0000000000199788

AUTHOR

L. Correa

showing 11 related works from this author

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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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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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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Ground-state binding energy of HΛ4 from high-resolution decay-pion spectroscopy

2016

Abstract A systematic study on the Λ ground state binding energy of hyperhydrogen H Λ 4 measured at the Mainz Microtron MAMI is presented. The energy was deduced from the spectroscopy of mono-energetic pions from the two-body decays of hyperfragments, which were produced and stopped in a 9Be target. First data, taken in the year 2012 with a high resolution magnetic spectrometer, demonstrated an almost one order of magnitude higher precision than emulsion data, while being limited by systematic uncertainties. In 2014 an extended measurement campaign was performed with improved control over systematic effects, increasing the yield of hypernuclei and confirming the observation with two indepen…

PhysicsNuclear and High Energy PhysicsSpectrometer010308 nuclear & particles physicsBinding energy01 natural sciencesNuclear physicsPion0103 physical sciencesSymmetry breaking010306 general physicsSpectroscopyGround stateMicrotronOrder of magnitudeNuclear 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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Experimental investigations of the hypernucleus $_Λ^4$H

2015

International audience; Negatively charged pions from two-body decays of stopped _Lambda^4H hypernuclei were studied in 2012 at the Mainz Microtron MAMI, Germany. The momenta of the decay-pions were measured with unprecedented precision by using high-resolution magnetic spectrometers. A challenge of the experiment was the tagging of kaons from associated K^+∧ production off a Be target at very forward angles. In the year 2014, this experiment was continued with a better control of the systematic uncertainties, with better suppression of coincident and random background, improved particle identification, and with higher luminosities. Another key point of the progress was the improvemen…

Lambda: hypernucleusQC1-999Nuclear TheoryAstrophysics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencestagged beamParticle identificationpi-010305 fluids & plasmasNuclear physicsMomentumMainz LinacPionCoincidentberyllium: target0103 physical sciencesCalibration010306 general physicsNuclear ExperimentMicrotronPhysicsSpectrometerPhysicspi: decayresolutionsuppressionHypernucleusmagnetic spectrometerKmicrotronhydrogenmomentum: calibrationbackground: randomHigh Energy Physics::Experimentluminosity: highparticle identification
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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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Deuteron form factor measurements at low momentum transfers

2016

A precise measurement of the elastic electron-deuteron scattering cross section at four-momentum transfers of 0.24 fm−1 ≤ Q ≤ 2.7 fm−1 has been performed at the Mainz Microtron. In this paper we describe the utilized experimental setup and the necessary analysis procedure to precisely determine the deuteron charge form factor from these data. Finally, the deuteron charge radius rd can be extracted from an extrapolation of that form factor to Q 2 = 0.

Scattering cross-sectionPhysics010308 nuclear & particles physicsPhysicsQC1-999Form factor (quantum field theory)ExtrapolationCharge (physics)01 natural sciencesMomentumNuclear physicsDeuteriumCharge radius0103 physical sciencesStatistical physics010306 general physicsMicrotronEPJ Web of Conferences
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Beam-Recoil Polarization Measurement of π0 Electroproduction on the Proton in the Region of the Roper Resonance

2017

The helicity-dependent recoil proton polarizations P_{x}^{'} and P_{z}^{'} as well as the helicity-independent component P_{y} have been measured in the p(e[over →],e^{'}p[over →])π^{0} reaction at four-momentum transfer Q^{2}≃0.1  GeV^{2}, center-of-mass proton emission angle θ_{p}^{*}≃90°, and invariant mass W≃1440  MeV. This first precise measurement of double-polarization observables in the energy domain of the Roper resonance P_{11}(1440) by exploiting recoil polarimetry has allowed for the extraction of its scalar electroexcitation amplitude at an unprecedentedly low value of Q^{2}, establishing a powerful instrument for probing the interplay of quark and meson degrees of freedom in t…

QuarkRoper resonanceMesonpseudoscalar meson: production[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Nuclear TheoryGeneral Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physicsRecoil0103 physical sciencesp: recoilInvariant masselectron: beamProton emissionnumerical calculations010306 general physicsNuclear ExperimentMonte Carlohydrogen: targetPhysicspolarizationN(1440)010308 nuclear & particles physicsbeam: currenthelicityAmplitudekinematicsdifferential cross sectionpi0: electroproductionBeam-Recoil Polarization MeasurementNucleon
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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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