Light Waves Are Not Field Waves
In this paper, http://milesmathis.com/photon2.html, Mathis says: "Since the wave of light belongs to each photon, via spin, the wave is neither longitudinal nor transverse. Longitudinal and transverse waves are defined as field waves, and light is not a field wave. Light is a spin wave, and the spin is neither transverse nor longitudinal."Gary said: [LK: Or they may shine by glow mode discharge.]
Closer, but the conventional model of rays of light doesn't work here either. A glow in the visible range again would fall off very quickly. With all recent instruments, they are looking for the spectra of the elements, and the strongest 'light' will be the Lyman Alpha hydrogen line, but this is in the UV, and we could not see it by eye. So what makes 'stars' visible in our night sky, or the dust and debris of the Milky Way visible, when the only emissions robust enough for us to 'see' are in the UV?
He says the photon is spinning and it can resemble either a transverse or longitudinal wave, depending, I think, on the direction of spin with respect to the forward or translational motion. Apparently, the mass of the photon is at a point on the spherical surface, so, as the photon advances, the mass moves both circularly and linearly, resulting in a stretched wave or corkscrew motion. I have a somewhat different model, but I haven't checked mine against many known facts, so I don't know if mine could explain such wave motions.
Why Photons Express Different Wavelengths
I recommend reading that paper. It's not real long. I guess it would help to quote some more of it.
I'm not clear on whether he suggests that photons can lose or gain "spin stacks" (and thus change "wavelength") in flight, or when encountering an atmosphere or a magnetic or electric field, but it seems possible. We should probably ask him, in the event that he may think it's worth a little time to answer. I decided to do a little more searching first though. And the following from http://milesmathis.com/photon3.pdf may be relevant.- But now we must move on to ask why and how photons express different wavelengths. Electromagnetic radiation, in the form of photons, comes in a wide range of wavelengths, as we know. How is this achieved? It is achieved by a wide variation of stacked spins. As I began to show in a previous paper, it turns out that photons can maintain a linear velocity very near c over a wide range of sizes. The photon does not reach a size limit that causes slowing until it approaches the spin radius just beneath the electron. At that limit, the largest photons begin absorbing the smallest photons, and the mass increase snowballs. This turns the nearly massless photon into the small-mass electron.
- The most common photons appear at the size range of 18213 less than the proton mass and size. This is where we find the infrared photons, as I showed previously. But the small mass of the photon allows it to stack spins over a wide range of radii. In this, it is unlike the electron or proton. The proton cannot add extra spins above the z-spin without creating instability. This is why “mesons” over the baryon size are not stable. The extra spins begin interfering with the energy of the inner spins. But with the photon this appears not to be the case. Extra spin levels do not cause appreciable slowing, nor do they cause appreciable instability. We may theorize that smaller photons would be more stable, but the difference in small photons and large ones is not easily measured from our level.
- What this means, specifically, is that if we give the infrared photon a z-spin as its outer spin, we can find a smaller photon whose outer spin is the y-spin. We can also find a larger photon with another axial or x-spin on top of the infrared’s z-spin. In this way, we find not only stacked spins, we find stacked levels. In other words, we find spins of a1, x1, y1, z1 and a2, x2, y2, z2 and a3, x3, y3, z3 and so on. By this analysis, a2 has twice the spin radius of z1. In fact, each spin has twice the radius of the spin under it.
- This means that photons do not come in a continuous spectrum. No, they come in stepped levels, each level double the one under it.
So, if the photon mass changes depending on the photon density around the photon, would that help solve the problem of light from objects in space reaching Earth? If mass changes, I suppose that means energy changes, and does that mean wavelength changes too? (By the way, toward the end of that paper he shows that the photon density [in Earth' lower atmosphere, I think] is about 56 million photons per cubic meter.)according to my theory and equations, there should be no universal charge density [= photon density]. Charge should be denser in galaxies than out of them, and denser near stars, and so on. By this analysis, it seems that the velocity of the photon would change in different densities. Because this appears not to be so, I assume that the mass of the photon may change depending on the charge density around it. Remember that mass is a function of energy according to the old equation Eγ = mγc2, which means that the photon's mass is already a function of the charge density. As the charge density grows, so will m. So that variable m already includes the charge density, in a way. This feedback mechanism may be what keeps c constant.