Chapter 16

Tensors

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Problem 1683

A tensor of type (1,0)(1,0) has components in the basis e1,…,ene_{1}, \ldots , e_{n} (i0i_{0} is a fixed number, 1⩽i0⩽n1 \leqslant i_{0} \leqslant n)

ai={1, if i=i00, if i≠i0 a^{i} = \begin{cases} 1, & \text{ if } i = i_{0} \\ 0, & \text{ if } i \neq i_{0} \end{cases}

Find the components of this tensor in the new basis e1′,…,en′e_{1}^{\prime }, \ldots , e_{n}^{\prime }, given the transition matrix C=(cji)C = \left(c_{j}^{i}\right) from the old basis to the new one.

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Problem 1684

A tensor of type (0,1)(0,1) has components in the basis e1,…,ene_{1}, \ldots , e_{n} (i0i_{0} is a fixed number, 1⩽i0⩽n1 \leqslant i_{0} \leqslant n)

ai={1, if i=i00, if i≠i0 a_{i} = \begin{cases} 1, & \text{ if } i = i_{0} \\ 0, & \text{ if } i \neq i_{0} \end{cases}

Find the components of this tensor in the new basis e1′,…,en′e_{1}^{\prime }, \ldots , e_{n}^{\prime }, given the transition matrix C=(cji)C = \left(c_{j}^{i}\right) from the old basis to the new one.

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Problem 1685

Verify that a vector (respectively a covector (linear function), a linear operator, a bilinear form) on VV defines a tensor of type (1,0)(1,0) (respectively (0,1),(1,1),(0,2)(0,1),(1,1),(0,2)).

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Problem 1686

Verify that the maps defined above between the spaces of tensors Tqp\mathbf{T}_{q}^{p} and multilinear functions Pqp\mathbf{P}_{q}^{p} are well-defined, linear, and bijective. How is the operation ⊗\otimes written in terms of Pqp\mathbf{P}_{q}^{p}?

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Problem 1687

Verify that the tensor product and contraction are well-defined tensor operations.

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Problem 1688

Show that assigning the Kronecker symbol δji\delta_{j}^{i} to every basis defines a tensor of type (1,1)(1,1). Which linear operator and which multilinear function correspond to it?

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Problem 1689

Show that εi1…in\varepsilon_{i_{1} \ldots i_{n}} is not a tensor.

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Problem 1690

Let v∈V,φ∈V∗v \in V, \varphi \in V^{*}. Find the image of the operator corresponding to the tensor v⊗φv \otimes \varphi in the space VV.

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Problem 1691

Fix a basis e1,e2,e3e_{1}, e_{2}, e_{3} in VV and define the tensor A=e1⊗e2−e2⊗e3+e3⊗e1∈T11A = e^{1} \otimes e_{2}-e^{2} \otimes e_{3}+e^{3} \otimes e_{1} \in \mathbf{T}_{1}^{1} and the trilinear map F∈P30F \in \mathbf{P}_{3}^{0}, F(v1,v2,v3)=det⁡∥vji∥F\left(v_{1}, v_{2}, v_{3}\right) = \det \left\| v_{j}^{i}\right\|, where vjiv_{j}^{i} is the ii-th coordinate of the vector vjv_{j} in the given basis. Compute (A⊗TF)21331\left(A \otimes T_{F}\right)_{2133}^{1} and (TF⊗A)21331\left(T_{F} \otimes A\right)_{2133}^{1}.

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Problem 1692

Let, in the basis e1,e2,e3e_{1}, e_{2}, e_{3}, the components of the tensor T∈T32(V)T \in \mathbf{T}_{3}^{2}(V) be defined as Tksmij=2iT_{k s m}^{i j} = 2 i. Find (T′)22312\left(T^{\prime }\right)_{223}^{12}, if ei′=∑j⩽i(i−j+1)eje_{i}^{\prime } = \sum_{j \leqslant i}(i-j+1) e_{j}.

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Problem 1693

Show that a tensor of type (1,1)(1,1), invariant under all orthogonal changes of coordinates in Rn\mathbb {R}^{n}, is proportional to the tensor δji\delta_{j}^{i}.

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Problem 1694

Show that a tensor of the third valence, invariant under arbitrary changes of coordinates, is equal to zero.

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Problem 1695

Find the general form of a tensor of the fourth valence, invariant under an arbitrary change of coordinates. Consider the various cases (p,q),p+q=4(p, q), p+q = 4.

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Problem 1696

Express the trace of the operator A as the result of tensor operations.

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Problem 1697

Express the determinant of the matrix of an operator as the result of tensor operations.

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Problem 1698

Let AA be a linear operator. Find expressions for the quantities Aii,AjiAij,AjiAkjAikA_{i}^{i}, A_{j}^{i} A_{i}^{j}, A_{j}^{i} A_{k}^{j} A_{i}^{k} in terms of the roots and coefficients of the characteristic polynomial det⁡(A−λE)\operatorname {det}\left(A-\lambda E\right).

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Problem 1699

Consider the multilinear function F∈Pnn(V),dim⁡V=nF \in \mathbf{P}_{n}^{n}(V), \operatorname {dim} V = n, given by the formula

F(φ1,…,φn,v1,…,vn)=det⁡∥φj(vi)∥,vi∈V,φj∈V∗ F\left(\varphi ^{1}, \ldots , \varphi ^{n}, v_{1}, \ldots , v_{n}\right) = \det \left\| \varphi ^{j}\left(v_{i}\right)\right\| , \quad v_{i} \in V, \quad \varphi ^{j} \in V^{*}

For a given basis e1,…,ene_{1}, \ldots , e_{n}, find the components of TFT_{F}.

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Problem 1700

Let φ∈Pqp\varphi \in \mathbf{P}_{q}^{p}. Show that the value of φ\varphi on a specific set of covector arguments ξj\xi^{j} and vector arguments viv_{i}, i.e. φ(ξ1,…,ξp,v1,…,vq)\varphi \left(\xi^{1}, \ldots , \xi^{p}, v_{1}, \ldots , v_{q}\right), coincides with the (p+q)(p+q)-fold contraction of the tensor Tφ⊗ξ1⊗…⊗ξp⊗v1⊗…⊗vqT_{\varphi } \otimes \xi^{1} \otimes \ldots \otimes \xi^{p} \otimes v_{1} \otimes \ldots \otimes v_{q} of type (p+q,p+q)(p+q, p+q).

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Problem 1701

Let Rn[x]\mathbb {R}_{n}[x] be the space of all polynomials of degree at most nn in the variable xx with real coefficients. Verify that the map l:Rn[x]→Rl: \mathbb {R}_{n}[x] \rightarrow \mathbb {R}, given by each of the following methods:

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(1)

l(p):=p(0),p∈Rn[x]l(p): = p(0), p \in \mathbb {R}_{n}[x],

(2)

l(p):=∫01p(x)dx,p∈Rn[x]l(p): = \int_{0}^{1} p(x) d x, p \in \mathbb {R}_{n}[x],

(3)

l(p):=∫01p(x)dx+p(0),p∈Rn[x]l(p): = \int_{0}^{1} p(x) d x+p(0), p \in \mathbb {R}_{n}[x],

defines a covector. Let

q=1+x+x2+…+xn q = 1+x+x^{2}+\ldots +x^{n}

and d=ddx∈T11(Rn[x])d = \frac{d}{d x} \in \mathbf{T}_{1}^{1}\left(\mathbb {R}_{n}[x]\right) be the differentiation operator. Find, in these three cases, Fd(l,q)F_{d}(l, q) (the value of the corresponding multilinear function).

Problem 1702

Verify that V⊗WV \otimes W is a linear space.

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Problem 1703

Let k[x]\mathbb {k}[x] be the space of all polynomials in the variable xx with coefficients in the field k\mathbb {k}, and let k[x,y]\mathbb {k}[x, y] be the space of polynomials in xx and yy. Prove that the correspondence f⊗g↦fgf \otimes g \mapsto f g defines a linear isomorphism k[x]⊗k[y]→k[x,y]\mathbb {k}[x] \otimes \mathbb {k}[y] \rightarrow \mathbb {k}[x, y].

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Problem 1704

Let kn[x]\mathbb {k}_{n}[x] be the space of all polynomials of degree at most nn in the variable xx with coefficients in the field k\mathbb {k}, and let kn,m[x,y]\mathbb {k}_{n, m}[x, y] be the space of polynomials in xx and yy of degree at most nn in xx and at most mm in yy. Prove that the correspondence f⊗g↦fgf \otimes g \mapsto f g defines a linear isomorphism kn[x]⊗km[y]→kn,m[x,y]\mathbb {k}_{n}[x] \otimes \mathbb {k}_{m}[y] \rightarrow \mathbb {k}_{n, m}[x, y].

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Problem 1705

Prove the associativity and commutativity (up to natural isomorphisms) of the tensor product operation on spaces.

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Problem 1706

Establish the natural isomorphism

Tqp(V)≅V⊗…⊗V⏟p⊗V∗⊗…⊗V∗⏟q \mathbf{T}_{q}^{p}(V) \cong \underbrace{V \otimes \ldots \otimes V}_{p} \otimes \underbrace{V^{*} \otimes \ldots \otimes V^{*}}_{q}
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Problem 1707

Consider F∈Pq+q′p+p′F \in \mathbf{P}_{q+q^{\prime }}^{p+p^{\prime }}. Prove that the map

V⊗…⊗V⏟q⊗V∗⊗…⊗V∗⏟p→Pq′p′(v1⊗…⊗vq⊗a1⊗…⊗ap)↦F^[v1,…vq,a1…,ap]F^[v1,…,vq,a1,…,ap](ap+1,…,ap+p′,vq+1,…vq+q′)==F(a1,…,ap+p′,v1,…vq+q′) \begin{gathered} \underbrace{V \otimes \ldots \otimes V}_{q} \otimes \underbrace{V^{*} \otimes \ldots \otimes V^{*}}_{p} \rightarrow \mathbf{P}_{q^{\prime }}^{p^{\prime }} \\ \left(v_{1} \otimes \ldots \otimes v_{q} \otimes a^{1} \otimes \ldots \otimes a^{p}\right) \mapsto \widehat{F}\left[v_{1}, \ldots v_{q}, a^{1} \ldots , a^{p}\right] \\ \widehat{F}\left[v_{1}, \ldots , v_{q}, a^{1}, \ldots , a^{p}\right]\left(a^{p+1}, \ldots , a^{p+p^{\prime }}, v_{q+1}, \ldots v_{q+q^{\prime }}\right) = \\ = F\left(a^{1}, \ldots , a^{p+p^{\prime }}, v_{1}, \ldots v_{q+q^{\prime }}\right) \end{gathered}

defines a linear map F~:Ppq→Pq′p′\widetilde{F}: \mathbf{P}_{p}^{q} \rightarrow \mathbf{P}_{q^{\prime }}^{p^{\prime }}.

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Problem 1708

Let dim⁡V=n,dim⁡W=m\operatorname {dim} V = n, \operatorname {dim} W = m, and let e1,…,ene_{1}, \ldots , e_{n} and f1,…,fmf_{1}, \ldots , f_{m} be some bases of the spaces VV and WW. Prove that dim⁡(V⊗W)=n⋅m\operatorname {dim}(V \otimes W) = n \cdot m, and that ei⊗fj,i=1,…,n,j=1,…,me_{i} \otimes f_{j}, i = 1, \ldots , n, j = 1, \ldots , m can be chosen as a basis.

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Problem 1709

Let there be given decompositions of spaces into direct sums: V=⨁iVi,W=⨁jWjV = \bigoplus_{i} V_{i}, W = \bigoplus_{j} W_{j}. Prove that V⊗W≅⨁i,jVi⊗WjV \otimes W \cong \bigoplus_{i, j} V_{i} \otimes W_{j} (after the natural identification).

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Problem 1710

In a special case, the isomorphism between the tensor product and the space of tensors (see problem 1706) becomes the canonical isomorphism τ:V∗⊗V→L(V)\tau : V^{*} \otimes V \rightarrow \mathscr {L}(V), where L(V)\mathscr {L}(V) is the space of linear operators. Compute (first justifying independence of the dimension):

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(1)

τ(e1⊗e3+2e2⊗e4)(e1+2e2−3e3)\tau \left(e^{1} \otimes e_{3}+2 e^{2} \otimes e_{4}\right)\left(e_{1}+2 e_{2}-3 e_{3}\right);

(2)

τ((e1+2e7)⊗e2−4e3⊗e4)(e1+e2+e3−e7)\tau \left(\left(e^{1}+2 e^{7}\right) \otimes e_{2}-4 e^{3} \otimes e_{4}\right)\left(e_{1}+e_{2}+e_{3}-e_{7}\right);

(3)

τ(e2⊗(e3−2e4)+3e4⊗e2)(e1+e2−e3−e4)\tau \left(e^{2} \otimes \left(e_{3}-2 e_{4}\right)+3 e^{4} \otimes e_{2}\right)\left(e_{1}+e_{2}-e_{3}-e_{4}\right).

Problem 1711

In the notation of the previous problem, find, for dim⁡V=4\operatorname {dim} V = 4

τ−1(τ(e1⊗e3−2e2⊗e4)∘τ(e2⊗(e3−e4)+2e4⊗e2)−2Id) \tau ^{-1}\left(\tau \left(e^{1} \otimes e_{3}-2 e^{2} \otimes e_{4}\right) \circ \tau \left(e^{2} \otimes \left(e_{3}-e_{4}\right)+2 e^{4} \otimes e_{2}\right)-2 \mathrm{Id}\right)

where ∘\circ denotes composition of maps.

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Problem 1712

Let V=Rn[x]V = \mathbb {R}_{n}[x] be the space of all polynomials of degree at most nn in the variable xx with real coefficients, and let the function l:V→Rl: V \rightarrow \mathbb {R}, given by the formula

l(p)=∫01p(x)dx+p(0),p∈Rn[x] l(p) = \int _{0}^{1} p(x) d x+p(0), \quad p \in \mathbb {R}_{n}[x]

define a covector. Also consider the polynomials r=1−x+x2r = 1-x+x^{2} and q=1+x+x2+…+xnq = 1+x+x^{2}+\ldots +x^{n}. Find τ(l⊗r)(q)\tau (l \otimes r)(q).

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Problem 1713

Show that f⊗gf \otimes g, as defined in the theoretical part, is a well-defined linear map.

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Problem 1714

Let us denote V⊗p=V⊗…⊗V⏟pV^{\otimes p} = \underbrace{V \otimes \ldots \otimes V}_{p} and f⊗p=f⊗…⊗f⏟pf^{\otimes p} = \underbrace{f \otimes \ldots \otimes f}_{p}, where ff is a linear map. Prove that rk⁡(f⊗p)=(rk⁡(f))p\operatorname {rk}\left(f^{\otimes p}\right) = (\operatorname {rk}\left(f\right))^{p}. In particular, the tensor power of an invertible operator is invertible.

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Problem 1715

For operators in the space VV, prove the formulas:

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(1)

(f∘g)⊗p=f⊗p∘g⊗p(f \circ g)^{\otimes p} = f^{\otimes p} \circ g^{\otimes p}

(2)

(IdV)⊗p=IdV⊗p\left(\mathrm{Id}_{V}\right)^{\otimes p} = \mathrm{Id}_{V^{\otimes p}};

(3)

for invertible ff we have (f⊗p)−1=(f−1)⊗p\left(f^{\otimes p}\right)^{-1} = \left(f^{-1}\right)^{\otimes p};

(4)

(c⋅f)⊗p=cp⋅f⊗p(c \cdot f)^{\otimes p} = c^{p} \cdot f^{\otimes p}, where c∈kc \in \mathbb {k}.

Here ∘\circ denotes composition of maps.

Problem 1716

Prove that tr⁡(f⊗p)=(tr⁡(f))p\operatorname {tr}\left(f^{\otimes p}\right) = (\operatorname {tr}(f))^{p}, where ff is a linear operator.

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Problem 1717

Let e1,…,epe_{1}, \ldots , e_{p} be (not necessarily distinct) eigenvectors of the operator f:V→Vf: V \rightarrow V, corresponding to the eigenvalues λ1,…,λp\lambda_{1}, \ldots , \lambda_{p} respectively. Prove that e1⊗…⊗epe_{1} \otimes \ldots \otimes e_{p} is an eigenvector of the operator f⊗pf^{\otimes p}, corresponding to the eigenvalue λ1⋅…⋅λp\lambda_{1} \cdot \ldots \cdot \lambda_{p}.

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Problem 1718

Let the linear operator f:V→Vf: V \rightarrow V be reducible to diagonal form. Prove that in this case f⊗pf^{\otimes p} is also diagonalizable. Is the converse statement true?

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Problem 1719

Let λk(k=1,…,n)\lambda_{k}(k = 1, \ldots , n) be all the eigenvalues of the operator f:V→Vf: V \rightarrow V, taken with multiplicity, dim⁡V=n\operatorname {dim} V = n. Prove that the set of all eigenvalues of the operator f⊗pf^{\otimes p}, taken with multiplicity, consists of all possible products

λk1⋅…⋅λkp,ks=1,…,n,s=1,…,p \lambda _{k_{1}} \cdot \ldots \cdot \lambda _{k_{p}}, \quad k_{s} = 1, \ldots , n, \quad s = 1, \ldots , p
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Problem 1720

Prove that det⁡(f⊗p)=(det⁡f)pnp−1\operatorname {det}\left(f^{\otimes p}\right) = (\det f)^{p n^{p-1}}, where ff is an operator in VV, dim⁡V=n\operatorname {dim} V = n.

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Problem 1721

Let the linear operators f:V→Vf: V \rightarrow V and g:W→Wg: W \rightarrow W have corresponding decompositions into invariant subspaces V=⨁iVi,W=⨁jWjV = \bigoplus_{i} V_{i}, W = \bigoplus_{j} W_{j}. Prove that V⊗W=⨁i,jVi⊗WjV \otimes W = \bigoplus_{i, j} V_{i} \otimes W_{j} is a decomposition into invariant subspaces for f⊗gf \otimes g.

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Problem 1722

Let ddx\frac{d}{d x} and ddy\frac{d}{d y} be the differentiation operators in the spaces of polynomials Rn[x]\mathbb {R}_{n}[x] and Rm[y]\mathbb {R}_{m}[y] respectively. Determine the analytic meaning of the operator ddx⊗ddy\frac{d}{d x} \otimes \frac{d}{d y} and find its Jordan form.

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Problem 1723

Find the Jordan form of the tensor product of two operators having the following Jordan forms:

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(1)

(2102),(1101)\left(\begin{smallmatrix} 2 & 1 \\ 0 & 2\end{smallmatrix}\right),\left(\begin{smallmatrix} 1 & 1 \\ 0 & 1\end{smallmatrix}\right);

(2)

(2102),(100031003)\left(\begin{smallmatrix} 2 & 1 \\ 0 & 2\end{smallmatrix}\right),\left(\begin{smallmatrix} 1 & 0 & 0 \\ 0 & 3 & 1 \\ 0 & 0 & 3\end{smallmatrix}\right)

(3)

(2102),(010001000)\left(\begin{smallmatrix} 2 & 1 \\ 0 & 2\end{smallmatrix}\right),\left(\begin{smallmatrix} 0 & 1 & 0 \\ 0 & 0 & 1 \\ 0 & 0 & 0\end{smallmatrix}\right).

Problem 1724

Verify that the operators Sym and Alt in the space T0p\mathbf{T}_{0}^{p} have the following properties (where ∘\circ denotes composition of maps):

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(1)

Sym ∘\circ Sym == Sym, Alt ∘\circ Alt == Alt, i.e. Sym and Alt are projectors;

(2)

Sym ∘\circ Alt == Alt ∘\circ Sym =0= 0 for p>1p > 1;

(3)

Ker⁡(Sym)∩Ker⁡(Alt)=0\operatorname {Ker}(\mathrm{Sym}) \cap \operatorname {Ker}(\mathrm{Alt}) = 0 for p=2p = 2 and Ker⁡(Sym)∩Ker⁡(Alt)≠0\operatorname {Ker}(\mathrm{Sym}) \cap \operatorname {Ker}(\mathrm{Alt}) \neq 0 for p>2p > 2;

(4)

(Id - Sym) (Id - Alt) is a projector. Find its rank for p=3p = 3.

Problem 1725

Show that S(V)S(V) with the operation ∙\bullet and Λ(V)\Lambda (V) with the operation ∧\wedge are associative algebras. Moreover:

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(1)

S∙T=T∙SS \bullet T = T \bullet S

(2)

S∧T=(−1)pqT∧SS \wedge T = (-1)^{p q} T \wedge S, if S∈Λp(V),T∈Λq(V)S \in \Lambda^{p}(V), T \in \Lambda^{q}(V);

(3)

the algebra S(V)\mathbf{S}(V) is isomorphic to the algebra k[x1,…,xn]\mathbb {k}\left[x_{1}, \ldots , x_{n}\right], where n=dim⁡Vn = \operatorname {dim} V.

Problem 1726

Let e1,…,ene_{1}, \ldots , e_{n} be a basis of the space VV. Prove that the tensors

e1∙…∙e1⏟s1∙…∙en∙…∙en⏟sn,s1+…+sn=p \underbrace{e_{1} \bullet \ldots \bullet e_{1}}_{s_{1}} \bullet \ldots \bullet \underbrace{e_{n} \bullet \ldots \bullet e_{n}}_{s_{n}}, \quad s_{1}+\ldots +s_{n} = p

form a basis of the space Sp(V)S^{p}(V). Compute its dimension.

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Problem 1727

Let e1,…,ene_{1}, \ldots , e_{n} be a basis of the space VV. Prove that the tensors

ei1∧…∧eip,1⩽i1<i2<…<ip⩽n e_{i_{1}} \wedge \ldots \wedge e_{i_{p}}, \quad 1 \leqslant i_{1} < i_{2} < \ldots < i_{p} \leqslant n

form a basis in Λp(V)\Lambda^{p}(V). Compute its dimension and the dimension of the space Λ(V)\Lambda (V). Carry out analogous reasoning for Ωq(V)\Omega_{q}(V).

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Problem 1728

Prove that the linear span of the set

{v∙…∙v⏟k∣v∈V} \left\{ \underbrace{v \bullet \ldots \bullet v}_{k} \mid v \in V \right\}

equals Sk(V)\mathbf{S}^{k}(V) (the field k\mathbb {k} has characteristic 0).

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Problem 1729

Prove that the natural embeddings

V1→V1⊕V2,v↦(v,0),V2→V1⊕V2,v↦(0,v) V_{1} \rightarrow V_{1} \oplus V_{2}, \quad v \mapsto (v, 0), \quad V_{2} \rightarrow V_{1} \oplus V_{2}, \quad v \mapsto (0, v)

induce isomorphisms

⨁i=0pSi(V1)⊗Sp−i(V2)≅Sp(V1⊕V2)⨁i=0pΛi(V1)⊗Λp−i(V2)≅Λp(V1⊕V2) \begin{aligned} & \bigoplus _{i = 0}^{p} \mathbf{S}^{i}\left(V_{1}\right) \otimes \mathbf{S}^{p-i}\left(V_{2}\right) \cong \mathbf{S}^{p}\left(V_{1} \oplus V_{2}\right) \\ & \bigoplus _{i = 0}^{p} \Lambda ^{i}\left(V_{1}\right) \otimes \Lambda ^{p-i}\left(V_{2}\right) \cong \Lambda ^{p}\left(V_{1} \oplus V_{2}\right) \end{aligned}
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Problem 1730

Let dim⁡V>2\operatorname {dim} V > 2. Show that the spaces Λ2(Λ2(V))\Lambda^{2}\left(\Lambda^{2}(V)\right) and Λ4(V)\Lambda^{4}(V) are not isomorphic.

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Problem 1731

Show that the exterior product a1∧a2∧…∧apa_{1} \wedge a_{2} \wedge \ldots \wedge a_{p} of the vectors a1,a2,…,apa_{1}, a_{2}, \ldots , a_{p} equals zero if and only if these vectors are linearly dependent.

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Problem 1732

Let TT be a skew-symmetric covariant tensor of valence nn in the space VV, with n=dim⁡Vn = \operatorname {dim} V. Show that all its components coincide, up to sign, with T12…nT_{12 \ldots n} (one says that the tensor TT has a single essential component). Prove that this component transforms according to the rule

T12…n′=det⁡C⋅T12…n T_{12 \ldots n}^{\prime } = \det C \cdot T_{12 \ldots n}

where det⁡C\det C is the determinant of the transition matrix to the new basis. Similarly, in the contravariant case, prove the formula (T′)12…n=(det⁡C)−1⋅T12…n\left(T^{\prime }\right)^{12 \ldots n} = (\det C)^{-1} \cdot T^{12 \ldots n}.

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Problem 1733

Let a1,…,apa_{1}, \ldots , a_{p} and b1,…,bpb_{1}, \ldots , b_{p} be two sets of linearly independent vectors. Prove that a1∧…∧ap=λ⋅b1∧…∧bpa_{1} \wedge \ldots \wedge a_{p} = \lambda \cdot b_{1} \wedge \ldots \wedge b_{p} if and only if the linear spans of the two sets of vectors coincide. Moreover, λ\lambda equals the determinant of the transition matrix from the second system of vectors to the first.

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Problem 1734

Show that the linear span of a system of linearly independent vectors a1,…,aka_{1}, \ldots , a_{k} coincides with the set of those vectors aa for which T∧a=0T \wedge a = 0, where T=a1∧…∧akT = a_{1} \wedge \ldots \wedge a_{k}.

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Problem 1735

Let T∈Λp(V)T \in \Lambda^{p}(V); define

Ann⁡(T)={a∈V∣T∧a=0} \operatorname {Ann}(T) = \left\{ a \in V \mid T \wedge a = 0\right\}

Prove that TT can be represented in the form T~∧S\widetilde{T} \wedge S, where S=a1∧…∧ak≠0S = a_{1} \wedge \ldots \wedge a_{k} \neq 0, if and only if ai∈Ann⁡(T)a_{i} \in \operatorname {Ann}(T) for i=1,…,ki = 1, \ldots , k.

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Problem 1736

Prove that the correspondence T↦Ann⁡(T)T \mapsto \operatorname {Ann}(T) is a bijection from the set of nonzero decomposable pp-vectors in VV (considered up to multiplication by a scalar) onto the set of pp-dimensional subspaces of the space VV.

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Problem 1737

Show that for T∈Λp(V)T \in \Lambda^{p}(V) the dimension of the space Ann⁡(T)\operatorname {Ann}(T) does not exceed pp, with equality holding precisely when TT is the exterior product of linearly independent vectors.

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Problem 1738

Let a skew-symmetric tensor T∈Λn−1(V)T \in \Lambda^{n-1}(V) be given, where dim⁡V=n\operatorname {dim} V = n. Prove that there exist vectors a1,…,an−1a_{1}, \ldots , a_{n-1} such that T=a1∧…∧an−1T = a_{1} \wedge \ldots \wedge a_{n-1} (i.e. the (n−1)(n-1)-vector TT is decomposable). Similarly, for S∈Ωn−1(V)S \in \Omega_{n-1}(V) there exist covectors ξ1,…,ξn−1\xi^{1}, \ldots , \xi^{n-1} such that S=ξ1∧…∧ξn−1S = \xi^{1} \wedge \ldots \wedge \xi^{n-1}.

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Problem 1739

Prove that a bivector TT can be represented in the form a∧ba \wedge b for some vectors aa and bb if and only if T∧T=0T \wedge T = 0.

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Problem 1740

Let φ\varphi be a nondegenerate bilinear function on VV. Prove that on the space Λ2(V)\Lambda^{2}(V) one can define a nondegenerate bilinear form Φ\Phi such that for any elements vi∈Vv_{i} \in V, i=1,…,4i = 1, \ldots , 4, we have

Φ(v1∧v2,v3∧v4)=∣φ(v1,v3)φ(v1,v4)φ(v2,v3)φ(v2,v4)∣ \Phi \left(v_{1} \wedge v_{2}, v_{3} \wedge v_{4}\right) =\left|\begin{smallmatrix} \varphi \left(v_{1}, v_{3}\right) & \varphi \left(v_{1}, v_{4}\right) \\ \varphi \left(v_{2}, v_{3}\right) & \varphi \left(v_{2}, v_{4}\right) \end{smallmatrix}\right|
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Problem 1741

Let f:V→Vf: V \rightarrow V be a linear operator. Show that the operator f⊗pf^{\otimes p} (the tensor power) commutes with the operator Alt, thereby defining a linear map f∧p:Λp(V)→Λp(V)f^{\wedge p}: \Lambda^{p}(V) \rightarrow \Lambda^{p}(V).

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Problem 1742

Let dim⁡V=n,f:V→V\operatorname {dim} V = n, f: V \rightarrow V be a linear operator. Prove that the operator f∧(n−1)f^{\wedge (n-1)} is either equal to 0, or nondegenerate, or has rank 1.

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Problem 1743

Let f:V→Vf: V \rightarrow V be a linear operator, dim⁡V=n\operatorname {dim} V = n. Since dim⁡Λn(V)=1\operatorname {dim} \Lambda^{n}(V) = 1, the operator f∧nf^{\wedge n} is multiplication by a scalar. Prove that this scalar equals det⁡f\det f.

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Problem 1744

Prove the formulas (∘\circ is composition):

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(1)

(f∘g)∧p=f∧p∘g∧p(f \circ g)^{\wedge p} = f^{\wedge p} \circ g^{\wedge p}

(2)

(Id⁡V)∧p=Id⁡V∧p\left(\operatorname {Id}_{V}\right)^{\wedge p} = \operatorname {Id}_{V^{\wedge p}};

(3)

for invertible ff we have (f∧p)−1=(f−1)∧p\left(f^{\wedge p}\right)^{-1} = \left(f^{-1}\right)^{\wedge p};

(4)

(c⋅f)∧p=cp⋅f∧p(c \cdot f)^{\wedge p} = c^{p} \cdot f^{\wedge p}, where c∈kc \in \mathbb {k}.

Problem 1745

Let e1,…,epe_{1}, \ldots , e_{p} be linearly independent eigenvectors of the operator f:V→Vf: V \rightarrow V, corresponding respectively to the eigenvalues λ1,…,λp\lambda_{1}, \ldots , \lambda_{p} (not necessarily distinct). Prove that e1∧…∧epe_{1} \wedge \ldots \wedge e_{p} is an eigenvector of the operator f∧pf^{\wedge p}, corresponding to the eigenvalue λ1⋅…⋅λp\lambda_{1} \cdot \ldots \cdot \lambda_{p}.

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Problem 1746

Let the linear operator f:V→Vf: V \rightarrow V be reducible to diagonal form. Prove that in this case f∧pf^{\wedge p} is also diagonalizable. Is the converse true?

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Problem 1747

Let λk(k=1,…,n)\lambda_{k}(k = 1, \ldots , n) be all the eigenvalues of the operator f:V→Vf: V \rightarrow V, taken with multiplicity, dim⁡V=n\operatorname {dim} V = n. Prove that the set of all eigenvalues of the operator f∧pf^{\wedge p}, taken with multiplicity, consists of all possible products

λk1⋅…⋅λkp,1⩽k1<k2<…<kp⩽n \lambda _{k_{1}} \cdot \ldots \cdot \lambda _{k_{p}}, \quad 1 \leqslant k_{1} < k_{2} < \ldots < k_{p} \leqslant n
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Problem 1748

Prove that det⁡(f∧p)=(det⁡f)(n−1p−1)\operatorname {det}\left(f^{\wedge p}\right) = (\det f)^{\binom {n-1}{p-1}}, where f:V→Vf: V \rightarrow V is a linear operator, dim⁡V=n\operatorname {dim} V = n.

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Problem 1749

Let the characteristic polynomial of the operator f:V→Vf: V \rightarrow V, dim⁡V=n\operatorname {dim} V = n, equal ∑p=0napλn−p\sum_{p = 0}^{n} a_{p} \lambda^{n-p}. Prove the equality tr⁡(f∧p)=(−1)n−pap\operatorname {tr}\left(f^{\wedge p}\right) = (-1)^{n-p} a_{p}.

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Problem 1750

Find the traces of the operators f∧pf^{\wedge p} for nontrivial Λp(V)\Lambda^{p}(V), if ff is given by its matrix:

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(1)

(2302−21−112)\left(\begin{smallmatrix} 2 & 3 & 0 \\ 2 & -2 & 1 \\ -1 & 1 & 2\end{smallmatrix}\right);

(2)

(1−2032−11−32)\left(\begin{smallmatrix} 1 & -2 & 0 \\ 3 & 2 & -1 \\ 1 & -3 & 2\end{smallmatrix}\right)

(3)

(2−13732−45005400−23)\left(\begin{smallmatrix} 2 & -1 & 3 & 7 \\ 3 & 2 & -4 & 5 \\ 0 & 0 & 5 & 4 \\ 0 & 0 & -2 & 3\end{smallmatrix}\right);

(4)

(1350−24−10203230−27)\left(\begin{smallmatrix} 1 & 3 & 5 & 0 \\ -2 & 4 & -1 & 0 \\ 2 & 0 & 3 & 2 \\ 3 & 0 & -2 & 7\end{smallmatrix}\right).

Problem 1751

Prove that if tr⁡(f∧p)=0\operatorname {tr}\left(f^{\wedge p}\right) = 0 for every p=1,2,…p = 1,2, \ldots, then the operator f:V→Vf: V \rightarrow V is nilpotent.

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Problem 1752

Find the Jordan form of f∧2f^{\wedge 2} from the known Jordan form of ff:

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(1)

(2100021000210002)\left(\begin{smallmatrix} 2 & 1 & 0 & 0 \\ 0 & 2 & 1 & 0 \\ 0 & 0 & 2 & 1 \\ 0 & 0 & 0 & 2\end{smallmatrix}\right);

(2)

(2100020000110001)\left(\begin{smallmatrix} 2 & 1 & 0 & 0 \\ 0 & 2 & 0 & 0 \\ 0 & 0 & 1 & 1 \\ 0 & 0 & 0 & 1\end{smallmatrix}\right);

(3)

(−1000020000110001)\left(\begin{smallmatrix} -1 & 0 & 0 & 0 \\ 0 & 2 & 0 & 0 \\ 0 & 0 & 1 & 1 \\ 0 & 0 & 0 & 1\end{smallmatrix}\right).

Problem 1753

Let WW be a kk-dimensional subspace of VV. Describe the natural embedding of Λp(W)\Lambda^{p}(W) into Λp(V)\Lambda^{p}(V). Prove that the operator f:V→Vf: V \rightarrow V has WW as an invariant subspace if and only if Λk(W)\Lambda^{k}(W) is invariant under f∧kf^{\wedge k}.

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Problem 1754

For a covector φ∈V∗\varphi \in V^{*}, define the interior product operator as the map

i(φ):T0p→T0p−1Fi(φ)T(φ1,…,φp−1)=FT(φ,φ1…,φp−1),φi∈V∗ \begin{gathered} i(\varphi ): \mathbf{T}_{0}^{p} \rightarrow \mathbf{T}_{0}^{p-1} \\ F_{i(\varphi ) T}\left(\varphi _{1}, \ldots , \varphi _{p-1}\right) = F_{T}\left(\varphi , \varphi _{1} \ldots , \varphi _{p-1}\right), \quad \varphi _{i} \in V^{*} \end{gathered}

where, as above, FT∈P0pF_{T} \in \mathbf{P}_{0}^{p} is the multilinear function corresponding to T∈T0pT \in \mathbf{T}_{0}^{p}. Prove that the interior product operator takes symmetric tensors to symmetric ones, and skew-symmetric ones to skew-symmetric ones. Let φ1\varphi_{1} and φ2\varphi_{2} be two covectors. Show that the operators i(φ1)i\left(\varphi_{1}\right) and i(φ2)i\left(\varphi_{2}\right) commute in S(V)S(V) and anticommute in Λ(V)\Lambda (V).

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Problem 1755

Let φ\varphi be a nondegenerate bilinear function. Prove that assigning to each basis the matrix inverse to the matrix of φ\varphi in this basis defines a tensor of type (2,0).

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Problem 1756

Represent the operations of raising and lowering an index (standing in any position) in terms of product and contraction. Thereby verify that raising and lowering are well-defined tensor operations.

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Problem 1757

Show that if we restrict ourselves to orthogonal changes of coordinates in a Euclidean space, then the transformation law for upper indices coincides with the transformation law for lower indices. More precisely, if in some orthogonal coordinate system Ti1…ip=Ti1…ipT^{i_{1} \ldots i_{p}} = T_{i_{1} \ldots i_{p}} for all i1,…,ipi_{1}, \ldots , i_{p}, then they are also equal in any other orthogonal coordinate system.

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Problem 1758

Let, in the basis e1,e2,e3e_{1}, e_{2}, e_{3}, the matrix of the scalar product equal (210110002)\left(\begin{smallmatrix} 2 & 1 & 0 \\ 1 & 1 & 0 \\ 0 & 0 & 2\end{smallmatrix}\right). Perform the lowering and raising of indices for the tensors (coordinates given in the indicated basis):

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(1)

e1⊗e2+e2⊗e3e^{1} \otimes e_{2}+e^{2} \otimes e_{3}

(2)

Tji=i+jT_{j}^{i} = i+j.

Give the answer as coordinates in this basis.

Problem 1759

In the space Rn[x]\mathbb {R}_{n}[x] of all polynomials of degree at most nn in the variable xx with real coefficients, consider the scalar product

⟨p,q⟩=∫01p(x)q(x)dx,p,q∈Rn[x] \left\langle p, q \right\rangle = \int _{0}^{1} p(x) q(x) d x, \quad p, q \in \mathbb {R}_{n}[x]

Let e0=1,e1=x,e2=x2,…,en=xne_{0} = 1, e_{1} = x, e_{2} = x^{2}, \ldots , e_{n} = x^{n} be a basis. Find the coordinates, in the dual basis, of the covector obtained by raising the index of q=1+2x+3x2q = 1+2 x+3 x^{2}, for n=2n = 2.

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Problem 1760

Let, in the basis (ei)(e_{i}), the matrix of the Euclidean scalar product in the space VV equal ∥gij∥\left\| g_{i j}\right\|, and let the equation a1x1+…+anxn=0a_{1} x^{1}+\ldots +a_{n} x^{n} = 0 define an (n−1)(n-1)-dimensional subspace (hyperplane) WW. Prove that the expressions vi=gijajv^{i} = g^{i j} a_{j}, regarded as the components of some vector in this basis, define a normal vector to WW.

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Problem 1761

Under the conditions of the previous problem, find formulas for computing the distance from the vector u=(ui)u = \left(u^{i}\right) to the hyperplane WW in terms of tensor operations.

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Problem 1762

Apply the formula from the previous problem to find the distance from u=(1,2,1,3)u = (1,2,1,3) to x1−2x2+x3−x4=0x^{1}-2 x^{2}+x^{3}-x^{4} = 0, if

G=(3100120000210011) G =\left(\begin{smallmatrix} 3 & 1 & 0 & 0 \\ 1 & 2 & 0 & 0 \\ 0 & 0 & 2 & 1 \\ 0 & 0 & 1 & 1 \end{smallmatrix}\right)
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Problem 1763

Let VV be a space with a scalar product, and let τ:V→V∗\tau : V \rightarrow V^{*} be the isomorphism defined by this product, (a,b)=τ(a)b(a, b) = \tau (a) b. Prove that the result of lowering the index of a vector a∈Va \in V (regarded as a tensor of type (1,0)(1,0)) coincides with the covector τ(a)\tau (a) in the case of a symmetric scalar product, and with −τ(a)-\tau (a) in the case of a symplectic one. Similarly, the result of raising the index of a covector ξ∈V∗\xi \in V^{*} coincides, respectively, with τ−1(ξ)\tau^{-1}(\xi ) and with −τ−1(ξ)-\tau^{-1}(\xi ).

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Problem 1764

Consider a linear operator f:V→Vf: V \rightarrow V in a space VV with a scalar product, and the corresponding bilinear function φf(a,b)=(f(a),b)\varphi_{f}(a, b) = (f(a), b). Show that the result of lowering the index into the first position for the operator ff, regarded as a tensor of type (1,1)(1,1), coincides with the tensor corresponding to the function φf\varphi_{f} in the case of a symmetric scalar product, and with −φf-\varphi_{f} in the case of a symplectic one.

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Problem 1765

Let G=∥gij∥G = \left\| g_{i j}\right\| be the matrix of the scalar product in the vector space VV. Show that raising the second index of GG produces the Kronecker symbol δij\delta_{i}^{j}, whereas raising the first index produces δji\delta_{j}^{i} for a symmetric scalar product and −δji-\delta_{j}^{i} for a symplectic one.

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Problem 1766

Let, as above, τ:V→V∗\tau : V \rightarrow V^{*} be the isomorphism defined by the given scalar product on the space VV. For a bilinear function φ\varphi on VV, define a bilinear function φ∗\varphi^{*} on V∗V^{*} by the formula

φ∗(ξ,η)=φ(τ−1(ξ),τ−1(η)) \varphi ^{*}(\xi , \eta ) = \varphi \left(\tau ^{-1}(\xi ), \tau ^{-1}(\eta )\right)

Let e1,…,ene_{1}, \ldots , e_{n} be some basis of the space VV, and e1,…,ene^{1}, \ldots , e^{n} the dual basis in V∗V^{*}. Let BB and GG be the matrices, in the basis {ei}\left\{ e_{i}\right\}, of the form φ\varphi and of the scalar product respectively. Verify that the tensor corresponding to φ∗\varphi^{*} is obtained from φ\varphi by raising the index twice. Show that the matrix of φ∗\varphi^{*} in the basis {ej}\left\{ e^{j}\right\} equals G−1BG−1G^{-1} B G^{-1} in the case of a symmetric scalar product and −G−1BG−1-G^{-1} B G^{-1} in the case of a skew-symmetric product. Consider the special case of φ\varphi equal to the scalar product on the space VV.

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Problem 1767

Prove that the oriented volume of the parallelepiped built on the vectors v1,…,vnv_{1}, \ldots , v_{n}, equals

Ve(v1,…,vn)=det⁡∥gij∥⋅det⁡∥vji∥ V_{e}\left(v_{1}, \ldots , v_{n}\right) = \sqrt{\det \left\| g_{i j}\right\| } \cdot \det \left\| v_{j}^{i}\right\|

where vjiv_{j}^{i} is the ii-th coordinate of the vector vjv_{j}. Moreover

(Ve(v1,…,vn))2=Γ(v1,…,vn) \left(V_{e}\left(v_{1}, \ldots , v_{n}\right)\right)^{2} = \Gamma \left(v_{1}, \ldots , v_{n}\right)

where Γ\Gamma is the Gram determinant.

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Problem 1768

Prove that the oriented volume of the parallelepiped built on the vectors v1,…,vnv_{1}, \ldots , v_{n}, equals

Ve(v1,…,vn)=vi1…inv1i1…vnin V_{e}\left(v_{1}, \ldots , v_{n}\right) = \mathbf{v}_{i_{1} \ldots i_{n}} v_{1}^{i_{1}} \ldots v_{n}^{i_{n}}

where vjiv_{j}^{i} is the ii-th coordinate of the vector vjv_{j}. What determines its sign? In the case of R3\mathbb {R}^{3}, how is it related to the oriented volume studied in the analytic geometry course?

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Problem 1769

Prove that:

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(1)

vi1…in=gi1k1…ginknvk1…kn\mathbf{v}^{i_{1} \ldots i_{n}} = g^{i_{1} k_{1}} \ldots g^{i_{n} k_{n}} \mathbf{v}_{k_{1} \ldots k_{n}};

(2)

vi1…in=gi1k1…ginknvk1…kn\mathbf{v}_{i_{1} \ldots i_{n}} = g_{i_{1} k_{1}} \ldots g_{i_{n} k_{n}} \mathbf{v}^{k_{1} \ldots k_{n}};

(3)

the oriented volume of the parallelepiped built on the vectors v1,…,vnv_{1}, \ldots , v_{n}, equals

Ve(v1,…,vn)=vi1…ingi1k1…ginknv1k1…vnkn V_{e}\left(v_{1}, \ldots , v_{n}\right) = \mathbf{v}^{i_{1} \ldots i_{n}} g_{i_{1} k_{1}} \ldots g_{i_{n} k_{n}} v_{1}^{k_{1}} \ldots v_{n}^{k_{n}}

where vjiv_{j}^{i} is the ii-th coordinate of the vector vjv_{j}.

Problem 1770

Describe, in terms of tensor operations, the computation of the scalar, vector, and mixed products in R3\mathbb {R}^{3}.

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Problem 1771

Consider, in R3\mathbb {R}^{3}, the volume element vijk\mathbf{v}_{i j k}. Show that the bilinear map V×V→V,(x,y)↦zV \times V \rightarrow V,(x, y) \mapsto z, defined by the formula zk=gkivijmxjymz^{k} = g^{k i} \mathbf{v}_{i j m} x^{j} y^{m}, coincides with the vector (cross) product (for bases of positive orientation).

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Problem 1772

Consider the tensor vijkl\mathbf{v}_{i j k l} in R4\mathbb {R}^{4}. Let vectors x,yx, y, and zz from R4\mathbb {R}^{4} be given. Assign to an arbitrary basis the set of numbers

ui=gimvmjksxjykzs u^{i} = g^{i m} \mathbf{v}_{m j k s} x^{j} y^{k} z^{s}

Prove that:

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(1)

uiu^{i} is a vector;

(2)

this vector is orthogonal to x,yx, y, and zz;

(3)

its length equals the three-dimensional volume of the parallelepiped built on x,yx, y, and zz.

Problem 1773

Let a∈T11(V)a \in \mathbf{T}_{1}^{1}(V) be a linear operator, dim⁡V=n\operatorname {dim} V = n. Prove that

∑k=1naikmεi1…ik−1mik+1…in=εi1…intr⁡(a) \sum _{k = 1}^{n} a_{i_{k}}^{m} \varepsilon _{i_{1} \ldots i_{k-1} m i_{k+1} \ldots i_{n}} = \varepsilon _{i_{1} \ldots i_{n}} \operatorname {tr}(a)
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Problem 1774

Prove the formulas:

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(1)

εijkεrst=∣δirδisδitδjrδjsδjtδkrδksδkt∣\varepsilon_{i j k} \varepsilon_{r s t} =\left|\begin{smallmatrix} \delta_{i r} & \delta_{i s} & \delta_{i t} \\ \delta_{j r} & \delta_{j s} & \delta_{j t} \\ \delta_{k r} & \delta_{k s} & \delta_{k t}\end{smallmatrix}\right|;

(2)

∑kεijkεrsk=δirδjs−δisδjr\sum_{k} \varepsilon_{i j k} \varepsilon_{r s k} = \delta_{i r} \delta_{j s}-\delta_{i s} \delta_{j r};

(3)

∑k,jεijkεrjk=2δir\sum_{k, j} \varepsilon_{i j k} \varepsilon_{r j k} = 2 \delta_{i r};

(4)

∑k,j,iεijkεijk=6\sum_{k, j, i} \varepsilon_{i j k} \varepsilon_{i j k} = 6,

where δ\delta is the Kronecker symbol, and ε\varepsilon is defined at the beginning of Chapter 16.

Problem 1775

For a kk-form T∈Ωk(Rn)T \in \Omega_{k}\left(\mathbb {R}^{n}\right) on the (oriented) space Rn\mathbb {R}^{n}, define the (n−k)(n-k)-form ∗T∈Ωn−k(Rn)* T \in \Omega_{n-k}(\mathbb {R}^{n}) by the formula

(∗T)i1…in−k=1k!vi1…in−kj1…jkgj1m1…gjkmkTm1…mk (* T)_{i_{1} \ldots i_{n-k}} = \frac{1}{k !} \mathbf{v}_{i_{1} \ldots i_{n-k} j_{1} \ldots j_{k}} g^{j_{1} m_{1}} \ldots g^{j_{k} m_{k}} T_{m_{1} \ldots m_{k}}

Verify that the (n−k)(n-k)-form ∗T* T is well-defined. Check the formula

∗(∗T)=(−1)k(n−k)T *(* T) = (-1)^{k(n-k)} T
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Problem 1776

Let e1,e2,e3e_{1}, e_{2}, e_{3} be a positively oriented orthonormal basis in R3\mathbb {R}^{3}, and eie^{i} the dual basis in (R3)∗\left(\mathbb {R}^{3}\right)^{*}. Verify directly that in this situation:

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(1)

∗e1=e2∧e3,∗e2=e3∧e1,∗e3=e1∧e2* e^{1} = e^{2} \wedge e^{3}, * e^{2} = e^{3} \wedge e^{1}, * e^{3} = e^{1} \wedge e^{2};

(2)

∗(e2∧e3)=e1,∗(e3∧e1)=e2,∗(e1∧e2)=e3*\left(e^{2} \wedge e^{3}\right) = e^{1}, *\left(e^{3} \wedge e^{1}\right) = e^{2}, *\left(e^{1} \wedge e^{2}\right) = e^{3};

(3)

∗c=ce1∧e2∧e3,∗(ce1∧e2∧e3)=c* c = c e^{1} \wedge e^{2} \wedge e^{3}, *\left(c e^{1} \wedge e^{2} \wedge e^{3}\right) = c, where c=c = const ∈Ω0(R3)\in \Omega_{0}\left(\mathbb {R}^{3}\right);

(4)

∗(∗T)=T*(* T) = T for all dimensions; how does this agree with the previous problem?

Problem 1777

Let R3[x]\mathbb {R}_{3}[x] be the space of all polynomials of degree at most 3 in the variable xx with real coefficients and scalar product (p,q)=∫01p(x)q(x)dx,p,q∈R3[x](p, q) = \int_{0}^{1} p(x) q(x) d x, p, q \in \mathbb {R}_{3}[x]. Let the covector q′q^{\prime } be obtained by lowering the index of q=1+x+x2+x3q = 1+x+x^{2}+x^{3}. Find ∗q′* q^{\prime }.

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Problem 1778

Let T,S∈Ωp(Rn)T, S \in \Omega_{p}\left(\mathbb {R}^{n}\right). Set

⟨T,S⟩=1p!gi1j1…gipjpTi1…ipSj1…jp \left\langle T, S \right\rangle = \frac{1}{p !} g^{i_{1} j_{1}} \ldots g^{i_{p} j_{p}} T_{i_{1} \ldots i_{p}} S_{j_{1} \ldots j_{p}}

Verify that

T∧∗S=⟨T,S⟩v T \wedge * S = \left\langle T, S \right\rangle \mathbf{v}

where v∈Ωn(Rn)\mathbf{v} \in \Omega_{n}\left(\mathbb {R}^{n}\right), as before, is the volume element.

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Problem 1779

Verify that ⟨T,S⟩\left\langle T, S \right\rangle is a scalar. Check that the operation ⟨T,S⟩\left\langle T, S \right\rangle defined in the previous problem gives a Euclidean scalar product on Ωp(Rn)\Omega_{p}\left(\mathbb {R}^{n}\right) for each pp.

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Problem 1780

Let e1,e2,e3e_{1}, e_{2}, e_{3} be an orthonormal basis in R3,ei\mathbb {R}^{3}, e^{i} the dual basis in (R3)∗\left(\mathbb {R}^{3}\right)^{*}. Compute, in Ω2(R3)\Omega_{2}\left(\mathbb {R}^{3}\right), the Euclidean distance in the sense of problem 1779 from e2∧e3e^{2} \wedge e^{3} to the line generated by the element e1∧e3−2e2∧e1e^{1} \wedge e^{3}-2 e^{2} \wedge e^{1}.

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Problem 1781

Let e1,e2,e3,e4e_{1}, e_{2}, e_{3}, e_{4} be an orthonormal basis in R4,ei\mathbb {R}^{4}, e^{i} the dual basis in (R4)∗\left(\mathbb {R}^{4}\right)^{*}. Compute, in Ω2(R4)\Omega_{2}\left(\mathbb {R}^{4}\right), the Euclidean distance in the sense of problem 1779 from e2∧e3+2e1∧e4e^{2} \wedge e^{3}+2 e^{1} \wedge e^{4} to the plane generated by the elements e1∧e3−e2∧e1e^{1} \wedge e^{3}-e^{2} \wedge e^{1} and e2∧e4−2e1∧e3e^{2} \wedge e^{4}-2 e^{1} \wedge e^{3}.

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