Search results for "CLEAR"

showing 10 items of 27042 documents

Johnson-Nyquist Noise Effects in Neutron Electric-Dipole-Moment Experiments

2021

Magnetic Johnson-Nyquist noise (JNN) originating from metal electrodes, used to create a static electric field in neutron electric-dipole-moment (nEDM) experiments, may limit the sensitivity of measurements. We present here the first dedicated study on JNN applied to a large-scale long-measurement-time experiment with the implementation of a co-magnetometry. In this study, we derive surface- and volume-averaged root-mean-square normal noise amplitudes at a certain frequency bandwidth for a cylindrical geometry. In addition, we model the source of noise as a finite number of current dipoles and demonstrate a method to simulate temporal and three-dimensional spatial dependencies of JNN. The c…

noiseNeutron electric dipole momentMagnetometerAtomic Physics (physics.atom-ph)FOS: Physical sciencesNeutron Physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNoise (electronics)010305 fluids & plasmaslaw.inventionPhysics - Atomic PhysicslawElectric field0103 physical sciencesNeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicshigh-precision experimentsprecision measurementJohnson–Nyquist noiseAtomic and molecular structure and dynamics[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Computational physicsDipoleNuclear Spin ResonanceAmplitudeElectromagnetic Field Calculations
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Latest Developments and Results of Radiation Tolerance CMOS Sensors with Small Collection Electrodes

2020

The development of radiation hard Depleted Monolithic Active Pixel Sensors (DMAPS) targets the replacement of hybrid pixel detectors to meet radiation hardness requirements of at least 1.5e16 1 MeV neq/cm2 for the HL-LHC and beyond. DMAPS were designed and tested in the TJ180 nm TowerJazz CMOS imaging technology with small electrodes pixel designs. This technology reduces costs and provides granularity of 36.4x36.4 um2 with low power operation (1 uW/pixel), low noise of ENC < 20 e-, a small collection electrode (3 um) and fast signal response within 25 ns bunch crossing. This contribution will present the latest developments after the MALTA and Mini-MALTA sensors. It will illustrate the imp…

noiseParticle tracking detectors ; Radiation-hard detectors ; Electronic detector readout concepts ; CMOS sensors ; Monolithic active pixel sensorsMaterials science010308 nuclear & particles physicsbusiness.industryintegrated circuitelectrode01 natural sciencesCMOSRadiation toleranceefficiency0103 physical sciencesElectrodeHardware_INTEGRATEDCIRCUITSelectronics: readoutOptoelectronicssemiconductor detector[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental Techniquescontrol system010306 general physicsbusiness
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Exclusive Vector Meson Production at the EIC

2020

We discuss how vector meson production at the future Electron Ion Collider can be used to probe non-linear dynamics in heavy nuclei. Additionally, the potential to study the evolution of proton and nuclear geometries with event-by-event fluctuations is illustrated. nonPeerReviewed

non-linear dynamics in heavy nucleiNuclear Theoryvector meson productionhiukkasfysiikkaNuclear Experiment
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Liver stiffness quantification in biopsy-proven nonalcoholic fatty liver disease patients using shear wave elastography in comparison with transient …

2021

Purpose: This study prospectively assessed the performance of liver stiffness measurements using point shear-wave elastography (p-SWE) in comparison with transient elastography (TE) in patients with biopsy-proven nonalcoholic fatty liver disease (NAFLD). Methods: Fifty-six consecutive adult patients with a histological diagnosis of NAFLD prospectively underwent TE and p-SWE on the same day. The median of 10 measurements (SWE-10), the first five (SWE-5), and the first three (SWE-3) measurements were analyzed for p-SWE. Liver biopsy was considered as the reference standard for liver fibrosis grade. Receiver operating characteristic (ROC) curves and areas under the ROC curves (AUROCs) were cal…

nonalcoholic fatty liver diseasemedicine.medical_specialtyGastroenterologySettore MED/01 - Statistica Medica030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineLiver stiffnessInternal medicineStatistical significanceBiopsyNonalcoholic fatty liver diseaseMedical technologymedicineRadiology Nuclear Medicine and imagingnonalcoholic steatohepatitisR855-855.5shear wave elastographymedicine.diagnostic_testReceiver operating characteristicbusiness.industryNonalcoholic fatty liver disease Nonalcoholic steatohepatitis Shear wave elastography Transient elastography Liver stiffnessmedicine.diseasetransient elastographyliver stiffnessLiver biopsyOriginal Article030211 gastroenterology & hepatologyElastographySettore MED/36 - Diagnostica Per Immagini E RadioterapiabusinessTransient elastographyUltrasonography
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Mass measurements of As, Se, and Br nuclei, and their implication on the proton-neutron interaction strength toward the N=Z line

2021

Mass measurements of the $^{69}$As, $^{70,71}$Se and $^{71}$Br isotopes, produced via fragmentation of a $^{124}$Xe primary beam at the FRS at GSI, have been performed with the multiple-reflection time-of-flight mass spectrometer (MR-TOF-MS) of the FRS Ion Catcher with an unprecedented mass resolving power of almost 1,000,000. For the $^{69}$As isotope, this is the first direct mass measurement. A mass uncertainty of 22 keV was achieved with only 10 events. For the $^{70}$Se isotope, a mass uncertainty of 2.6 keV was obtained, corresponding to a relative accuracy of $\delta$m/m = 4.0$\times 10^{-8}$, with less than 500 events. The masses of the $^{71}$Se and $^{71}$Br isotopes were measured…

nucl-thNuclear TheoryFOS: Physical sciencesInteraction strengthnucl-exMass spectrometry01 natural sciences7. Clean energyarseeniIonNuclear Theory (nucl-th)Nuclear physicsFragmentation (mass spectrometry)0103 physical sciencesddc:530NeutronbromiNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicsIsotope010308 nuclear & particles physicsMass measurementAtomic massseleeniydinfysiikkaPhysical Review C
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Saturation and forward jets in proton-lead collisions at the LHC

2019

We investigate the forward-jet energy spectrum within the Color Glass Condensate framework at 5 TeV center-of-mass energy. In particular, we focus on the kinematic range covered by the CMS-CASTOR calorimeter. We show that our saturation-model calculations are compatible with the CASTOR measurements and that to optimally reproduce the data, effects of multi-parton interactions need to be included. We predict a significant nuclear suppression - reaching down to 50% at the lowest considered jet energies $E_{\rm jet} \sim 500 \, {\rm GeV}$.

nucl-thNuclear TheoryRAPIDITIESAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesNUCLEARhiukkasfysiikka01 natural sciences7. Clean energy114 Physical sciencesColor-glass condensateNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEnergy spectrumJ/PSI PRODUCTION010306 general physicsSaturation (magnetic)Nuclear theoryINELASTIC EP SCATTERINGParticle Physics - PhenomenologyPhysicsLarge Hadron Collider010308 nuclear & particles physicsCOLOR GLASS CONDENSATEhep-phHADRON-PRODUCTIONDEUTERON-GOLD COLLISIONSHigh Energy Physics - PhenomenologyNuclear Physics - TheoryHigh Energy Physics::Experiment
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Shape staggering of midshell mercury isotopes from in-source laser spectroscopy compared with density-functional-theory and Monte Carlo shell-model c…

2019

Neutron-deficient Hg177-185 isotopes were studied using in-source laser resonance-ionization spectroscopy at the CERN-ISOLDE radioactive ion-beam facility in an experiment combining different detection methods tailored to the studied isotopes. These include either α-decay tagging or multireflection time-of-flight gating for isotope identification. The endpoint of the odd-even nuclear shape staggering in mercury was observed directly by measuring for the first time the isotope shifts and hyperfine structures of Hg177-180. Changes in the mean-square charge radii for all mentioned isotopes, magnetic dipole, and electric quadrupole moments of the odd-A isotopes and arguments in favor of I=7/2 s…

nucl-thNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]3106ResearchInstitutes_Networks_Beacons/photon_science_instituteharmonic-oscillator basisMonte Carlo methodFOS: Physical sciencesPhoton Science Institute[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exNuclear Structure01 natural sciences7. Clean energyodd-massNuclear Theory (nucl-th)Atomic orbitalCharge radius0103 physical sciencesNuclear Physics - ExperimentDalton Nuclear InstituteNeutronneutron-deficient hgNuclear Experiment (nucl-ex)nuclear charge-distribution010306 general physicsNuclear ExperimentNuclear ExperimentHyperfine structurePhysics010308 nuclear & particles physicsGénéralitésexcited structuresstatesResearchInstitutes_Networks_Beacons/dalton_nuclear_institutehyperfine-structure13. Climate actionNuclear Physics - Theoryoblate-prolate transitionaxially deformed solutionQuadrupolemomentsDensity functional theoryAtomic physicsPräzisionsexperimente - Abteilung BlaumMagnetic dipole
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Heavy ions at the Future Circular Collider

2016

The Future Circular Collider (FCC) Study is aimed at assessing the physics potential and the technical feasibility of a new collider with centre-of-mass energies, in the hadron-hadron collision mode, seven times larger than the nominal LHC energies. Operating such machine with heavy ions is an option that is being considered in the accelerator design studies. It would provide, for example, Pb-Pb and p-Pb collisions at sqrt{s_NN} = 39 and 63 TeV, respectively, per nucleon-nucleon collision, with integrated luminosities above 30 nb^-1 per month for Pb-Pb. This is a report by the working group on heavy-ion physics of the FCC Study. First ideas on the physics opportunities with heavy ions at th…

nucl-thNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]heavy-ion physicsFOS: Physical scienceshiukkasfysiikka[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]SDG 7 - Affordable and Clean EnergyNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentParticle Physics - Phenomenology/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energyhep-exHigh Energy Physics::Phenomenologyhep-phHigh Energy Physics - PhenomenologyFuture Circular Collider[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment
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The beta-delayed proton and gamma decay of 27P for nuclear astrophysics

2013

The creation site of 26Al is still under debate. It is thought to be produced in hydrogen burning and in explosive helium burning in novae and supernovae, and possibly also in the H-burning in outer shells of red giant stars. Also, the reactions for its creation or destruction are not completely known. When 26Al is created in novae, the reaction chain is: 24Mg(p, γ) 25Al(β +ν) 25Mg(p, γ) 26Al, but this chain can be by-passed by another chain, 25Al(p, γ) 26Si(p, γ) 27P and it can also be destroyed directly. The reaction 26mAl(p, γ) 27Si∗ is another avenue to bypass the production of 26Al and it is dominated by resonant capture. We find and study these resonances by an indirect method, throug…

nuclear astro-physicsindirect methodsdaughter nucleusproduction ofresonant capturehelium-burningreaction chainslow-energy protons
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Recent experiments at the JYFLTRAP Penning trap

2020

AbstractThe JYFLTRAP double Penning trap mass spectrometer at the Ion Guide Isotope Separator On-Line (IGISOL) facility offers excellent possibilities for high-precision mass measurements of radioactive ions. Around 400 atomic masses, including around 50 isomeric states, have been measured since JYFLTRAP became operational. JYFLTRAP has also been used as a high-resolution mass separator for decay spectroscopy experiments as well as an ion counter for fission yield studies. In this contribution, an overview of recent activities at the JYFLTRAP Penning trap is given, with a focus on nuclei discussed in the PLATAN2019 meeting.

nuclear binding energymassaspektrometriaNuclear and High Energy PhysicstutkimuslaitteetFission product yieldMass spectrometry7. Clean energy01 natural sciencesIonNuclear physicsPhysics in General0103 physical sciencesPhysical and Theoretical Chemistry010306 general physicsSpectroscopyPhysicsIsotope010308 nuclear & particles physicsatomic masspenning trapCondensed Matter PhysicsPenning trapAtomic and Molecular Physics and OpticsAtomic massNuclear binding energyisomersydinfysiikkaHyperfine Interactions
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