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Transition between energy levels

Nuclear magnetic resctnance involves the transitions between energy levels of the fourth quantum number, the spin quantum number, and only certain nuclei whose spin is not zero can be studied by this technique. Atoms having both an even number of protons and neutrons have a zero spin for example, carbon 12, oxygen 16 and silicon 28. [Pg.62]

The atomic spectra can be understood in terms of transitions between energy levels corresponding to these particular values of energy. [Pg.265]

It would thus seem that promotion of a given electron in a molecule could result either in a singlet or a triplet excited state depending on the amount of energy added. However, this is often not the case because transitions between energy levels are governed by selection rales, which state that certain transitions are forbidden . There are several types of forbidden transitions, two of which are more important than the others. [Pg.309]

The transitions between energy levels in an AX spin system are shown in Fig. 1.44. There are four single-quantum transitions (these are the normal transitions A, A, Xi, and X2 in which changes in quantum number of 1 occur), one double-quantum transition 1% between the aa and j8 8 states involving a change in quantum number of 2, and a zero-quantum transition 1% between the a)3 and fia states in which no change in quantum number occurs. The double-quantum and zero-quantum transitions are not allowed as excitation processes under the quantum mechanical selection rules, but their involvement may be considered in relaxation processes. [Pg.70]

The rotational spectrum of a molecule involves transitions between energy levels, say the R(8) transition / = 8 and J = 9, but if there are no molecules rotating in the J = 8 level then there can be no R(8) transition. The local thermal collisions will populate some of the higher J levels in a general principle called equipartition. The general expression is the Boltzmann Law, given by ... [Pg.70]

As noted above, not all possible transitions between energy levels are theoretically allowed. Each energy level is uniquely characterized by a set of quantum numbers. The integer used to define the energy level in the above discussion (1,2, 3, etc.) is called the principal quantum number, n. The sub-levels described by the letters (s, p, d, /, etc.) are associated with the second quantum number, given the symbol /, with l = 1 synonymous with s, 2 =p, etc. The multiplicity of levels associated with each sub-level (i.e., the number of horizontal lines for each orbital in Figure Al.l) is defined by a third quantum number mh which has values 0, 1... 1. Thus, -orbitals only have one sub-level, p-orbitals have three (with m/ values 0 and d= 1), d-orbitals have five, etc. The selection rules can... [Pg.417]

Figure 1.16 Transitions between energy levels in the ruby laser... Figure 1.16 Transitions between energy levels in the ruby laser...
Transitions between energy levels in organic molecules are subject to certain constraints, referred to as selection rules. [Pg.42]

Fig. 1 The effect of size on metals. Whereas bulk metal and metal nanoparticles have a continuous band of energy levels, the limited number of atoms in metal clusters results in discrete energy levels, allowing interaction with light by electronic transitions between energy levels. Metal clusters bridge the gap between single atoms and nanoparticles. Even though in the figure the energy levels are denoted as singlets, we must remark that the spin state of the silver clusters is not yet firmly established... Fig. 1 The effect of size on metals. Whereas bulk metal and metal nanoparticles have a continuous band of energy levels, the limited number of atoms in metal clusters results in discrete energy levels, allowing interaction with light by electronic transitions between energy levels. Metal clusters bridge the gap between single atoms and nanoparticles. Even though in the figure the energy levels are denoted as singlets, we must remark that the spin state of the silver clusters is not yet firmly established...
Mossbauer spectroscopy is based on transition between energy levels of nuclei with different values of the nuclear spin quantum number /. When a nucleus emits a y-ray, the energy of the emitted radiation is lowered by the recoil of the nucleus. Conversely, the energy needed for absorption is higher than that needed for transition, because the absorbing nucleus absorbs energy in the recoil process. For nuclei tightly bound in solids, however, the effective mass of the emitter and... [Pg.221]

For light to induce a transition between energy levels of an atom or molecule, it is necessary that the frequency of the hght and the energy difference between the levels satisfy, at least approximately, the Planck relationship ... [Pg.97]

We now consider the electric-dipole selection rules for radiative transitions between energy levels of the same electronic state of a polyatomic molecule. The electric-dipole transition moment is (4.91), which becomes... [Pg.382]

For the spectrum corresponding to transitions between energy levels (transition array), the probability of the ith line can be expressed in terms... [Pg.380]

X-ray (ESCA, PES) O O f Transitions between energy levels of inner electrons of atoms and molecules... [Pg.6]

Magnetic resonance spectroscopy deals with the observation of the interaction between an oscillating magnetic field and matter, which results in transition between energy levels of the magnetic dipoles, the degeneracy of which is usually removed by an externally applied steady magnetic field. [Pg.361]

NMR arises from transitions between energy levels, just as in other branches of spectroscopy, with transitions induced by the absorption of energy from an applied electromagnetic field with a magnetic amplitude of 2B,.The interaction... [Pg.18]

In Eq. 11.48 we saw that the basis functions for our density matrix are divided into three groups with fz = 1,0, and —1, respectively. As we saw in Chapter 6, transitions between energy levels El - E2, E3 E4, Ex E3, and E2 -> E4 each result in Afz = 1 and are called single quantum transitions, while transitions Ex E4 and E2 E3 are termed double quantum and zero quantum transitions, respectively. The usual selection rules from time-dependent perturbation theory show that only single quantum transitions are permitted in such simple experiments as excitation by a 90° pulse. Moreover, for weakly coupled nuclei, the single quantum transitions each involve only a single type of nucleus, I or 5, as indicated in Fig. 6.2. [Pg.295]

Even with CD, spectra are not always easily interpreted because there may be overlapping bands of different signs. Interpretation requires determination of the overall symmetry around the metal ion and assignment of absorption spectra to specific transitions between energy levels (discussed in Chapter 11) in order to assign specific CD peaks to the appropriate transitions. Even then, there are cases in which the CD peaks do not match the absorption peaks and interpretation becomes much more difficult. [Pg.323]

Use the Bohr model to calculate the energy levels of one-electron atoms and to find the freqnencies and wavelengths of light emitted in transitions between energy levels (Section 4.3, Problems 19-22). [Pg.162]

The interaction of radiation with matter can cause redirection of the radiation or transitions between energy levels of the atoms and molecules, or both. More subtle effects involve not only the color or wavelength of the radiation but its change in intensity and in the polarization of the light. It is by spectroscopy that we are able to... [Pg.19]

Off-diagonal elements are created by rf pulses. They describe coherent transitions between energy levels, which a large number of the spins undergo, with the same initial... [Pg.47]

While microwave spectroscopy must rely on rather indirect means to obtain barrier height information, transitions between energy levels of different n can be directly observed by infrared and Raman studies. Resolution is much poorer in these techniques thus while microwave studies are limited primarily by model errors, the limit to optical studies is to a large extent due to experimental uncertainties. [Pg.402]


See other pages where Transition between energy levels is mentioned: [Pg.320]    [Pg.110]    [Pg.270]    [Pg.40]    [Pg.94]    [Pg.22]    [Pg.45]    [Pg.32]    [Pg.320]    [Pg.100]    [Pg.169]    [Pg.1759]    [Pg.108]    [Pg.270]    [Pg.454]    [Pg.267]    [Pg.86]    [Pg.255]    [Pg.5]    [Pg.41]    [Pg.840]    [Pg.6]    [Pg.5]    [Pg.233]    [Pg.16]   
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