Search results for "current"

showing 10 items of 2224 documents

ChemInform Abstract: Photoelectrochemical Study of Electrochemically Formed Semiconducting Yttrium Hydride (YH3-x).

2010

Abstract The first photoelectrochemical study of semiconducting YH 3− x films formed by etching bulk Y metal in 0.5 M H 2 SO 4 solution is reported. The formation of semiconducting hydride having an indirect optical band gap, E g opt , of about 2.35 eV is confirmed by in situ photocurrent spectroscopy. The photoelectrochemical behaviour of such a phase was investigated both in alkaline and in acidic solutions. The flat band potential was estimated to be U fb =−1.25 V/NHE, independent of pH.

In situMetalPhotocurrentHydrideBand gapEtching (microfabrication)Chemistryvisual_artPhase (matter)visual_art.visual_art_mediumAnalytical chemistryGeneral MedicineSpectroscopyChemInform
researchProduct

Study and optimization of near UV InGaN/GaN based Light Emitting Diodes at low injection current regimes

2006

InGaN/GaN LEDs low injection currentSettore ING-INF/01 - Elettronica
researchProduct

Exchange Rate and Macroeconomic Fluctuations as Sources of Luck in CEO Compensation

2011

Exchange rate and other macroeconomic fluctuations can be considered sources of good or bad “luck” for corporate performance. Incentive effects of performance-based compensation for management may be weakened or biased by macroeconomic influences on remuneration depending on the ability of management to adjust operations. We decompose the changes in CEO-compensation to distinguish between (anticipated-and unanticipated) macroeconomic and “intrinsic” sources. Total US CEO-compensation is measured both including options awarded and options exercised. Both depend strongly on variations in macro-factors but the time patterns differ. Allowing for asymmetric effects on compensation we find that c…

IncentiveCurrent compensationExchange rateExecutive compensationLuckmedia_common.quotation_subjectRemunerationEconomicsMonetary economicsSalarymedia_commonCompensation (engineering)SSRN Electronic Journal
researchProduct

"Table 3" of "Spin asymmetries A(1) and structure functions g1 of the proton and the deuteron from polarized high energy muon scattering."

1998

The virtual photon proton asymmetries in smaller X and Q**2 bins. bins. Errors are statistical only.

Inclusive13.729-18.903Asymmetry MeasurementNeutral CurrentDeep Inelastic ScatteringAstrophysics::Cosmology and Extragalactic AstrophysicsPhysics::Data Analysis; Statistics and ProbabilityMU+ P --> MU+ XMuon productionASYM
researchProduct

"Table 1" of "Spin asymmetries A(1) and structure functions g1 of the proton and the deuteron from polarized high energy muon scattering."

1998

The virtual photon proton asymmetries.

Inclusive13.729-18.903Asymmetry MeasurementNuclear TheoryNeutral CurrentDeep Inelastic ScatteringPhysics::Accelerator PhysicsPhysics::OpticsHigh Energy Physics::ExperimentNuclear ExperimentMU+ P --> MU+ XMuon productionASYM
researchProduct

"Table 9" of "Spin asymmetries A(1) and structure functions g1 of the proton and the deuteron from polarized high energy muon scattering."

1998

No description provided.

Inclusive13.729-18.903Neutral CurrentDeep Inelastic ScatteringMU+ P --> MU+ XINTG1*DXMuon productionMU+ DEUT --> MU+ X
researchProduct

"Table 12" of "Spin asymmetries A(1) and structure functions g1 of the proton and the deuteron from polarized high energy muon scattering."

1998

The first moment integral for the nonsinglet structure function G1(NS).

Inclusive13.729-18.903Neutral CurrentDeep Inelastic ScatteringMU+ P --> MU+ XINTG1*DXMuon productionMU+ DEUT --> MU+ X
researchProduct

"Table 6" of "Spin asymmetries A(1) and structure functions g1 of the proton and the deuteron from polarized high energy muon scattering."

1998

The spin-dependent structure function G1(P) evolved to Q**2=10 GeV**2.. The second systematic (DSYS) error is due to the uncertainty in the QCD evolution.

Inclusive13.729-18.903Spin Dependent Structure FunctionG1Neutral CurrentDeep Inelastic ScatteringHigh Energy Physics::ExperimentMU+ P --> MU+ XMuon production
researchProduct

"Table 11" of "Spin asymmetries A(1) and structure functions g1 of the proton and the deuteron from polarized high energy muon scattering."

1998

The nonsinglet spin-dependent structure function G1(NS) evolved to Q**2=10 GeV**2.. The second systematic (DSYS) error is due to the uncertainty in the QCD evolution.

Inclusive13.729-18.903Spin Dependent Structure FunctionG1Neutral CurrentDeep Inelastic ScatteringHigh Energy Physics::ExperimentMU+ P --> MU+ XMuon productionMU+ DEUT --> MU+ X
researchProduct

"Table 10" of "Spin asymmetries A(1) and structure functions g1 of the proton and the deuteron from polarized high energy muon scattering."

1998

The nonsinglet spin-dependent structure function G1(NS) calculated from themeasured the G1(P) and G1(D).

Inclusive13.729-18.903Spin Dependent Structure FunctionG1Neutral CurrentDeep Inelastic ScatteringMU+ P --> MU+ XMuon productionMU+ DEUT --> MU+ X
researchProduct