Gaussian potentials facilitate access to quantum Hall states in rotating Bose gases

Through exact numerical diagonalization for small numbers of atoms, we show that it is possible to access quantum Hall states in harmonically confined Bose gases at rotation frequencies well below the centrifugal limit by applying a repulsive Gaussian potential at the trap center. The main idea is to reduce or eliminate the effective trapping frequency in regions where the particle density is appreciable. The critical rotation frequency required to obtain the bosonic Laughlin state can be fixed at an experimentally accessible value by choosing an applied Gaussian whose amplitude increases linearly with the number of atoms while its width increases as the square root.Comment: 4 pages, 4 figure

Genetic Change in Farmer-Recycled Maize Seed: A Review of the Evidence

Crop Production/Industries, Research and Development/Tech Change/Emerging Technologies,

Liver Resection: To Drain or not to Drain?

Purpose: A prospective, randomized trial was performed to determine if intra-abdominal drainage catheters are necessary after elective liver resection

QSO hosts and environments at z=0.9 to 4.2: JHK images with adaptive optics

We have observed nine QSOs with redshifts 0.85 to 4.16 at near-IR wavelengths with the adaptive optics bonnette of the Canada-France-Hawaii telescope. Exposure times ranged from 1500 to 24000s (mostly near 7000s) in J, H, or K bands, with pixels 0.035 arcsec on the sky. The FWHM of the co-added images at the location of the quasars are typically 0.16 arcsec. Including another QSO published previously, we find associated QSO structure in at least eight of ten objects, including the QSO at z = 4.16. The structures seen in all cases include long faint features which appear to be tidal tails. In four cases we have also resolved the QSO host galaxy, but find them to be smooth and symmetrical: future PSF removal may expand this result. Including one object previously reported, of the nine objects with more extended structure, five are radio-loud, and all but one of these appear to be in a dense small group of compact galaxy companions. The radio-quiet objects do not occupy the same dense environments, as seen in the NIR. In this small sample we do not find any apparent trends of these properties with redshift, over the range 0.8 < z < 2.4. The colors of the host galaxies and companions are consistent with young stellar populations at the QSO redshift. Our observations suggest that adaptive optic observations in the visible region will exhibit luminous signatures of the substantial star-formation activity that must be occurring.Comment: 22 pages including 10 tables, plus 11 figures. To appear in A

A Framework for the Analysis of Sport Sponsorship and the Cola Wars

The primary purpose of this article was to explore the concept of understanding sports contribution to sponsorship through understanding the structure and function of the sponsorship industry. The colas were selected as an example industry to develop the concept of understanding sponsorship using a molecular analysis. This type of molecular analysis will provide perspective and foster better relationships of how the sponsor can do business on the sport and its event. Sponsors are demanding accountability and this type of approach opens the dialogue for exploring symbiotic relationships among the sport and the sponsor

A Typology for the Understanding of Structure and Function of a Sports Industry: A Case Study of NASCAR

Examination of sport from a molecular level will help to increase understanding about the nature of a sport. NASCAR (National Association of Stock Car Racing) is a growing sport that has the potential to serve as a case study to understand the structure and function of sport from a molecular level. A framework was developed to analyze the relationships among the actors in NASCAR

Topological Entropy of Quantum Hall States in Rotating Bose Gases

Through exact numerical diagonalization, the von Neumann entropy is calculated for the Laughlin and Pfaffian quantum Hall states in rotating interacting Bose gases at zero temperature in the lowest Landau level limit. The particles comprising the states are indistinguishable, so the required spatial bipartitioning is effected by tracing over a subset of single-particle orbitals. The topological entropy is then extracted through a finite-size scaling analysis. The results for the Laughlin and the Pfaffian states agree with the expected values of $\ln\sqrt{2}$ and $\ln\sqrt{4}$, respectively.Comment: 4 pages, 4 figure

Effects Of Caffeine Dose Timing On Total Urine Excretion During Sodium-Aided Hyperhydration Protocols

When used alone, both caffeine and sodium-aided hyperhydration (SAH) can be ergogenic. Although caffeine use in conjunction with SAH promotes diuresis, hyperhydration can be achieved, albeit at lower levels compared to SAH alone. Previous caffeine and SAH work has suggested most of the caffeine induced diuresis occurs within 15 min of consumption of a bolus of caffeine, sodium and water. This response suggests that caffeine-induces diuresis for only 15 min following its consumption, and/or that the diuretic effects of caffeine are dependent on hydration levels. PURPOSE: To determine the effects of caffeine, consumed at different time-points, on diuresis during SAH protocols. METHODS: Subjects were 17 healthy males (23 ± 5 yr, 177 ± 8 cm, 83.4 ± 15.3 kg). Each performed 4, 90 min hyperhydration trials in a randomized, double-blind fashion. Protocols began with a bladder void and measurement of urine specific gravity (USG) followed by ingestion of 15 mL H2O ∙ kg bm-1 with one of four treatments: Placebo (PL), 70.5 mg NaCl ∙ kg bm-1 (Na), or a combination of NaCl and caffeine consumed in two different strategies: 70.5 mg NaCl + 5 mg caffeine ∙ kg bm-1 taken at the start of the trial (NaCaf0), or 70.5 mg NaCl ∙ kg bm-1 taken at the start and 5 mg caffeine ∙ kg bm-1 taken at 75 min of the trial (NaCaf75). After consuming the water, subjects rested for 90 min performing a measured bladder void every 15 min. Total urine excreted (TUE) was expressed as a percentage of the total fluid consumed during the hyperhydration protocols. USG and TUE were compared using one-way repeated measures ANOVA with Sidak post hoc analyses. Levels of significance were set a priori at P \u3c 0.05. RESULTS: USGs were 1.007 ± 0.003 (PL), 1.008 ± 0.003 (Na), 1.007 ± 0.004 (NaCaf0), and 1.009 ± 0.004 (NaCaf75) (P \u3e 0.05). TUE for PL (87 ± 30%) was significantly higher than all other protocols (P \u3c 0.05). TUE for NaCaf0 (73 ± 16%) was significantly higher than Na (56 ± 18%, P = 0.02) and NaCaf75 (52 ± 13% P \u3c 0.01). NSD in TUE was observed between Na and NaCaf75. CONCLUSION: The results reaffirm that, when caffeine is consumed at the beginning of a SAH strategy, hyperhydration can be achieved, but at a lower level compared to SAH without caffeine. The results also suggest that waiting to consume caffeine until 75 min after water is consumed does not result in caffeine induced diuresis during a SAH protocol