0000000000054547

AUTHOR

T. Kolar

showing 12 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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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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Detector response of Cherenkov radiators for calorimetry in the energy range below 14 MeV

2020

Abstract A study of the detector response of PbF 2  crystals and three different types of lead glass blocks to electrons from a 14-MeV beam of the Mainz Microtron MAMI is presented. For the first time, signal height, signal width, and homogeneity of the response of these Cherenkov radiators were determined for energies between 10 and 14 MeV. To complement the beam tests, optical properties of the materials, in particular measured transmittances in the near UV and visible spectrum, were studied. The measured detector responses were also compared to Monte Carlo simulations of energy-loss, light production, transport, and detection. These Cherenkov radiators are considered as active material o…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsbusiness.industryDetectorMonte Carlo methodSignal WidthElectron01 natural sciencesLead glassOpticsvisual_art0103 physical sciencesvisual_art.visual_art_mediumPhysics::Accelerator PhysicsNuclear Experiment010306 general physicsbusinessInstrumentationLight dark matterMicrotronCherenkov radiationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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Electron beam studies of light collection in a scintillating counter with embedded fibers

2021

The light collection of several fiber configurations embedded in a box-shaped plastic scintillating counter was studied by scanning with minimum ionizing electrons. The light was read out by silicon photomultipliers at both ends. The light yield produced by the 855-MeV beam of the Mainz Microtron showed a strong dependence on the transverse distance from the beam position to the fibers. The observations were modeled by attributing the collection of indirect light inside of the counter and of direct light reaching a fiber to the total light yield. The light collection with fibers was compared to that of a scintillating counter without fibers. These studies were carried out within the develop…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Physics - Instrumentation and DetectorsPhysics::Instrumentation and Detectorsbusiness.industryFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)ElectronOpticsSilicon photomultiplierCathode rayPhysics::Accelerator PhysicsFiberNuclear Experiment (nucl-ex)businessNuclear ExperimentInstrumentationLight dark matterMicrotronBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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Operation and characterization of a windowless gas jet target in high-intensity electron beams

2021

Abstract A cryogenic supersonic gas jet target was developed for the MAGIX experiment at the high-intensity electron accelerator MESA. It will be operated as an internal, windowless target in the energy-recovering recirculation arc of the accelerator with different target gases, e.g., hydrogen, deuterium , helium, oxygen, argon, or xenon. Detailed studies have been carried out at the existing A1 multi-spectrometer facility at the electron accelerator MAMI. This paper focuses on the developed handling procedures and diagnostic tools, and on the performance of the gas jet target under beam conditions. Considering the special features of this type of target, it proves to be well suited for a n…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsNuclear engineeringchemistry.chemical_elementFOS: Physical sciencesElectron01 natural scienceslaw.inventionXenonlaw0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsInstrumentationNuclear ExperimentHeliumPhysicsJet (fluid)Argon010308 nuclear & particles physicsParticle acceleratorInstrumentation and Detectors (physics.ins-det)chemistryPhysics::Accelerator PhysicsElectron scatteringBeam (structure)
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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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Vertical Beam Polarization at MAMI

2017

For the first time a vertically polarized electron beam has been used for physics experiments at MAMI in the energy range between 180 and 855 MeV. The beam-normal single-spin asymmetry $A_{\mathrm{n}}$, which is a direct probe of higher-order photon exchange beyond the first Born approximation, has been measured in the reaction $^{12}\mathrm C(\vec e,e')^{12}\mathrm C$. Vertical polarization orientation was necessary to measure this asymmetry with the existing experimental setup. In this paper we describe the procedure to orient the electron polarization vector vertically, and the concept of determining both its magnitude and orientation with the available setup. A sophisticated method has …

Accelerator Physics (physics.acc-ph)Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhotonmedia_common.quotation_subjectVertical polarization[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]FOS: Physical sciencesElectron acceleratorElectronMott polarimeter01 natural sciencesAsymmetrylaw.inventionOpticsMøller polarimeterlaw0103 physical sciencesCompton polarimeter[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det][ PHYS.PHYS.PHYS-ACC-PH ] Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Born approximation010306 general physicsNuclear Experiment[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Instrumentationmedia_commonPhysicsWien filter010308 nuclear & particles physicsbusiness.industryParticle acceleratorPolarimeterInstrumentation and Detectors (physics.ins-det)Wien filterPolarization (waves)Electron accelerator ; Vertical polarization ; Wien filter ; Compton polarimeter ; Mott polarimeter ; Møller polarimeterPhysics - Accelerator Physicsbusiness
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First Measurement of the $Q^2$ Dependence of the Beam-Normal Single Spin Asymmetry for Elastic Scattering off Carbon

2018

We report on the first Q^{2}-dependent measurement of the beam-normal single spin asymmetry A_{n} in the elastic scattering of 570 MeV vertically polarized electrons off ^{12}C. We cover the Q^{2} range between 0.02 and 0.05  GeV^{2}/c^{2} and determine A_{n} at four different Q^{2} values. The experimental results are compared to a theoretical calculation that relates A_{n} to the imaginary part of the two-photon exchange amplitude. The result emphasizes that the Q^{2} behavior of A_{n} given by the ratio of the Compton to charge form factors cannot be treated independently of the target nucleus.

carbon: targetelectron: polarized beammedia_common.quotation_subjectGeneral Physics and AstronomyElectron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]momentum transfer dependence01 natural sciencesAsymmetryMainz Linac0103 physical sciencesgallium: arsenicpolarization: transverseelektronsko raspršenje010306 general physicsNuclear ExperimentSpin-½media_commonPhysicsElastic scatteringform factor: ratioform factor: chargeexchange: two-photon010308 nuclear & particles physicsnucleus: targetizmjena dva fotonaelectron nucleus: elastic scatteringCharge (physics)amplitude analysisNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.spin: asymmetry: measuredElektronsko raspršenje izmjena dva fotonaAmplitudeCover (topology)High Energy Physics::ExperimentAtomic physicsradiation: laserBeam (structure)photoelectronexperimental results
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