954 research outputs found
Dynamical model of the dielectric screening of conjugated polymers
A dynamical model of the dielectric screening of conjugated polymers is
introduced and solved using the density matrix renormalization group method.
The model consists of a line of quantized dipoles interacting with a polymer
chain. The polymer is modelled by the Pariser-Parr-Pople (P-P-P) model. It is
found that: (1) Compared to isolated, unscreened single chains, the screened
1Bu- exciton binding energy is typically reduced by ca. 1 eV to just over 1 eV;
(2) Covalent (magnon and bi-magnon) states are very weakly screened compared to
ionic (exciton) states; (3) Screening of the 1Bu- exciton is closer to the
dispersion than solvation limit.Comment: 12 pages, 2 figure
Computational Investigations of the Primary Excited States of Poly(para-phenylene vinylene)
The Pariser-Parr-Pople model of pi-conjugated electrons is solved by the
density matrix renormalization group method for the light emitting polymer,
poly(para-phenylene vinylene). The energies of the primary excited states are
calculated. When solid state screening is incorporated into the model
parameters there is excellent agreement between theory and experiment, enabling
an identification of the origin of the key spectroscopic features.Comment: 6 pages, 3 figure
Can Quantum Lattice Fluctuations Destroy the Peierls Broken Symmetry Ground State?
The study of bond alternation in one-dimensional electronic systems has had a
long history. Theoretical work in the 1930s predicted the absence of bond
alternation in the limit of infinitely long conjugated polymers; a result later
contradicted by experimental investigations. When this issue was re-examined in
the 1950s it was shown in the adiabatic limit that bond alternation occurs for
any value of electron-phonon coupling. The question of whether this conclusion
remains valid for quantized nuclear degrees of freedom was first addressed in
the 1980s. Since then a series of numerical calculations on models with gapped,
dispersionless phonons have suggested that bond alternation is destroyed by
quantum fluctuations below a critical value of electron-phonon coupling. In
this work we study a more realistic model with gapless, dispersive phonons. By
solving this model with the DMRG method we show that bond alternation remains
robust for any value of electron-phonon coupling
Relaxation energies and excited state structures of poly(para-phenylene)
We investigate the relaxation energies and excited state geometries of the
light emitting polymer, poly(para-phenylene). We solve the
Pariser-Parr-Pople-Peierls model using the density matrix renormalization group
method. We find that the lattice relaxation of the dipole-active
state is quite different from that of the state and the
dipole-inactive state. In particular, the state is
rather weakly coupled to the lattice and has a rather small relaxation energy
ca. 0.1 eV. In contrast, the and states are strongly
coupled with relaxation energies of ca. 0.5 and ca. 1.0 eV, respectively. By
analogy to linear polyenes, we argue that this difference can be understood by
the different kind of solitons present in the , and
states. The difference in relaxation energies of the
and states accounts for approximately one-third of the exchange
gap in light-emitting polymers.Comment: Submitted to Physical Review
Quantized Lattice Dynamic Effects on the Spin-Peierls Transition
The density matrix renormalization group method is used to investigate the
spin-Peierls transition for Heisenberg spins coupled to quantized phonons. We
use a phonon spectrum that interpolates between a gapped, dispersionless
(Einstein) limit to a gapless, dispersive (Debye) limit. A variety of
theoretical probes are used to determine the quantum phase transition,
including energy gap crossing, a finite size scaling analysis, bond order
auto-correlation functions, and bipartite quantum entanglement. All these
probes indicate that in the antiadiabatic phonon limit a quantum phase
transition of the Berezinskii-Kosterlitz-Thouless type is observed at a
non-zero spin-phonon coupling, . An extrapolation from the
Einstein limit to the Debye limit is accompanied by an increase in for a fixed optical () phonon gap. We therefore conclude that the
dimerized ground state is more unstable with respect to Debye phonons, with the
introduction of phonon dispersion renormalizing the effective spin-lattice
coupling for the Peierls-active mode. We also show that the staggered spin-spin
and phonon displacement order parameters are unreliable means of determining
the transition.Comment: To be published in Phys. Rev.
Peierls transition in the quantum spin-Peierls model
We use the density matrix renormalization group method to investigate the
role of longitudinal quantized phonons on the Peierls transition in the
spin-Peierls model. For both the XY and Heisenberg spin-Peierls model we show
that the staggered phonon order parameter scales as (and the
dimerized bond order scales as ) as (where
is the electron-phonon interaction). This result is true for both linear and
cyclic chains. Thus, we conclude that the Peierls transition occurs at
in these models. Moreover, for the XY spin-Peierls model we show
that the quantum predictions for the bond order follow the classical prediction
as a function of inverse chain size for small . We therefore conclude
that the zero phase transition is of the mean-field type
Molecular Orbital Models of Benzene, Biphenyl and the Oligophenylenes
A two state (2-MO) model for the low-lying long axis-polarised excitations of
poly(p-phenylene) oligomers and polymers is developed. First we derive such a
model from the underlying Pariser-Parr-Pople (P-P-P) model of pi-conjugated
systems. The two states retained per unit cell are the Wannier functions
associated with the valence and conduction bands. By a comparison of the
predictions of this model to a four state model (which includes the non-bonding
states) and a full P-P-P model calculation on benzene and biphenyl, it is shown
quantitatively how the 2-MO model fails to predict the correct excitation
energies. The 2-MO model is then solved for oligophenylenes of up to 15 repeat
units using the density matrix renormalisation group (DMRG) method. It is shown
that the predicted lowest lying, dipole allowed excitation is ca. 1 eV higher
than the experimental result. The failure of the 2-MO model is a consequence of
the fact that the original HOMO and LUMO single particle basis does not provide
an adequate representation for the many body processes of the electronic
system.Comment: LaTeX, 12 pages, 3 eps figures included using epsf. To appear in
Chemical Physics, 199
Screening and the quantitative π-model description of the optical spectra and polarizations of phenyl based oligomers
The long standing problem of the inability of many semiempirical models to correctly predict the polarization of the higher dipole allowed optical transitions of phenyl based π-conjugated polymers and molecules is examined and related to the issue of internal and external screening of π-π electron Coulomb interactions within the molecules. Following a review of previous theoretical and experimental work, π electron only the Complete Neglect of Differential Overlap (CNDO) model is presented which, for the first time, is able to predict accurately the energies and symmetries of all the observed optical transitions of benzene, biphenyl and trans -stilbene, up to ~8-10 eV. In so doing, it is demonstrated that the problem with previous calculations was the noninclusion of screening from outside the p electron system itself. By fitting separately the spectra in hydrocarbon based condensed phases, in the gas phase and in solid rare gas matrices, and comparing the resulting model parameters, we show that, while the effects of screening from the environment are certainly noticeable, the most important spectral features - in particular the ordering of dipole allowed transitions - come from effective screening by the s electrons. We find that both of these effects can be adequately accounted for within a π electron only model by using a dielectric constant and appropriate parameter renormalization
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