gauge symmetry

Posted by doug
QMN:1009.9466
Douglas Sweetser
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latex pdf: 
Mathematica Notebook: 
abstract: 

The Maxwell action of electromagnetism is represented using the noncommutative division algebra of quaternions. The potential in the electromagnetic action is then rewritten with the weak force gauge symmetry SU(2), also known as the unit quaternions. The potential can be recast again with electroweak symmetry as the product of U(1) and SU(2) symmetries. The conjugate of one electroweak symmetry times another for the potential in the action is enough to account for the strong force symmetry SU(3). A 4D commutative division algebra is constructed from the hypercomplex numbers modulo eigenvalues equal to zero. The action is rewritten again with the hypercomplex multiplication rules in a gauge invariant way. Like charges attract for the hypercomplex action based on an analysis of spin of the field strength density, the spin in the phase of the current coupling term, and the field equations that result by applying the Euler-Lagrange equation. The first field equation of the hypercomplex action contains Newton's law of gravity paired with a time-dependent term and thus is consistent with special relativity. There is also an Ampere-like equation so that a 4-potential theory can account for bending of both time and space caused by gravity. It is shown how the Rosen metric is a solution to the field equations, and thus passes weak field tests of gravity to first-order parametrized post-Newtonian (PPN) accuracy. The proposal is distinguishable from general relativity at second-order PPN accuracy, predicting for example 0.7 microarcseconds more bending of light around the Sun than the Schwarzschild metric. The lowest mode of wave emission for this simple field theory is a quadrupole. The final rewrite of the action has gauge-dependent electromagnetic and gravity field strength densities where the two gauges cancel out, leaving a gauge-independent unified action. Since the Higgs mechanism is unnecessary for this unified standard model proposal, it is predicted no Higgs boson will be found.

0. Author's note
1. Introduction
2. The Maxwell Lagrangian Using Quaternions
3. The Lagrangian Using Hypercomplex Numbers
4. Hypercomplex Field Equation Solutions
5. The Lagrangian Using Quaternions and Hypercomplex Numbers
6. Quantization
7. A New Implementation
8. Mathematical fields, quaternions and hypercomplex numbers
9. Standard model groups, tensors and quaternions
10. References

Document Description
# of pages: 
18
# of figures: 
2
Change Log: 
Nov 23, 2010. Added Epstein and Shapiro reference for 2nd order bending of light by the Sun. April 13, 2011. Switched from actions to Lagrangians to reflect what is done with Mathematica. Added scalar operators on Lagrangians.
Tags
Physics Tag: 
gauge symmetry
unified field theory
gravity
Math Tag: 
quaternions
hypercomplex numbers
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 SU(3) is created by taking the Euclidean product of two electroweak symmetries. Nature may need less tools than the standard model suggests.

description: 

This groups is the completely uniform unit quaternion sphere, starting from t=-1, expanding to its maximal size at t=0, then contracting to t=+1. For an observer is now at the center of their private Universe - (0, 0, 0, 0) - when they see an event, no matter what the cause, the event can be scaled to fit on this sphere. The norm of any event in the unit sphere is exactly 1, even if with rulers and atomic clocks a big or small sized measurement could be made.

<p>Because the symmetries U(1), SU(2) and U(1)xSU(2) are formally subgroups of SU(3), there is no need for a larger group to unify these groups. A rather large effort is still required to connect to all we know of the standard model.

command: 
q_graph -dir vp -out group_su3 -loop 0 -box 1.1 -command q_group -group U1xSU2xSU3 -n 50000
youtube embed: 
math
equation: 

(\frac{A}{|A|} exp(A - A^*))^* \frac{B}{|B|} exp(B - B^*) \in SU(3)

tags
Physics Tag: 
standard model
gauge symmetry
Math Tag: 
groups
Programming Tag: 
command line quaternions
q_group
g_su3
Tags:
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
Posted by doug
summary: 

The group for the unit circle in a complex plane, U(1), can be at an arbitrary angle in 3D space. The transverse waves of EM have this symmetry.

description: 

If one picks a quaternion at random, normalize it, then take n powers of that number, one ends up with this animation. It looks like tilted circles in the complex planes. The motion is fasted at the creation and annihilation. The velocity of the dots is slowest when the two have their largest separation. This group is symmetric in both time and space reflection. Recall that time reflection requires recall, memories of the path taken, while space reflection involves mirrors.

<p>On pleasing aspect of this animation is that it starts to make sense of a transverse wave. Mapping that wave to electric or magnetic fields will require considerably more work.

command: 
q_graph -dir vp -out group_u1 -loop 0 -box 1.1 -command "g_u1 1 2 3 4 1000"
youtube embed: 
math
equation: 

\frac{A}{|A|} \in U(1)

tags
Physics Tag: 
standard model
electromagnetism
gauge symmetry
U(1)
Math Tag: 
groups
U(1)
Programming Tag: 
command line quaternions
g_u1