Existence of Linear Operators with Matching Subspaces in Vector Spaces

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SUMMARY

This discussion establishes that for every subspace B of a vector space C, there exists at least one linear operator L: C→C such that ker(L) = B, and at least one linear operator L': C→C such that L'(C) = B. The operators are defined by their action on basis vectors, with L mapping basis vectors of B to 0 and L' mapping the entirety of C into B. The discussion emphasizes the importance of linear independence and spanning sets in defining these operators.

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  • #31
I'm confused as to how to think about this. I need a vi where L'(C)=B. So I would need a basis for C that would map an element to B?
 
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  • #32
LosTacos said:
I'm confused as to how to think about this. I need a vi where L'(C)=B. So I would need a basis for C that would map an element to B?

No! You just need to define a mapping that takes all of the vi's into B. Use the same basis as before. Some of those vi's are in B, aren't they? Just define f(vi) for each i.
 
  • #33
Okay so then {v1, v2, ... , vk} is a basis for B, and {v1, v2, ... , vk, vk+1, vn} is a basis for C.
Could I use the map where for all i>k L(vi) = L(v1) which is in B.
 
  • #34
LosTacos said:
Okay so then {v1, v2, ... , vk} is a basis for B, and {v1, v2, ... , vk, vk+1, vn} is a basis for C.
Could I use the map where for all i>k L(vi) = L(v1) which is in B.

Yes, you could. Now what to do you propose for i<=k?
 
  • #35
L(v1) = 1
L(v2) = 2
...
For all i<=k: L(vi) = i
 
  • #36
LosTacos said:
L(v1) = 1
L(v2) = 2
...
For all i<=k: L(vi) = i

I think you mean the right thing. But you certainly aren't saying the right thing. 1 and 2 aren't vectors, are they?
 
  • #37
Sorry. It would be L(v1) = v1, L(v2) = v2,... L(vi)=vi
 
  • #38
LosTacos said:
Sorry. It would be L(v1) = v1, L(v2) = v2,... L(vi)=vi

Ok, so L(vi)=vi for i<=k and L(vi)=v1 for i>k? Does that work? Is L(C)=B? Explain why? For extra points tell me some other ways you could have defined L such that L(C)=B.
 
  • #39
Yes. Since {v1, v2, ... , vk} is a basis for B, and {v1, v2, ... , vk, vk+1, vn} is a basis for C,
for i<=k, L(vi) = vi which is apart of both Basis of B and Basis of C because v1 < vi < vk. Then, for any i > k, L(vi) = L(v1) = v1 which is apart of Basis B and Basis C.
 
  • #40
I could of defined L(C)=B such that if i>k, then L(vi) = ker(L) = B = 0
 
  • #41
LosTacos said:
I could of defined L(C)=B such that if i>k, then L(vi) = ker(L) = B = 0

Yes, I THINK you've essentially got it, but you don't really express yourself very well, so I'm guessing. The point is that both ways you've defined L, L(C)=span(v1,v2,...,vk). Which defines B. There are many other ways to define L as well, agree?
 

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