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_P.-Powell-auth.-Principles-of-Organometallic-Chemistry-Springer-Netherlands-1988

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Organometallic compounds of the transition elements

The allylligand possesses no rotation symmetry axis coincident with the z-axis.

While the description here is therefore only approximate, it gives a useful pictorial

representation.

(a) BONDING IN BIS(BENZENE)CHROMIUM. In this section, the symmetry

arguments outlined above are developed further for the complex

bis(benzene )chromium. This molecule has a sandwich structure in which the

rings adopt an eclipsed conformation. The vertical six-fold rotation z-axis (C 6 ), six

vertical planes of symmetry (aJ each of which includes a C 2 axis, and the

horizontal plane (ah) characterize the point group as D 6 h. In addition to the

symmetry elements mentioned, attention is drawn to a centre of symmetry (i),

situated at the chromium atom. The twelve C(2pz) orbitals. six on each ring,

transform according to a 1 g + a 2u + e 1 g + e 10 + e 2g + e 2u + b 2g + b 10 • Reference to

the character table ofD 6 h reveals that the metal orbitals transform as follows: a­

orbitals, d,z, s (a 1 g), Pz (a 2 u); n-orbitals, dzx, dyz (e 1 g), Px• Py (e 10 ); <5-orbitals, dxz-yz, dxy

( e 2 g). The symbols g and u refer to the parity on inversion through the metal atom.

s- and d-orbitals have even (gerade) and p-orbitals odd (ungerade) parity. The

ligand m.o.s on the two rings can be combined either to form sets of even a 1 g (a),

e 1 g (n), e 2 g (<5) and b 2 g (non-bonding) or odd a 1 u (a), e 1 u (n), e 2 u and b 1 u (nonbonding)

parities. The interactions between the metal and ligand orbitals which

are permitted on symmetry grounds are illustrated in Fig. 6.9.

The next step is to construct a qualitative molecular orbital energy level diagram

(Fig. 6.10). It must be stressed that this approach is qualitative; molecular orbital

calculations might be expected to yield a different order for the molecular orbitals,

this relative order varying depending on the assumptions made in the method of

calculation chosen. Calculations of good quality would also not neglect the

carbon s, Px and Py orbitals and the hydrogen 1s orbitals which are involved

mainly in holding together the skeletons of the benzene rings.

The metal d-orbitals are split, dzx and dyz ( e 1 g) becoming antibonding through n­

interaction with filled n 2 ligand orbitals, and dxz-yz, d,Y (e 2 g) somewhat bonding

through <5-interaction with empty n 3 ligand orbitals. dzz should be weakly

antibonding through overlap with the low-lying filled a 1 g (a) combination of n 1

ligand orbitals. There will be some mixing with the high lying metal 4s orbital.

which is also of a 1 g symmetry, however, so that the metal-centred orbital

(approximately dzz) seems to be essentially non-bonding. The 18 valence

electrons, six from chromium and six from each of the benzene rings, fill all the

bonding and non-bonding (i.e. a 1 g) orbitals. Bis(benzene)chromium is readily

oxidized in solution to an air-stable 17 -electron cation (C 6 H 6 ) 2 Cr+. The ease of

removal of one electron suggests that the highest occupied m.o. is fairly high

lying.

UV -photoelectron spectroscopy provides a means of studying the energy levels

of molecules experimentally. Simple interpretation of PE spectra relies on

Koopmans' theorem which states that the same order of molecular orbitals

204

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