0000000000054541

AUTHOR

E. Piasetzky

showing 14 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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Comparing proton momentum distributions in A = 2 and 3 nuclei via 2H 3H and 3He (e,e′p) measurements

2019

We report the first measurement of the $(e,e'p)$ reaction cross-section ratios for Helium-3 ($^3$He), Tritium ($^3$H), and Deuterium ($d$). The measurement covered a missing momentum range of $40 \le p_{miss} \le 550$ MeV$/c$, at large momentum transfer ($\langle Q^2 \rangle \approx 1.9$ (GeV$/c$)$^2$) and $x_B>1$, which minimized contributions from non quasi-elastic (QE) reaction mechanisms. The data is compared with plane-wave impulse approximation (PWIA) calculations using realistic spectral functions and momentum distributions. The measured and PWIA-calculated cross-section ratios for $^3$He$/d$ and $^3$H$/d$ extend to just above the typical nucleon Fermi-momentum ($k_F \approx 250$ …

production [pi]Nuclear and High Energy Physicsdata analysis methodPhotonNuclear TheoryNuclear TheoryinterferenceFOS: Physical sciencesElectronImpulse (physics)Inelastic scattering01 natural sciencesxperimental results | Jefferson Lab | electron p: scattering | parity: violation | inelastic scattering | structure function | interference | photon | Z0 | pi: production | spin: asymmetry | data analysis methodNuclear Theory (nucl-th)structure function0103 physical sciencesZ0Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsMomentum transferphotoninelastic scatteringscattering [electron p]Eikonal approximationNATURAL SCIENCES. Physics.lcsh:QC1-999PRIRODNE ZNANOSTI. Fizika.Deuteriumxperimental resultsHigh Energy Physics::Experimentviolation [parity]Atomic physicsNucleonasymmetry [spin]lcsh:PhysicsJefferson LabPhysics Letters B
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Search for Effects Beyond the Born Approximation in Polarization Transfer Observables ine→pElastic Scattering

2011

Intensive theoretical and experimental efforts over the past decade have aimed at explaining the discrepancy between data for the proton electric to magnetic form factor ratio, $$G_{E}/G_{M}$$, obtained separately from cross section and polarization transfer measurements. One possible explanation for this difference is a two-photon-exchange (TPEX) contribution. In an effort to search for effects beyond the one-photon-exchange or Born approximation, we report measurements of polarization transfer observables in the elastic $$H(\vec{e},e'\vec{p})$$ reaction for three different beam energies at a fixed squared momentum transfer $Q^2 = 2.5$ GeV$^2$, spanning a wide range of the virtual photon p…

Elastic scatteringPhysicsParticle physics010308 nuclear & particles physicsHadronMomentum transferGeneral Physics and AstronomyElementary particle01 natural sciencesBaryon0103 physical sciencesMagnetic form factorHigh Energy Physics::ExperimentBorn approximation010306 general physicsNucleonPhysical Review Letters
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Polarization observables in deuteron photodisintegration below 360 MeV

2010

High precision measurements of induced and transferred recoil proton polarization in d(polarized gamma, polarized p})n have been performed for photon energies of 277--357 MeV and theta_cm = 20 degrees -- 120 degrees. The measurements were motivated by a longstanding discrepancy between meson-baryon model calculations and data at higher energies. At the low energies of this experiment, theory continues to fail to reproduce the data, indicating that either something is missing in the calculations and/or there is a problem with the accuracy of the nucleon-nucleon potential being used.

PhysicsNuclear and High Energy PhysicsPhotonMeson010308 nuclear & particles physicsNuclear TheoryPolarization observablesFOS: Physical sciencesPolarization (waves)01 natural sciencesRecoil protonNuclear physicsBaryonDeuteriumPhotodisintegration0103 physical sciencesNuclear Experiment (nucl-ex)Atomic physicsNuclear Experiment010306 general physicsNuclear ExperimentPhysics Letters B
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High Resolution Spectroscopy ofBΛ12by Electroproduction

2007

An experiment measuring electroproduction of hypernuclei has been performed in Hall A at Jefferson Lab on a $^{12}$C target. In order to increase counting rates and provide unambiguous kaon identification two superconducting septum magnets and a Ring Imaging CHerenkov detector (RICH) were added to the Hall A standard equipment. An unprecedented energy resolution of less than 700 keV FWHM has been achieved. Thus, the observed \lam{12}{B} spectrum shows for the first time identifiable strength in the core-excited region between the ground-state {\it s}-wave $\Lambda$ peak and the 11 MeV {\it p}-wave $\Lambda$ peak.

PhysicsSuperconductivity010308 nuclear & particles physicsResolution (electron density)General Physics and AstronomyOrder (ring theory)Lambda01 natural sciencesRing-imaging Cherenkov detectorNuclear physicsFull width at half maximum0103 physical sciencesNuclear Experiment010306 general physicsSpectroscopyEnergy (signal processing)Physical Review Letters
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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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Polarization-transfer measurement to a large-virtuality bound proton in the deuteron

2017

Possible differences between free and bound protons may be observed in the ratio of polarization-transfer components, $P'_x/P'_z$. We report the measurement of $P'_x/P'_z$, in the $^2\textrm{H}(\vec{e},e^{\prime}\vec{p})n$ reaction at low and high missing momenta. Observed increasing deviation of $P'_x/P'_z$ from that of a free proton as a function of the virtuality, similar to that observed in \hefour, indicates that the effect in nuclei is due to the virtuality of the knock-out proton and not due to the average nuclear density. The measured differences from calculations assuming free-proton form factors ($\sim10\%$), may indicate in-medium modifications.

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciencesPolarization (waves)01 natural sciencesNATURAL SCIENCES. Physics.lcsh:QC1-999Nuclear physicsPRIRODNE ZNANOSTI. Fizika.Deuterium0103 physical sciencesd(e e’p) ; Electron-scatteringPhysics::Accelerator PhysicsNuclear Experiment (nucl-ex)Electron-scattering010306 general physicsNuclear Experimentd(ee'p)Electron scatteringNuclear ExperimentNuclear densitylcsh:PhysicsPhysics Letters B
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Spectroscopy ofLiΛ9by electroproduction

2015

Background: In the absence of accurate data on the free two-body hyperon-nucleon interaction, the spectra of hypernuclei provides information on the details of the effective hyperon-nucleon interaction.Purpose: To obtain a high-resolution binding-energy spectrum for the ${}^{9}\mathrm{Be}(e,{e}^{\ensuremath{'}}{K}^{+})_{\ensuremath{\Lambda}}^{9}\mathrm{Li}$ reaction.Method: Electroproduction of the hypernucleus $_{\ensuremath{\Lambda}}^{9}\mathrm{Li}$ has been studied for the first time with sub-MeV energy resolution in Hall A at Jefferson Lab on a $^{9}\mathrm{Be}$ target. In order to increase the counting rate and to provide unambiguous kaon identification, two superconducting septum magn…

SuperconductivityPhysicsNuclear and High Energy PhysicsNuclear TheoryOrder (ring theory)Atomic physicsNuclear ExperimentGround stateHypernucleusSpectroscopyLambdaEnergy (signal processing)Spectral linePhysical Review C
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Measurement of double-polarization asymmetries in the quasi-elastic Process

2018

We report on a precise measurement of double-polarization asymmetries in electron-induced breakup of He3 proceeding to pd and ppn final states, performed in quasi-elastic kinematics at Q2=0.25(GeV/c)2 for missing momenta up to 250MeV/c. These observables represent highly sensitive tools to investigate the electromagnetic and spin structure of He3 and the relative importance of two- and three-body effects involved in the breakup reaction dynamics. The measured asymmetries cannot be satisfactorily reproduced by state-of-the-art calculations of He3 unless their three-body segment is adjusted, indicating that the spin-dependent part of the nuclear interaction governing the three-body breakup pr…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryObservableKinematicsSpin structurePolarization (waves)Breakup01 natural sciencesp-processNuclear interactionNuclear physicsReaction dynamics0103 physical sciencesNuclear Experiment010306 general physicsPhysics Letters
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