Solving Tricky Pauli Matrices with Einstein Notation

emma83
Messages
31
Reaction score
0
Hello,
I am trying to recover the following calculation (where K,A are 4x4 matrices in SL(2,C)):

--(start)--
"We expand K'=AKA^{\dagger} in terms of k^a and k'^{a}=(\delta_a^{b} + \lambda_a^{b} d\tau)k^b. Multiplying by a general Pauli matrix and using the relation \frac{1}{2}tr(\sigma_{a}\sigma_{b})=\delta_{ab} yields the expression:
<br /> \lambda_b^{a} = \frac{1}{2}\eta^{ac}tr(\sigma_{b}\sigma_{c}A+\sigma_{c}\sigma_{b}A^{\dagger})<br />."
--(end)--

I have been playing with the relations for a while but I guess I miss some knowledge on the properties of Pauli matrices because I don't manage to find the result. In particular, what would the "expansion" of AKA^{\dagger} (which I guess is necessary here?) look like in Einstein summation notation ? Any help would be extremely appreciated!
 
Physics news on Phys.org
the answer lies on wikipedia.
 
ryuunoseika said:
the answer lies on wikipedia.

Well, give a link, then :rolleyes:which article? :smile:
 
Well I had of course already checked beforehand the wikipedia page on Pauli matrices (http://en.wikipedia.org/wiki/Pauli_matrices) but had not found a relation to solve this problem... So Ryuunoseika, which article are you talking about ?
 
Something here seems either not quite right or incomplete.

If k&#039;^{a} = \left(\delta_b^{a} + \lambda_b^{a} d\tau \right) k^b (careful with index placement) and d \tau is infinitesimal (?), then k&#039; and k differ by an infinitesimal amount, so the transformation is an infinitesimal version of K&#039;=AKA^{\dagger}. Then, the sum in final result could come from the product rule.

I'm just guessing. More context is needed.
 
Dear George,

Thanks a lot for your answer. First, yes sorry I misplaced the indices in the first relation, the correct relation is:
k&#039;_{a}=(\delta_a^{b} + \lambda_a^{b} d\tau)k_b

Concerning d\tau, it is actually a \delta u, where u is the affine parameter along the trajectory of a photon.

But what do you mean by "product rule" ? Do I have to develop explicitely AKA^{\dagger} in indices notation and try to recover at the end the A and A^{\dagger} which appear in the trace ?
 
In this video I can see a person walking around lines of curvature on a sphere with an arrow strapped to his waist. His task is to keep the arrow pointed in the same direction How does he do this ? Does he use a reference point like the stars? (that only move very slowly) If that is how he keeps the arrow pointing in the same direction, is that equivalent to saying that he orients the arrow wrt the 3d space that the sphere is embedded in? So ,although one refers to intrinsic curvature...
ASSUMPTIONS 1. Two identical clocks A and B in the same inertial frame are stationary relative to each other a fixed distance L apart. Time passes at the same rate for both. 2. Both clocks are able to send/receive light signals and to write/read the send/receive times into signals. 3. The speed of light is anisotropic. METHOD 1. At time t[A1] and time t[B1], clock A sends a light signal to clock B. The clock B time is unknown to A. 2. Clock B receives the signal from A at time t[B2] and...
So, to calculate a proper time of a worldline in SR using an inertial frame is quite easy. But I struggled a bit using a "rotating frame metric" and now I'm not sure whether I'll do it right. Couls someone point me in the right direction? "What have you tried?" Well, trying to help truly absolute layppl with some variation of a "Circular Twin Paradox" not using an inertial frame of reference for whatevere reason. I thought it would be a bit of a challenge so I made a derivation or...
Back
Top