The quantum photon represents a fundamental quantum mystery because although a quantum photon is a particle of light, all quantum particles also have the properties of bound waves called wavepackets. Of course, since all quantum particles have this particle-wave duality, the mystery of quantum photons is actually rather the basis of our quantum reality and so not really a mystery at all. The mystery is why the classical reality that we experience shows mostly particles and only shows the bound waves of photons in rainbows and edge and slit diffraction.

Planck in 1901 first proposed the notion of a quantum of light to limit the energy of light of an atom but it was Einstein in 1905 who made the connection between the Planck quantum and photons of light. Einstein connected Planck's quanta of light from measurements of the photoelectric effect, where illumination of a vacuum diode resulted in the detection of single electrons emitted by single photons when the light frequency exceeded a certain threshold. It was somewhat later in 1926 that G.N. Lewis coined the name photon.

The propagation of a photon wavepacket from an emitter through space to an absorber along with its spectrum defines the nature of each photon. Although each photon has a characteristic energy and mass from its frequency as *E = hn*, *m = hn/c ^{2}*, the quantum phase of the photon spectrum also reflects the nature of each matter action emitter and absorber as well as their lifetimes. The emitter-absorber resonance gives a photon its matter and phase spectrum and a matter-action of that excited resonance can spontaneously decay into heat at either the absorber or emitter. However, by definition, the absorber decays to heat faster than the emitter and this is what gives the arrow of time.

The emitter-absorber excited state is really emitter-absorber matter action that defines the photon spectrum and includes any in-between phase shifts due to things like slits and so each photon spectrum is rather unique.

There is no space or time in the two slit quantum causal set, just the mass of 254 nm mercury photon, Planck's action constant, and the quantum phase angle, q. All of the resonant single photon causal vertices are reversible and so split the single photon events 50:50 between the emitter and absorber decays. Each photon has a vertex that includes both slits, which alters the phase of the photon, but not its frequency, energy, or mass.

Gorard has built a hypergraph for the two slit function by propagating 23 bits from the sequence of "o"'s with two “X” amplitudes

oooooooooXoooXooooooooo

down a 10 layer hypergraph to create 75 events for the causal graph below.

However, this is just a classical wave diffraction pattern with a splitting of 16 units and results from two coherent sources or slits spaced 4 units apart with a light wavelength of 4 units and a slit width of 1 unit.

Since this hypergraph is determinate and not probabilistic, it simply represents a classical wave diffraction pattern of two point sources. In other words, this is not a quantum two slit multiway hypergraph since it does not represent any emitter-absorber quantum phase resonances at all.

Each photon event is a quantum resonance path of the hypergraph when the emitter and absorber are in resonance. The figure above shows two possible paths hypergraph paths in red.The resonance therefore is a superposition between the emitter and absorber and occurs because of a quantum phase resonance between the emitter and absorber. The quantum phase resonance also depends on any phase shifts of intervening causal layers like the collimator and two slits, but the emitter and absorber quantum phases are essentially random.

Therefore, the results of these multiway hypergraph layers are simply spatial smoothing functions for the classical two emitter diffraction and has no collimator. Random excitations of graph resonances can occur when the emitters and absorbers are in phase and those result in a photon states that then decay irreversibly. The states release heat to either the absorber or emitter depending on relative decay times to transit times. When a photon decay occurs in the absorber, we call that a photon event and all of the other emitter photons decay in the emitter.

Randomly exciting 1,000 quantum resonances of the two-slit hypergraph will generate the accumulation of single quantum photon results noted above for this case. However, it is a lot easier just to use the two-slit analytic expression in the first place.

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