07.04.2013 Views

Essentials of Computational Chemistry

Essentials of Computational Chemistry

Essentials of Computational Chemistry

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

BIBLIOGRAPHY AND SUGGESTED ADDITIONAL READING 515<br />

Table 14.5 Measured and predicted absorption and emission energies (eV)<br />

for 8-hydroxyquinoline and Alq3<br />

Process Level <strong>of</strong> theory 8-hydroxyquinoline Alq3<br />

Absorption CIS/3-21+G∗∗ 5.35 4.68<br />

CIS/pVTZ 5.80<br />

CIS/INDO/S (12x12) 3.48<br />

CIS/INDO/S (15x15) 3.83 3.28<br />

TD-B3LYP/3-21+G∗∗ 3.76 3.00<br />

TD-B3LYP/6-31G(d) 3.72 2.90<br />

Experiment 3.84 3.20<br />

Emission CIS/3-21+G∗∗ 3.58<br />

TD-B3LYP/3-21+G∗∗ 2.30<br />

Experiment 2.40<br />

6-31G(d) results again would seem to indicate that the former basis set may be regarded<br />

as adequate.<br />

With respect to emission, the geometry computed for the excited-state Alq3 structure at<br />

the CIS/3-21+G ∗∗ level was found to be significantly different from that for the ground<br />

state. This leads to a Stokes shift <strong>of</strong> 0.8 eV, which is not particularly well reproduced at<br />

the CIS level but is quite accurately predicted at the TD-B3LYP level.<br />

Having obtained good agreement with experiment for the various spectroscopic data,<br />

Halls and Schlegel go on to analyze the MOs involved in the photoluminescence. They<br />

find that the orbitals involved are highly localized on a single one <strong>of</strong> the three aryl ligands<br />

in Alq3, and that these orbitals are quite similar to those involved in the S0 → S1 absorption/emission<br />

<strong>of</strong> 8-hydroxyquinoline itself. They also express the difference between the<br />

excited-state geometry and the ground-state geometry <strong>of</strong> Alq3 in terms <strong>of</strong> the normal modes<br />

(this procedure is in essence a multilinear regression involving displacement vectors). They<br />

find that a particular normal mode having high intensity in the vibrational spectrum makes<br />

a significant contribution in this analysis, thereby rationalizing observations <strong>of</strong> vibrational<br />

structure in the absorption and emission spectra <strong>of</strong> Alq3 under matrix isolation conditions.<br />

They carry out their vibrational analysis using BLYP/6-31G(d) frequencies, as these were<br />

found to be in very good agreement with the experimental ground-state IR spectrum.<br />

The work <strong>of</strong> Halls and Schlegel illustrates particularly effectively how different levels<br />

<strong>of</strong> theory may be used for studying different aspects <strong>of</strong> a complex chemical problem.<br />

Furthermore, repeated comparisons <strong>of</strong> theoretical predictions to experimental measurements<br />

in order to validate the chosen levels <strong>of</strong> theory provides solid support for the quality <strong>of</strong><br />

further predictions using those levels.<br />

Bibliography and Suggested Additional Reading<br />

Aguilar, M. A. 2001. ‘Separation <strong>of</strong> the Electric Polarization into Fast and Slow Components: A<br />

Comparison <strong>of</strong> Two Partition Schemes’ J. Phys. Chem. A, 105, 10 393.<br />

Cave, R. J., Burke, K., and Castner, E. W., Jr. 2002. ‘Theoretical Investigation <strong>of</strong> the Ground and<br />

Excited States <strong>of</strong> Coumarin 151 and Coumarin 120’ J. Phys. Chem. A, 106, 9294.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!