2024-08-11

722: For Vectors Space and 2 Same-Finite-Dimensional Vectors Subspaces, There Is Common Complementary Subspace

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description/proof of that for vectors space and 2 same-finite-dimensional vectors subspaces, there is common complementary subspace

Topics


About: vectors space

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Starting Context



Target Context


  • The reader will have a description and a proof of the proposition that for any vectors space and any 2 same-finite-dimensional subspaces, there is a common complementary subspace.

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 }
V: { the F vectors spaces }
V1: { the k -dimensional subspaces of V}
V2: { the k -dimensional subspaces of V}
//

Statements:
V3{ the subspaces of V}(V3{ the complementary subspaces of V1}{ the complementary subspaces of V2})
//


2: Natural Language Description


For any field, F, any F vectors space, V, and any k-dimensional subspaces, V1,V2, there is a common complementary subspaces of V1 and V2, V3V.


3: Proof


Whole Strategy: we are going to explicitly construct a V3; Step 1: take any basis of V1V2 as {e1,...,el}; Step 2: add to {e1,...,el} some elements of Vj to form a basis of Vj, {e1,...,el,ej,l+1,...,ej,k}; Step 3: see that {e1,...,el,e1,l+1,...,e1,k,e2,l+1,...,e2,k} is linearly independent; Step 4: add to the bases of V1 and V2 {e1,l+1+e2,l+1,...,e1,k+e2,k} and see that the results are linearly independent and span the same subspace spanned by {e1,...,el,e1,l+1,...,e1,k,e2,l+1,...,e2,k}; Step 5: add to {e1,...,el,e1,l+1,...,e1,k,e2,l+1,...,e2,k} some elements of V, {e1,e2,...}, to form a basis of V; Step 6: define V3 as the space spanned by {e1,l+1+e2,l+1,...,e1,k+e2,k,e1,e2,...}; Step 7: see that V3 is indeed a common complementary subspace of V1 and V2.

Let us construct a common complementary subspace.

Step 1:

V1V2 is a subspace of a dimension, lk, by the proposition that for any vectors space, the intersection of any possibly uncountable number of finite-dimensional subspaces is a subspace with a dimension equal to or smaller than the minimum dimension of the subspaces. Let us take any basis of V1V2, {e1,...,el}. l may be 0, and in that case, it becomes the empty set.

Step 2:

{e1,...,el} is linearly independent on V1, because otherwise, j{1,...,l}cjej=0 would have a not-all-zero (c1,...,cl), which would mean that {e1,...,el} was linearly dependent on V1V2. Likewise, {e1,...,el} is linearly independent on V2.

Let us add some kl elements of V1, {e1,l+1,...,e1,k}, to {e1,...,el} to form a basis for V1 and add some kl elements of V2, {e2,l+1,...,e2,k}, to {e1,...,el} to form a basis for V2, which is possible by the proposition that for any finite-dimensional vectors space, any linearly independent subset can be expanded to be a basis by adding a finite number of elements.

Step 3:

{e1,...,el,e1,l+1,...,e1,k,e2,l+1,...,e2,k} is linearly independent on V, because if a e2,l+j was a linear combination of the other elements as e2,l+j=m{1,...,l}cmem+n{1,...,kl}cne1,l+n+o{1,...,j1,j+1,...,kl}coe2,l+o, e2,l+jo{1,...,j1,j+1,...,kl}coe2,l+o=m{1,...,l}cmem+n{1,...,kl}cne1,l+n, but the left hand side would not be 0 because (e2,l+1,...,e2,k) would be linearly independent, and the right hand side would be a vector on V1, and so, e2,l+jo{1,...,j1,j+1,...,kl}coe2,l+o would be in V1V2, which would imply that it would be a linear combination of e1,e2,...,el, a contradiction against {e1,...,el,e2,l+1,...,e2,k}'s being linearly independent.

Step 4:

Let us add e1,l+1+e2,l+1 to the both bases. Then, the both results are linearly independent, because for V1, {e1,...,el,e1,l+1,...,e1,k,e1,l+1+e2,l+1} is linearly independent from the fact in the previous paragraph (for m{1,...,l}cmem+n{1,...,kl}cne1,l+n+c1(e1,l+1+e2,l+1)=m{1,...,l}cmem+(c1+c1)e1,l+1+n{2,...,kl}cne1,l+n+c1e2,l+1)=0, c1=0 and c1+c1=0, so, c1=0, and all the other coefficients are 0), and likewise for V2.

Then, let us add e1,l+2+e2,l+2 to the both results of the previous paragraph. Then, the both results are linearly independent, because for V1, {e1,e2,...,el,e1,l+1,e1,l+2,...,e1,k,e1,l+1+e2,l+1,e1,l+2+e2,l+2} is linearly independent (for m{1,...,l}cmem+n{1,...,kl}cne1,l+n+c1(e1,l+1+e2,l+1)+c2(e1,l+2+e2,l+2)=m{1,...,l}cmem+(c1+c1)e1,l+1+(c2+c2)e1,l+2+n{3,...,kl}cne1,l+n+c1e2,l+1+c2e2,l+2)=0, c1,c2=0 and c1+c1,c2+c2=0, so, c1,c2=0, and all the other coefficients are 0), and likewise for V2.

And so on until we have added e1,k+e2,k. Then, the both results span the same subspace, the space spanned by {e1,...,el,e1,l+1,...,e1,k,e2,l+1,...,e2,k}, denoted as V4. That is because while each element of {e1,...,el,e1,l+1,...,e1,k,e1,l+1+e2,l+1,...,e1,k+e2,k} is a linear combination of {e1,...,el,e1,l+1,...,e1,k,e2,l+1,...,e2,k}, each element of {e1,...,el,e1,l+1,...,e1,k,e2,l+1,...,e2,k} is a linear combination of {e1,...,el,e1,l+1,...,e1,k,e1,l+1+e2,l+1,...,e1,k+e2,k}: e2,j=e1,j+e2,je1,j, and likewise for {e1,...,el,e2,l+1,...,e2,k,e1,l+1+e2,l+1,...,e1,k+e2,k}. {e1,...,el,e1,l+1,...,e1,k,e2,l+1,...,e2,k}, {e1,...,el,e1,l+1,...,e1,k,e1,l+1+e2,l+1,...,e1,k+e2,k}, and {e1,...,el,e2,l+1,...,e2,k,e1,l+1+e2,l+1,...,e1,k+e2,k} are some bases of V4.

Step 5:

Let us add some vectors, {e1,e2,...} (although indexed like that here for convenience of expression, they may be uncountably many vectors), to the 1st basis of V4 to form a basis of V, {e1,...,el,e1,l+1,...,e1,k,e2,l+1,...,e2,k,e1,e2,...}, which is possible by the proposition that for any vectors space and any linearly independent subset, the subset can be expanded to be a basis. In fact, obviously, also {e1,...,el,e1,l+1,...,e1,k,e1,l+1+e2,l+1,...,e1,k+e2,k,e1,e2,...} and {e1,...,el,e2,l+1,...,e2,k,e1,l+1+e2,l+1,...,e1,k+e2,k,e1,e2,...} are some bases of V.

Step 6:

Then, we define V3 as the space spanned by {e1,l+1+e2,l+1,...,e1,k+e2,k,e1,e2,...}.

Step 7:

Let us see that V3 is indeed a complementary subspace of V1.

Let us see that V=V1+V3. V is spanned by {e1,...,el,e1,l+1,...,e1,k,e1,l+1+e2,l+1,...,e1,k+e2,k,e1,e2,...}. V1 is spanned by {e1,...,el,e1,l+1,...,e1,k}. V3 is spanned by {e1,l+1+e2,l+1,...,e1,k+e2,k,e1,e2,...}.

Let us see that V1V3={0}. For any nonzero element of V3, c1(e1,l+1+e2,l+1)+...+ck(e1,k+e2,k)+c1e1+c2e2+..., it cannot be any linear combination of the basis of V1, {e1,...,el,e1,l+1,...,e1,k}, because the 2nd basis of V, {e1,...,el,e1,l+1,...,e1,k,e1,l+1+e2,l+1,...,e1,k+e2,k,e1,e2,...} is linearly independent, which means that it is not any element of V1.

Likewise, V3 is indeed a complementary subspace of V2.

It is clear that it does not matter if l=0 or l=k or k equals 0 or the dimension of V. In fact, if l=0, we can do just without {e1,...,el}; if l=k, the 2 subspaces are the same, and there is a common complementary subspace anyway; if k=0, the 2 subspaces are the same {0} and the whole V is the common complementary subspace; if k equals the dimension of V, the 2 subspaces are the same V and {0} is the common complementary subspace.


References


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