![](https://assets.website-files.com/6328cdc408ec36f39964df93/632cc8b88f7e56410324e2d8_Image%20background.png)
01.
Jitter
Using the scientific method, we experimented.
![](https://assets.website-files.com/6328cdc408ec36f39964df93/632fa7f44a0d2f37816ffcce_experiment-img.png)
![](https://assets.website-files.com/6328cdc408ec36f39964df93/6331c122c3e8274919b3d0e3_experiment-img-mobile.png)
Experimental results
6 sigma of periodicity explained by the hypothesis
a.
Fourier Transform of magnitude of jitter on atomic clock for the past 2 years.
b.
The spike at one cycle per sidereal day is explained by the hypothesis.
![](https://assets.website-files.com/6328cdc408ec36f39964df93/643ec04fec13e96fe599c33f_Graph-new.png)
![](https://assets.website-files.com/6328cdc408ec36f39964df93/643ec0903a2e422559c65708_spike-new.png)
Data is further supportive of hypothesis
a.
A measurement of the phase reveals when jitter is maximum
By measuring the phase at 1 cycle per sidereal day we find the boarder of the constellation Leo/Crater is on the Easter Horizon when the jitter is at a maximum
b.
A measurement of the magnitude reveals how fast we are moving towards Virgo
$$\text { We find that } v_{z \perp}=0.001 \mathrm{c}$$
c.
This measurement matches the velocity of Earth in the Cosmic Microwave Reference Frame as measured by the Planck Collaboration
![](https://assets.website-files.com/6328cdc408ec36f39964df93/643ebd07a4ebb506dd5dd147_experimeny-img-2.png)
02.
Johnson
Our first experiment is measuring diffusion in time. A second experiment is underway to ratify our hypothesis
Our next experiment is measuring diffusion in space. In this case 2 spikes should be present, one at 1 cycle per sidereal day from the variance in sample timing and one at 2 cycles per sidereal day as the main dimension of the resistor orients itself with the Sun’s velocity. Conclusions should be available soon.
JOHNSON
[Formula]
\begin{align}\text{Signal} &= \text{AC Power}_{s}^{2} + \text{AC Power}_{x}^{2} \notag \\&= k_{B} T B \frac{\lvert v_{e} \rvert}{c} \sqrt{\frac{\hbar}{\mathtt{t}mc^{2}}} cos(2 \pi f_{SR} t - \vartheta )\notag \\&+\frac{\left|v_{z\perp}\right|^{2}}{4c^{2}}\frac{\hbar}{\mathtt{t}^{2}} \cos(2 \pi 2 f_{SR}t - 2 \varsigma +\pi) \notag\end{align}