The low-lying excitations of polydiacetylene
The Pariser-Parr-Pople Hamiltonian is used to calculate and identify the nature of the low-lying vertical transition energies of polydiacetylene. The model is solved using the density matrix renormalisation group method for a fixed acetylenic geometry for chains of up to 102 atoms. The non-linear op...
| Main Authors: | , , |
|---|---|
| Format: | Conference item |
| Published: |
2001
|
| _version_ | 1826300920243159040 |
|---|---|
| author | Race, A Barford, W Bursill, R |
| author_facet | Race, A Barford, W Bursill, R |
| author_sort | Race, A |
| collection | OXFORD |
| description | The Pariser-Parr-Pople Hamiltonian is used to calculate and identify the nature of the low-lying vertical transition energies of polydiacetylene. The model is solved using the density matrix renormalisation group method for a fixed acetylenic geometry for chains of up to 102 atoms. The non-linear optical properties of polydiacetylene are considered, which are determined by the third-order susceptibility. The experimental 1Bu data of Giesa and Schultz are used as the geometric model for the calculation. For short chains, the calculated E(1Bu) agrees with the experimental value, within solvation effects (ca. 0.3 eV). The charge gap is used to characterise bound and unbound states. The nBu is above the charge gap and hence a continuum state; the 1Bu, 2Ag and mAg are not and hence are bound excitons. For large chain lengths, the nBu tends towards the charge gap as expected, strongly suggesting that the nBu is the conduction band edge. The conduction band edge for PDA is agreed in the literature to be ca. 3.0 eV. Accounting for the strong polarisation effects of the medium and polaron formation gives our calculated E(nBu) ca. 3.6 eV, with an exciton binding energy of ca. 1.0 eV. The 2Ag state is found to be above the 1Bu, which does not agree with relaxed transition experimental data. However, this could be resolved by including explicit lattice relaxation in the Pariser- Parr-Pople-Peierls model. Particle-hole separation data further suggest that the 1Bu, 2Ag and mAg are bound excitons, and that the nBu is an unbound exciton. |
| first_indexed | 2024-03-07T05:24:29Z |
| format | Conference item |
| id | oxford-uuid:e0172559-12ae-4a3c-8934-9a3fb240cb3d |
| institution | University of Oxford |
| last_indexed | 2024-03-07T05:24:29Z |
| publishDate | 2001 |
| record_format | dspace |
| spelling | oxford-uuid:e0172559-12ae-4a3c-8934-9a3fb240cb3d2022-03-27T09:44:14ZThe low-lying excitations of polydiacetyleneConference itemhttp://purl.org/coar/resource_type/c_5794uuid:e0172559-12ae-4a3c-8934-9a3fb240cb3dSymplectic Elements at Oxford2001Race, ABarford, WBursill, RThe Pariser-Parr-Pople Hamiltonian is used to calculate and identify the nature of the low-lying vertical transition energies of polydiacetylene. The model is solved using the density matrix renormalisation group method for a fixed acetylenic geometry for chains of up to 102 atoms. The non-linear optical properties of polydiacetylene are considered, which are determined by the third-order susceptibility. The experimental 1Bu data of Giesa and Schultz are used as the geometric model for the calculation. For short chains, the calculated E(1Bu) agrees with the experimental value, within solvation effects (ca. 0.3 eV). The charge gap is used to characterise bound and unbound states. The nBu is above the charge gap and hence a continuum state; the 1Bu, 2Ag and mAg are not and hence are bound excitons. For large chain lengths, the nBu tends towards the charge gap as expected, strongly suggesting that the nBu is the conduction band edge. The conduction band edge for PDA is agreed in the literature to be ca. 3.0 eV. Accounting for the strong polarisation effects of the medium and polaron formation gives our calculated E(nBu) ca. 3.6 eV, with an exciton binding energy of ca. 1.0 eV. The 2Ag state is found to be above the 1Bu, which does not agree with relaxed transition experimental data. However, this could be resolved by including explicit lattice relaxation in the Pariser- Parr-Pople-Peierls model. Particle-hole separation data further suggest that the 1Bu, 2Ag and mAg are bound excitons, and that the nBu is an unbound exciton. |
| spellingShingle | Race, A Barford, W Bursill, R The low-lying excitations of polydiacetylene |
| title | The low-lying excitations of polydiacetylene |
| title_full | The low-lying excitations of polydiacetylene |
| title_fullStr | The low-lying excitations of polydiacetylene |
| title_full_unstemmed | The low-lying excitations of polydiacetylene |
| title_short | The low-lying excitations of polydiacetylene |
| title_sort | low lying excitations of polydiacetylene |
| work_keys_str_mv | AT racea thelowlyingexcitationsofpolydiacetylene AT barfordw thelowlyingexcitationsofpolydiacetylene AT bursillr thelowlyingexcitationsofpolydiacetylene AT racea lowlyingexcitationsofpolydiacetylene AT barfordw lowlyingexcitationsofpolydiacetylene AT bursillr lowlyingexcitationsofpolydiacetylene |