Graduate The product of a matrix exponential and a vector

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The discussion centers on the application of matrix exponentials in the context of the Glashow-Weinberg-Salam theory. Participants clarify how the exponential of a diagonal matrix results in a diagonal matrix with the exponentials of the diagonal elements. The exponential of a matrix can be computed using a series expansion, but practical algorithms often utilize eigenvalues for efficiency. It is noted that the transformation of the matrix into a diagonal form can simplify calculations. Understanding these concepts is crucial for correctly applying matrix exponentials to vectors in theoretical physics.
Aleolomorfo
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Hello everybody!
I was studying the Glashow-Weinberg-Salam theory and I have found this relation:
$$e^{\frac{i\beta}{2}}\,e^{\frac{i\alpha_3}{2} \begin{pmatrix} 1 & 0 \\ 0 & -1 \\ \end{pmatrix}}\, \frac{1}{\sqrt{2}}\begin{pmatrix} 0\\ v \\ \end{pmatrix} = e^{\frac{i\beta}{2}}\,e^{-\frac{i\alpha_3}{2}}\, \frac{1}{\sqrt{2}}\begin{pmatrix} 0\\ v \\ \end{pmatrix}$$
I do not know how the exponential matrix acts on the vector.
Thanks in advance!
 
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The exponential of a diagonal matrix is diagonal matrix containing the exponential of the diagonal elements:
$$
\exp \left[ \begin{pmatrix} d_1 & 0 & 0 \\ 0 & d_2 & 0 \\ 0 & 0 & d_3 \end{pmatrix} \right] = \begin{pmatrix} e^{d_1} & 0 & 0 \\ 0 & e^{d_2} & 0 \\ 0 & 0 & e^{d_3} \end{pmatrix}
$$
which can easily be shown using the series expansion of the exponential.

I guess that the right-hand side of the equation you wrote only has ##v##, not the original vector.
 
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More here: https://en.wikipedia.org/wiki/Matrix_exponential
But you got what you need from DrClaude.
The easy way is to transform the matrix into a diagonal with eigen vectors and such. Do the exponent thing above and, if you want, transform it back.
 
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Aleolomorfo said:
Hello everybody!
I was studying the Glashow-Weinberg-Salam theory and I have found this relation:
$$e^{\frac{i\beta}{2}}\,e^{\frac{i\alpha_3}{2} \begin{pmatrix} 1 & 0 \\ 0 & -1 \\ \end{pmatrix}}\, \frac{1}{\sqrt{2}}\begin{pmatrix} 0\\ v \\ \end{pmatrix} = e^{\frac{i\beta}{2}}\,e^{-\frac{i\alpha_3}{2}}\, \frac{1}{\sqrt{2}}\begin{pmatrix} 0\\ v \\ \end{pmatrix}$$
I do not know how the exponential matrix acts on the vector.
Thanks in advance!

The exponential of an ##m \times m## matrix is another ##m \times m## matrix:
$$e^A \equiv I + A + \frac{1}{2!} A^2 + \frac{1}{3!} A^3 + \cdots + \frac{1}{n!} A^n + \cdots,$$ where ##I## is the identity matrix. This series converges for any finite matrix ##A##.

The series is usually avoided when we actually want to compute ##e^A##. Instead, there are several quite good algorithms available to do the computation, mostly based on the use of eigenvalues.
 
Ray Vickson said:
The exponential of an ##m \times m## matrix is another ##m \times m## matrix:
$$e^A \equiv I + A + \frac{1}{2!} A^2 + \frac{1}{3!} A^3 + \cdots + \frac{1}{n!} A^n + \cdots,$$ where ##I## is the identity matrix. This series converges for any finite matrix ##A##.

The series is usually avoided when we actually want to compute ##e^A##. Instead, there are several quite good algorithms available to do the computation, mostly based on the use of eigenvalues.
And one can use the characteristic polynomial of the matrix to convert the infinite series to a finite-order 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...

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