Search results for "Cross Section"

showing 10 items of 3111 documents

"Table 1" of "First measurement of the quark to photon fragmentation function"

1995

2-jet events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).

FDSIG/SIGAstrophysics::High Energy Astrophysical PhenomenaIntegrated Cross SectionE+ E- --> GAMMA QUARK QUARKBARJet ProductionCross SectionE+ E- --> (HADRONS) 2HADRONDijet ProductionE+ E- ScatteringExclusiveHigh Energy Physics::Experiment90.912E+ E- --> 2JET
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"Table 2" of "First measurement of the quark to photon fragmentation function"

1995

2-jet events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).

FDSIG/SIGAstrophysics::High Energy Astrophysical PhenomenaIntegrated Cross SectionE+ E- --> GAMMA QUARK QUARKBARJet ProductionCross SectionE+ E- --> (HADRONS) 2HADRONDijet ProductionE+ E- ScatteringExclusiveHigh Energy Physics::Experiment90.912E+ E- --> 2JET
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"Table 5" of "First measurement of the quark to photon fragmentation function"

1995

3-JET events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).

FDSIG/SIGE+ E- --> 3JETAstrophysics::High Energy Astrophysical PhenomenaE+ E- ScatteringIntegrated Cross SectionExclusiveHigh Energy Physics::ExperimentE+ E- --> GAMMA QUARK QUARKBAR90.912Jet ProductionCross SectionE+ E- --> (HADRONS) 2HADRON
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"Table 6" of "First measurement of the quark to photon fragmentation function"

1995

3-JET events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).

FDSIG/SIGE+ E- --> 3JETAstrophysics::High Energy Astrophysical PhenomenaE+ E- ScatteringIntegrated Cross SectionExclusiveHigh Energy Physics::ExperimentE+ E- --> GAMMA QUARK QUARKBAR90.912Jet ProductionCross SectionE+ E- --> (HADRONS) 2HADRON
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"Table 7" of "First measurement of the quark to photon fragmentation function"

1995

3-JET events. Variable Z has been defined as E(gamma)/(E(gamma)+E(had)), where E(gamma) is the energy of the hard photon in 'photon-jet', E(had) is the energy of the rest hadrons in jet. Ycut is jet resolution parameter (see paper).

FDSIG/SIGE+ E- --> 3JETAstrophysics::High Energy Astrophysical PhenomenaE+ E- ScatteringIntegrated Cross SectionExclusiveHigh Energy Physics::ExperimentE+ E- --> GAMMA QUARK QUARKBAR90.912Jet ProductionCross SectionE+ E- --> (HADRONS) 2HADRON
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Know your full potential: Quantitative Kelvin probe force microscopy on nanoscale electrical devices

2018

In this study we investigate the influence of the operation method in Kelvin probe force microscopy (KPFM) on the measured potential distribution. KPFM is widely used to map the nanoscale potential distribution in operating devices, e.g., in thin film transistors or on cross sections of functional solar cells. Quantitative surface potential measurements are crucial for understanding the operation principles of functional nanostructures in these electronic devices. Nevertheless, KPFM is prone to certain imaging artifacts, such as crosstalk from topography or stray electric fields. Here, we compare different amplitude modulation (AM) and frequency modulation (FM) KPFM methods on a reference s…

FM-KPFMMaterials scienceNanostructureGeneral Physics and Astronomy02 engineering and technologylcsh:Chemical technology01 natural sciencesAM-KPFMlcsh:TechnologyFull Research Paperlaw.inventioncrosstalkfield effect transistorlawElectric field0103 physical sciencesMicroscopySolar cellNanotechnologyfrequency modulation sidebandGeneral Materials Sciencelcsh:TP1-1185Electrical and Electronic Engineeringlcsh:Sciencequantitative Kelvin probe force microscopy010302 applied physicsKelvin probe force microscopecross sectionbusiness.industrylcsh:Tfrequency modulation heterodyne021001 nanoscience & nanotechnologyAM off resonanceAM lift modelcsh:QC1-999NanoscienceAM second eigenmodesolar cellsOptoelectronicsField-effect transistorlcsh:Q0210 nano-technologybusinessFrequency modulationlcsh:PhysicsVoltageBeilstein Journal of Nanotechnology
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Simultaneous measurement of the muon neutrino charged-current cross section on oxygen and carbon without pions in the final state at T2K

2020

Authors: K. Abe,56 N. Akhlaq,45 R. Akutsu,57 A. Ali,32 C. Alt,11 C. Andreopoulos,54,34 L. Anthony,21 M. Antonova,19 S. Aoki,31 A. Ariga,2 T. Arihara,59 Y. Asada,69 Y. Ashida,32 E. T. Atkin,21 Y. Awataguchi,59 S. Ban,32 M. Barbi,46 G. J. Barker,66 G. Barr,42 D. Barrow,42 M. Batkiewicz-Kwasniak,15 A. Beloshapkin,26 F. Bench,34 V. Berardi,22 L. Berns,58 S. Bhadra,70 S. Bienstock,53 S. Bolognesi,6 T. Bonus,68 B. Bourguille,18 S. B. Boyd,66 A. Bravar,13 D. Bravo Berguño,1 C. Bronner,56 S. Bron,13 A. Bubak,51 M. Buizza Avanzini ,10 T. Campbell,7 S. Cao,16 S. L. Cartwright,50 M. G. Catanesi,22 A. Cervera,19 D. Cherdack,17 N. Chikuma,55 G. Christodoulou,12 M. Cicerchia,24,† J. Coleman,34 G. Collazu…

Fermi gasPhysics::Instrumentation and DetectorsMonte Carlo methodmeasured [channel cross section]KAMIOKANDEmuon neutrino01 natural sciencesPhysics Particles & FieldsHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)secondary beam [neutrino/mu][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Particle Physics ExperimentsMuon neutrinoQDCharged currentQCPhysicsneutrino: energy spectrumJ-PARC LabPhysicsinteraction [neutrino nucleus]T2K experimentoscillation [neutrino]Monte Carlo [numerical calculations]suppressionNuclear & Particles PhysicskinematicsPhysical Sciences0202 Atomic Molecular Nuclear Particle and Plasma PhysicsGround statenumerical calculations: Monte Carlochannel cross section: measuredParticle Physics - Experiment530 PhysicsFOS: Physical sciencesAstronomy & Astrophysics530Nuclear physicsPionnear detector0103 physical sciencessimultaneous measurement0201 Astronomical and Space SciencesSCATTERINGddc:530010306 general physicsNeutrino oscillation0206 Quantum Physicscross section: charged currentMuonScience & Technologynucleus: ground stateNUCLEI010308 nuclear & particles physicsnucleus: targethep-excarbonenergy spectrum [neutrino]neutrino nucleus: interactionground state [nucleus]neutrino/mu: secondary beamtarget [nucleus]random phase approximationcharged current [cross section]High Energy Physics::Experimentneutrino: oscillationoxygenexperimental resultsPhysical Review D
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"Table 5" of "In-medium modifications of the pi pi interaction in photon-induced reactions."

2005

Differential cross section for PI0PI+/- production with a Carbon target. Errors are statistical only.

GAMMA C --> PI0 PI-Single Differential Cross SectionGAMMA C --> PI0 PI+PhotoproductionDSIG/DMExclusiveGAMMA NUCLEUS --> PI- PI0GAMMA NUCLEUS --> PI+ PI0
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"Table 2" of "C-12 (gamma,p) B-11 cross-section from 80 to 157 MeV"

1995

EX = 7 (FROM 6.5 TO 8.0 MEV). ANGULAR BINS OF 5 DEG WIDTH.

GAMMA NUCLEUS --> BOR11* PPhotoproductionIntegrated Cross SectionExclusiveGAMMA C12 --> BOR11* PCross SectionSIG
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"Table 3" of "C-12 (gamma,p) B-11 cross-section from 80 to 157 MeV"

1995

EX = 13 (FROM 12.0 TO 13.5 MEV). ANGULAR BINS OF 5 DEG WIDTH.

GAMMA NUCLEUS --> BOR11* PPhotoproductionIntegrated Cross SectionExclusiveGAMMA C12 --> BOR11* PCross SectionSIG
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