ar X iv : h ep - p h / 06 02 03 6 v 1 3 F eb 2 00 6 Photon : history , mass , charge ∗
نویسنده
چکیده
The talk consists of three parts. " History " briefly describes the emergence and evolution of the concept of photon during the first two decades of the 20th century. " Mass " gives a short review of the literature on the upper limit of the photon's mass. " Charge " is a critical discussion of the existing interpretation of searches for photon charge. Schemes, in which all photons are charged, are grossly inconsistent. A model with three kinds of photons (positive, negative and neutral) seems at first sight to be more consistent, but turns out to have its own serious problems. 1 History The idea that light consists of rapidly moving particles can be traced from the writings of ancient authors to Descartes and Newton. The wave theory of light was put forward by Huyghens and was later decisively proved to be correct through discovery of interference and diffraction by Young and Fres-nel. Maxwell's theory of light as electromagnetic waves was one of the greatest achievements of the 19th century. The history of the photon in the 20th century started in 1901 with the formula by Planck for radiation of a black body and introduction of what was called later the quantum of action h [1]. In 1902 Lenard discovered that energy of electrons in photoeffect does not depend on the intensity of light, while it depends on the wavelength of the latter [2]. In his fundamental article " On an euristic point of view concerning the production and transformation of light " published in 1905 Einstein pointed out that the discovery of Lenard meant that energy of light is distributed in space not uniformly, but in a form of localized light quanta [3]. He has shown that all experiments related to the black body radiation, photoluminescence and production of cathode rays by ultraviolate light can be explained by the quanta of light. 1 The proof that Einstein's light quanta behave as particles, carrying not only energy, but also momentum, was given in 1923 in the experiments by Compton on scattering of X-rays on electrons [4]. The term " photon " for particles of light was coined by Lewis in 1926 in an article " The conservation of photons " [5]. His notion of a photon was different from the notion we use today. He considered photons to be " atoms " of light, which analogously to the ordinary atoms …
منابع مشابه
ar X iv : h ep - p h / 06 02 02 0 v 1 2 F eb 2 00 6 Automated Resummation and Hadron Collider Event Shapes ∗
whereHmn are numerical coefficients and we have introduced the shorthand L ≡ ln 1/v. The double logarithms are associated with non-cancellation between soft and collinear divergences in real and virtual graph, since limiting v suppresses real radiation but not the corresponding virtual terms. When v is small (ln v ∼ α s ) all terms αs L 2m become of the same magnitude (∼ 1) and reliable calcula...
متن کاملar X iv : h ep - p h / 00 06 08 2 v 2 1 3 Ju n 20 00 LUNFD 6 / ( NFFL - 7187 ) 2000 PHOTON STRUCTURE AT HERA
The structure of the virtual photon and its contribution to small x processes in deep inelastic scattering at HERA is discussed.
متن کاملar X iv : h ep - p h / 06 03 05 3 v 1 7 M ar 2 00 6 OUTP - 06 06 P Triviality and the ( Supersymmetric ) See - Saw
For the D = 5 Majorana neutrino mass operator to have a see-saw ultraviolet completion that is viable up to the Planck scale, the see-saw scale is bounded above due to triviality limits on the see-saw couplings. For supersymmetric see-saw models, with realistic neutrino mass textures, we compare constraints on the see-saw scale from triviality bounds, with those arising from experimental limits...
متن کاملar X iv : h ep - p h / 07 02 06 3 v 1 6 F eb 2 00 7 UT - 07 - 06 Solutions to large B and L breaking in the Randall - Sundrum model
The stability of proton and neutrino masses are discussed in the Randall-Sundrum model. We show that relevant operators should be suppressed, if the hierarchical Yukawa matrices are explained only by configurations of wavefunctions for fermions and the Higgs field along the extra dimension. We assume a Z N discrete gauge symmetry to suppress those operators. In the Dirac neutrino case, there is...
متن کاملar X iv : h ep - p h / 06 02 08 0 v 1 9 F eb 2 00 6 D s ( 2317 ) as a tetraquark state with QCD sum rules in heavy quark limit
In this article, we take the point of view that the charmed scalar meson Ds(2317) be a tetraquark state and calculate its mass within the framework of the QCD sum rules approach in the heavy quark limit. The numerical values for the mass of the Ds(2317) are consistent with the experimental data. There must be some tetraquark component in the Ds(2317) state. PACS number: 12.38.Aw, 12.38.Qk
متن کاملذخیره در منابع من
با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید
عنوان ژورنال:
دوره شماره
صفحات -
تاریخ انتشار 2008