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Diatomic molecules formation

Fig. 2. Illustration to the JT and PJT effect in diatomic molecule formation. In the homonuclear case (a) the two atomic states at large interatomic distances <2m = l/R = 0 form a double degenerate term which at larger QM (smaller R) splits due to bonding, thus reducing the energy and symmetry quite similar to any other JT E bi problem (cf. Fig. la at Q > 0) for heteronuclear diatomics (b) the bonding picture is that of the pseudo JT effect (cf. Fig. lc at Q > 0). Fig. 2. Illustration to the JT and PJT effect in diatomic molecule formation. In the homonuclear case (a) the two atomic states at large interatomic distances <2m = l/R = 0 form a double degenerate term which at larger QM (smaller R) splits due to bonding, thus reducing the energy and symmetry quite similar to any other JT E bi problem (cf. Fig. la at Q > 0) for heteronuclear diatomics (b) the bonding picture is that of the pseudo JT effect (cf. Fig. lc at Q > 0).
It is possible to create an atomic Mott insulator phase in an optical lattice, in which sites in a given region are occupied by a specific integer number of atoms [98], A lattice with two atoms per site is ideal for making diatomic molecules by PA (or MA) and protecting them from collisions in a sense, PA is then converted from a free -> bound process to a bound -> bound process, because the two atoms are confined in the lattice site. Homonuclear and heteronuclear diatomic molecule formation in this and other ways has been proposed ([99] and [100], respectively) and more recently observed ([101-104] and [67,105], respectively). [Pg.194]

A more useful quantity for comparison with experiment is the heat of formation, which is defined as the enthalpy change when one mole of a compound is formed from its constituent elements in their standard states. The heat of formation can thus be calculated by subtracting the heats of atomisation of the elements and the atomic ionisation energies from the total energy. Unfortunately, ab initio calculations that do not include electron correlation (which we will discuss in Chapter 3) provide uniformly poor estimates of heats of formation w ith errors in bond dissociation energies of 25-40 kcal/mol, even at the Hartree-Fock limit for diatomic molecules. [Pg.105]

The requiremenfs for formation of MOs are fhe same as for a diatomic molecule, namely, fhaf fhe orbifals from which fhey are formed musf be of comparable energy and of fhe righf... [Pg.261]

All bond enthalpies are positive because heat must be supplied to break a bond. In other words, bond breaking is always endothermic and bond formation is always exothermic. Table 6.7 lists bond enthalpies of some diatomic molecules. [Pg.375]

It is this resonance energy that would be in the main responsible for the difference in energy of the crystal and the gas of diatomic molecules Li2. But the heat of formation of Li2 molecules from atoms is only 6-6 kcal./g.-atom, whereas that of the metal is 39kcal./g.-atom. It seems unlikely, by comparison for example with the analogous case of Kekule-like resonance in aromatic molecules, that the great difference, 32-4 kcal./g.-atom, could result from the synchronized resonance, of type f Li—Li Li Li)... [Pg.375]

Giant molecular clouds the GMCs have a lifetime of order 106—10s years and are the regions of new star formation. The Orion nebula (Orion molecular cloud, OMC) is some 50 ly in diameter and 1500 ly from Earth. The temperature within the cloud is of order 10 K and the atomic density is 106 cm-3. The chemical composition is diverse and contains small diatomic molecules, large polyatomic molecules and dust particles covered with a thick ice mantle. [Pg.121]

The trigonal bond orbitals in the ten valence electron system as well as the two sets of trigonal lone pair orbitals in the 14 valence electron system are superpositions of it orbitals and o orbitals. The formation of such trigonally symmetric molecular orbitals from a-type and w-type molecular orbitals is entirely analogous in character to the formation of the three (sp2) hybrid atomic orbitals from one (s) and two ip) atomic orbitals which was discussed in the preceding section. This can be visualized by looking at the diatomic molecule... [Pg.49]

ICRU Report 55 [36], and references therein. Fast electrons predominantly interact via the coulomb force with the bound electrons of the medium resulting in ionization, i.e., leading to formation of free electrons and residual positive ions. The residual ions can be left in any of a wide variety of final states ranging from their ground ionic state, to states resulting from simultaneous ionization and excitation, and/or dissociation of molecular constituents of the target material. The interaction of a primary electron gp with the diatomic molecule AB can precede via many channels, e.g., ionization can occur by any of the following reaction pathways... [Pg.41]

Lewis and many other chemists had recognized the shortcomings of the ionic bond. When diatomic molecules, such as or Cl, were considered, there was no reason why one atom should lose an electron and an identical atom should gain an electron. There had to be another explanation for how diatomic molecules formed. We have seen how the octet rule applies to the formation of ionic compounds by the transfer of electrons. This rule also helps explain the formation of covalent bonds when molecules (covalent compounds) form. Covalent bonds result when atoms share electrons. Using fluorine, F, as a representative halogen, we can see how the octet rule applies to the formation of the molecule. Each fluorine atom has seven valence electrons and needs one more electron to achieve the stable octet valence configuration. If two fluorines share a pair of electrons, then the stable octet configuration is achieved ... [Pg.76]

J. Li, J. T. Bahns, and W. C. Stwalley. Scheme for state-selective formation of highly rotationally excited diatomic molecules. J. Chem. Phys., 112(14) 6255-6261 (2000). [Pg.412]

Figure 4.1 The c and n orbital overlaps between 2p atomic orbitals in the formation of some diatomic molecules... Figure 4.1 The c and n orbital overlaps between 2p atomic orbitals in the formation of some diatomic molecules...
In the following, we will discuss a number of different adsorption systems that have been studied in particular using X-ray emission spectroscopy and valence band photoelectron spectroscopy coupled with DFT calculations. The systems are presented with a goal to obtain an overview of different interactions of adsorbates on surfaces. The main focus will be on bonding to transition metal surfaces, which is of relevance in many different applications in catalysis and electrochemistry. We have classified the interactions into five different groups with decreasing adsorption bond strength (1) radical chemisorption with a broken electron pair that is directly accessible for bond formation (2) interactions with unsaturated it electrons in diatomic molecules (3) interactions with unsaturated it electrons in hydrocarbons ... [Pg.68]

This makes the heat of formation of the ion pair from C2H6, AHt = 140 kcal. with an estimated uncertainty arising mainly from uncertainty in rt of about 15 kcal. The dissociation energy of the ion pair, Qc = 148 kcal. is quite reasonable compared to the values of 124 kcal./mole9 for the dissociation of the diatomic molecule NaCl(r( = 2.36 A.) into gaseous Na+ + Cl- ions. For KF(,i + F < ) the value is 136 kcal. [Pg.10]

Carbon monoxide (CO) is a well-studied species in which the two ends of the diatomic molecule have similar coordinative properties. In the formation of any real crystal of solid CO, a statistical fraction of the molecules are therefore found to enter the lattice in backward orientation ... [Pg.188]

Table A-10. Enthalpies of Formation of Diatomic Molecules at 1 atm and O K in the Ideal Gas State ... Table A-10. Enthalpies of Formation of Diatomic Molecules at 1 atm and O K in the Ideal Gas State ...

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See also in sourсe #XX -- [ Pg.208 ]




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Formation of Diatomic Molecules and Radicals in the Gas Phase

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