable per basis
vector of .
The isomorphism depends on the basis, exactly as the
coordinate isomorphism does; is the basis-free
version of “polynomials in variables”, and is the
basis-free version of “homogeneous polynomials of degree
”. Read backwards,
the theorem also computes something Chapter 6 never did:
the number of monomials of degree in variables is .
Symmetric
powers versus symmetric tensors
Here is the trap, and it is worth the space. Many
treatments define the -th symmetric power as a
subspace of : the
tensors left fixed by every permutation of the slots.
That is a different construction from the quotient
above, and over a field of characteristic the two agree. Over
they do not,
and the reason is a single division by .
We first need the permutation operators.
Lemma
15.7.7 (Permuting the Slots of a Tensor)
For each there is a unique linear operator on with and for all ,
with .
Proof. The map is -linear, since in slot
it is in slot . So (T1)
gives a unique linear with the stated
values, and uniqueness holds because those tensors span
. For
the composition rule, put ; then and , which is the -th argument of . Both
sides are linear and agree on simple tensors, hence are
equal. This proves the lemma.
Definition
15.7.5 (Symmetric Tensor)
A tensor is symmetric if for
every . The
symmetric tensors form a subspace of , which we
write ; it is the intersection of the
kernels of the linear maps .
Theorem
15.7.8 (Symmetric Tensors and the Symmetric
Power)
Let and , and let be
the restriction of the quotient map .
- (a) Over
every field, .
- (b) If
or , then is an
isomorphism.
- (c) If , ,
and , then
is
neither injective nor surjective.
Idea. For (a), a symmetric tensor
must have equal coordinates along each orbit of basis
tensors, so the orbit sums are a basis;
orbits correspond to multisets, which Theorem 15.7.3 already
counted. For (b), average: maps everything into
the symmetric tensors and kills , so is an
inverse for —
provided is
invertible, which is exactly the hypothesis. For (c),
the tensor is symmetric and
nonzero, but its image is .
Proof.
- (a) Let be a basis of . For a tuple write ,
so that is a basis
of
(Theorem 15.6.3), and note
, where is the tuple
. Two tuples lie in the same
orbit when one is a rearrangement of
the other, that is, when they have the same multiplicity
vector. For each nondecreasing let , the sum over the orbit of .
Each is
symmetric, because permutes . The are independent,
because distinct orbits involve disjoint sets of basis
vectors. They span: if satisfies for every
, then
comparing coordinates in gives for
all and , so is constant
on orbits and . Hence is a basis, with
one member per orbit, that is, per multiplicity vector
of total . By the
bijection in the proof of Theorem 15.7.3 there are
of
those. No division occurred, so this holds over every
field.
- (b) Let , a linear operator on . By Lemma 15.7.7, for any
, since and
are bijections of . The first identity
says . The second gives , and
the generators of are exactly the
elements ,
so .
By hypothesis in . Indeed in , a product of factors; if
none of them is ,
and if then for by Definition 0.7.2. A
field has no zero divisors, so the product is nonzero,
hence invertible. Since , Theorem 4.4.10
gives a linear map with
.
Now compute both composites. For , each
differs
from by an
element of , so
, whence and is
surjective, so . Conversely, if is symmetric then , so . Hence is an isomorphism
with inverse .
- (c) Let , ,
, and put
. It is symmetric,
since the only nonidentity element of swaps the two
summands, and it is nonzero, being a sum of two distinct
basis vectors of (Theorem 15.6.3). But because in . So
and is not injective.
By (a) the two spaces have the same finite dimension, so
a surjective
would be injective by Theorem 2.3.1; hence
is not
surjective either. This proves the theorem.
Part (b) is where the division lives, and part (c) is
what it costs. The operator still exists over ; what fails is the
rescaling , and with
it the splitting of the quotient.
Warning. In characteristic
, “symmetric
power” and “symmetric tensors” are different
objects. They have the same dimension by Theorem 15.7.8 (a), so
they are abstractly isomorphic, but the natural
map between them is not an isomorphism, and no natural
one is available. So: do not define as , do
not write without saying that is invertible, and do
not transport a statement proved for one to the other.
This is Chapter 14’s discipline again, where alternating
and skew-symmetric forms coincided only away from
characteristic
(Theorem 14.3.3): the same
clause, the same division, and the same smallest
witness, .
Everything else in this section is
characteristic-free. In particular Theorem 15.7.3, Theorem 15.7.6, and the
dimension hold
over every field, because the quotient construction
never divides. The next section takes the same care with
the same reward: the exterior power is built from a
relation chosen so that no division is ever needed.
Exercises
A. Check your
understanding
Exercise
(A1)
- (a) State the
universal property (S1), with every quantifier, and say
which maps are required to factor.
- (b) Which subspace
of is
divided out to build ? Write down its generators for .
- (c) Let . Compute and .
- (d) Determine
whether is
a subspace of . Justify your answer.
- (e) What hypothesis
on makes the
symmetric tensors of degree naturally isomorphic to
, and which
step of the proof needs it?
Solution.
(a) For every
vector space over
and every
symmetric -linear map , there
exists exactly one linear with . Only the symmetric maps factor; a
nonsymmetric one cannot, since is
symmetric for every linear .
(b) The subspace
of Theorem 15.7.2, spanned by
the differences .
For the
generators are the six differences obtained from the six
, for
all .
(c) and .
(d) No. It is a
quotient of , and its elements are cosets of , not tensors. (Over a
field of characteristic there is a subspace of
naturally isomorphic to it, namely the symmetric
tensors, but the isomorphism is not an equality, and it
does not exist in characteristic .)
(e)
or , so that is invertible in (Theorem 15.7.8 (b)). The
step that needs it is the construction of the inverse
map , which
divides the symmetrization by .
B. Practice
Exercise
(B1: Expanding symmetric products)
Let .
- (a) Expand in the
basis of .
- (b) Expand
in the basis of given by Theorem 15.7.3.
Solution.
(a) Expanding one
slot at a time and then using ,
(b) The basis is
, of size .
Expanding the first two slots, and the two middle terms are equal after
sorting, so they cancel: In the polynomial language of Theorem 15.7.6 this is
.
Exercise
(B2: Counting)
- (a) Compute for and .
- (b) For , compute in closed
form and check it against the number of entries on or
above the diagonal of an matrix.
- (c) Determine all
pairs with
for which
. Justify your answer.
Solution.
(a) for , giving for .
(b) . An matrix has diagonal entries and
entries
strictly above the diagonal, and .
The agreement is the remark after Theorem 15.7.6: a
symmetric bilinear form is the same data as a functional
on , and
also the same data as a symmetric matrix.
(c) Exactly those
with , or with
. If both sides are
. If both sides are
. Otherwise and , and then are two basis
tensors with the same image, so and
by Theorem 4.4.5.
Exercise
(B3: A form factored through the symmetric
square)
Let be a
symmetric bilinear form on . Prove that there is a
unique linear functional with for all ,
and compute on the basis of
Theorem 15.7.3 when and .
Solution. is a symmetric
-linear map (Definition 15.7.1 with
, ), so (S1) gives
exactly one linear with , which is the displayed identity.
For the given : , , and . So in the
coordinates given by the basis the
functional reads , and under Theorem 15.7.6 it is the
rule “read off the coefficients of and and subtract”.
C. Going deeper
Exercise
(C1: The characteristic-two witness in full)
Let
and ,
and take .
- (a) Write down a
basis of and verify that its dimension is
.
- (b) Compute and , and
identify
and for
the map of Theorem 15.7.8.
- (c) Are and
isomorphic
as vector spaces? Explain why this does not repair the
situation.
Solution.
(a) Here
with the
swap, and
exchanges
with
and fixes
and .
So is symmetric if
and only if .
A basis is the orbit sums of Theorem 15.7.8 (a), so the
dimension is .
(b) is spanned by the
elements . Writing and and expanding both slots, the
and
terms cancel and So is
the line spanned by , the sign being
irrelevant over , and and
by Theorem 4.4.5.
Now , of dimension , and is therefore
-dimensional,
spanned by and ; it misses
.
(c) Yes, they are
isomorphic: both have dimension over , and Theorem 2.5.4 applies.
It does not repair anything, because the isomorphism is
not and does
not respect the structure maps: an isomorphism chosen by
hand would not satisfy , so it could not be used to
transport statements about products of vectors. A
construction is only as good as its universal property,
and has none here.
Exercise
(C2: is the
free commutative algebra)
- (a) Prove that the
products
with span , and deduce that an algebra homomorphism out
of is
determined by its restriction to .
- (b) Prove that for
every commutative associative unital
-algebra and every linear map
there is a unique algebra homomorphism with .
- (c) Explain in one
sentence why (b) fails if the word “commutative” is
deleted, and name the algebra that has the corresponding
property for all .
Solution.
(a) is spanned
by its simple tensors (Theorem 15.6.2) and is surjective and
linear, so their images, the products ,
span . If
are
algebra homomorphisms agreeing on , then , and both send
to ; since these elements
span and
both maps are linear, .
(b) For the map is
-linear, as in the
proof of Theorem 15.6.6, and it is
symmetric because is commutative (the
third example after Definition 15.7.1). By
(S1) it induces a linear ; set and on the direct sum.
Multiplicativity is checked on products of vectors,
which span, exactly as in Theorem 15.6.6, and . Uniqueness
is (a).
(c) It fails
because
would have to satisfy , so the images of would be forced to
commute, which need not happen in a noncommutative . The algebra with the
property for all is the tensor algebra
, by
Theorem 15.6.6.
Exercise
(C3: One variable)
Let .
- (a) Prove that for
every , and deduce
that the quotient map assembled from the ’s is an isomorphism of
algebras.
- (b) Hence deduce
that , and reconcile this
with the fact that is
noncommutative for .
Solution.
(a) Write . By Theorem 15.6.3, is spanned
by . A generator of is ;
writing and expanding, both terms equal
, since the scalars
multiply in the same way whatever the order. So every
generator is and . Hence
each is an isomorphism (Theorem 4.4.5, or
directly: its kernel is ), and the assembled
map is a bijective algebra homomorphism, so an
isomorphism.
(b) By Example (The tensor algebra of a line),
, so (a) gives as
well; the same conclusion comes from Theorem 15.7.6 with . There is no
tension with noncommutativity: is
commutative precisely when , because
noncommutativity needs two independent vectors to put in
the two slots (the warning after Theorem 15.6.5). With one
variable there is nothing to reorder, so imposing the
symmetry relations imposes nothing.