MHB 311.1.5.17 geometric description

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The solution set of the given system of equations is geometrically described as the single point at the origin (0,0,0). The reduced row echelon form indicates that the system has a unique solution, confirming that it is a "one to one" transformation. The determinant of the associated matrix is non-zero, further supporting the conclusion of a unique solution. Therefore, the only vector mapped to the zero vector is the zero vector itself. This establishes that the geometric description of the solution set is simply the point at the origin.
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$\tiny{311.1.5.17}$
Give a geometric description of the solution set.

$\begin{array}{rrrrr}
-2x_1&+2x_2&+4x_3&=0\\
-4x_1&-4x_2&-8x_3&=0\\
&-3x_2&-3x_3&=0
\end{array}$
this can be written as
$\left[\begin{array}{rrr|rr}-2&2&4&0\\-4&-4&-8&0\\&-3&-3&0\end{array}\right]$

$\text{RREF}=\left[ \begin{array}{ccc|c} 1 & 0 & 0 & 0 \\ 0 & 1 & 0 & 0 \\ 0 & 0 & 1 & 0 \end{array} \right]$
ok I am not sure how you get a geometric description with everything going to zero
 
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the point (0,0,0)
 
Equivalently the matrix [math]\begin{bmatrix}-2 & 2 & 4 \\ -4 & -4 & 8 \\ 0 & -3 & -3\end{bmatrix}[/math] has determinant [math]\left|\begin{array}{ccc}-2 & 2 & 4 \\ -4 & -4 & 8 \\ 0 & -3 & -3 \end{array}\right|= 3\left|\begin{array}{cc}-2 & 4 \\ -4 & 8\end{array}\right|- 3\left|\begin{array}{cc}-2 & 2 \\ -4 & -4\end{array}\right|= 3(-16+ 16)- 3(8+ 8)= -3(16)= -48 [/math] which is not 0 so is a "one to one" transformation. The only vector that is mapped to the 0 vector is the 0 vector itself.
 
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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