Is graphene on copper doped?

Angle-resolved photoemission spectroscopy (ARPES) and X-ray photoemission spectroscopy have been used to characterise epitaxially ordered graphene grown on copper foil by low-pressure chemical vapour deposition. A short vacuum anneal to 200 °C allows observation of ordered low energy electron diffraction patterns. High quality Dirac cones are measured in ARPES with the Dirac point at the Fermi level (undoped graphene). Annealing above 300 °C produces n-type doping in the graphene with up to 350 meV shift in Fermi level, and opens a band gap of around 100 meV. Dirac cone dispersion for graphene on Cu foil after vacuum anneals (left: 200 °C, undoped; right: 500 °C, n-doped). Centre: low energy electron diffraction from graphene on Cu foil after 200 °C anneal. Data from Antares (SOLEIL)

Caltech-UCSD Birds 200

Caltech-UCSD Birds 200 (CUB-200) is a challenging image dataset annotated with 200 bird species. It was created to enable the study of subordinate categorization, which is not possible with other popular datasets that focus on basic level categories (such as PASCAL VOC, Caltech-101, etc). The images were downloaded from the website Flickr and filtered by workers on Amazon Mechanical Turk. Each image is annotated with a bounding box, a rough bird segmentation, and a set of attribute labels

Impacts of nitrate on the water resources of Malta

High density of population (1250 persons/km2) and livestock (300 head/km2). • Heavy dependence on groundwater for public supply and agriculture. • Complex landuse with multiple cropping and small landholdings. • Semi-arid Mediterranean climate with low and variable infiltration (<200 mm/year). • Two aquifers, ‘perched’ and ‘mean sea level’ (MSL) separated by impermeable clay. • Water level in MSL aquifer depressed to 5 m above sea level by abstraction

Commissioning of the ATLAS Level-1 Trigger with Cosmic Rays

The ATLAS detector at CERN's Large Hadron Collider will be exposed to proton-proton collisions from beams crossing at 40 MHz. A three-level trigger system was designed to select potentially interesting events and reduce the incoming rate to 100-200 Hz. The first trigger level (LVL1) is implemented in custom-built electronics, the second and third trigger levels are realized in software. Based on calorimeter information and hits in dedicated muon-trigger detectors, the LVL1 decision is made by the central-trigger processor yielding an output rate of less than 100 kHz. The allowed latency for the trigger decision at this stage is less than 2.5 microseconds. Installation of the final LVL1 trigger system at the ATLAS site is in full swing, to be completed later this year. We present a status report of the main components of the first-level trigger and the in-situ commissioning of the full trigger chain with cosmic-ray muons.Comment: On behalf of the ATLAS TDAQ Level-1 Trigger Group. Proceedings for 2007 Europhysics Conference on High Energy Physics, Manchester, July 200

Children First! Child Care Assistance in Erie County

Child care subsidies are distributed in each county in New York by the county’s Department of Social Services. Due to a drop in state funding, Erie County has changed its eligibility level from 200% to 125% of the poverty line. The former level for eligibility should be reinstated because subsidized child care has social, financial and societal benefits

S&P Breaks Key Tecnical Mark

The S&P fell below its 200-day moving average, a key negative technical indicator. Investors should pay close attention to see if this level holds. See article here, yahoo

Frictional magnetodrag between spatially separated two-dimensional electron systems: Coulomb versus phonon mediated electron-electron interaction

We study the frictional drag due to Coulomb and phonon mediated electron-electron interaction in a double layer electron system exposed to a perpendicular magnetic field. Within the random phase approximation we calculate the dispersion relation of the intra Landau level magnetoplasmons at finite temperatures and distinguish their contribution to the magnetodrag. We calculate the transresistivity $\rho_{Drag}$ as a function of magnetic field $B$, temperature $T$, and interlayer spacing $\Lambda$ for a matched electron density. For $\Lambda =200$ nm we find that $\rho_{Drag}$ is solely due to phonon exchange and shows no double-peak structure as a function of $B$. For $\Lambda =30$ nm, $\rho_{Drag}$ shows the double-peak structure and is mainly due to Coulomb interaction. The value of $\rho_{Drag}$ is about 0.3 $\Omega$ at T=2 K and for the half-filled second Lanadau level, which is about 13 times larger than the value for $\Lambda =200$ nm. At lower edge of the temperature interval from 0.1 to 8 K, $\rho_{Drag}/ T^{2}$ remains finite for $\Lambda =30$ nm while it tends to zero for $\Lambda =200$ nm. Near the upper edge of this interval, $\rho_{Drag}$ for $\Lambda =30$ nm is approximately linear in $T$ while for $\Lambda =200$ nm it decreases slowly in $T$. Therefore, the peak of $\rho_{Drag}/ T^{2}$ is very sharp for $\Lambda =200$ nm. This strikingly different magnetic field and temperature dependence of $\rho_{Drag}$ ascribe we mainly to the weak screening effect at large interlayer separations.Comment: replaced with revised versio

Singe Top Production at LEP 200

We present exact tree level cross sections for the single top production process $e^- e^+ \rightarrow e^- \bar{\nu}_e t \bar{b}$ at LEP~200. The results reproduce roughly those obtained earlier by using the equivalent real photon approximation and we confirm the observation that detecting a top heavier than half the c.m.~energy is not feasible at LEP~200. The calculation has been performed by a new automatic Feynman amplitude generator MadGraph which produces HELAS code for the helicity amplitudes.Comment: 7 pages, 4 postscript figure