3,546 research outputs found
Extraction of contact resistance in carbon nanofiber via interconnects with varying lengths
A method to extract the contact resistance and bulk resistivity of vertically grown carbon nanofibers (CNFs) or similar one-dimensional nanostructures is described. Using a silicon-compatible process to fabricate a terrace test structure needed for the CNF length variation, the contact resistance is extracted by measuring in situ the resistances of individual CNFs with different lengths and within a small range of diameters using a nanoprober inside a scanning electron microscope. Accurate determination of contact resistances for various combinations of catalysts and underlayer metals can lead to eventual optimization of materials’ growth and device fabrication processes for CNF via interconnects
DETERMINATION OF PCB ELIMINATION COEFFICIENTS IN ROUND GOBY AND TUBENOSE GOBY
Whole-body elimination coefficients of polychlorinated biphenyls (PCBs) were determined in two Great Lakes invasive fish species, round goby (Neogobius melanostomus) and tubenose goby (Proterorhinus semilunaris). Elimination rates were determined for a set of model PCB congeners (n=12 congeners) dosed to fish by intraperitoneal injection and allowed to depurate at a temperature of 21.4oC for 90 d. Eight PCBs (PCB 6, 13, 21, 57, 62, 68, 89, 112 and 125) exhibited significant elimination by round goby and had corresponding half lives ranging from 13 to 39.8 d. For tubenose goby, four congeners (PCBs 21, 58, 62 and 68) exhibited significant elimination with half lives in the range from 18.8 to 48.8 d. Whole-body elimination rate coefficients were significantly higher for round gobies compared to tubenose goby. In both cases, PCB elimination rate coefficients were negatively related to chemical log KOW
Cohesive/Adhesive strengths of CsOH-chemisorbed SS304 surfaces
During the Fukushima Daiichi Nuclear Power Plant (1F) accident, volatile radioactive fission products (FPs) such as Cs-137 were released, which significantly influenced mid- to long-term decommissioning strategies. A substantial amount of the remaining cesium in the pressure vessel may have deposited onto the 304 stainless steel (SS304) steam separators and dryers. This deposited cesium presents a safety hazard during 1F’s decommissioning, as it can generate radioactive dust and complicate waste storage. However, the cohesive and adhesive strengths of CsOH-chemisorbed oxide scales, crucial for understanding the release of cesium-bearing particles from SS304 surfaces, remain undefined. In this study, we explore how CsOH chemisorption affects the cohesive and adhesive strengths between oxide scales and SS304 substrates using a scratch tester. Our tests revealed that cracks formed at approximately the same load, but the overall cohesive strength of the oxide scales decreased following CsOH chemisorption. Furthermore, the transition from cracks to bulk separation occurred more rapidly in CsOH-chemisorbed SS304 substrates, especially those with lower silicon content. Finally, we found that adhesive failure could not be achieved even at 70 N, suggesting that the deposited cesium cannot be completely removed from SS304 during the decommissioning of 1F
Bose-Einstein Condensation of Long-Lifetime Polaritons in Thermal Equilibrium
Exciton-polaritons in semiconductor microcavities have been used to
demonstrate quantum effects such as Bose-Einstein condensation, superfluity,
and quantized vortices. However, in these experiments, the polaritons have not
reached thermal equilibrium when they undergo the transition to a coherent
state. This has prevented the verification of one of the canonical predictions
for condensation, namely the phase diagram. In this work, we have created a
polariton gas in a semiconductor microcavity in which the quasiparticles have a
lifetime much longer than their thermalization time. This allows them to reach
thermal equilibrium in a laser-generated confining trap. Their energy
distributions are well fit by equilibrium Bose-Einstein distributions over a
broad range of densities and temperatures from very low densities all the way
up to the threshold for Bose-Einstein condensation. The good fits of the
Bose-Einstein distribution over a broad range of density and temperature imply
that the particles obey the predicted power law for the phase boundary of
Bose-Einstein condensation
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