Basic equation in Vector Space - Cooperstein Exercise 1, Section 1.3

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SUMMARY

The discussion centers around Exercise 1 from Section 1.3 of Bruce Cooperstein's book, "Advanced Linear Algebra," which addresses the properties of vector spaces over arbitrary fields. Participants analyze the proof structure using Cooperstein's notation, demonstrating that if \( c0 = c0 + c0 \), it follows that \( 0 = c0 \). This proof employs axioms A2, A3, and M1, showcasing the relationship between vector spaces and group theory. The conversation highlights the complexity of deriving solutions compared to understanding them.

PREREQUISITES
  • Familiarity with vector space axioms (A1-A4)
  • Understanding of group theory concepts
  • Knowledge of linear algebra fundamentals
  • Ability to interpret mathematical notation and proofs
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  • Study the properties of vector spaces in "Advanced Linear Algebra" by Bruce Cooperstein
  • Explore the relationship between vector spaces and group theory
  • Practice solving exercises related to vector space axioms
  • Learn about the implications of scalar multiplication in vector spaces
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I am reading Bruce Cooperstein's book: Advanced Linear Algebra ... ...

I am focused on Section 1.3 Vector Spaces over an Arbitrary Field ...

I need help with Exercise 1 of Section 1.3 ...

Exercise 1 reads as follows:View attachment 5107Although apparently simple, I cannot solve this one and would appreciate help ...

Peter*** EDIT ***

To give MHB readers an idea of Cooperstein's notation and approach I am providing Cooperstein's definition of a vector space ... as follows:View attachment 5108
 
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$0 = 0 + 0$ (A3)
$c0 = c(0 + 0)$ (multiplying both sides by $c$)
$c0 = c0 + c0$ (M1)
$c0 + (-c0) = (c0 + c0) + (-c0)$ (adding $-c0$, which exists by A4, to both sides)
$0 = (c0 + c0) + (-c0)$ (A4, again, on the LHS))
$0 = c0 + (c0 + -(c0))$ (A2, on the RHS)
$0 = c0 + 0$ (A4)
$0 = c0$ (A3).

The crux of this argument has its origins in a similar theorem from group theory:

In a group $(G,\ast)$ if $a\ast a = a$, then $a = e$. The only part of it that is "vector-y" is where we invoke M1 to write $c0$ as $c0 + c0$. This is an oft-used type of proof, for example in the real numbers, to show $x = 0$, it suffices to show that $x = 2x$, and in the non-zero reals, if $t$ is a root of $t^2 - t$, then $t = 1$ (we have to exclude $t = 0$ from the reals to get a *group* as $0$ has no multiplicative inverse).
 
Last edited:
Deveno said:
$0 = 0 + 0$ (A3)
$c0 = c(0 + 0)$ (multiplying both sides by $c$)
$c0 = c0 + c0$ (M1)
$c0 + (-c0) = (c0 + c0) + (-c0)$ (adding $-c0$, which exists by A4, to both sides)
$0 = (c0 + c0) + (-c0)$ (A4, again, on the LHS))
$0 = c0 + (c0 + -(c0))$ (A2, on the RHS)
$0 = c0 + 0$ (A4)
$0 = c0$ (A3).
Thanks Deveno ...

hmm ... easy to follow the solution ... but not so easy to dream up or create solution ... :(

Thanks again for the help ... much appreciated ...

Peter
 

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