Search results for "INELASTIC"

showing 10 items of 700 documents

"Table 28" of "Measurement of the proton and deuteron structure functions, F2(p) and F2(d), and of the ratio sigma(L)/sigma(T)."

1997

Corrected F2D measurements averaged over all energies. Data are the statistically weighted averages given at the centre of each bin.

F2InclusiveStructure FunctionDeep Inelastic ScatteringHigh Energy Physics::ExperimentMUON DEUT --> MUON XMuon production
researchProduct

"Table 22" of "Measurement of the proton and deuteron structure functions, F2(p) and F2(d), and of the ratio sigma(L)/sigma(T)."

1997

Corrected F2D measurements averaged over all energies. Data are the statistically weighted averages given at the centre of each bin.

F2InclusiveStructure FunctionDeep Inelastic ScatteringHigh Energy Physics::ExperimentMUON DEUT --> MUON XMuon production
researchProduct

"Table 26" of "Measurement of the proton and deuteron structure functions, F2(p) and F2(d), and of the ratio sigma(L)/sigma(T)."

1997

Corrected F2D measurements averaged over all energies. Data are the statistically weighted averages given at the centre of each bin.

F2InclusiveStructure FunctionDeep Inelastic ScatteringHigh Energy Physics::ExperimentMUON DEUT --> MUON XMuon production
researchProduct

"Table 31" of "Measurement of the proton and deuteron structure functions, F2(p) and F2(d), and of the ratio sigma(L)/sigma(T)."

1997

Corrected F2D measurements averaged over all energies. Data are the statistically weighted averages given at the centre of each bin.

F2InclusiveStructure FunctionDeep Inelastic ScatteringHigh Energy Physics::ExperimentMUON DEUT --> MUON XMuon production
researchProduct

"Table 21" of "Measurement of the proton and deuteron structure functions, F2(p) and F2(d), and of the ratio sigma(L)/sigma(T)."

1997

Corrected F2D measurements averaged over all energies. Data are the statistically weighted averages given at the centre of each bin.

F2InclusiveStructure FunctionDeep Inelastic ScatteringHigh Energy Physics::ExperimentMUON DEUT --> MUON XMuon production
researchProduct

"Table 19" of "Measurement of the proton and deuteron structure functions, F2(p) and F2(d), and of the ratio sigma(L)/sigma(T)."

1997

Corrected F2D measurements averaged over all energies. Data are the statistically weighted averages given at the centre of each bin.

F2InclusiveStructure FunctionDeep Inelastic ScatteringHigh Energy Physics::ExperimentMUON DEUT --> MUON XMuon production
researchProduct

"Table 27" of "Measurement of the proton and deuteron structure functions, F2(p) and F2(d), and of the ratio sigma(L)/sigma(T)."

1997

Corrected F2D measurements averaged over all energies. Data are the statistically weighted averages given at the centre of each bin.

F2InclusiveStructure FunctionDeep Inelastic ScatteringHigh Energy Physics::ExperimentMUON DEUT --> MUON XMuon production
researchProduct

"Table 2" of "Precision measurement of structure function ratios for Li-6, C-12 and Ca-40"

1992

Overall normalization error of 0.8%, due to uncertainties in target thickness, not included in the table.

F2InclusiveStructure FunctionNeutral CurrentDeep Inelastic ScatteringMU+ NUCLEUS --> MU+ XMU+ CA --> MU+ XMU+ LI --> MU+ XMuon production
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"Table 3" of "Precision measurement of the structure function ratios F2 (He) / F2 (D), F2 (C) / F2 (D) and F2 (Ca) / F2 (D)"

1991

No description provided.

F2InclusiveStructure FunctionNeutral CurrentDeep Inelastic ScatteringMU+ NUCLEUS --> MU+ XMU+ CA --> MU+ XMuon productionMU+ DEUT --> MU+ X
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Supercurrent Induced Charge-Spin Conversion in Spin-Split Superconductors

2017

We study spin-polarized quasiparticle transport in a mesoscopic superconductor with a spin- splitting field in the presence of co-flowing supercurrent. In such a system, the nonequilibrium state is characterized by charge, spin, energy and spin energy modes. Here we show that in the presence of both spin splitting and supercurrent, all these modes are mutually coupled. As a result, the supercurrent can convert charge imbalance, that in the presence of spin splitting decays on a relatively short scale, to a long-range spin accumulation decaying only via inelastic scattering. This effect enables coherent charge-spin conversion controllable by a magnetic flux, and it can be detected by studyin…

Field (physics)superfluid densityFOS: Physical sciences02 engineering and technologyInelastic scattering01 natural sciencessuprajohteetSuperconductivity (cond-mat.supr-con)transport propertiesCondensed Matter::Superconductivity0103 physical sciences010306 general physicsSpin-½PhysicsSuperconductivityspin accumulationMesoscopic physicsspin currentta114Condensed matter physicsCondensed Matter - SuperconductivityCharge (physics)021001 nanoscience & nanotechnologyspin relaxationMagnetic fluxQuasiparticleCondensed Matter::Strongly Correlated Electrons0210 nano-technology
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