SU(2)

Posted by doug
summary: 

The group U(1)xSU(2) can be represented using all four parts of a quaternion, three in the exponential, the fourth as a normalized quaternion. The group covers the entire unit sphere, but has a bias for the past.

description: 

Quaternions do not commute in general, but they will commute if two quaternions point in the same direction. The common way to represent the group U(1) is with a normalized complex number. The same thing can be done with a quaternion. This will commute with a unitary quaternion if they both use the same quaternion pointing in the same direction. Electroweak symmetry uses all the degrees freedom available in a quaternion.

command: 
q_graph -dir vp -out group_u1xsu2 -loop 0 -box 1.1 -command 'q_group -group U1xSU2 -n 20000'
youtube embed: 
math
equation: 

\frac{A}{|A|} exp(A - A^*) \in U(1) \times SU(2)

tags
Physics Tag: 
standard model
electroweak force
gauge symmetry
electromagnetism
weak force
Math Tag: 
groups
U(1)
SU(2)
U(1)xSU(2)
Programming Tag: 
command line quaternions
q_group
q_random_n_11
Posted by doug
summary: 

The group of unitary quaternions is the symmetry underlying the weak force of radioactive decay. Who would have thought the symmetry looks like this?

description: 

If one takes the vector part of a quaternion and takes the exponential, the norm is always equal to 1. The animation starts out at 8 points, those for exp(0, +/-1, +/-1, +/-1). These points grow into each other until they form a sphere. That sphere then shrinks to the point (1, 0, 0, 0), the furthest into the future the exponential can reach.

command: 
q_graph -dir vp -out group_SU2 -loop 0 -box 1.1 -command 'q_random_n_11 50000 | q_vector | q_exp'
youtube embed: 
math
equation: 

exp(A - A^*)\in SU(2)

tags
Physics Tag: 
standard model
gauge symmetry
weak force
Math Tag: 
groups
SU(2)
Programming Tag: 
command line quaternions
g_su2