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A Bunker

Publications and source records attributed to A Bunker.

9 recordsLinked to original sources

Ultra-relativistic electrons in Jupiter's radiation belts.

Ground-based observations have shown that Jupiter is a two-component source of microwave radio emission: thermal atmospheric emission and synchrotron emission from energetic electrons spiralling in Jupiter's magnetic field. Later in situ measurements confirmed the existence of Jupiter's high-energy electron-radiation belts, with evidence for electrons at energies up to 20[?]MeV. Although most radiation belt models predict electrons at higher energies, adiabatic diffusion theory can account only for energies up to around 20[?]MeV. Unambiguous evidence for more energetic electrons is lacking. Here we report observations of 13.8[?]GHz synchrotron emission that confirm the presence of electrons with energies up to 50[?]MeV; the data were collected during the Cassini fly-by of Jupiter. These energetic electrons may be repeatedly accelerated through an interaction with plasma waves, which can transfer energy into the electrons. Preliminary comparison of our data with model results suggests that electrons with energies of less than 20[?]MeV are more numerous than previously believed.

Journal Article↗

Parallel excluded volume tempering for polymer melts.

We have developed a technique to accelerate the acquisition of effectively uncorrelated configurations for off-lattice models of dense polymer melts that makes use of both parallel tempering and large-scale Monte Carlo moves. The method is based upon simulating a set of systems in parallel, each of which has a slightly different repulsive core potential, such that a thermodynamic path from full excluded volume to an ideal gas of random walks is generated. While each system is run with standard stochastic dynamics, resulting in an NVT ensemble, we implement the parallel tempering through stochastic swaps between the configurations of adjacent potentials, and the large-scale Monte Carlo moves through attempted pivot and translation moves that reach a realistic acceptance probability as the limit of the ideal gas of random walks is approached. Compared to pure stochastic dynamics, this results in an increased efficiency even for a system of chains as short as N=60 monomers, however at this chain length the large-scale Monte Carlo moves were ineffective. For even longer chains, the speedup becomes substantial, as observed from preliminary data for N=200. We also compare our scheme to the end bridging algorithm of Theodorou et al. For N=60, end bridging must allow a polydispersity of more than 10% in order to relax the end-to-end vector more quickly than our method. The comparison is, however, hampered by the fact that the end-to-end vector becomes a somewhat artificial quantity when one implements end bridging, and is perhaps no longer the slowest dynamic variable.

Algorithms↗

Longitudinal magnetic excitations in classical spin systems

Using spin dynamics simulations we predict the splitting of the longitudinal spin-wave peak in all antiferromagnets with single site anisotropy into two peaks separated by twice the energy gap at the Brillouin zone center. This phenomenon has yet to be observed experimentally but can be easily investigated through neutron scattering experiments on MnF2 and FeF2. We have also determined that for all classical Heisenberg models the longitudinal propagative excitations are entirely multiple spin wave in nature.

Journal Article↗

A mechanism for toxin insertion into membranes is suggested by the crystal structure of the channel-forming domain of colicin E1.

BACKGROUND: Channel-forming colicins, including colicin E1, are a sub-family of bacteriocins. The toxic action of colicin E1 is derived from its ability to form a voltage-gated channel, which causes depolarization of the cytoplasmic membrane of sensitive Escherichia coli cells. In this process, the toxin-like colicin E1 molecule must undergo a substantial structural transition from a soluble state, in which it binds the target cell, to a membrane-bound state. Details of the structural changes that accompany this conversion may be directly applicable to other channel-forming toxins, as well as to the mechanism by which proteins insert into or cross membranes. RESULTS: The structure of the 190-residue channel-forming domain of colicin E1 in its soluble form has been solved at 2.5 A resolution. This structure contains 10alpha helices arranged in three layers (A-C) with a central hydrophobic helical hairpin in layer B, which is proposed to anchor the membrane-bound form in the bilayer. The extended N-terminal helix I provides a connection to the rest of the colicin E1 molecule, and the loop I-II may act as a hinge for re-orientation of the domain for membrane binding. A set of conserved positively charged residues on layer C may provide the docking surface on the molecule for membrane attachment. A large internal cavity between layers B and C may allow these layers to disengage, suggesting a mechanism for unfolding the molecule on the membrane that involves the perturbation of the interhelical hydrophobic interactions in layer C. CONCLUSION: On the basis of the structure of the colicin E1 channel-forming domain, its comparison with the structure of the colicin A domain and the known requirement for initial electrostatic and subsequent hydrophobic interactions, molecular details of the docking, unfolding and insertion of the channel-forming domain into the membrane are proposed. The model for docking and initial interaction with the membrane positions the hydrophobic hairpin 'anchor' approximately parallel to the membrane surface. Hydrophobic interactions in the docking layer may then be displaced by interactions with the membrane, spreading the helices on the surface and exposing the hydrophobic hairpin for insertion into the membrane.

Amino Acid Sequence↗