The grand unified theory of classical quantum mechanics

Stationary inverted Lyman populations and free-free and bound-free emission of lower-energy state hydride ion formed by an exothermic catalytic reaction of atomic hydrogen and certain group I catalysts

“…This is consistent with the previously given theory [12], the reported series of lower-energy hydrogen emission with energies of q · 13.6 eV 1 , the reported energy states of hydrino products 1 [3-25, 25, 26, 26, 27, 27, 28, 28-35], and previous studies which show very large energy balances [25, 27-29, 31, 32, 37].…”

“…(2.69) of Ref. [12] and the required quantization of flux in integer units of the magnetic flux quantum during binding, the corresponding emission is at a longer wavelength having an energy equal to the binding energy minus an integer times the fine structure energy [12,39]. Since the hydride ion has a vanishing emission cross section in the region of its binding energy [56], but the fine structure transition has a significant cross section, the coupling of the electron binding to the fine structure transition and hyperfine structure levels within the fine structure may greatly increase the emission at this energy.…”

“…The catalyst product H(1/2) was predicted to be a highly reactive intermediate that further reacts to form a novel hydride ion H − (1/2) with a predicted binding energy of 3.0471 eV given by the following formula [12,25,39] for the hydride binding energies E B :…”

“…Due to the requirement that flux is linked by the hydrogen or H(1/ ) in integer units of the magnetic flux quantum, the energy is quantized, and the emission due to hydride ion formation comprises a series of hyperfine lines in the corresponding bound-free band. The derivation of the bound-free hyperfine lines due to interactions of the free and bound electrons was given previously [12,39]. From the electron factor, bound-free hyperfine structure lines of H − (1/2) were predicted with energies E HF given by the sum of the observed binding energy peak E * B , the spin-spin energy E , and the fluxon energy E Φ : + 3.0583 eV with the unperturbed E B given by Eqs.…”

“…≈ 10 3 K) and an extraordinary low field strength of about 1-2 V/cm from atomic hydrogen and certain atomized elements or certain gaseous ions which singly or multiply ionize at integer multiples of the potential energy of atomic hydrogen, 27.2 eV. The theory given previously [12][13][14][15][16][17][18][19][20][21][22] …”