0000000000054562

AUTHOR

L. Debenjak

showing 24 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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Observation ofHΛ4Hyperhydrogen by Decay-Pion Spectroscopy in Electron Scattering

2015

At the Mainz Microtron MAMI, the first high-resolution pion spectroscopy from decays of strange systems was performed by electron scattering off a ^9B

PhysicsParticle physicsSpectrometerNuclear TheoryGeneral Physics and Astronomychemistry.chemical_elementHypernucleusNuclear physicsPionchemistryHigh Energy Physics::ExperimentBerylliumNuclear ExperimentSpectroscopyMicrotronElectron scatteringPhysical Review Letters
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Measurement of the Generalized Polarizabilities of the Proton at Intermediate $Q^2$

2021

Background: Generalized polarizabilities (GPs) are important observables to describe the nucleon structure, and measurements of these observables are still scarce. Purpose: This paper presents details of a virtual Compton scattering (VCS) experiment, performed at the A1 setup at the Mainz Microtron by studying the $e p \to e p \gamma$ reaction. The article focuses on selected aspects of the analysis. Method: The experiment extracted the $P_{LL} -P_{TT} / \epsilon$ and $P_{LT}$ structure functions, as well as the electric and magnetic GPs of the proton, at three new values of the four-momentum transfer squared $Q^2$: 0.10, 0.20 and 0.45 GeV$^2$. Results: We emphasize the importance of the ca…

MAINZ-A1ProtonNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]higher-orderHadronic Physics and QCDFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]momentum transfer dependence01 natural scienceselectron p: scatteringNuclear Theory (nucl-th)Cross section (physics)High Energy Physics - Phenomenology (hep-ph)Polarizability0103 physical sciencesCalibrationp: structure functionNuclear Experiment (nucl-ex)010306 general physicsMicrotronNuclear ExperimentPhysics010308 nuclear & particles physicsCompton scatteringObservablecross section: measuredcalibrationComputational physicsHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]p: polarizabilityelectron p --> electron p photonNucleonCompton scatteringexperimental results
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Particle tracking in kaon electroproduction with cathode-charge sampling in multi-wire proportional chambers

2011

Abstract Wire chambers are routinely operated as tracking detectors in magnetic spectrometers at high-intensity continuous electron beams. Especially in experiments studying reactions with small cross-sections the reaction yield is limited by the background rate in the chambers. One way to determine the track of a charged particle through a multi-wire proportional chamber (MWPC) is the measurement of the charge distribution induced on its cathodes. In practical applications of this read-out method, the algorithm to relate the measured charge distribution to the avalanche position is an important factor for the achievable position resolution and for the track reconstruction efficiency. An al…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Physics - Instrumentation and DetectorsSpectrometerPhysics::Instrumentation and DetectorsFOS: Physical sciencesCharge densityInstrumentation and Detectors (physics.ins-det)ElectronTracking (particle physics)Charged particleParticle detectorNuclear physicsCathode rayNuclear Experiment (nucl-ex)tracking and position-sensitive detectors; multi-wire proporational chambersNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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Search at the Mainz Microtron for light massive gauge bosons relevant for the muon g-2 anomaly.

2014

A massive, but light, Abelian U(1) gauge boson is a well-motivated possible signature of physics beyond the standard model of particle physics. In this Letter, the search for the signal of such a U(1) gauge boson in electron-positron pair production at the spectrometer setup of the A1 Collaboration at the Mainz Microtron is described. Exclusion limits in the mass range of 40  MeV/c^{2} to 300  MeV/c^{2}, with a sensitivity in the squared mixing parameter of as little as ε^{2}=8×10^{-7} are presented. A large fraction of the parameter space has been excluded where the discrepancy of the measured anomalous magnetic moment of the muon with theory might be explained by an additional U(1) gauge …

PhysicsGauge bosonParticle physicsMuonAnomalous magnetic dipole momentPhysics beyond the Standard ModelGeneral Physics and AstronomyDark photonNATURAL SCIENCES. Physics.Nuclear physicsPRIRODNE ZNANOSTI. Fizika.U(1)SPair productiondark photondark photon; U(1)SAnomaly (physics)Nuclear ExperimentMicrotronPhysical review letters
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The frontiers of the virtual photons program at MAMI

2012

The most recent results and the future physics program of the high precision electron-scattering experiment at MAMI are briefly outlined. The A1 high-resolution spectrometers facility allows for a unique quality of virtual photon experiments. High precision form factor measurements, few-baryon systems highresolution structure studies and the innovative way in the search of dark photons illustrate the interplay between such diverse fields as precision atomic physics, nuclear astrophysics and astroparticle physics, where hadron physics plays a central and connecting role.

Astroparticle physicsPhysicsParticle physicsPhotonSpectrometerPhysicsQC1-999Form factor (quantum field theory)Virtual particleEngineering physicsHadron physicsNuclear astrophysicsvirtual photon; form factor measurements; dark photon; precision spectroscopy of light hypernucleiNuclear Experiment
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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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First measurement of proton's charge form factor at very low $Q^2$ with initial state radiation

2017

We report on a new experimental method based on initial-state radiation (ISR) in e-p scattering, in which the radiative tail of the elastic e-p peak contains information on the proton charge form factor ($G_E^p$) at extremely small $Q^2$. The ISR technique was validated in a dedicated experiment using the spectrometers of the A1-Collaboration at the Mainz Microtron (MAMI). This provided first measurements of $G_E^p$ for $0.001\leq Q^2\leq 0.004 (GeV/c)^2$.

experimental methodsProtonelastic scattering01 natural sciencesHigh Energy Physics - ExperimentLamb shiftHigh Energy Physics - Experiment (hep-ex)Initial state radiation ; Proton ; Form factor ; Radiative correctionsRadiative transfer[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentMicrotronElastic scatteringPhysicsForm factor (quantum field theory)beam: currentRadiative correctionslcsh:QC1-9993. Good healthPRIRODNE ZNANOSTI. Fizika.ProtonNuclear and High Energy PhysicsFOS: Physical sciencesBethe-Heitler25.30.BfRadiation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear physicselectron p: scatteringMainz Linac[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]12.20.-m0103 physical sciencesradiation: initial-state interaction010306 general physicsnumerical calculationsform factor: charge41.60.-m010308 nuclear & particles physicsScatteringp: chargeNATURAL SCIENCES. Physics.microtronForm factorLamb shiftspectrometerInitial state radiationlcsh:Physicsexperimental results
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Search for Light Gauge Bosons of the Dark Sector at the Mainz Microtron

2011

A new exclusion limit for the electromagnetic production of a light U(1) gauge boson {\gamma}' decaying to e^+e^- was determined by the A1 Collaboration at the Mainz Microtron. Such light gauge bosons appear in several extensions of the standard model and are also discussed as candidates for the interaction of dark matter with standard model matter. In electron scattering from a heavy nucleus, the existing limits for a narrow state coupling to e^+e^- were reduced by nearly an order of magnitude in the range of the lepton pair mass of 210 MeV/c^2 < m_e^+e^- < 300 MeV/c^2. This experiment demonstrates the potential of high current and high resolution fixed target experiments for the search fo…

Particle physicsPhysics beyond the Standard Modelgauge bosonsFOS: Physical sciencesGeneral Physics and AstronomyElementary particle01 natural sciences7. Clean energyHigh Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciencesGrand Unified TheoryNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentMicrotronBosonPhysicsGauge boson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.electron scattering; gauge bosonselectron scatteringLepton
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STATUS OF STRANGENESS ELECTRO-PRODUCTION AT MAMI

2009

At the Institut für Kernphysik in Mainz, Germany, the microtron MAMI has been upgraded to 1.5 GeV electron beam energy and can now be used to study strange hadronic systems. The magnetic spectrometer KAOS from GSI was dismantled and re-installed in the spectrometer facility operated by the A1 collaboration. The spectrometer's primary purpose is to study strangeness electro-production. Its compact design and its capability to detect negative and positive charged particles simultaneously under forward scattering angles complements the existing spectrometers. In 2008, an important milestone has been reached by the successful measurement of kaon production off a liquid hydrogen target. The ide…

magnetic spectrometer; particle detector design; kaon electro-production; hypernuclei electro-productionPhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerPhysics::Instrumentation and DetectorsScatteringNuclear TheoryHadronDetectorGeneral Physics and AstronomyStrangenessCharged particleNuclear physicsPhysics::Accelerator PhysicsVacuum chamberNuclear ExperimentMicrotronStrangeness in Nuclear and Hadronic Systems
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High-Precision Determination of the Electric and Magnetic Form Factors of the Proton

2010

New precise results of a measurement of the elastic electron-proton scattering cross section performed at the Mainz Microtron MAMI are presented. About 1400 cross sections were measured with negative four-momentum transfers squared up to Q^2=1 (GeV/c)^2 with statistical errors below 0.2%. The electric and magnetic form factors of the proton were extracted by fits of a large variety of form factor models directly to the cross sections. The form factors show some features at the scale of the pion cloud. The charge and magnetic radii are determined to be r_E=0.879(5)(stat.)(4)(syst.)(2)(model)(4)(group) fm and r_M=0.777(13)(stat.)(9)(syst.)(5)(model)(2)(group) fm.

Particle physicsProtonMesonelastic electron scattering13.40.Gp 14.20.Dh 25.30.BfHadronGeneral Physics and AstronomyFOS: Physical sciencesElementary particle[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicselastic electron scattering; proton electromagnetic form factors010308 nuclear & particles physicsForm factor (quantum field theory)Charge (physics)NATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Crystallographyproton electromagnetic form factorsHigh Energy Physics::ExperimentNucleonDimensionless quantity
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Unpolarized and polarized elementary kaon electroproduction cross sections measured at MAMI

2012

Present and future research into the electroproduction of kaons plays an im- portant role at Mainz Microtron MAMI. With the Kaos spectrometer employed for kaon detection in the multi-spectrometer facility, cross section measurements of the exclusive p(e;e 0 K + ); 0 reactions at low momentum transfers have been performed. Isobar and Regge-plus-resonance models were compared with the data. These measurements have clearly discriminated between e ective Lagrangian models for photo- and electroproduc- tion of strangeness. New experiments with polarized beam at low four-momentum transfer are addressing the imaginary part of the longitudinal-transverse response in this process, that can be separa…

Coupling constantPhysicsParticle physicsPhysicsQC1-999HadronNuclear TheoryStrangenessHelicityMomentumNuclear physicsIsobarHigh Energy Physics::ExperimentNuclear ExperimentMicrotronBeam (structure)EPJ Web of Conferences
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In-beam tests of scintillating fibre detectors at MAMI and at GSI

2008

The performance of scintillating fibre detectors was studied with electrons at the spectrometer facility of the Mainz microtron MAMI, as well as in a C-12 beam of 2 AGeV energy and in a beam of different particle species at GSI. Multi-anode photomultipliers were used to read out one or more bundles of 128 fibres each in different geometries. For electrons a time resolution of FWHM = 1 ns was measured in a single detector plane with a detection efficiency epsilon &gt; 99%. A time resolution of 310 ps (FWHM) between two planes of fibres was achieved for carbon ions, leading to a FWHM = 220 ps for a single detector. The hit position residual was measured with a width of FWHM = 0.27 mm. The var…

PhysicsNuclear and High Energy PhysicsPhotomultiplierSpectrometerbusiness.industryDetectorFOS: Physical sciencesCharged particleParticle detectorNuclear physicsFull width at half maximumOpticsNuclear Experiment (nucl-ex)businessInstrumentationMicrotronNuclear ExperimentBeam (structure)
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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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Measurement of the p(e,e′π+)n reaction close to threshold and at low Q2

2017

The cross section of the $p(e,e'\pi^+)n$ reaction has been measured for five kinematic settings at an invariant mass of $W = 1094$ MeV and for a four-momentum transfer of $Q^2 = 0.078$ (GeV/$c$)$^2$. The measurement has been performed at MAMI using a new short-orbit spectrometer (SOS) of the A1 collaboration, intended for detection of low-energy pions. The transverse and longitudinal cross section terms were separated using the Rosenbluth method and the transverse-longitudinal interference term has been determined from the left-right asymmetry. The experimental cross section terms are compared with the calculations of three models: DMT2001, MAID2007 and $\chi$MAID. The results show that we …

Particle physicsNuclear and High Energy Physicsmedia_common.quotation_subjectKinematicsInterference (wave propagation)01 natural sciencesAsymmetryNuclear physicsCross section (physics)Low-energy pionsPion0103 physical sciencesInvariant mass010306 general physicsNuclear ExperimentNuclear Experimentmedia_commonPhysicsSpectrometer010308 nuclear & particles physicslcsh:QC1-999NATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Electroproduction experimentsTransverse planeShort-orbit spectrometer ; Low-energy pions ; Electroproduction experimentsShort-orbit spectrometerlcsh:Physics
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Overview of the electromagnetic production of strange mesons at MAMI

2013

Abstract The Mainz Microtron MAMI provides a continuous-wave unpolarized or spin-polarized electron beam with energies up to 1.6 GeV and high degrees of polarization. Electro-production of strange mesons is performed in the multi-spectrometer facility with the Kaos spectrometer for kaon detection and a high-resolution spectrometer for electron detection in plane or out of plane. Differential cross section measurements of exclusive p ( e , e ′ K + ) Λ , Σ 0 reactions at low four-momentum transfers in the nucleonʼs third resonance region have been done, followed by a measurement of the beam helicity asymmetry for p ( e → , e ′ K + ) Λ . These studies are important for the understanding of the…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonMesonHadronStrangenessLambda baryonHelicitySigma baryonNuclear physicsstrangeness reactions; kaon electro-production; missing mass spectroscopy; structure functionsNuclear ExperimentMicrotronNuclear Physics A
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New Insight in the $Q^2$-Dependence of Proton Generalized Polarizabilities

2019

Virtual Compton scattering on the proton has been investigated at three yet unexplored values of the four-momentum transfer $Q^2$: 0.10, 0.20 and 0.45 GeV$^2$, at the Mainz Microtron. Fits performed using either the low-energy theorem or dispersion relations allowed the extraction of the structure functions $P_{LL} -P_{TT} / \epsilon$ and $P_{LT}$, as well as the electric and magnetic generalized polarizabilities $\alpha_{E1}(Q^2)$ and $\beta_{M1}(Q^2)$. These new results show a smooth and rapid fall-off of $\alpha_{E1}(Q^2)$, in contrast to previous measurements at $Q^2$ = 0.33 GeV$^2$, and provide for the first time a precise mapping of $\beta_{M1}(Q^2)$ in the low-$Q^2$ region.

PhysicsProtonCompton scatteringFOS: Physical sciencesGeneral Physics and Astronomy25.30.Dh[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Nuclear physics13.60.FzVirtual Compton Scattering VCS Proton Polarizability MAMI0103 physical sciences14.20.DhNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear Physics
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Strange hadronic physics in electroproduction experiments at the Mainz Microtron

2012

Abstract Present and future research into the electroproduction of strangeness plays an important role at Mainz Microtron MAMI. With the Kaos spectrometer for kaon detection operated in the multi-spectrometer facility first cross section measurements of the exclusive p ( e , e ′ K + ) Λ , Σ 0 reactions at low-momentum transfers have been performed. These measurements have clearly discriminated between effective Lagrangian models for photo- and electroproduction of strangeness. Recently, the Kaos spectrometer was upgraded to a double-arm spectrometer for the measurement of elementary cross sections at very forward scattering angles and for the missing mass spectroscopy of hypernuclear states…

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerNuclear TheoryHadronStrangeness reactions; Kaon electroproduction; Missing mass spectroscopy; Hypernuclei; Decay-pion spectroscopyStrangenessNuclear physicsCross section (physics)Effective lagrangianNuclear ExperimentSpectroscopyMicrotronBeam (structure)Nuclear Physics A
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Prospects for hypernuclear physics at Mainz: From KAOS@MAMI to PANDA@FAIR

2013

Abstract At the Mainz Microtron hypernuclei are produced by ( e , e ′ K ) reactions. A dedicated kaon spectrometer located at 0° with respect to the electron beam is used to detect kaons emitted in forward direction thus tagging events involving strangeness production. By measuring the momenta of pions from two body weak decays using high resolution magnetic spectrometers one gains direct access to the ground state masses of the produced hyperfragments. At FAIR the PANDA Collaboration intends to produce double-hypernuclei by numbers with an antiproton beam and study their high resolution γ -spectroscopy thus providing for the first time precise information on the level structure of these nu…

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerNuclear TheoryStrangeness productionHypernucleusNuclear physicsPionAntiproton beamhypernuclei; weak decay; spectroscopyKAOSGround stateNuclear ExperimentMicrotron
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Kaon Tagging at 0° Scattering Angle for High-Resolution Decay-Pion Spectroscopy

2014

At the Mainz Microtron hypernuclei can be studied by (e,e'K) reactions. By detecting the kaon which is emitted in forward direction, with the KAOS spectrometer placed at 0 scattering angle, reactions involving open strangeness production are tagged. High-resolution magnetic spectrometers are then used to coincidentally detect the mono- energetic decay-pions from mesonic two-body weak decays of light hypernuclei at rest. As a pioneering experiment has confirmed, the KAOS spectrometer is exposed to a large flux of background particles, mostly positrons from bremsstrahlung pair production. In order to increase the e ciency of kaon identification the KAOS spectrometer was modi- fied to suppress…

PhysicsParticle physicsSpectrometerScatteringPhysicsQC1-999Nuclear TheoryBremsstrahlungStrangeness productionNuclear physicsMomentumPionPair productionElectron Scattering; Hypernuclei; MAMI; KAOS; Decay-Pion SpectroscopyHigh Energy Physics::ExperimentNuclear ExperimentMicrotronEPJ Web of Conferences
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Initial state radiation experiment at MAMI

2014

In an attempt to contribute further insight into the discrepancy between the Lamb shift and elastic scattering determinations of the proton charge radius, a new experiment at MAMI is underway, aimed at measuring proton form-factors at very low momentum transfers by using a new technique based on initial state radiation. This paper reports on the conclusions of the pilot measurement performed in 2010, whose main goal was to check the feasibility of the proposed experiment and to recognize and overcome any obstacles before running the full experiment. The modifications to the experimental apparatus are then explained which significantly improved the quality of data collected in the full scale…

Elastic scatteringPhysicsProtonPhysicsQC1-999Full scaleRadiationLamb shiftNuclear physicsMomentumCharge radiusState (computer science)Statistical physicsElectron Scattering; MAMI; Proton Charge RadiusEPJ Web of Conferences
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First measurements of Λ and hyperons in elementary electroproduction at MAMI

2010

Abstract Since 2008 the magnetic spectrometer Kaos , dedicated to the detection of charged kaons, is operating at the 1.5 GeV electron beam of MAMI at the Institut fur Kernphysik in Mainz, Germany. The strangeness programme performed in 2008–9 is addressing some important issues in the field of elementary kaon photoelectro-production reactions. The identification of Λ and Σ 0 hyperons in the missing mass spectra from kaon production off a liquid hydrogen target demonstrates the capability of the extended facility to perform strangeness electro-production spectroscopy at low momentum transfers Q 2 0.5 ( GeV / c ) 2 . Systematic uncertainties in the cross-section extraction from the data are …

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerField (physics)010308 nuclear & particles physicsNuclear TheoryHyperonStrangeness01 natural sciencesNuclear physicsMomentum0103 physical sciencesMass spectrumHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsSpectroscopyNuclear Physics A
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Front-End Electronics for the KAOS Spectrometer at MAMI

2009

A new front-end electronics system has been developed for the electron arm tracking detectors in the Kaos spectrometer at the Mainz microtron MAMI. The signals of multi-anode photomultipliers are collected by 96-channel front-end boards, digitized by double-threshold discriminators and the signal time is picked up by F1 TDC chips. The system was designed to process more than 4,000 channels and to cope with the high electron flux in the spectrometer and the high count rate requirement of the detectors. A subset of 288 channels was installed and successfully used in the 2008 data taking period of the Kaos spectrometer.

PhysicsNuclear and High Energy PhysicsPhotomultiplierSpectrometerbusiness.industryDetectorElectrical engineeringTracking (particle physics)Signaldouble-threshold discriminator; front-end electronics; multi-anode photomultiplier; microtronNuclear Energy and EngineeringNuclear electronicsElectrical and Electronic EngineeringKAOSbusinessMicrotronIEEE Transactions on Nuclear Science
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