MHB Finding a 3rd polynomial to create a basis.

  • Thread starter Thread starter Harambe1
  • Start date Start date
  • Tags Tags
    Basis Polynomial
Click For Summary
To find a third polynomial \( t_3 \) in the space \( T \) such that \( \{t_1, t_2, t_3\} \) forms a basis, the polynomials must satisfy the condition \( t(1)=0 \). The existing polynomials \( t_1 \) and \( t_2 \) are already defined, and since \( T \) is a subspace of \( P_3(\mathbb{R}) \) with dimension 3, it requires a third polynomial that is linearly independent from \( t_1 \) and \( t_2 \). The discussion emphasizes the need to identify a polynomial that meets these criteria while adhering to the specified condition. Finding \( t_3 \) involves ensuring it complements the existing polynomials to span the subspace \( T \).
Harambe1
Messages
5
Reaction score
0
Hi,

I am struggling with the following problem:

"Let $V=P_3(\Bbb{R})$ and let $t_1=3x^3-x-2$ and $t_2=x^3-3x+2$ with $T=\left\{ t\in V \:|\: t(1)=0 \right\}$. Find ${t_3}\in\left\{T\right\}$ such that $\left\{t_1, t_2, t_2\right\}$ is a basis of T.

Not sure where to go as each column matrix will have 4 elements but then there is only 3 polynomials in the basis.Thanks.
 
Physics news on Phys.org
Harambe said:
Hi,

I am struggling with the following problem:

"Let $V=P_3(\Bbb{R})$ and let $t_1=3x^3-x-2$ and $t_2=x^3-3x+2$ with $T=\left\{ t\in V \:|\: t(1)=0 \right\}$. Find ${t_3}\in\left\{T\right\}$ such that $\left\{t_1, t_2, t_2\right\}$ is a basis of T.

Not sure where to go as each column matrix will have 4 elements but then there is only 3 polynomials in the basis.Thanks.

Hi Harambe! Welcome to MHB! ;)

Indeed, there are 4 elements, so a basis of $V$ will have 4 polynomials.
However, $T$ has the restriction $t(1)=0$, meaning we will be left with a basis of 3 polynomials.

Do you have any ideas how we might find that 3rd polynomial?
 
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...

Similar threads

  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 39 ·
2
Replies
39
Views
4K
  • · Replies 2 ·
Replies
2
Views
2K
Replies
2
Views
2K
  • · Replies 3 ·
Replies
3
Views
1K
Replies
27
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 6 ·
Replies
6
Views
1K
Replies
8
Views
2K
  • · Replies 12 ·
Replies
12
Views
2K