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Energy levels of atoms

Whereas the gas lasers described use energy levels characteristic of individual atoms or ions, laser operation can also employ molecular energy levels. Molecular levels may correspond to vibrations and rotations, in contrast to the electronic energy levels of atomic and ionic species. The energies associated with vibrations and rotations tend to be lower than those of electronic transitions thus the output wavelengths of the molecular lasers tend to He farther into the infrared. [Pg.6]

Energy level of atom Energy corresponding to the principal quantum number, n, 140... [Pg.686]

Energy-level diagram of uranium, 31-34 Energy levels,of atoms, 30, 31 Engstrom s investigations, 144, 225, 226, 296... [Pg.345]

Figure 10.5 Energy levels of atomic orbitals, n is the principal quantum number, and the 5, p, d notation indicates the azimuthal quantum number (/). For / = 1 and above the orbital is split into multiple suborbitals (indicated by the number of lines), corresponding to the values of the magnetic quantum number m Each of these lines can hold two electrons (corresponding to spin up and spin down ), giving rise to the rules for filling up the orbitals. Figure 10.5 Energy levels of atomic orbitals, n is the principal quantum number, and the 5, p, d notation indicates the azimuthal quantum number (/). For / = 1 and above the orbital is split into multiple suborbitals (indicated by the number of lines), corresponding to the values of the magnetic quantum number m Each of these lines can hold two electrons (corresponding to spin up and spin down ), giving rise to the rules for filling up the orbitals.
Jf(t) which we shall use in this chapter. We must mention, however, that somewhat more complicated forms have been introduced in order to consider some special aspects of the problem. Some of the most notable include that used by Bloss and Hone (which has a core level in the solid and two orbitals on the atom), those which take into account the scattering of atoms with large velocity components parallel to the surface and that recently considered by Kawai et in order to suggest a possible new experimental technique for studying energy levels of atoms in collision with surfaces. [Pg.341]

According to quantum mechanics, electrons in atoms occupy the allowed energy levels of atomic orbitals that are described by four quantum numbers the principal, the azimuthal, the magnetic, and the spin quantum numbers. The orbitals are usually expressed by the principal quantum numbers 1, 2, 3, —increasing from the lowest level, and the azimuthal quantum numbers conventionally eiqiressed by s (sharp), p (principal), d (diffuse), f (fundamental), — in order. For instance, the atom of oxygen with 8 electrons is described by (Is) (2s) (2p), where the superscript indicates the munber of electrons occupying the orbitals, as shown in Fig. 2-1. [Pg.15]

You will already know from your studies that the energy levels of atoms and molecules are quantized, i.e. there are discrete energy levels in atoms and molecules (Figure 1.1). [Pg.1]

The energy levels of atoms and molecules (and so the difference in energy between these levels) have discrete values (quanta). [Pg.6]

This energy-level diagram shows the relative energy levels of atomic orbitals in a multielectron atom (in this case rubidium, Rb, atomic number 37). [Pg.162]

The properties of absorption and luminescence emissions of atoms are important in analytical techniques as well as in spectroscopy in general. The absorption and emission spectra of atoms are line spectra which provide the unmistakable fingerprint of each element, and this is used in the analytical technique known as atomic absorption spectroscopy for example. Although the energy levels of atoms are shown as simple lines in a qualitative picture such as that of Figure 3.3, the absorption and emission lines which correspond to transitions between these levels are not infinitely narrow (that is, absolutely monochromatic) because of several effects. [Pg.30]

As we have seen in Chapter 11, the energy levels of atoms and ions, depending on the relative role of various intra-atomic interactions, are classified with the quantum numbers of different coupling schemes (11.2)— (11.5) or their combinations. Therefore, when calculating electron transition quantities, the accuracy of the coupling scheme must be accounted for. The latter in some cases may be different for initial and final configurations. Then the selection rules for electronic transitions are also different. That is why in Part 6 we presented expressions for matrix elements of electric multipole (Ek) transitions for various coupling schemes. [Pg.357]

Lines, corresponding to different transitions from initial states with vacancy in the shells with the same n, compose a series of spectra, e.g. K-, L-, M-series etc. Main diagram lines correspond to electric dipole ( 1) transitions between shells with different n. The lines of 2-transitions also belong to diagram lines. Selection rules of 1-radiation as well as the one-particle character of the energy levels of atoms with closed shells and one inner vacancy cause, as a rule, a doublet nature of the spectra, similar to optical spectra of alkaline elements. X-ray spectra are even simpler than optical spectra because their series consist of small numbers of lines, smaller than the number of shells in an atom. The main lines of the X-ray radiation spectrum, corresponding to transitions in inner shells, preserve their character also for the case of an atom with open outer shells, because the outer shells hardly influence the properties of inner shells. [Pg.399]

Another example of zero-point energy arises in the detailed quantum theory of the electromagnetic field, known as quantum electrodynamics. The empty vacuum with no photons present is actually the zero-point level with n = 0. The non-zero energy of this state cannot be measured directly, but does have some observable consequences. The vacuum is really a state of fluctuating electric and magnetic fields that are significant at the atomic level. Without them, there would be no mechanism for the spontaneous emission of photons from excited states. There also have very small effects on the energy levels of atoms (see Section 4.4). [Pg.46]

The energy levels of atomic Rydberg states are described by a hydrogen-type formula ... [Pg.272]

Figure 2.5 Schematic molecular orbital energy level diagram for a transition metal coordination cluster, [ML6]. (a) Energy levels of atomic orbitals of the free cation, M (b) energy levels for the six ligands, L, before bonding (c) molecular orbital energy levels for the octahedral [ML6] cluster. Figure 2.5 Schematic molecular orbital energy level diagram for a transition metal coordination cluster, [ML6]. (a) Energy levels of atomic orbitals of the free cation, M (b) energy levels for the six ligands, L, before bonding (c) molecular orbital energy levels for the octahedral [ML6] cluster.
Periodic Trends Involving the Sizes and Energy Levels of Atoms... [Pg.33]

Draw Lewis structures to model the arrangements of electrons in the outer energy levels of atoms. [Pg.61]

Figure 2.4 Filling in the chart determines the energy levels of atomic orbitals. Figure 2.4 Filling in the chart determines the energy levels of atomic orbitals.
Fig. 11. Zeeman energy levels of atomic oxygen in the P states. Fig. 11. Zeeman energy levels of atomic oxygen in the P states.

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See also in sourсe #XX -- [ Pg.8 ]




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Atomic energy levels

Atomic level energy and the scale of electromagnetic waves

ENERGY LEVELS OF ATOMIC ORBITALS

Electronic energy levels of atoms

Energy levels and terms schemes of many-electron atoms

Energy levels of hydrogen atom

Energy levels, atom

Energy of atom

Levels atomic

The energy levels of one-electron atoms

The permitted energy levels of hydrogenic atoms

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