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Radiation quantum

The results of the theory of quantum mechanics require that nuclear states have discrete energies. This is in contrast to classical mechanical systems, which can have any of a continuous range of energies. This difference is a critical fact in the appHcations of radioactivity measurements, where the specific energies of radiations are generally used to identify the origin of the radiation. Quantum mechanics also shows that other quantities have only specific discrete values, and the whole understanding of atomic and nuclear systems depends on these discrete quantities. [Pg.445]

But occurrence of a chemical reaction along one or even several mean free paths is quite surprising, and to explain such a large reaction rate and large velocity of propagation, these authors resorted to electrons and radiation, quantum-mechanical resonance of collectively moving particles and direct impact of rapid active centers of a chain reaction. [Pg.200]

The concentration of the colored form at steady state concentration is largely dependent on the intensity of the incident radiation, quantum yield, kinetics of the reverse reaction, and temperature and solvent sensitivity of both the forward and reverse reactions. Normally the kinetics for the reverse reaction will be first or second order, although some systems are considerably more complex. Most reverse reactions are thermally sensitive and a few are accelerated by irradiation. [Pg.278]

Dyakin VM, Skobelev IYu, Faenov AYa, Bartnik A, Fiedorowicz H, Szczurek M, Osterheld A, Nilsen J (1997) Precision measurements of the wavelengths of spectral lines of multiply charged krypton and argon ions formed in a gas target heated by laser radiation. Quantum Electron. 27 691-695... [Pg.250]

In the case of NMR spectroscopy we will be concerned only with absorption and emission of rf radiation. Quantum mechanics, the field of physics that deals with energy at the microscopic (atomic) level, allows us to define selection rules that describe the probability for a photon to be absorbed or emitted under a given set of circumstances. But even classical (i.e., pre-quantum-mechanical) physics tells us there is one requirement shared by all forms of absorption and emission spectroscopy For a particle to absorb (or emit) a photon, the particle itself must first be in some sort of uniform periodic motion with a characteristic fixed frequency. Most important, the frequency of that motion must exactly match the frequency of the absorbed (or emitted) photon ... [Pg.3]

In the above equations t and r represent whole numbers. If r = r = 0, 0 = 0, and the incident radiation quantum passes through the crystal without deflection. It will keep on traveling through the crystal until it reaches a point where either r or r differs from 0. Suppose... [Pg.2]

To compare these equations with the forms often used to describe the defraction of rays by a crystal we may put e = hc/ where X denotes soijie parameter connected with the radiation quantum e, but need not be regarded in our present theory as the distance between waves, as in the wave theory. Equations (4) then become ... [Pg.4]

As a second problem, take the radiation reflected from a thin plate of thickness t. As before, let the radiation quantum fall on the surface at the angle i with the normal and suppose that inside of the plate its direction of motion makes the angle r with the normal. Let the velocity inside of the plate be c that outside c, and let the length of the plate be /. Taking components of the momentum parallel to the surface of the plate we have the equation ... [Pg.6]

The reverse of upconversion is downconversion, where each quantum of (vacuum) ultraviolet radiation is converted to several quanta of infrared or visible radiation (quantum cutting) [386]. For example, the highest energy emission for the excitation of Cs2LiTmCl6 Nd31 by 476.9 nm radiation is below ca. 11,300 cm-1, since the cross-relaxation of 4G4 Tm3+ level leads to the excitation of Tm3+ 3H5 and Nd3+ 4F3/2 [344]. [Pg.264]

Various PAGs have been synthesized specifically for use in chemical amplification resists, reflecting their important impact on lithographic performance (Fig. 7) [13,30]. The choice of PAG depends on a number of factors such as the nature of radiation, quantum efficiency of acid generation, solubility, miscibility with resin, thermal and hydrolytic stability, plasticization effect, toxicity, strength and size of generated acid, impact on dissolution rates, cost, etc. In... [Pg.48]

Discharges in aerosols play an important role in plasma-chemical applications. Photoelectron emission often makes an important contribution in the ionization of aerosols, especially if a radiation quantum exceeds the work function of macro-particles but is below the ionization potential of neutral gas species. In this case, the steady-state electron density is determined by photo-ionization of aerosols and electron attachment to the macro-particles. [Pg.46]

The MCT (mercury cadmium teUuride) detector is much more sensitive and faster than the DTGS detector. The operation of MCT detectors is based on an internal photo efiecL Each IR radiation quantum excites one bound electron of the detector material to a free state, i. e. the electrical conductivity of the MCT detector element increases. A serious drawback of the MCT detector is its spectral working range. [Pg.53]

We now consider the interaction of an atom or molecule with electromagnetic radiation. A proper quantum-mechanical approach would treat both the atom and the radiation quantum mechanically, but we shall simplify things by using the classical picture of the light as an electromagnetic wave of oscUlating electric and magnetic fields. [Pg.275]

Hans Albrecht Bethe (1906-2005) was an American physicist, a professor at Cornell University, and a student of Arnold Sommerfeld. Bethe contributed to many branches of physics, such as crystal field theory, interaction of matter with radiation, quantum electrodynamics, and the structure and nuclear reactions of stars (for the latter achievement, he received the Nobel Prize in physics in 1967). [Pg.155]

Scintillation detectors are based on luminescence. Some materials have the special property that as they absorb a radiation quantum, a light flash is produced. The intensity of the flash is proportional to the radiation energy. The flash is amplified with a photoelectron multiplier. The energy resolution, though poor when compared with that of semiconductor detectors, is sufficient for many purposes. [Pg.4164]

Planck, Max (1858-1947) A German theoretical physicist credited with foimding quantum theory— which affects all matter in the universe—Planck earned a doctoral degree at the age of twenty-one before becoming a professor at the imiversities of Kiel and Berlin. He explored electromagnetic radiation, quantum mechanics, thermodynamics, black-bodies, and entropy. He formulated the Planck constant, which describes the proportions between the energy and frequency of a photon and provides understanding of atomic strucmre. He was awarded the 1918 Nobel Prize in Physics for his discoveries. [Pg.2013]


See other pages where Radiation quantum is mentioned: [Pg.480]    [Pg.97]    [Pg.98]    [Pg.553]    [Pg.4]    [Pg.187]    [Pg.4]    [Pg.405]    [Pg.405]    [Pg.407]    [Pg.409]    [Pg.411]    [Pg.62]    [Pg.7]    [Pg.51]    [Pg.4164]    [Pg.5]    [Pg.95]    [Pg.408]    [Pg.6]    [Pg.917]    [Pg.917]   
See also in sourсe #XX -- [ Pg.44 ]




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