Two-Dimensional Supersolid Formation in Dipolar Condensates

Dipolar condensates have recently been coaxed to form the long-sought supersolid phase. While one-dimensional supersolids may be prepared by triggering a roton instability, we find that such a procedure in two dimensions (2D) leads to a loss of both global phase coherence and crystalline order. Unlike in 1D, the 2D roton modes have little in common with the supersolid configuration. We develop a finite-temperature stochastic Gross-Pitaevskii theory that includes beyond-mean-field effects to explore the formation process in 2D and find that evaporative cooling directly into the supersolid phase-hence bypassing the first-order roton instability-can produce a robust supersolid in a circular trap. Importantly, the resulting supersolid is stable at the final nonzero temperature. We then experimentally produce a 2D supersolid in a near-circular trap through such an evaporative procedure. Our work provides insight into the process of supersolid formation in 2D and defines a realistic path to the formation of large two-dimensional supersolid arrays.

Instability of Rotationally Tuned Dipolar Bose-Einstein Condensates

The possibility of effectively inverting the sign of the dipole-dipole interaction, by fast rotation of the dipole polarization, is examined within a harmonically trapped dipolar Bose-Einstein condensate. Our analysis is based on the stationary states in the Thomas-Fermi limit, in the corotating frame, as well as direct numerical simulations in the Thomas-Fermi regime, explicitly accounting for the rotating polarization. The condensate is found to be inherently unstable due to the dynamical instability of collective modes. This ultimately prevents the realization of robust and long-lived rotationally tuned states. Our findings have major implications for experimentally accessing this regime.

Quantum Ferrofluid Turbulence

We study the elementary characteristics of turbulence in a quantum ferrofluid through the context of a dipolar Bose gas condensing from a highly nonequilibrium thermal state. Our simulations reveal that the dipolar interactions drive the emergence of polarized turbulence and density corrugations. The superfluid vortex lines and density fluctuations adopt a columnar or stratified configuration, depending on the sign of the dipolar interactions, with the vortices tending to form in the low-density regions to minimize kinetic energy. When the interactions are dominantly dipolar, the decay of the vortex line length is enhanced, closely following a t^{-3/2} behavior. This system poses exciting prospects for realizing stratified quantum turbulence and new levels of generating and controlling turbulence using magnetic fields.

Evaluating a split processing model of visual word recognition: effects of word length

A new theory of visual word recognition is based on the fact that the fovea is split in humans. When a reader fixates the center of a written word, the initial letters of the word that are to the left of fixation are projected first to the right cerebral hemisphere (RH) while the final letters are projected to the left cerebral hemisphere (LH). This paper explores the possibility that this has consequences for the early processing of the beginning and ends of centrally fixated words: specifically that lexical decision RTs are affected by the number of letters to the left of fixation but not by the number of letters to the right of fixation. For centrally presented five- and eight-letter words, we manipulated number of letters presented to the right or to the left of a fixation point (Experiment 1). We found that longer latencies to longer letter strings characterised the processing of the initial letters of words while LH word recognition features characterised the ends of words. Experiment 2 was a lateralized version of Experiment 1, and revealed the well established visual field and word length interaction. The results supported the split fovea theory.

Mutagenesis of the histidine ligand in human lactoferrin: iron binding properties and crystal structure of the histidine-253-->methionine mutant

The contribution of the conserved His ligand to iron binding in transferrins has been addressed by site-directed mutagenesis and X-ray crystallographic analysis. His 253 in the N-terminal half-molecule of human lactoferrin, LfN (residues 1-333), has been changed to Gly, Ala, Pro, Thr, Leu, Phe, Met, Tyr, Glu, Gln, and Cys by oligonucleotide-directed mutagenesis. The proteins have been expressed in baby hamster kidney cells, at high levels, and purified. The results show that the His ligand is essential for the stability of the iron binding site. All of the substitutions destabilized iron binding irrespective of whether the replacements were potential iron ligands or not. Iron was lost below pH approximately 6 for the Cys, Glu, and Tyr mutants and below pH 7 or higher for the others, compared with pH 5.0 for LfN. The destabilization is attributed to both steric and electronic effects. The importance of electronic effects has been shown by the crystal structure of the H253M mutant, which has been determined at an effective resolution of 2.5 A and refined to a final R factor of 0.173. The iron atom is changed from six-coordinate to five-coordinate; the Met 253 side chain is not bound to iron even though there appears to be no steric barrier. This is attributed to the poorer affinity of the thioether ligand for Fe(III) compared with imidazole nitrogen. The decreased stability of the iron binding is attributed solely to the loss of the His ligand as the protein conformation and interdomain interactions are unchanged.

Altered domain closure and iron binding in transferrins: the crystal structure of the Asp60Ser mutant of the amino-terminal half-molecule of human lactoferrin

The crystal structure of a site-specific mutant of the N-terminal half-molecule of human lactoferrin, Lf(N), in which the iron ligand Asp60 has been mutated to Ser, has been determined at 2.05 A resolution in order to determine the effects of the mutation on iron binding and domain closure. Yellow monoclinic crystals of the D60S mutant, in its iron-bound form, were prepared, and have unit cell dimensions a = 110.2 A, b = 57.0 A, c = 55.2 A, beta = 97.6 degrees, space group C2, with one molecule of 333 residues in the asymmetric unit. The structure was determined by molecular replacement, using the wild-type Lf(N) as search model, and was refined by restrained least-squares methods. The final model, comprising 2451 protein atoms (from residues 2 to 315) one Fe3+ and one CO2-(3), and 107 water molecules, gives an R-factor of 0.175 for all data in the resolution range 20.0 to 2.05 A. The model conforms well with standard geometry, having root-mean-square deviations of 0.014 A and 1.2 degrees from standard bond lengths and angles. The structure of the D60S mutant deviates in two important respects from the parent Lf(N) molecule. At the mutation site the Ser side-chain neither binds to the iron atom nor makes any interdomain contact as the substituted Asp does; instead a water molecule fills the iron coordination site and participates in interdomain hydrogen bonding. The domain closure is also changed, with the D60S mutant having a more closed conformation. Consideration of crystal packing suggests that the altered domain closure is a genuine molecular property but both the iron coordination and interdomain contacts are consistent with weakened iron binding in the mutant. The implications for iron binding in transferrins generally are discussed.