MHB Proving $\{w_1, \ldots , w_m\}$ is a Basis of $\text{Lin}(v_1, \ldots , v_k)$

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SUMMARY

The discussion focuses on proving that a subset of vectors $\{w_1, \ldots, w_m\}$ can form a basis for the linear span of a set of vectors $\{v_1, \ldots, v_k\}$ in $\mathbb{R}^n$. A basis is defined as a linearly independent set that spans the vector space. The key argument presented is that if the original set is not linearly independent, one can express one vector as a linear combination of others, thereby reducing the set while maintaining its span. This process continues until a linearly independent subset that spans the space is obtained.

PREREQUISITES
  • Understanding of linear independence and spanning sets in vector spaces.
  • Familiarity with linear combinations of vectors.
  • Basic knowledge of vector spaces in $\mathbb{R}^n$.
  • Concept of finite sets and their properties in linear algebra.
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  • Study the concept of linear independence in depth.
  • Learn about the process of finding bases for vector spaces.
  • Explore the method of Gaussian elimination for determining linear independence.
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mathmari
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Hey! :o

Let $1\leq n\in \mathbb{N}$ and $v_1, \ldots , v_k\in \mathbb{R}^n$. Show that there exist $w_1, \ldots , w_m\in \{v_1, \ldots , v_k\}$ such that $(w_1, \ldots , w_m)$ is a basis of $\text{Lin}(v_1, \ldots , v_k)$. I have done the following:

A basis of $\text{Lin}(v_1, \ldots , v_k)$ is a linearly independent set of vectors of $\{v_1, \ldots , v_k\}$.

So let $\{w_1, \ldots , w_m\}\subseteq \{v_1, \ldots , v_k\}$ be a linearly independent set.

$\text{Lin}(v_1, \ldots , v_k)$ is the set of all linear combinations of $v_1, \ldots , v_k$. So it left to show that we can express every linear combination of that set using the vectors $\{w_1, \ldots , w_m\}$, or not? (Wondering)
 
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mathmari said:
Hey! :o

Let $1\leq n\in \mathbb{N}$ and $v_1, \ldots , v_k\in \mathbb{R}^n$. Show that there exist $w_1, \ldots , w_m\in \{v_1, \ldots , v_k\}$ such that $(w_1, \ldots , w_m)$ is a basis of $\text{Lin}(v_1, \ldots , v_k)$. I have done the following:

A basis of $\text{Lin}(v_1, \ldots , v_k)$ is a linearly independent set of vectors of $\{v_1, \ldots , v_k\}$.

So let $\{w_1, \ldots , w_m\}\subseteq \{v_1, \ldots , v_k\}$ be a linearly independent set.

$\text{Lin}(v_1, \ldots , v_k)$ is the set of all linear combinations of $v_1, \ldots , v_k$. So it left to show that we can express every linear combination of that set using the vectors $\{w_1, \ldots , w_m\}$, or not?

Hey mathmari!

Yes, a basis must also span the space. (Thinking)
 
That was implied in the first post. mathmari said that the basis we seek is a linearly independent subset of \{v_1, v_2, \cdot\cdot\cdot, v_k\} which was already said to span the space.

mathmari, you say "let \{w_1, w_2, \cdot\cdot\cdot, w_m\}\subseteq \{v_1, v_2, \cdot\cdot\cdot, v_k\}<br /> be a linearly independent subset". You are missing the crucial point- proving that such a linearly independent subset, that still spans the space, exists! You need to say something like "If \{v_1, v_2, \cdot\cdot\cdot, v_k\}<br />, which spans the space, is also linearly independent then we are done- it is a basis. If not then there exist numbers, \alpha_1, \alpha_2, \cdot\cdot\cdot, \alpha_k, not all 0, such that \alpha_1v_1+ \alpha_2v_2+ \cdot\cdot\cdot+ \alpha_kv_k= 0. Let \alpha_n be one of the non-zero \alphas. Then v_n= -\frac{1}{\alpha_n}(\alpha_1v_1+ \alpha_2v_2+ \cdot\cdot\cdot+ \alpha_{n-1}v_{n-1}+ \alpha_{n+2}v_{n+2}+ \cdot\cdot\cdot+ \alpha_kv_k) so that v_n can be replaced by that linear combination of the other vectors. This smaller set of vectors still spans the vector space. If it is linearly independent we are done, we have a basis. If it is not repeat the process. Since the initial set of vectors was finite, this will eventually terminate.
 
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I got it! Thank you very much! (Smile)
 
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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