- #1
Froggeh
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- Homework Statement
- Show that:
$$ \frac{1}{2} \epsilon^{\mu \nu \rho \sigma} M_{\mu \nu} M_{\rho \sigma} = - \mathbf{J} \cdot \mathbf{K}$$
Where ##M_{\mu \nu}## is an antisymmetric tensor constructed as follows: ##M_{0i} = K_{i}## and ##M_{ij} = \epsilon_{ijk}J_{k}##
- Relevant Equations
- ##J_{i}## are the three generators of the Lorentz rotations, and ##K_{i}## are the three generators of the Lorentz boosts (my textbook calls them pure transformations, but my understanding is that they're the same thing).
The ##J## matrices are Hermitian, while the ##K## matrices are symmetric.
Maybe it's also worth mentioning the commutator
$$ [J_i, K_j] = i\epsilon_{ijk}K_k$$
Hello everyone, I am new here, so please let me know if I am doing something wrong regarding the formatting or the way I am asking for help.
I did not really know how to start off, so first I tried to just write out all the ##\mu \nu \rho \sigma## combinations for which ##\epsilon \neq 0## and assign them signs. In essence, I just used Mathematica to find these. However, when I plugged them in, and replaced each corresponding entry of ##M_{\mu \nu}##, I obtained the result ## 2(\mathbf{K} \cdot \mathbf{J} + \mathbf{J} \cdot \mathbf{K})##, which, unless I am missing something crucial, is just plain wrong.
Since each time I attempted this was taking up a large chunk of time, I thought of changing my approach, by fixing one index and seeing what comes out:
Say ##\mu = 0##, then ##\nu \rho \sigma = ijk##, and this leaves us with
$$ \frac{1}{2} \epsilon^{0ijk}M_{0i}M_{jk} = \frac{1}{2} \epsilon^{0ijk}K_{i}\epsilon_{jkl}J_{l} $$
This is where I am unable to move forward with certainty. I am thinking that ##\epsilon^{0ijk} = \epsilon^{ijk} ## because if the first component is zero, then we need only consider permutations of the other three components. This in turn would allow me to easily contract the two ##\epsilon## terms into a simple Kronecker-##\delta##. If I do this, I end up with
$$ \frac{1}{2} \epsilon^{ijk}\epsilon_{jkl}K_{i}J_{l} = \frac{1}{2} \epsilon^{ijk}\epsilon_{ljk}K_{i}J_{l} = \frac{1}{2} 2\delta^{i}_{l} K_{i} J_{l} = K_{l}J_{l}$$
But this seems wrong too, I am missing a negative sign. And my indices seem to be in the wrong positions.
At this point I'm unsure of whether I am on the right track. I suppose I would have to try this for each index ## = 0##, but even then I cannot see the terms combining to give me a negative dot-product.
I did not really know how to start off, so first I tried to just write out all the ##\mu \nu \rho \sigma## combinations for which ##\epsilon \neq 0## and assign them signs. In essence, I just used Mathematica to find these. However, when I plugged them in, and replaced each corresponding entry of ##M_{\mu \nu}##, I obtained the result ## 2(\mathbf{K} \cdot \mathbf{J} + \mathbf{J} \cdot \mathbf{K})##, which, unless I am missing something crucial, is just plain wrong.
Since each time I attempted this was taking up a large chunk of time, I thought of changing my approach, by fixing one index and seeing what comes out:
Say ##\mu = 0##, then ##\nu \rho \sigma = ijk##, and this leaves us with
$$ \frac{1}{2} \epsilon^{0ijk}M_{0i}M_{jk} = \frac{1}{2} \epsilon^{0ijk}K_{i}\epsilon_{jkl}J_{l} $$
This is where I am unable to move forward with certainty. I am thinking that ##\epsilon^{0ijk} = \epsilon^{ijk} ## because if the first component is zero, then we need only consider permutations of the other three components. This in turn would allow me to easily contract the two ##\epsilon## terms into a simple Kronecker-##\delta##. If I do this, I end up with
$$ \frac{1}{2} \epsilon^{ijk}\epsilon_{jkl}K_{i}J_{l} = \frac{1}{2} \epsilon^{ijk}\epsilon_{ljk}K_{i}J_{l} = \frac{1}{2} 2\delta^{i}_{l} K_{i} J_{l} = K_{l}J_{l}$$
But this seems wrong too, I am missing a negative sign. And my indices seem to be in the wrong positions.
At this point I'm unsure of whether I am on the right track. I suppose I would have to try this for each index ## = 0##, but even then I cannot see the terms combining to give me a negative dot-product.
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