MHB Linear Dependency: Proving Vector Independence in V

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In a vector space V with three linearly independent vectors e1, e2, and e3, the task is to prove that the vectors e1+e2, e2-e3, and e3+2e1 are also linearly independent. The approach involves setting up a linear combination of the new vectors and equating it to zero. By rearranging the terms, the coefficients of e1, e2, and e3 can be expressed in terms of c1, c2, and c3. Since e1, e2, and e3 are independent, it follows that the coefficients must all equal zero, confirming the linear independence of the new vectors. This completes the proof of their independence.
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Hello,

I need some help with this one...any guidance will be appreciated.

In a vector space V there are 3 linearly independent vectors e1,e2,e3. Prove that the vectors:

e1+e2 , e2-e3 , e3+2e1

are also linearly independent.

Thanks...
 
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Yankel said:
Hello,

I need some help with this one...any guidance will be appreciated.

In a vector space V there are 3 linearly independent vectors e1,e2,e3. Prove that the vectors:

e1+e2 , e2-e3 , e3+2e1

are also linearly independent.

Thanks...

We want to see when the combination
\[c_1(e_1+e_2)+c_2(e_2-e_3)+c_3(e_3+2e_1)=0\]
Rearranging the terms we get
\[(c_1+2c_3)e_1+(c_1+c_2)e_2+(c_3-c_2)e_3=0\]
Since $e_1,e_2,e_3$ are independent, what does that say about the value of the coefficients $c_1+2c_3, c_1+c_2, c_3-c_2$?

You should have enough information now to finish off this problem.
 
I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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