J. Tinka Gammel
Los Alamos National Laboratory
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Featured researches published by J. Tinka Gammel.
Synthetic Metals | 1989
A. R. Bishop; J. Tinka Gammel; S.R. Phillpot
Abstract We consider a two-band discrete tight-binding Peierls-Hubbard model for an isolated chain of a halogen-bridged, mixed-valence, transition metal linear chain complex (MX chain), which includes as parameters the difference between metal (M) and halogen (X) on site affinities, ϵM − ϵX = 20, a distance dependence βM,X of the on-site energies, the M-X hopping integral t and its distance dependence α, and an effective M-X spring K. We investigate: (1) ground states as functions of the model parameters; and (2) excitations — kinks, polarons, bipolarons, and photoexcitations — and their corresponding intra-gap absorption features.
Synthetic Metals | 1989
J. Tinka Gammel; S.M. Weber-Milbrodt; E.Y. Loh; A. R. Bishop
Abstract We have studied the effects of correlations in a simple two-band discrete tight-binding Peierls-Hubbard model for MX chains using perturbation theory, Hartree-Fock and exact diagonalization for classical adiabatic phonons, and a variational approach for quantum phonons.
Synthetic Metals | 1987
J.C. Hicks; J. Tinka Gammel; Han-Yong Choi; E. J. Mele
Abstract To allow for direct comparison with experiment we calculate the conductivity due to phonons in polyacetylene using a multicomponent Hamiltonian. A single soliton on a discrete lattice modeled the photoexcited data, while heavily doped systems were modeled with continuum soliton and polaron-like lattices. We discuss the effect of the IR active Goldstone mode, the third bound mode, and the recently predicted IR acoustic modes on the photoexcited spectra. The differences in the IR spectra for heavily doped soliton and polaron-like lattices and the consequences on the proposed first order phase transition are also discussed.
Synthetic Metals | 1988
David K. Campbell; J. Tinka Gammel; E.Y. Loh
Abstract We investigate the effects of including “off-diagonal” terms-nearest-neighbor bond-bond repulsion ( W ) and bond-site repulsion ( X ) — in the extended Peierls-Hubbard model. As a specific illustration we study the ground state dimerization in the one-dimensional, half-filled-band models that have been widely applied to conjugated polymers such as trans -polyacetylene and related charge density wave systems.
Physical Review B | 1998
Ya-Sha Yi; Z. G. Yu; A. R. Bishop; J. Tinka Gammel
We model nickelate-centered and oxygen-centered stripe phases in doped
Journal of Applied Physics | 2014
Dana M. Dattelbaum; Joshua D. Coe; P. A. Rigg; R. Jason Scharff; J. Tinka Gammel
{\mathrm{La}}_{2}{\mathrm{NiO}}_{4}
Synthetic Metals | 1993
J. Tinka Gammel; David K. Campbell; E.Y. Loh
materials. We use an inhomogeneous Hartree-Fock and random-phase approximation approach including both electron-electron and electron-lattice (e-l) coupling for a layer of
Synthetic Metals | 1991
J. Tinka Gammel; David K. Campbell; Sumit Mazumdar; S.N. Dixit; E.Y. Loh
{\mathrm{La}}_{2}{\mathrm{NiO}}_{4}.
Synthetic Metals | 1991
Robert J. Donohoe; Laura A. Worl; J. Tinka Gammel; Avadh Saxena; I. Batistic; A. R. Bishop
We find that whether the ground state after commensurate hole doping comprises Ni-centered or O-centered charge-localized stripes depends sensitively on the e-l interaction. With increasing e-l interaction strength, a continuous transition from an O-centered stripe phase to a Ni-centered one is found. Various low- and high-energy signatures of these two kinds of stripe phases are predicted, which can clearly distinguish them. These signatures reflect the strongly correlated spin-charge-lattice features in the vicinity of Ni-centered or O-centered stripe domains. The importance of e-l interaction for recent experiments on stripe phases is discussed.
Physica B-condensed Matter | 1990
J. Tinka Gammel; I. Batistic; A. R. Bishop; E.Y. Loh; S. Marianer
Shock compression of two molded, carbon fiber-filled polymer composites was performed in gas gun-driven plate impact experiments at impact velocities up to ≈5 km/s. Hugoniot states for both composites were obtained from <5 GPa to nearly 50 GPa. The two materials contained a high fill percentage of chopped carbon fibers, bound by either phenolic or cyanate ester polymeric resins. Their dynamic responses were similar, although the 10 wt. % difference of carbon fill produced measureable divergence in shock compressibility. The chopped carbon fibers in the polymer matrix led to moderately anisotropic shocks, particularly when compared with the more commonly encountered filament-wound carbon fiber-epoxy composites. A discontinuity, or cusp, was observed in the principal Hugoniot of both materials near 25 GPa. We attribute the accompanying volume collapse to shock-driven chemical decomposition above this condition. Inert and reacted products equations of state were used to capture the response of the two materi...