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7.4 Tensor, Symmetric and Exterior Algebra of a Vector Space
Let F be a field and let V be an F-vector space. We define a sequence Tr(V )
of F-vector spaces by setting T0(V ) = F, T1(V ) = V , and in general,
Tr(V ) =
Or
i=1
V = V F · · · F V (r factors ).
Note that “” gives a natural “multiplication:”
: Tr(V ) × Ts(V ) −! Tr+s(V ),
where (_, _) 7! _ _. As a result, if we set
T(V ) =
1M
r=0
Tr(V ),
we have a natural F-algebra structure on T(V ), with multiplication given
by . The algebra T(V ) so determined is called the tensor algebra of V .
If we denote by i : V ! T(V ) the composition V = T1(V ) ,! T(V ), then
we have the following universal mapping property. If A is any F-algebra,
and if f : V ! A is any linear transformation, then there exists a unique
F-algebra homomorphism _ : T(V ) ! A that extends f. In other words, we
have the commutative triangle below:
V A,
T(V )
-
_ @
@
@
@
@R
f
i _
where i : V ! T(V ) is the inclusion map.
In order to facilitate discussions of the symmetric and exterior algebras
of the vector space V , we pause to make a few more comments concerning
166 CHAPTER 7. TENSOR PRODUCTS
the tensor algebra T(V ) of V . First of all if A is any F-algebra admitting a
direct sum decomposition A =
L1
i=0 Ar such that for all indices r, s we have
ArAs _ Ar+s, then we call A a graded algebra. Elements of Ai are called
homogeneous elements of degree r. Therefore, it is clear that the tensor
algebra T(V ) is a graded algebra.
Next, if A is a graded algebra and if I _ A is a 2-sided ideal in A,
we say that I is a homogeneous ideal (sometimes called a graded ideal) , if
I =
L1
r=0 Ar \ I.
The following is pretty routine:
Proposition 7.4.1 Let A be a graded algebra and let I be a 2-sided ideal
generated by homogeneous elements. Then I is a homogeneous ideal. In
this case A/I =
L1
r=0 Ar/(Ar \ I) is a graded algebra.
With the above in place, we now define the symmetric algebra of the
vector space V as the quotient algebra S(V ) = T(V )/I, where I is the
homogeneous ideal generated by tensors of the form vw−wv, v,w 2 V .
By Proposition 7.4.1, S(V ) =
L
Sr(V ) is a graded algebra, where Sr(V ) =
Tr(V )/(Tr(V ) \ I).
Multiplication in S(V ) is usually denoted by juxtaposition; in particular,
if v,w 2 V _ S(V ), then vw is the product of v and w. Equivalently vw
is just the coset: vw = v w + I, and vw = wv v,w 2 V . As a result, if
{v1, v2, . . . , vn} is a basis of V , then Sr(V ) is spanned by elements of the
form ve1
1 ve2
2 · · · ven
n , where e1+e2+· · ·+en = r. In fact, these elements form
a basis of Sr(V ); see Proposition 7.4.2, below.
Note that there is a very natural isomorphism i : V
_=!
S1(V ) ,! S(V ).
The symmetric algebra S(V ) then enjoys the following universal property.
If A is any commutative F-algebra, and if f : V ! A is any linear transformation,
then there exists a unique F-algebra homomorphism : S(V ) ! A
that extends f. In other words, we have the commutative triangle below:
V A,
S(V )
-
_ @
@
@
@
@R
f
i
7.4. TENSOR, SYMMETRIC AND EXTERIOR ALGEBRA 167
Actually the symmetric algebra is a pretty familiar object:
Proposition 7.4.2 Let V have F-dimension n, and set A = F[x1, x2, . . . , xn],
where x1, x2, . . . xn are indeterminates over F. Then S(V ) _= A.
Finally, we turn to the so-called exterior algebra of the vector space
V . This time we start with the homogeneous ideal J _ T(V ) of T(V )
generated by homogeneous elements v v, v 2 V . By Proposition 7.4.1, if
we set E(V ) = T(V )/J,
Vr(V ) = Tr(V )/(Tr L (V ) \ J), then then E(V ) = 1
r=0
Vr(V ) is a graded algebra (sometimes denoted
V
V ).
Again, we have a natural inclusion i : V ,! E(V ), and E(V ) has the
predictable universal mapping property: If If A is any F-algebra, and if
f : V ! A is any linear transformation satisfying f(v)2 = 0 for all v 2 V ,
then there exists a unique F-algebra homomorphism _ : E(V ) ! A that
extends f. In other words, we have the commutative triangle below:
V A,
E(V )
-
_ @
@
@
@
@R
f
i _
If we regard V as a subspace of E(V ) via the map i above, and if v,w 2 V ,
we denote the product of v and w by v ^ w; again, this is just the coset
v ^wvw+J. Therefore, it is clear that v ^v = 0, and if v,w 2 V we have
(v + w) ^ (v + w) = 0, which implies that v ^ w = −w ^ v. In particular, if
dim V = n and if v1, v2, . . . vr 2 V , where r > n, then v1 ^ v2 ^ · · · ^ vr = 0.
Therefore, r > n implies that
Vr(V ) = 0 for all m > n.
Proposition 7.4.3 Assume that V is finite dimensional and that A =
{v1, . . . , vn} is a basis of V . Let R = {i1, . . . , ir}, where 1 _ i1 < · · · < ir _
n, set N = {1, 2, . . . , n}, and set vR = vi1 ^ · · · ^ vir . Then {vR| R _ A}
spans E(V ) as a vector space. In particular dim E(V ) _ 2n.
In fact, in the above proposition, we get equality: dim E(V ) = 2n. To
prove this, it suffices to prove that dim
Vr V = (nr
) . The method of doing
168 CHAPTER 7. TENSOR PRODUCTS
this is interesting in its own right; we sketch the argument here. First of all,
let f1, f2, . . . , fr 2 V _ (the F-dual of V ), and define
F = F(f1,f2,...,fr) : V × V × · · · × V −! F
by setting F(w1,w2, . . . ,wr) = f1(w1)f2(w2) · · · fr(wr). It is routine to check
that F is multilinear; thus there exists a unique linear map
_ = _(f1,f2,...,fr) : V V · · · V −! F
satisfying _(w1 w2 . . . wr) = f1(w1)f2(w2) · · · fr(wr).
Now let {v1, v2, . . . , vn} be the above basis of V , and let f1, f2, . . . , fn be
the dual functionals, i.e., satisfying fi(vj) = _ij . Let R = {i1, . . . , ir}, where
1 _ i1 < · · · < ir _ n, and define the linear map
_R =
X
_2Sr
sgn(_)_(fi_(1),fi_(2),···fi_(r)) : V V · · · V −! F.
It is easy to check that _R factors through
Vr V , giving a linear map
fK :
Vr V −! F,
satisfying
fR(w1 ^ · · · ^ wr) =
X
_2Sr
sgn(_)fi_(1)(w1)fi_(2)(w2) · · · fi_(r)(wr).
From the above, it follows immediately that fR(vR0) = _RR0 , which implies
that the set {vR| |R| = r} is a linearly independent subset of
Vr V. This
proves what we wanted, viz.,
Theorem 7.4.4 The exterior algebra E(V ) of the n-dimensional vector
space V has dimension 2n.
Exercises 7.4
1. Assume that the F-vector space V has dimension n. For each r _ 0,
compute the F-dimension of Sr(V ).
7.4. TENSOR, SYMMETRIC AND EXTERIOR ALGEBRA 169
2. Let V andW be F-vector spaces. An n-linear map f : V ×V ×· · ·×V !
W is called alternating if for any v 2 V , we have
f(. . . , v, . . . , v, . . .) = 0.
Prove that in this case there exists an F-linear map ˆ f :
Vn V ! W
such that
f(v1, v2, . . . , vn) = ˆ f(v1 ^ v2 ^ · · · ^ vn).
In particular, how can the determinant be interpreted as a linear functional
on
Vn V ?
3. Let T : V ! V be a linear transformation, and let r be a non-negative
integer. Show that there exists a unique linear transformation
Vr V T : r V !
Vr V satisfying
Vr T(v1 ^v2 ^· · ·^vr) = T(v1)^T(v2)^· · ·^
T(vr), where v1, v2, . . . , vr 2 V .
4. Let T : V ! V be a linear transformation, and assume that dim V =
n. Show that
Vn T = det T · 1Vn V :
Vn V !
Vn V.
5. Let G be a group represented on the F-vector space V (see page 146).
Show that the mapping G ! GLF(
Vr V ) given by g 7!
Vr g defines a
group representation on
Vr V, r _ 0.
6. VLet V be a vector space and let v 2 V . Define the linear map · ^ v : r V !
Vr+1 V by ! 7! ! ^ v. If dim V = n, compute the dimension
of the kernel of · ^ v.
7. Let V be an n-dimensional F-vector space. If d _ n, define the (n, d)-
Grassmann space, Gd(V ) as the set of all d-dimensional subspaces of
V . In particular, if d = 1, the set G1(V ) is more frequently called the
projective space on V , and is denoted by P(V ). We define a mapping
_ : Gd(V ) −! P(
Vd V ),
as follows. If U 2 Gd(V ), let {u1, . . . , ud} be a basis of U, and let _(U)
be the 1-space in P(
Vd V ) spanned by u1 ^ · · · ^ ud. Prove that _ :
Gd(V ) ! P(
Vd V ) is a well-defined injection of Gd(V ) into P(
Vd V ).
(This mapping is called the Pl¨ucker embedding .)
8. Let V be an n-dimensional over the finite field Fq. Show that the
Pl¨ucker embedding _ : Gn−1(V ) −! P(
Vn−1 V ) is surjective. This
170 CHAPTER 7. TENSOR PRODUCTS
implies that every element of z 2
Vn−1 V can be written as a “decomposable
element” of the form z = v1^v2^· · ·^vn−1 for suitable vectors
v1, v2, . . . , vn−1 2 V . (Actually this result is true independently of the
field F; see, e.g., M. Marcus, Finite Dimensional Linear Algebra, part
II, Pure and Applied Mathematics, Marcel Dekker, Inc., New York,
1975, page 7. An alternative approach, suggested to me by Ernie Shult,
is sketched in the exercise below.)
9. Let G = GL(V ) acting naturally on the n-dimensional vector space V .
(a) Show that the recipe g(f) = det g ·f _g−1, g 2 G, f 2 V _ defines
a representation of G on V _, the dual space of V .
(b) Show that in the above action, G acts transitively on the non-zero
vectors of V _.
(c) Fix any isomorphism
Vn V _= F; show that the map
Vn−1 V !
V _ given by ! 7! ! ^ · is a G-equivarient isomorphism. (See
page 7.)
(d) Since G clearly acts on the set of decomposable vectors in
Vn−1 V ,
conclude that every vector is decomposable.
10. Let V,W be F-vector spaces. Prove that there is an isomorphism
M
i+j=r
Vi V _
Vj W −!
Vr(V _W).
11. Let V be an F-vector space, where char F 6= 2. Define the linear
transformation S : V V ! V V by setting S(v w) = w v.
(a) Prove that S has minimal polynomial mS(x) = (x − 1)(x + 1).
(b) If V1 = ker(S − I), V−1 = ker(S + I), conclude that V V =
V1 _ V−1.
(c) Prove that V1
_= S2(V ), V−1
_=
V2(V ).
(d) If T : V ! V is any linear transformation, prove that V1 and V−1
are T T-invariant subspaces of V V .
12. Let V an n-dimensional F-vector space.
(a) Prove that E(V ) is graded-commutative in the sense of Exercise 5
of Section 7.3.
7.4. TENSOR, SYMMETRIC AND EXTERIOR ALGEBRA 171
(b) If L is a one-dimensional F-vector space, prove that as gradedcommutative
algebras,
E(V ) _= E(L) E(L) · · · E(L) (n factors).
172 CHAPTER 7. TENSOR PRODUCTS
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