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HOW PHOTONS TRAVEL
© Lloyd
  1. http://milesmathis.com/photon2.html (HOW DO PHOTONS TRAVEL?)
  2. From a previous paper, we know that the radius of the B-photon is G times less than the radius of the proton.
  3. This gives us a photon radius of 2.74 x 10^-24m.
  4. The z-spin is 8 times the radius, so we should find a basic wavelength of 2.2 x 10^-23m.
  5. Obviously, we don't find photons with a wavelength that small.
  6. *Why? Simply because the wavelength we measure has been stretched out by the velocity of the photon.
  7. The photon would be measured to have a wavelength of 2.2 x 10^-23m only if it were at rest.
  8. A spin is a motion: a motion that takes time.
  9. Even if the photon were spinning at velocity c, one rotation must take some real time.
  10. We know that the linear velocity of light is not infinite, so we must assume the speed of spin is also not infinite.
  11. If it is not infinite, it must take time.
  12. If it takes time, then it will be stretched by the linear motion.
  13. While the surface of the photon is spinning, the photon as a whole is moving some linear distance x.
  14. So how much does the velocity stretch out the wavelength?
  15. We can discover that most easily by using this simple equation: E = mc^2 = hc/?; ? = h/mc
  16. The mass equivalence of the infrared photon is 2.77 x 10^-37 kg, so we just solve: ? = h/mc = 8 x 10^-6m
  17. If we compare that to the wavelength at rest, we find the wavelength has been stretched out by a factor of about 3.63 x 10^15.
  18. Since that is very nearly c^2, we assume that the transform is in fact c^2, and that the difference is a difference between the size of the B-photon and of the infrared photon.
  19. Remember that we developed the at-rest wavelength from the B-photon and the moving wavelength from the infrared photon.
  20. Our assumption is borne out by the numbers, since if we divide 8 x 10^-6 m by c^2, we get 8.9 x 10^-23 m, which is almost exactly 4 times our B-photon wavelength.
  21. We may assume that the infrared photon is about 4 times larger than our B-photon.
  22. The most common photons appear at the size range of 1821^3 less than the proton mass and size.
  23. But the small mass of the photon allows it to stack spins over a wide range of radii.
  24. In this, it is unlike the electron or proton.
  25. The proton cannot add extra spins above the z-spin without creating instability.
  26. *This is why "mesons" over the baryon size are not stable.
  27. The extra spins begin interfering with the energy of the inner spins.
  28. But with the photon this appears not to be the case.
  29. Extra spin levels do not cause appreciable slowing, nor do they cause appreciable instability.
  30. *In other words, we find spins of a1, x1, y1, z1 and a2, x2, y2, z2 and a3, x3, y3, z3 and so on.
  31. >>>LK: How can there be a2, a3 etc?
  32. In fact, each spin has twice the radius of the spin under it.
  33. This means that photons do not come in a continuous spectrum.
  34. You will remember that number comes from (c^2) 8.8 x 10^-23 m.
  35. If we want the next photon larger than that, we double the spin radius to 1.76 x 10^-22 m and multiply by c^2, which gives us 1.6 x 10^-5 m.
  36. If we measure light with an average wavelength in between those numbers, we must have a mixture of photons.


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