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Study the Luminescence of Phosphors and Doped Materials
(1) Computational Methodology
Semi-empirical methods are used for both optimization and calculation of the excitation spectrum:
- Polymer system structures are optimized using the PM3 method within Hyperchem software.
- INDO/1 parameterized for spectroscopy is used to calculate the many absorption spectra using ZINDO software.
(2) Calculating the Stoke's Shift
- In most cases the emission spectrum is a mirror image of the absorption spectrum shifted to lower energy.
- ZINDO is a well parameterized to accurately calculate the absorption spectra but does not calculate emission spectra.
- In the past we have been using the experimental Stoke's shift but this does not allow the computational effort to be independent.
- The most desirable technique would be a blend of speed and accuracy due to the many structures we whish to investigate.
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(a) Rough Estimate for Stoke's Shift
- Reoptimization energies of molecules in the first excited state are usually calculated with expensive Configuration interaction calculations.
- Because most of the S0 to S1 transitions are HOMO to LUMO transitons, we can get a rough estimate of the reoptimization energy for a single configuration calculation, where one electron is excited from the HOMO to the LUMO while keeping the total spin the same (singlet state).
(3) Test Cases
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a) General Method
- There are two ways to calculate an estimate for the luminescence peak.
- Both rely on calculating the geometry of the single configuration representing S1.
- After the geometry is calculated the Stoke's shift can be calculated by either.
- Calculation of the energy used to changed the molecular structure
- Because the energy between S0 and S1 changes we can use ZINDO to calculate the energy difference between these states. (This is technically absorption but it does give a method of how far apart the energy states are at the new geometry).
- PPP-OR11 and PPP-R10 will be used as test cases.
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b) PPP-OR11
- This model contains a total of 142 atoms.
- The model is a reproduction of the system shown below with one repeat unit (n=1).
- Excitation spectra are calculated using models with four repeat units (n=4).
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i) Calculations
- Calculated with ZINDO method.
- This method calculates the energy difference between the S0 and S1 states.
- Very good agreement for this rough approximation.
- Reoptimization method calculates almost identical emission peak.
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c) PPP-R10
- This model contains a total of 126 atoms.
- The model is a reproduction of the system below with one repeat unit (n=1).
- Excitation spectra are calculated using models with four repeat units (n=4).
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i) Calculations
- Calculated with ZINDO method.
- This method calculates the energy difference between the S0 and S1 states.
- Again very good agreement for this rough approximation.
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d) UV-Vis Absorbance and Emission of 2-Styrylthiophene
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Predicted Values |
Published Values* |
| Solvent |
Vacuum |
MeOH |
BuCN |
AcCN |
Aq. |
n He |
| λABS(nm) |
359 |
321 |
324 |
321 |
306 |
321 |
| λEM(nm) |
421 |
375 |
370 |
380 |
360 |
354 |
*Note: The experimental values were determined in solvent and exhibit a shift from predicted values in vacuum.
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e) Dependence of S0 to S1 Transition on Structure and Angle
Relative total energy and S0 to S1 transition energy as a function of a fixed dihedral angle for the unsubstituted TV-PPV structure.
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Relative total energy and S0 to S1 transition energy as a function of a fixed dihedral angle for the substituted TV-PPV structure.
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(4) Summary
- We have used the single configuration of one electron moving from the HOMO to the LUMO to estimate the geometry of the molecule in the first excited state.
- With this geometry we can calculate the reoptimization energy directly or we can calculate the energy difference between the S0 and S1 states.
- In the cases of PPP-R10 and PPP-OR11 both yield surprisingly accurate estimates for emission.
- Comparisons to the literature for functionalized oligomers shows good agreement between the predicted and measured values.
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