2025-02-23

1023: Tensor Product of k Finite-Dimensional Vectors Spaces Has Basis That Consists of Classes Induced by Basis Elements

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description/proof of that tensor product of k finite-dimensional vectors spaces has basis that consists of classes induced by basis elements

Topics


About: vectors space

The table of contents of this article


Starting Context



Target Context


  • The reader will have a description and a proof of the proposition that the tensor product of any k finite-dimensional vectors spaces has the basis that consists of the classes induced by any basis elements.

Orientation


There is a list of definitions discussed so far in this site.

There is a list of propositions discussed so far in this site.


Main Body


1: Structured Description


Here is the rules of Structured Description.

Entities:
F: { the fields }
{V1,...,Vk}: { the finite-dimensional F vectors spaces }
{B1,...,Bk}: Bl{ the bases for Vl}
V1...Vk: = the tensor product 
B: ={[((b1,j1,...,bk,jk))]|bl,jlBl}
//

Statements:
B{ the bases for V1...Vk}
//

Let us call B "the standard basis with respect to {B1,...,Bk}": it is not determined unless {B1,...,Bk} is specified.


2: Note


Each Vj needs to be finite-dimensional, because Proof uses the dual of Bj: the definition of dual basis for covectors (dual) space of basis for finite-dimensional vectors space requires Vj to be finite-dimensional.


3: Proof


Whole Strategy: Step 1: see that B spans V1...Vk; Step 2: see that B is linearly independent.

Step 1:

Let us see that B spans V1...Vk.

Each element of V1...Vk is [r1((v1,1,...,v1,k))+...+rl((vl,1,...,vl,k))] by the definition of tensor product of k vectors spaces.

[r1((v1,1,...,v1,k))+...+rl((vl,1,...,vl,k))]=r1[((v1,1,...,v1,k))]+...+rl[((vl,1,...,vl,k))], which is by the definition of quotient vectors space of vectors space by sub-'vectors space'.

Let us look at each rj[((vj,1,...,vj,k))].

rj[((vj,1,...,vj,k))]=rj[((m1S1,jvj,1m1b1,m1,...,mkSk,jvj,kmkbk,mk))], where Sl,j is a finite index set, =rjm1S1,jvj,1m1[((b1,m1,...,mkSk,jvj,kmkbk,mk))], which is by "the 2 legitimate rules", =...=rjm1S1,jvj,1m1...mkSk,jvj,kmk[((b1,m1,...,bk,mk))], which means that rj[((vj,1,...,vj,k))] is a linear combination of B.

So, [r1((v1,1,...,v1,k))+...+rl((vl,1,...,vl,k))]=r1[((v1,1,...,v1,k))]+...+rl[((vl,1,...,vl,k))] is a linear combination of B.

So, B spans V1...Vk.

Note that this step did not use finite-dimensional-ness of Vj s, so, B spans V1...Vk even when Vj s are infinite-dimensional.

Step 2:

Let us see that B is linearly independent.

Let r1[((b1,j1,1,...,bk,j1,k))]+...+rl[((b1,jl,1,...,bk,jl,k))]=0.

Let us take the dual basis of each Bj, Bj={bjl}.

Let us take the multilinear map, fjm,1,...,jm,k:V1×...×VkF=b1jm,1...bkjm,k.

By the proposition that for any multilinear map from any finite product vectors space, there is the unique linear map from the tensor product of the finite number of vectors spaces such that the multilinear map is the linear map after the canonical map from the product vectors space into the tensor product, there is the unique linear map, fjm,1,...,jm,k:V1...VkF, such that fjm,1,...,jm,k=fjm,1,...,jm,kg, where g:V1×...×VkV1...Vk,(v1,...,vk)[((v1,...,vk))].

0=fjm,1,...,jm,k(0)=fjm,1,...,jm,k(r1[((b1,j1,1,...,bk,j1,k))]+...+rl[((b1,jl,1,...,bk,jl,k))])=r1fjm,1,...,jm,k([((b1,j1,1,...,bk,j1,k))])+...+rlfjm,1,...,jm,k([((b1,jl,1,...,bk,jl,k))]), because fjm,1,...,jm,k is linear, but fjm,1,...,jm,k([((b1,jn,1,...,bk,jn,k))])=fjm,1,...,jm,kg((b1,jn,1,...,bk,jn,k))=fjm,1,...,jm,k((b1,jn,1,...,bk,jn,k))=b1jm,1...bkjm,k((b1,jn,1,...,bk,jn,k))=b1jm,1(b1,jn,1)...bkjm,k(bk,jn,k)=δm,n, so, 0=rm.

So, B is linearly independent.


References


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