This one may seem a bit long but essentially the problem reduces to some matrix calculations. You may skip the background if you're familiar with Lorentz representations.(adsbygoogle = window.adsbygoogle || []).push({});

1. The problem statement, all variables and given/known data

A Lorentz transformation can be represented by the matrix ##M(\Lambda)=exp(\frac{i}{2}\omega_{\mu\nu}J^{\mu\nu})##, where ##J^{\mu\nu}## are the 6 Lorentz generators which satisfy the Lorentz commutator algebra. From these generators we can express both boosts ##K^i=J^{0i}## and rotations ##J^i=\epsilon^{ijk}J^{jk}/2## (here ##i,j=1,2,3##, while ##\mu,\nu=1,2,3,4##).

In particular, we can form two independent linear combinations:

$$\vec{J_I}=\frac{1}{2}(\vec{J}+i\vec{K}) \ \ \ \vec{J_D}=\frac{1}{2}(\vec{J}-i\vec{K})$$

Which satisfy the SU(2) algebra (i.e. ##[J^i_{I,D},J^j_{I,D}]=i\epsilon^{ijk}J^k_{I,D}/2##), and even commute between themselves.

This is extremedly useful as we can build any Lorentz representation by knowing how to represent SU(2) only. We know this from QM courses, that is, we can build the SU(2) matrices ##\vec{J}^{[j]}## of dimension ##(2j+1)## by giving their spin 0,1/2,1,etc. (i.e, for j=0, ##\vec{J}^{[0]}=1##; for j=1/2, ##\vec{J}^{[1/2]}=\vec{\sigma}/2##; and so on).

From above, we see we can express then the rotation generators as ##\vec{J}=\vec{J_I}+\vec{J_D}##. However, for ##\vec{J_I}## and ##\vec{J_D}## we can have different spins ##j_I## and ##j_D##, in general ##j_I\neq j_D##, so both matrices will have a different dimensions. We can fix this by taking "reducible" representations where the ##\vec{J_I}## have the irreducible blocks ##\vec{J}^{[j_I]}## repeated ##(2j_D+1)## times on its diagonal; similarly for ##\vec{J^{D}}##. Now both matrices of have dimension ##(2j_I+1)(2j_D+1)## and can be written, with ##l=(l_I,l_D)##, as:

$$(\vec{J_I}_{l'l})=\vec{J}^{[j_I]}_{l'_Il_I}\delta_{l'_Dl_D} \ \ \ (\vec{J_D}_{l'l})=\vec{J}^{[j_D]}_{l'_Dl_D}\delta_{l'_Il_I}$$

Therefore, the rotation generators are ##\vec{J}=\vec{J_I}+\vec{J_D}##, so the Lorentz representation ##(j_I,j_D)## of dimension ##(2j_I+1)(2j_D+1)## can be in general reduced with respect to the subgroup of rotations, and includes the total spins ##|j_I-j_D|,...,j_I+j_D## obtained by combining spins ##j_I## and ##j_D##.

Now, after doing all this separation, we can now rebuild the ##M(\Lambda)## Lorentz transformation in terms of ##J_I## and ##J_D## (it's more convenient to write ##\Lambda=exp[i\vec{\theta}\cdot\vec{J}+i\vec{\alpha}\cdot\vec{K}]##).

Question: Show that ##M(\Lambda)## decomposes into a product:

$$M^{l'l}=M^I_{l'_Il_I}M^D_{l'_Dl_D}$$

(I include the next one just for context, as this raises some problems with my results as I'll show later)

After finding the above expresions for the matrices, consider the following:

The vectors ##\phi## on which the matrices ##M## act have components ##\phi_l=\phi(l_I,l_D)##, so they can be thought as rectangular matrices ##(2j_I+1)x(2j_D+1)##. Show that these "vectors" transform as ##\phi\rightarrow M^I\phi (M^D)^T##.

2. Relevant equations

$$\vec{J_I}=\frac{1}{2}(\vec{J}+i\vec{K}) \ \ \ \vec{J_D}=\frac{1}{2}(\vec{J}-i\vec{K})$$

$$(\vec{J_I}_{l'l})=\vec{J}^{[j_I]}_{l'_Il_I}\delta_{l'_Dl_D} \ \ \ (\vec{J_D}_{l'l})=\vec{J}^{[j_D]}_{l'_Dl_D}\delta_{l'_Il_I}$$

$$\vec{J}=\vec{J_I}+\vec{J_D}$$

$$\vec{K}=i(\vec{J_I}-\vec{J_D})$$

$$e^{AB}=e^Ae^B \ \ \ \ , \ \ \ \ if \ \ \ \ \ [A,B]=0$$

3. The attempt at a solution

Let's now focus on the main question, since the second problem is trivial.

I began by replacing ##\vec{J}=\vec{J_I}+\vec{J_D}## and ##\vec{K}=i(\vec{J_I}-\vec{J_D})## to separate the exponential into two parts:

$$M(\Lambda)=exp[i\vec{\theta}\cdot\vec{J}+i\vec{\alpha}\cdot{K}]=exp[\vec{J_I}\cdot(i\vec{\theta}-\vec{a})+\vec{J_D}\cdot(i\vec{\theta}+\vec{a})]$$

Since by definition ##J_I## and ##J_D## commute, we can indeed separate them (by the BCH theorem):

$$M(\Lambda)=exp[\vec{J_I}\cdot(i\vec{\theta}-\vec{a})]exp[\vec{J_D}\cdot(i\vec{\theta}+\vec{a})]$$

Substituting the definitions of ##J_I## and ##J_D## in terms of ##J^{[j_I]}## and ##J^{[j_D]}##, we get:

$$M(\Lambda)=exp[\vec{J}^{[j_I]}_{l'_Il_I}\delta_{l'_Dl_D}\cdot(i\vec{\theta}-\vec{a})]exp[\vec{J}^{[j_D]}_{l'_Dl_D}\delta_{l'_Il_I}\cdot(i\vec{\theta}+\vec{a})]$$

And defining:

$$M^I_{l'_Il_I}=exp[\vec{J}^{[j_I]}_{l'_Il_I}\delta_{l'_Dl_D}\cdot(i\vec{\theta}-\vec{a})] \ \ \ \ ; \ \ \ \ M^I_{l'_Dl_D}=exp[\vec{J}^{[j_D]}_{l'_Dl_D}\delta_{l'_Il_I}\cdot(i\vec{\theta}+\vec{a})]$$

It seems the problem is complete, and both ##M^I_{l'_Il_I}## and ##M^I_{l'_Dl_D}## are square matrices of dimension ##(2j_I+1)(2j_D+1)##.

However, at a later exercise where I use this matrices, for it to be solvable, I must need that ##M^I_{l'_Il_I}## and ##M^I_{l'_Dl_D}## be instead of dimensions ##(2j_I+1)## and ##(2j_D+1)## respectively! So either my definitions are incorrect and the matrices have the wrong dimensions, or the other exercise is wrong (or I'm interpreting it incorrectly).

In other words, Since I calculated that ##M^I## is a square matrix of size ##(2j_I+1)(2j_D+1)## and ##\phi## is a rectangular matrix of size ##(2j_I+1)x(2j_D+1)## we can't even multiply the first product ##M^I \phi## as the matrix sizes don't even match up.

Do you have any idea, or know if I can find a similar development in another source (I've looked everywhere but only the Weinberg has a brief page with information and only definitions). I appreciate any suggestions.

*Reference: S. Weinberg (1995), The Theory of Quantum Fields Vol. I, p. 229*

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# General Irreducible Representation of Lorentz Group

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