quantum mechanics

The Method

14 Aug 2010
Posted by doug

Here is the method:

  1. Ignore all factors of 'i' since quaternions come with i, j, and k pre-installed.
  2. Group 4-vectors together. Examples:
    • (c t, R)
    • (E, P c)
    • (d/dt, c d/dR)
  3. Keep all constants as a check: c, h, G
  4. If possible, make dimensionless
  5. Treat the wave function as quaternion-valued (3 complex numbers that share the same real)
Posted by doug
summary: 

Each and every photon is identical to every other, but by coloring in those where t = 0, we can cheat and see the phase.

description: 

Part of the great mystery of quantum mechanics is that all particles are identical. There is no adding a tag or painting one red while the rest are yellow. As a programmer, we can cheat, do something not allowed in Nature, and mark all those where t = 0 in red. The shift is the same as before, but now we can spot its trail.

What is so tricky in quantum mechanics is not the vectors - those we can always point at with our fingers. Instead it is the scalars that provide the challenge, the unpointables. Each scalar is connected to three vectors to make 3 complex numbers, but the scalar can be shared by other events. The scalar become the thread within a pattern of events, and between separate patterns of events. It is wonderfully ironic that the simplest core component can be so confusing by playing many roles.

command: 
q_graph -out amp_shifted_marked -dir int14 -box 1.6 -command 't_function -t_func cos -x_func sin -y_func zero -z_func zero -n_steps 0 -pi 10 -n_t_cycles 1000 -n_t_step 0.0314 1 1 0 0 | q_add 0 0 -1.5 -.1 | q_add_n_m 0 0 0.003 0 1 1000' -color red -command 't_function -t_func cos -x_func sin -y_func zero -z_func zero -n_steps 1000 -pi 10 -n_t_cycles 1000 -n_t_step 0.0314 1 1 0 0 | q_add 0 0 -1.5 0 | q_add_n_m 0 0 0.003 0 1000 1000' -color yellow
math
equation: 

\phi = (cos(\omega t + \delta), sin(\omega t + \delta), k ~ \delta, 0) \, \textrm{with} \, \delta: 0 \to 10 \pi
\textrm{red} = (cos(\delta), sin(\delta), k ~ \delta, 0) \, \textrm{with} \, \delta: 0 \to 10 \pi

tags
Physics Tag: 
quantum mechanics
wave function
wave equation
phase
Math Tag: 
sine
cosine
Programming Tag: 
command line quaternions
t_function
q_add
q_add_n_m
Posted by doug
summary: 

A phase shift is added to a wave function, but you cannot tell due to the periodic boundary condition.

description: 

A change in the phase was included. Each event above another event has a different starting time due to the phase shift, but given enough time, all the same locations in spacetime are experienced, so the pattern looks the same.

command: 
q_graph -out amp_shifted -dir int14 -box 1.6 -command 't_function -t_func cos -x_func sin -y_func zero -z_func zero -n_steps 1000 -pi 10 -n_t_cycles 1000 -n_t_step 0.0314 1 1 0 0 | q_add 0 0 -1.5 0 | q_add_n_m 0 0 0.003 0 1000 1000' -color yellow
math
equation: 

\phi = (cos(\omega t + \delta), sin(\omega t + \delta), k \delta, 0) \, \textrm{with} \, \delta: 0 \to 10 \pi

tags
Physics Tag: 
quantum mechanics
wave function
wave equation
Programming Tag: 
command line quaternions
t_function
q_add
q_add_n_m

Quantum Mechanics

16 Apr 2009
Posted by doug

The 2 images on the right hand side of these animations may be a way to visually represent quantum mechanics. The wave function is the superposition of all possible states a system governed by a complex-valued wave function can be in. The story is complete, even if uncertain due to the complex numbers which are not a totally ordered set. The upper right image is literally a superposition of every frame that appears in the animation that is front and center. Below all that is possible is a random sampling of those what is possible.

Posted by doug

The paper "Experimental realization of Wheeler's delayed-choice GadenkenExperiment" by Jacques et al. quant-ph/0610241v1 was recommended to me. I reads like a seminal paper on the topic, the one where the experimentalists "go it right". Here is the first three lines of their abstract:

Posted by doug
Tags:
Posted by doug
Tags: