Nuclear
Quadrupole Resonance (NQR):
Atoms which have nuclear spins
greater than ½ behave as if the distribution of charge within the nucleus is
non-spherical. The nucleus does not behave as a dipole because the nuclear
charge distribution remains centrosymmetric. It does, however, possess an
electrical quadrupole moment (C02, which is centrosymmetric and
linear, is an example of a molecule which has an electric quadrupole moment).
Species
|
Ionic character of the M-Cl bond %
|
[PtCI6]2-
|
44
|
[PdC16]
2-
|
43
|
[lrCI6]
2-
|
47
|
[0sCI6]
2-
|
46
|
[ReCl6]
2-
|
45
|
[WCl6]
2-
|
43
|
[SnCI6]
2-
|
66
|
[TeCl6]
2-
|
68
|
[SeCI6]
2-
|
59
|
In an applied non-uniform electrostatic field,
the non-uniformly charged nucleus can
take up at least two
orientations, one of which
is more stable than the
others (the number
of orientations depends on the
magnitude of the nuclear
quadrupole moment). It is possible to excite the nucleus from a lower to an
upper state by application of suitable radio-frequency radiation. This is a
classical description of the phenomenon, but the essentials are carried over
into a quantum mechanical treatment. In practice,
the non-uniform electrostatic field is generated by the charge distribution
around, but very close to, the nucleus. Clearly, this is a
phenomenon which is only applicable to atoms in a low-symmetry
environment (but, note carefully, this does not
automatically mean a low-symmetry complex).
The most-studied of the nuclei which exhibit quadrupole resonance
spectra are 35Cl and 37Cl.
The method is inherently insensitive and the high concentrations of these
isotopes in samples such as solid K2[PtC16]
is a
great advantage. Only solids can be studied, anyhow, because the
molecular tumbling in a liquid or gas averages the effect to zero. The
sensitivity of the method has increased in recent years by the advent of pulse (such
as those used in NMR) and also, in suitable cases, by not looking at the NQR
nucleus itself but, rather, at one which is energetically coupled to it and
which is NMR-active.
It is likely that because of these developments
the future will see a wider use of NQR spectroscopy. It is also likely
that the interpretation of the data will become more sophisticated. Traditionally, the experimental data have
been interpreted to give the percentage ionic character of a bond. This is because, for example, in the Cl-
ion all of the p orbitals are equally occupied whilst in Cl2 the σ
bond, if composed of p orbitals only, corresponds to one electron in the pσ
orbital of each chlorine atom, and so Cl- and Cl2
differ in their resonant frequencies. Interpolation allows a
value for the ionic character of a Cl-M bond to be determined from the
chlorine resonance frequencies in Cl- and Cl2.
Some correction may be applied to allow for the fact that a pure chlorine p orbital may not be involved in the M-Cl bond. When there are
two non-equivalent NQR nuclei in the unit cell of a solid these give rise to
separate resonances which may be resolvable.
In this way NQR spectroscopy gives structural information. Both bromine, 79Br
and 81Br,
and iodine,
127I,
but not fluorine, give NQR spectra, as too may 14N, 55Mn, 59Co, 63Cu, 65Cu, 75As, 121Sb, 123Sb, 201
Hg, and 2o9Bi.
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