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Resonance conditions

In an electron spin resonance spectrometer, transitions between the two states are brought about by the application of the quantum of energy hv which is equal to g H. The resonance condition is defined when hv = g H and this is achieved experimentally by varying H keeping the frequency (v) constant. Esr spectroscopy is used extensively in chemistry in the identification and elucidation of structures of radicals. [Pg.152]

The transition occurs with significant probability only if the frequency of the light is very close to the familiar resonance condition, namely hv = AE, where h is Planck s constant and AE is the difference in energy of the... [Pg.1125]

Okamoto H and Yoshihara K 1990 Femtosecond time-resolved coherent Raman scattering under various polarization and resonance conditions J. Opt. Soc. B7 1702-8... [Pg.1230]

The locations of the maxima of the -field and the E-field are different depending on the mode chosen for the EPR experuuent. It is desirable to design the cavity in such a way that the B field is perpendicular to the external field B, as required by the nature of the resonance condition. Ideally, the sample is located at a position of maxuuum B, because below saturation the signal-to-noise ratio is proportional to Simultaneously, the sample should be placed at a position where the E-field is a minimum in order to minimize dielectric power losses which have a detrimental effect on the signal-to-noise ratio. [Pg.1560]

With help of the four-level diagram of the =I= system (see figure BL15.8 two conniion ways for recording ELDOR spectra will be illnstrated. In freqnency-swept ELDOR the magnetic field is set at a value that satisfies the resonance condition for one of the two EPR transitions, e.g. 4<- 2, at the fixed observe klystron frequency, The pump klystron is then turned on and its frequency, is swept. When the pump... [Pg.1571]

As an example, we mention the detection of iodine atoms in their P3/2 ground state with a 3 + 2 multiphoton ionization process at a laser wavelength of 474.3 run. Excited iodine atoms ( Pi/2) can also be detected selectively as the resonance condition is reached at a different laser wavelength of 477.7 run. As an example, figure B2.5.17 hows REMPI iodine atom detection after IR laser photolysis of CF I. This pump-probe experiment involves two, delayed, laser pulses, with a 200 ns IR photolysis pulse and a 10 ns probe pulse, which detects iodine atoms at different times during and after the photolysis pulse. This experiment illustrates a frindamental problem of product detection by multiphoton ionization with its high intensity, the short-wavelength probe laser radiation alone can photolyse the... [Pg.2135]

From this equaiion one can determine the required value of neutral circuit impedance for a particular level of ground fault current. The external impedance will be Z, less the ground impedance. In HT systems one c in also delermine the likely value of a ground inductor coil to achieve a near-resonance condition, to eliminate the arcing grounds, on the one hand, and facilitate a strike-free extinction of an arc hy the interrupting device, on the other. [Pg.671]

The simplest place to start is with a hydrogen atom. The experimental ESR spectrum shows two lines separated by 1420.4 MHz (often reported as a magnetic induction, since transitions occur at the resonance condition hv = In... [Pg.310]

A capacitor bank will represent reducing impedance to currents of increasing frequency. Such reducing impedance, if matched with a similarly increasing inductance impedance of a transformer or a supply system, can cause a resonant condition. In plants where equipment produces harmonic current, a full survey of the installation is recommended prior to installation of the capacitors. [Pg.222]

If there is no resonant condition to modify the resultant vibration phase, then the phase for both vertical and horizontal readings are essentially the same even though the vertical and horizontal amplitudes do not necessarily correspond. In actual practice, this may be slightly off due to other vibration sources such as misalignment. In performing the analysis, what counts is that when the source of the vibration is primarily from imbalance, then the vertical reading phase differences between one end of the rotor and the other will be very similar to the phase differences when measured horizontally. For example, vibrations 60° out of phase vertically would show 60° out of phase horizontally within 20 per cent. [Pg.940]

The room temperature Raman spectrum excited in pre-resonance conditions [351 indeed shows bands at 169 cm-1 and 306 cm, which are in agreement with the modes observed in the fluorescence spectrum and that have been assigned by ab initio calculations to totally symmetric vibrations jl3). [Pg.409]

Tabic 6-5. Comparison of (he aK vibrational modes in the ground and excited states. The totally symmetric vibrations of the ground stale measured in tire Raman spectrum excited in pre-resonance conditions 3S] and in the fluorescence spectrum ]62 ate compared with the results of ab initio calculations [131- The corresponding vibrations in the excited stale arc measured in die absorption spectrum. [Pg.416]

In order to compute the lifetime of a phonon of energy E, one averages the Golden Rule scattering rate (7ig A /pCj )tanh(p /2) with respect to n(e, A), subject to the resonance condition E = y/EA + A [8, 11, 93]. This yields two contributions to the decay rate ... [Pg.175]

The fact that the photon does traverse the lattice planes does not mean that the photon wUl be absorbed or even scattered by the solid. The reflectance of the photon is a function of the nature of the compositional surface, whereas absorption depends upon the interior composition of the solid. A "resonance" condition must exist before the photon can transfer energy to the solid (absorption of the photon), hi the following, we show this resonance condition in general terms of both R A. [Pg.414]


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Contents Resonance Condition

Electronic Zeeman interaction resonance condition

Magnetic fields resonance conditions

Microwave resonance condition

Mossbauer resonance condition

Resonance A condition occurring when

Resonance A condition occurring when more

Resonance A condition occurring when more than one valid Lewis structure can

Resonance A condition occurring when more than one valid Lewis structure can be written

Resonance condition anisotropy

Resonance condition aqueous solutions

Resonance condition bifurcation

Resonance condition chemical bonds

Resonance condition cytochrome

Resonance condition damping effects

Resonance condition diffusion coefficient

Resonance condition electrodynamics

Resonance condition energy splitting

Resonance condition formula

Resonance condition frequency changes

Resonance condition hyperfine interactions

Resonance condition hyperfine structure

Resonance condition integer spins

Resonance condition interactions

Resonance condition interpretation

Resonance condition microwave frequency

Resonance condition model components

Resonance condition morphological change

Resonance condition overlap

Resonance condition perturbation theory

Resonance condition porphyrin

Resonance condition rhombicity

Resonance condition rotation number

Resonance condition second-order effects

Resonance condition spin Hamiltonian

Resonance condition spin-orbit coupling

Resonance condition systems

Resonance condition transition ions

Resonance condition zero-field interactions

Resonance condition, geometrical

Resonant conditions

Resonant conditions, nonlinear optics

Rotary-resonance condition

Rotational resonance conditions

Self resonance condition

Specific resonance condition

Symmetry Conditions for Resonance Hybrids

The Resonance Condition

Transverse resonance condition

Viscoelastic resonant conditions

Zeeman interaction resonance condition

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