On the radiation from point charges

Haus, H. A.

doi:10.1119/1.14729

Cited by 34 publications

(21 citation statements)

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“…The central feature of this theory is that all particles (atomic-size and macroscopic particles) obey the same physical laws. Whereas Schrödinger postulated a boundary condition: Ψ → 0 as r → ∞ , the boundary condition in Mills' theory was derived from Maxwell's equations [28] The mathematics for all three theories converge to Eq. (38.66).…”

Section: Classical Solution Of the Schrödinger Equationmentioning

confidence: 99%

“…The condition for radiation by a moving charge is derived from Maxwell's equations [28]. The condition for nonradiation of a moving charge-density function is that the spacetime Fourier transform of the current-density function must not possess waves synchronous with waves traveling at the speed of light, that is synchronous with …”

Section: Backward Peak In the Electron Spectrum From Collisions Of 70mentioning

confidence: 99%

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The hydrogen atom revisited

Mills

2000

International Journal of Hydrogen Energy

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Several myths about quantum mechanics exist due to a loss of awareness of its details since its inception in the beginning of the last century or based on recent experimental evidence. It is taught in textbooks that atomic hydrogen cannot go below the ground state. Atomic hydrogen having an experimental ground state of 13.6 eV can only exist in a vacuum or in isolation, and atomic hydrogen cannot go below this ground state in isolation. However, there is no known composition of matter containing hydrogen in the ground state of 13.6 eV. It is a myth that hydrogen has a theoretical ground state based on first principles. Historically there were many directions in which to proceed to solve a wave equation for hydrogen. The Schrödinger equation gives the observed spontaneously radiative states and the nonradiative energy level of atomic hydrogen. On this basis alone, it is justified despite its inconsistency with physical laws as well as with many experiments. A solution compatible with first principles and having first principles as the basis of quantization was never found. Scattering results required the solution to be interpreted as probability waves that give rise to the uncertainty principle which in turn forms the basis of the wave particle duality. The correspondence principal predicts that quantum predictions must approach classical predictions on a large scale. However, recent data has shown that the Heisenberg uncertainty principle as the basis of the wave particle duality and the correspondence principle taught in textbooks are experimentally incorrect.Recently, a reconsideration of the postulates of quantum mechanics, has given rise to a closed form solution of a Schrödinger-like wave equation based on first principles [1]. Hydrogen at predicted lower energy levels has been identified in previous data. The transition of hydrogen to fractional quantum energy levels is reported by the assignment of soft X-ray emissions from the interstellar medium observed by Labov and Bowyer [2] and by the assignment of the source of 50 eV anomalous thermal broadening of the Balmer lines observed by Kuraica and Konjevic [3] during a glow discharge of hydrogen-argon mixtures which was not observed with neon-hydrogen mixtures or pure hydrogen irrespective of cathode material.Certain inorganic ions predicted by Mills [1] serve as "transition catalysts" which resonantly accept energy from hydrogen atoms and release the energy to the surroundings. Argon ion is a catalyst that was present in the hydrogen glow discharge of Kuraica and Konjevic [3]. Lower-energy hydrogen atoms, hydrinos, can cause an autocatalytic acceleration of this "transition reaction" which is the mechanism corresponding to the interstellar lines. © 2000 by BlackLight Power, Inc. All rights reserved. 561The detection of the transition of atomic hydrogen from the traditional "ground" state (n = 1) to the fractional quantum energy level n = 1/ 2 below the traditional "ground" state-hydrinos-is further reported by the assignment of the anomalous 31 eV ...

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Section: Classical Solution Of the Schrödinger Equationmentioning

confidence: 99%

Section: Backward Peak In the Electron Spectrum From Collisions Of 70mentioning

confidence: 99%

The hydrogen atom revisited

Mills

2000

International Journal of Hydrogen Energy

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“…The time-structure of the resultant radiation is dictated by the time -structure of the radiating electron bunch. Due to electron-electron interactions within an electron bunch, a bunch 9 An electron traveling at constant velocity will not emit radiation unless the radiation matches a particular mode allowed by a medium (e.g., Cerenkov radiation) [Hau86].…”

Section: Bend Magnetsmentioning

confidence: 99%

Toward Femtosecond X-ray Spectroscopy at the Advanced Light Source

Chong¹

2004

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The ultrashort pulse x-ray source developed at the Advanced Light Source at the Lawrence Berkeley Laboratory is based on electron slicing in storage rings, and generates ~100 femtosecond pulses of synchrotron radiation spanning wavelengths from the farinfrared to the hard x-ray region of the electromagnetic spectrum. The tunability of the source allows for the adaptation of a broad range of static x-ray spectroscopies to useful pump -probe measurements.Initial experiments are attempted on transition metal complexes that exhibit relatively large structural changes upon photo-excitation and which have excited-state evolution determined by strongly interacting structural, electronic and magnetic degrees of freedom. Specifically, iron(II) complexes undergo a spin-crossover transition upon 2 optical irradiation. The dynamics of the transition involve a metal-to-ligand charge transfer, a ∆S=2 change in magnetic moment and 10% bond dilation in the first coordination shell of the iron. Studies of the electronic dynamics are studied with timeresolved optical absorption measurements. The current progress of time-resolved structural studies to complete the picture of the spin-crossover transition is presented.i

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“…This phenomenon, which is of great interest in high-energy physics, has been studied widely in the literature [1][2][3][4][5][6][7][8][9][10][11][12][13][14]. Although this effect is generally discussed for the case of point-charge particles, its analysis can be used on extended charge distributions [15] or a bunch of charges [13,[16][17].…”

Section: Introductionmentioning

confidence: 99%

On the Cherenkov radiation from extended charge distributions

Villavicencio¹,

Jiménez²,

Roa-Neri³

2000

Can. J. Phys.

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In this work the Cherenkov effect for extended charge distributions is analyzed using two different methods. In the first method, the Poynting vector is employed to determine the energy radiated, whereas in the second one, we apply the idea of generating time-dependent elemental dipoles, induced by a charge distribution moving with constant velocity, inside a material medium. An explicit expression for the Cherenkov radiation generated by some different kinds of spherically symmetric charge, travelling inside a medium, is obtained. PACS Nos.: 03.50. De, 41.20.Bt, 41.60.Bq Résumé : À l'aide de deux méthodes différentes, nous analysons ici l'effet Cherenkov pour des distributions de charge étendues. Dans la première, nous utilisons le vecteur de Poynting pour déterminer l'énergie irradiée, alors que dans la seconde, nous utilisons la génération de dipôles élémentaires variant dans le temps induits par une distribution de charge se déplaçant à vitesse constante dans le milieu. Nous obtenons une expression explicite pour la radiation Cherenkov générée par une sorte différente de distribution sphériquement symétrique en déplacement à travers le milieu. [Traduit par la rédaction]

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On the radiation from point charges

Cited by 34 publications

References 0 publications

The hydrogen atom revisited

The hydrogen atom revisited

Toward Femtosecond X-ray Spectroscopy at the Advanced Light Source

On the Cherenkov radiation from extended charge distributions

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