0000000000054558

AUTHOR

Israel Mardor

showing 17 related works from this author

Quasi-elastic polarization-transfer measurements on the deuteron in anti-parallel kinematics

2019

We present measurements of the polarization-transfer components in the H2(e→,e′p→) reaction, covering a previously unexplored kinematic region with large positive (anti-parallel) missing momentum, pmiss, up to 220MeV/c, and Q2=0.65 (GeV/c)2. These measurements, performed at the Mainz Microtron (MAMI), were motivated by theoretical calculations which predict small final-state interaction (FSI) effects in these kinematics, making them favorable for searching for medium modifications of bound nucleons in nuclei. We find in this kinematic region that the measured polarization-transfer components Px and Pz and their ratio agree with the theoretical calculations, which use free-proton form factor…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciencesKinematicsPolarization (waves)01 natural scienceslcsh:QC1-999NATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Parallel kinematicsNuclear physicsDeuterium0103 physical sciencesddc:530Nuclear Experiment (nucl-ex)010306 general physicsNucleonNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Nuclear ExperimentMicrotronlcsh:Physicspolarization-transfer ; deuteron ; anti-parallel kinematics
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Separation of atomic and molecular ions by ion mobility with an RF carpet

2021

Gas-filled stopping cells are used at accelerator laboratories for the thermalization of high-energy radioactive ion beams. Common challenges of many stopping cells are a high molecular background of extracted ions and limitations of extraction efficiency due to space-charge effects. At the FRS Ion Catcher at GSI, a new technique for removal of ionized molecules prior to their extraction out of the stopping cell has been developed. This technique utilizes the RF carpet for the separation of atomic ions from molecular contaminant ions through their difference in ion mobility. Results from the successful implementation and test during an experiment with a 600~MeV/u $^{124}$Xe primary beam are…

low-energy RIBPhysics - Instrumentation and DetectorsOrders of magnitude (temperature)beam purificationFOS: Physical sciences010402 general chemistrynucl-ex01 natural sciences530Ionmenetelmätion mobilityIonizationMoleculeddc:530Physical and Theoretical ChemistryfysiikkaNuclear Experiment (nucl-ex)Nuclear ExperimentInstrumentationphysics.ins-detSpectroscopyIon transporterRange (particle radiation)ionitChemistry010401 analytical chemistryExtraction (chemistry)gas cellpuhdistusInstrumentation and Detectors (physics.ins-det)Condensed Matter Physics0104 chemical sciencesmolecular contaminationBeamlinespace chargeAtomic physicserottaminen (tekniikka)epäpuhtaudet
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Multi-nucleon transfer reactions at ion catcher facilities : a new way to produce and study heavy neutron-rich nuclei

2020

Abstract The production of very neutron-rich nuclides heavier than fission fragments is an ongoing experimental challenge. Multi-nucleon transfer reactions (MNT) have been suggested as a method to produce these nuclides. By thermalizing the reaction products in gas-filled stopping cells, we can deliver them as cooled high-quality beams to decay, laser and mass spectrometry experiments. High precision mass spectrometry will allow for the first time to universally and unambiguously identify the atomic and proton numbers of the ions produced in MNT reactions. In this way their ground and isomeric state properties can be studied in high-precision measurements. In experiments at IGISOL, Finland …

PhysicsHistory010308 nuclear & particles physics01 natural sciences7. Clean energyComputer Science ApplicationsEducationIonNuclear physics0103 physical sciencesNeutron010306 general physicsNucleonydinfysiikka
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Components of polarization-transfer to a bound proton in a deuteron measured by quasi-elastic electron scattering

2018

We report the first measurements of the transverse (Px and Py) and longitudinal (Pz) components of the polarization transfer to a bound proton in the deuteron via the H2(e→,e′p→) reaction, over a wide range of missing momentum. A precise determination of the electron beam polarization reduces the systematic uncertainties on the individual components to a level that enables a detailed comparison to a state-of-the-art calculation of the deuteron using free-proton electromagnetic form factors. We observe very good agreement between the measured and the calculated Px/Pz ratios, but deviations of the individual components. Our results cannot be explained by medium modified electromagnetic form f…

PhysicsNuclear reactionNuclear and High Energy PhysicsProton010308 nuclear & particles physicsScatteringHadronNuclear TheoryFOS: Physical sciencesElectronPolarization (waves)7. Clean energy01 natural scienceslcsh:QC1-999Deuterium0103 physical sciencespolarization-transfer ; deutronAtomic physicsNuclear Experiment (nucl-ex)010306 general physicsNucleonNuclear ExperimentNuclear Experimentlcsh:PhysicsPhysics Letters
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The influence of Fermi motion on the comparison of the polarization transfer to a proton in elastic e→p and quasi-elastic e→A scattering

2019

Abstract A comparison between polarization-transfer to a bound proton in quasi-free kinematics by the A ( e → , e ′ p → ) knockout reaction and that in elastic scattering off a free proton can provide information on the characteristics of the bound proton. In the past the reported measurements have been compared to those of a free proton with zero initial momentum. We introduce, for the first time, expressions for the polarization-transfer components when the proton is initially in motion and compare them to the 2H data measured at the Mainz Microtron (MAMI). We show the ratios of the transverse ( P x ) and longitudinal ( P z ) components of the polarization transfer in H 2 ( e → , e ′ p → …

PhysicsElastic scatteringNuclear and High Energy Physics010308 nuclear & particles physicsScatteringInitial momentumNuclear TheoryKinematicsPolarization (waves)01 natural sciences7. Clean energyTransverse plane0103 physical sciencesPhysics::Accelerator PhysicsAtomic physicsNuclear Experiment010306 general physicsMicrotronFermi Gamma-ray Space TelescopePhysics Letters B
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Measurements of the induced polarization in the quasi-elastic A(e,e′p→) process in non-coplanar kinematics

2020

Abstract We report measurements of the induced polarization P → of protons knocked out from 2H and 12C via the A ( e , e ′ p → ) reaction. We have studied the dependence of P → on two kinematic variables: the missing momentum p miss and the “off-coplanarity” angle ϕ p q between the scattering and reaction planes. For the full 360° range in ϕ p q , both the normal ( P y ) and, for the first time, the transverse ( P x ) components of the induced polarization were measured with respect to the coordinate system associated with the scattering plane. P x vanishes in coplanar kinematics, however in non-coplanar kinematics, it is on the same scale as P y . We find that the dependence on ϕ p q is si…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsPlane (geometry)ScatteringShell (structure)7. Clean energy01 natural sciencesInduced polarizationp-processMomentumTransverse planeDeuterium0103 physical sciencesAtomic physics010306 general physicsPhysics Letters B
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Measurements of the electron-helicity asymmetry in the quasi-elastic A(e→,e′p) process

2022

Abstract We present measurements of the electron helicity asymmetry in quasi-elastic proton knockout from 2H and 12C nuclei by polarized electrons. This asymmetry depends on the fifth structure function, is antisymmetric with respect to the scattering plane, and vanishes in the absence of final-state interactions, and thus it provides a sensitive tool for their study. Our kinematics cover the full range in off-coplanarity angle ϕ p q , with a polar angle θ p q coverage up to about 8°. The missing energy resolution enabled us to determine the asymmetries for knock-out resulting in different states of the residual 11B system. We find that the helicity asymmetry for p-shell knockout from 12C d…

PhysicsNuclear and High Energy PhysicsMissing energyProton010308 nuclear & particles physicsScatteringAntisymmetric relationmedia_common.quotation_subjectElectron01 natural sciencesHelicityAsymmetry3. Good healthMomentum0103 physical sciencesAtomic physics010306 general physicsmedia_commonPhysics Letters B
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Comparison of recoil polarization in the C12(e→,e′p→) process for protons extracted from s and p shells

2020

Abstract We present the first measurements of the double ratio of the polarization-transfer components ( P x ′ / P z ′ ) p / ( P x ′ / P z ′ ) s for knock-out protons from the s and p shells in C 12 measured by the C 12 ( e → , e ′ p → ) reaction in quasi-elastic kinematics. The data are compared to theoretical predictions in the relativistic distorted-wave impulse approximation. Our results show that the differences between s- and p-shell protons, observed when compared at the same initial momentum (missing momentum), largely disappear when the comparison is done at the same proton virtuality. We observe no difference in medium modifications between protons from the s and p shells with the…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsInitial momentumNuclear TheoryImpulse (physics)Polarization (waves)01 natural sciencesp-processRecoil0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsPhysics Letters B
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Measurement of polarization-transfer to bound protons in carbon and its virtuality dependence

2017

We measured the ratio Px/Pz of the transverse to longitudinal components of polarization transferred from electrons to bound protons in C12 by the C12(e→,e′p→) process at the Mainz Microtron (MAMI). We observed consistent deviations from unity of this ratio normalized to the free-proton ratio, (Px/Pz)C12/(Px/Pz)H1, for both s- and p-shell knocked out protons, even though they are embedded in averaged local densities that differ by about a factor of two. The dependence of the double ratio on proton virtuality is similar to the one for knocked out protons from H2 and He4, suggesting a universal behavior. It further implies no dependence on average local nuclear density.

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciencesElectronPolarization (waves)01 natural scienceslcsh:QC1-999Transverse plane0103 physical sciencesPhysics::Accelerator PhysicsNuclear Experiment (nucl-ex)Atomic physics010306 general physicsNuclear ExperimentMicrotronNuclear Experimentlcsh:PhysicsNuclear density
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A Novel Method for the Measurement of Half-Lives and Decay Branching Ratios of Exotic Nuclei

2019

A novel method for simultaneous measurement of masses, Q-values, isomer excitation energies, half-lives and decay branching ratios of exotic nuclei has been demonstrated. The method includes first use of a stopping cell as an ion trap, combining containment of precursors and decay-recoils for variable durations in a cryogenic stopping cell (CSC), and afterwards the identification and counting of them by a multiple-reflection time-of-flight mass spectrometer (MR-TOF-MS). Feasibility has been established by recording the decay and growth of $^{216}$Po and $^{212}$Pb (alpha decay) and of $^{119m2}$Sb (t$_{1/2}$ = 850$\pm$90 ms) and $^{119g}$Sb (isomer transition), obtaining half-lives and bran…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsFOS: Physical sciencesdecay branching ratiosBranching (polymer chemistry)Mass spectrometry01 natural sciences530half-livesexotic nuclei0103 physical sciencesddc:530novel methodmeasurementIon trapAlpha decayAtomic physicsNuclear Experiment (nucl-ex)Nuclear Experimentydinfysiikka010306 general physicsNuclear ExperimentExcitation
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Mass and half-life measurements of neutron-deficient iodine isotopes

2020

The European physical journal / A 56(5), 143 (2020). doi:10.1140/epja/s10050-020-00153-5

Nuclear and High Energy PhysicsALPHA-DECAYSEPARATORMass spectrometry01 natural sciences530Ionjodi0103 physical sciencesNuclear fusionNeutronddc:530010306 general physicsNuclear ExperimentPhysicsisotoopitIsotope010308 nuclear & particles physicsPERFORMANCESPECTROMETRYQuadrupoleFRS; PROJECTILEAlpha decayAtomic physicsydinfysiikkaGround stateSYSTEM
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Polarization transfer to bound protons measured by quasi-elastic electron scattering on $^{12}$C

2020

We report the measurements of the transverse ($P'x$) and longitudinal ($P'z$) components of the polarization transfer to a bound proton in carbon via the quasi-free $^{12}{\rm C}(\vec e,e'\vec p)$ reaction, over a wide range of missing momenta. We determine these polarization-transfers separately for protons knocked out from the $s$- and $p$-shells. The electron-beam polarization was measured to determine the individual components with systematic uncertainties which allow a detailed comparison with theoretical calculations.

PhysicsProton010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciencesPolarization (waves)01 natural sciencesTransverse plane0103 physical sciencesAtomic physicsNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentElectron scatteringNuclear Experiment
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Removal of molecular contamination in low-energy RIBs by the isolation-dissociation-isolation method

2020

Nuclear instruments & methods in physics research / B 463, 324 - 326 (2020). doi:10.1016/j.nimb.2019.04.072

low-energy RIBNuclear and High Energy PhysicsMaterials scienceCollision-induced dissociationbeam purificationtutkimuslaitteet53001 natural sciencesDissociation (chemistry)RF-quadrupolelaw.inventionIonlawDipole magnet0103 physical sciencesddc:530Instrumentation010308 nuclear & particles physics010401 analytical chemistryContaminationSynchrotronIon source0104 chemical sciencesmolecular contaminationBeamlinecollision-induced dissociationPhysics::Accelerator PhysicsAtomic physicsydinfysiikkaNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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The science case of the FRS Ion Catcher for FAIR Phase-0

2019

The FRS Ion Catcher at GSI enables precision experiments with thermalized projectile and fission fragments. At the same time it serves as a test facility for the Low-Energy Branch of the Super-FRS at FAIR. The FRS Ion Catcher has been commissioned and its performance has been characterized in five experiments with 238U and 124Xe projectile and fission fragments produced at energies in the range from 300 to 1000 MeV/u. High and almost element-independent efficiencies for the thermalization of short-lived nuclides produced at relativistic energies have been obtained. High-accuracy mass measurements of more than 30 projectile and fission fragments have been performed with a multiple-reflection…

ydinreaktiotMR-TOF-MSNuclear Theorymass measurementsddc:530exotic nuclidesNuclear Experimentydinfysiikkanuclear reactionsbeta-delayed neutron emissionemissio (fysiikka)
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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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High-resolution, accurate multiple-reflection time-of-flight mass spectrometry for short-lived, exotic nuclei of a few events in their ground and low…

2019

Physical review / C covering nuclear physics 99(6), 064313 (2019). doi:10.1103/PhysRevC.99.064313

massaspektrometriaProtonResolution (mass spectrometry)FissionBinding energyMass spectrometrynucl-ex01 natural sciences530binding energy and massesnuclear bindingNuclear physics0103 physical sciencesNeutronddc:530NuclideNuclear Experiment010306 general physicsphysics.ins-detPhysicsbeam diagnostics010308 nuclear & particles physicsnuclear fragmentationlifetimes and widthsTime-of-flight mass spectrometryisomer decaysydinfysiikka
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Studying Gamow-Teller transitions and the assignment of isomeric and ground states at $N=50$

2022

Direct mass measurements of neutron-deficient nuclides around the N=50 shell closure below $^{100}$Sn were performed at the FRS Ion Catcher (FRS-IC) at GSI, Germany. The nuclei were produced by projectile fragmentation of $^{124}$Xe, separated in the fragment separator FRS and delivered to the FRS-IC. The masses of 14 ground states and two isomers were measured with relative mass uncertainties down to 1×10−7 using the multiple-reflection time-of-flight mass spectrometer of the FRS-IC, including the first direct mass measurements of $^{98}$Cd and $^{97}$Rh. A new QEC=5437±67 keV was obtained for $^{98}$Cd, resulting in a summed Gamow-Teller (GT) strength for the five observed transitions (0+…

nuclear isomersNuclear and High Energy PhysicsMultiple-reflection time-of-flight massNuclear shell structuremultiple-reflection time-of-flight mass[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]N = 50 isotonesFOS: Physical sciencesGamow-Teller transition?s strength114 Physical sciencesSpectrometerexotic nucleiGamow-Teller transition's strengthnuclear shell structureNuclear isomersspectrometerN=50 isotonesNuclear Experiment (nucl-ex)ydinfysiikkaNuclear ExperimentExotic nuclei
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