0000000001299232

AUTHOR

M. Pfeiffer

showing 22 related works from this author

Double pi(0) photoproduction off the proton at threshold

2003

The reaction $\gamma p \to \pi^0 \pi^0 p$ has been measured using the TAPS BaF$_2$ calorimeter at the tagged photon facility of the Mainz Microtron accelerator. Chiral perturbation theory (ChPT) predicts that close to threshold this channel is significantly enhanced compared to double pion final states with charged pions. In contrast to other reaction channels, the lower order tree terms are strongly suppressed in 2$\pi^0$ photoproduction. The consequence is the dominance of pion loops in the 2$\pi^0$ channel close to threshold - a result that opens new prospects for the test of ChPT and in particular its inherent loop terms. The present measurement is the first which is sensitive enough fo…

PhysicsTAPSNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMesonProtonNuclear TheoryHigh Energy Physics::LatticeNEUTRAL-PION-PHOTOPRODUCTIONHadronNuclear TheoryElementary particleCHIRAL PERTURBATION-THEORYNuclear physicsPionTAGGED PHOTON SPECTROMETERNucleonNuclear ExperimentMicrotronNuclear Experiment
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A new recoil distance technique using low energy coulomb excitation in inverse kinematics

2011

Abstract We report on the first experiment combining the Recoil Distance Doppler Shift technique and multistep Coulomb excitation in inverse kinematics at beam energies of 3–10 A MeV. The setup involves a standard plunger device equipped with a degrader foil instead of the normally used stopper foil. An array of particle detectors is positioned at forward angles to detect target-like recoil nuclei which are used as a trigger to discriminate against excitations in the degrader foil. The method has been successfully applied to measure lifetimes in 128Xe and is suited to be a useful tool for experiments with radioactive ion beams.

PhysicsPlungerNuclear and High Energy PhysicsInverse kinematicsPhysics::Instrumentation and DetectorsDetectorCoulomb excitationsymbols.namesakeRecoilsymbolsPhysics::Accelerator PhysicsAtomic physicsNuclear ExperimentInstrumentationDoppler effectFOIL methodBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Shape dynamics in neutron-rich Kr isotopes: Coulomb excitation of 92Kr, 94Kr and 96Kr

2013

We report on the study of excited states in 92,94,96Kr populated via projectile Coulomb excitation at safe energies. The radioactive ion beams at energies of 2.85 MeV/u were delivered by the REX-ISOLDE facility at CERN and impinged on self-supporting 194,196Pt targets. The emitted γ -rays were detected by the Miniball detector-array. A detailed description of the experimental techniques used for extracting diagonal and transitional matrix elements and of the theoretical framework is given. The present experiment reveals the moderate evolution of the collective structure in the considered neutron-rich Kr isotopic chain, which is supported by the interacting boson model combined with the self…

Nuclear reactionPhysicsNuclear and High Energy PhysicsLarge Hadron Colliderta114[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsProjectileCoulomb excitation01 natural sciences7. Clean energyNuclear physicsMatrix (mathematics)Excited state0103 physical sciencesPhysics::Accelerator PhysicsNeutronInteracting boson modelAtomic physicsNuclear Experiment010306 general physics
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New results on the Roper resonance and the P_{11} partial wave

2008

Properties of the Roper resonance, the first scalar excitation of the nucleon, are determined. Pole positions and residues of the $P_{11}$ partial wave are studied in a combined analysis of pion- and photo-induced reactions. We find the Roper pole at $\{(1371\pm7)-i(92\pm10)\}$ MeV and an elasticity of $0.61\pm 0.03$. The largest decay coupling is found for the $N\sigma$ ($\sigma=(\pi\pi)$-$S$-wave). The analysis is based on new data on $\gamma p\to p\pi^0\pi^0$ for photons in the energy range from the two-pion threshold to 820 MeV from TAPS at Mainz and from 0.4 to 1.3 GeV from Crystal Barrel at Bonn and includes further data from other experiments. The partial wave analysis excludes the p…

TAPSNuclear and High Energy PhysicsRoper resonancePhotonProtonPHOTON SPECTROMETERPartial wave analysisNuclear TheoryDalitz plotFOS: Physical sciencesPION-PHOTOPRODUCTIONPROTONTHRESHOLDNuclear physicsPionHigh Energy Physics - Phenomenology (hep-ph)Nuclear ExperimentPhysicsPI(0) PHOTOPRODUCTIONHigh Energy Physics - PhenomenologyRELATIVISTIC QUARK-MODELSTRANGE-BARYON SPECTRUMPOSITIVE-STRANGENESSFORCESNucleonExcitation
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Collective 2$^{+1}$ excitations in$^{206}$Po and$^{208,210}$Rn

2016

In the present study, $B(E2; 2^{+}_{1}\rightarrow 0^{+}_{1})$ values have been measured in the 208,210Rn and 206Po nuclei through Coulomb excitation of re-accelerated radioactive beams in inverse kinematics at CERN-ISOLDE. These nuclei have been proposed to lie in, or at the boundary of the region where the seniority scheme should persist. However, contributions from collective excitations are likely to be present when moving away from the N=126 closed shell. Such an effect is confirmed by the observed increased collectivity of the $2^{+}_{1}\rightarrow 0^{+}_{1}$ transitions. Experimental results have been interpreted with the aid of theoretical studies carried out within the BCS-based QRP…

PhysicsNuclear reactionNuclear and High Energy Physics010308 nuclear & particles physicsHadronNuclear TheoryradonCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesIsotopes of palladiumcollective excitationExcited state0103 physical sciencesQuasiparticlePhysics::Accelerator PhysicsAtomic physics010306 general physicsNuclear ExperimentOpen shellpoloniumExcitationexcited states
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Coulomb excitation of re-accelerated 208Rn and 206Po beams

2013

In the present study, B( E2; 2(+)-> 0(+) ) values have been measured in the Rn-208 and Po-206 nuclei through Coulomb excitation of re-accelerated radioactive beams in inverse kinematics at CERN-ISOLDE. The resulting B(E2; 2(+)-> 0(+)) in 208Rn is similar to 0.08 e(2)b(2). These nuclei lie in, or at the boundary of the region where seniority scheme should persist. However, contributions from collective excitations may be present when moving away from the N = 126 shell closure. To date, surprisingly little is known of the transition probabilities between the low-spin states in this region.

PhysicsAngular momentumta114Isotope010308 nuclear & particles physicsPhysicsQC1-999Shell (structure)Boundary (topology)Coulomb excitation114 Physical sciences01 natural sciencesExperimental Nuclear PhysicsPhysics and AstronomySTATES0103 physical sciencesQuasiparticleApplied mathematicsPhysics::Accelerator PhysicsAtomic physics010306 general physicsSpin (physics)Nuclear ExperimentExcitation
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Evidence for a Smooth Onset of Deformation in the Neutron-Rich Kr Isotopes

2012

The neutron-rich nuclei Kr94,96 were studied via projectile Coulomb excitation at the REX-ISOLDE facility at CERN. Level energies of the first excited 2 + states and their absolute E2 transition strengths to the ground state are determined and discussed in the context of the E(21+) and B(E2;21+→01+) systematics of the krypton chain. Contrary to previously published results no sudden onset of deformation is observed. This experimental result is supported by a new proton-neutron interacting boson model calculation based on the constrained Hartree-Fock-Bogoliubov approach using the microscopic Gogny-D1M energy density functional. © 2012 American Physical Society.

Quantum phase transition[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]REX-ISOLDENuclear TheoryQUANTUM PHASE-TRANSITIONSGeneral Physics and Astronomychemistry.chemical_elementContext (language use)Coulomb excitationNuclear Structure01 natural sciencesREGIONNuclear physics0103 physical sciencesNuclear Physics - ExperimentNeutron010306 general physicsNuclear ExperimentDETECTORINTERACTING BOSONSPhysicsEXCITATIONSCOLLECTIVE NUCLEAR-STATESta114010308 nuclear & particles physicsKryptonFísicachemistryExcited stateSHELL-MODELInteracting boson modelAtomic physicsGround statePhysical Review Letters
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Erratum: Evidence for a Smooth Onset of Deformation in the Neutron-Rich Kr Isotopes [Phys. Rev. Lett.108, 062701 (2012)]

2012

Nuclear physicsPhysicsIsotopeGeneral Physics and AstronomyNeutronCoulomb excitationDeformation (meteorology)Physical Review Letters
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Corrigendum to: “Shape dynamics in neutron-rich Kr isotopes: Coulomb excitation of 92Kr, 94Kr and 96Kr” [Nucl. Phys. A 899 (2013) 1–28]

2016

Nuclear physicsPhysicsNuclear and High Energy PhysicsIsotope0103 physical sciencesNeutronCoulomb excitation010306 general physicsShape dynamics01 natural sciencesNuclear Physics A
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In-medium modifications of the pi pi interaction in photon-induced reactions

2002

Differential cross sections of the reactions $(\gamma,\pi^\circ\pi^\circ)$ and $(\gamma,\pi^\circ\pi^++\pi^\circ\pi^-)$ have been measured for several nuclei ($^1$H,$^{12}$C, and $^{\rm nat}$Pb) at an incident-photon energy of $E_{\gamma}$=400-460 MeV at the tagged-photon facility at MAMI-B using the TAPS spectrometer. A significant nuclear-mass dependence of the $\pi\pi$ invariant-mass distribution is found in the $\pi^\circ\pi^\circ$ channel. This dependence is not observed in the $\pi^\circ\pi^{+/-}$ channel and is consistent with an in-medium modification of the $\pi\pi$ interaction in the $I$=$J$=0 channel. The data are compared to $\pi$-induced measurements and to calculations within …

PhysicsPhotonMesonPAIRSHadronCarbon-12General Physics and AstronomyElementary particleNONPERTURBATIVE APPROACHCHIRAL-SYMMETRY RESTORATIONPionNUCLEAR MEDIUMPiSPECTROMETERMESONAtomic physicsNuclear ExperimentNuclear ExperimentMATTERBoson
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Determination of the B(E3, 0+ → 3−)-excitation strength in octupole-correlated nuclei near A ≈224 by the means of Coulomb excitation at REX-ISOLDE

2013

The IS475 collaboration conducted Coulomb-excitation experiments with postaccelerated radioactive 220Rn and 224Ra beams at the REX-ISOLDE facility. The beam particles (Ebeam ≈ 2.83 MeV/u) were Coulomb excited using 60Ni, 114Cd, and 120Sn scattering targets. De-excitation γ-rays were detected employing the Miniball array and scattered particles were detected in a silicon detector. Exploiting the Coulomb-excitation code GOSIA for each nucleus several matrix elements could be obtained from the measured γ-ray yields. The extracted 3−||Ê3||0+ matrix element allows for the conclusion that, while 220Rn represents an octupole vibrational system, 224Ra has already substantial octupole correlations i…

PhysicsHistoryScatteringCoulomb excitationPhysics and Astronomy(all)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Charged particleParticle detectorComputer Science ApplicationsEducationNuclear physics25.70.De; 27.90.+b; 23.20.Js/dk/atira/pure/subjectarea/asjc/3100Excited stateCoulombPhysics::Accelerator PhysicsAtomic physicsGround stateExcitationComputingMilieux_MISCELLANEOUS
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Transparency ratio in γA→η′A′ and the in-medium η′ width

2012

Abstract The photoproduction of η ′ -mesons off different nuclei has been measured with the CBELSA/TAPS detector system for incident photon energies between 1500–2200 MeV. The transparency ratio has been deduced and compared to theoretical calculations describing the propagation of η ′ -mesons in nuclei. The comparison indicates a width of the η ′ -meson of the order of Γ = 15 – 25 MeV at ρ = ρ 0 for an average momentum p η ′ = 1050 MeV / c , at which the η ′ -meson is produced in the nuclear rest frame. The inelastic η ′ N cross section is estimated to be 3–10 mb. Parameterizing the photoproduction cross section of η ′ -mesons by σ ( A ) = σ 0 A α , a value of α = 0.84 ± 0.03 has been dedu…

PhysicsNuclear and High Energy PhysicsPhotonProtonMeson010308 nuclear & particles physicsScatteringNuclear TheoryNiobiumchemistry.chemical_elementRest frame7. Clean energy01 natural sciencesMomentumNuclear physicsCross section (physics)chemistry0103 physical sciencesHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment010306 general physicsPhysics Letters B
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Studies of pear-shaped nuclei using accelerated radioactive beams

2013

There is strong circumstantial evidence that certain heavy, unstable atomic nuclei are ‘octupole deformed’, that is, distorted into a pear shape. This contrasts with the more prevalent rugby-ball shape of nuclei with reflection-symmetric, quadrupole deformations. The elusive octupole deformed nuclei are of importance for nuclear structure theory, and also in searches for physics beyond the standard model; any measurable electric-dipole moment (a signature of the latter) is expected to be amplified in such nuclei. Here we determine electric octupole transition strengths (a direct measure of octupole correlations) for short-lived isotopes of radon and radium. Coulomb excitation experiments we…

PhysicsMultidisciplinaryIsotopeta114010308 nuclear & particles physicsNuclear TheoryNuclear structureCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physics0103 physical sciencesAtomic nucleusQuadrupolePhysics::Accelerator PhysicsNeutronNuclidePhysics::Atomic PhysicsAtomic physics010306 general physicsNucleonNuclear Experiment
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Do nuclei go pear-shaped? Coulomb excitation of 220Rn and 224Ra at REX-ISOLDE (CERN)

2014

Artículo escrito por muchos autores, sólo se referencian el primero, los autores que firman como Universidad Autónoma de Madrid y el grupo de colaboración en el caso de que aparezca en el artículo

Materials scienceta114PhysicsQC1-999Coulomb excitationREX-ISOLDEFísicaradon[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energyNucleiradiumNuclear magnetic resonancePhysics::Accelerator PhysicsGamma spectroscopypear-shaped nuclei
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The Reactionγp→π0γ′pand the Magnetic Dipole Moment of theΔ+(1232)Resonance

2002

The reaction $\ensuremath{\gamma}p\ensuremath{\rightarrow}{\ensuremath{\pi}}^{0}{\ensuremath{\gamma}}^{\ensuremath{'}}p$ has been measured with the TAPS calorimeter at the Mainz Microtron accelerator facility MAMI for energies between $\sqrt{s}=1221--1331\text{ }\text{ }\mathrm{M}\mathrm{e}\mathrm{V}$. The cross section's differential in angle and energy have been determined for the photon ${\ensuremath{\gamma}}^{\ensuremath{'}}$ in three bins of the excitation energy. This reaction channel provides access to the magnetic dipole moment of the ${\ensuremath{\Delta}}^{+}(1232)$ resonance and, for the first time, a value of ${\ensuremath{\mu}}_{{\ensuremath{\Delta}}^{+}}=\mathbf{[}{2.7}_{\ensu…

BaryonPhysicsCrystallographyParticle physicsAngular distributionMagnetic momentPiGeneral Physics and AstronomyResonanceNuclear ExperimentEnergy (signal processing)Physical Review Letters
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"Table 6" of "In-medium modifications of the pi pi interaction in photon-induced reactions."

2005

Differential cross section for PI0PI+/- production with a Lead target. Errors are statistical only.

Single Differential Cross SectionPhotoproductionDSIG/DMGAMMA PB --> PI0 PI+GAMMA PB --> PI0 PI-ExclusiveGAMMA NUCLEUS --> PI- PI0GAMMA NUCLEUS --> PI+ PI0
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"Table 2" of "In-medium modifications of the pi pi interaction in photon-induced reactions."

2005

Differential cross section for PI0PI0 production with a Carbon target. Errors are statistical only.

GAMMA NUCLEUS --> PI0 PI0Single Differential Cross SectionPhotoproductionDSIG/DMGAMMA C --> PI0 PI0Exclusive
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"Table 1" of "In-medium modifications of the pi pi interaction in photon-induced reactions."

2005

Differential cross section for PI0PI0 production with a proton target. Errors are statistical only. Note that the data given in this table are sightly different (newer) than the data points presented in the paper.

Single Differential Cross SectionGAMMA P --> PI0 PI0PhotoproductionDSIG/DMExclusive1.277-1.32
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"Table 4" of "In-medium modifications of the pi pi interaction in photon-induced reactions."

2005

Differential cross section for PI0PI+ production with a proton target. Errors are statistical only. Note that the data given in this table are sightly different (newer) than the data points presented in the paper.

Single Differential Cross SectionPhotoproductionDSIG/DMExclusiveGAMMA P --> PI0 PI+1.277-1.32
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"Table 3" of "In-medium modifications of the pi pi interaction in photon-induced reactions."

2005

Differential cross section for PI0PI0 production with a Lead target. Errors are statistical only.

GAMMA NUCLEUS --> PI0 PI0Single Differential Cross SectionPhotoproductionDSIG/DMExclusiveGAMMA PB --> PI0 PI0
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"Table 1" of "Double pi0 photoproduction off the proton at threshold."

2004

Total cross section measurement. Statistical errors only.

PhotoproductionIntegrated Cross SectionGAMMA P --> PI0 PI0 PExclusiveCross SectionSIG1.211-1.289
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"Table 5" of "In-medium modifications of the pi pi interaction in photon-induced reactions."

2005

Differential cross section for PI0PI+/- production with a Carbon target. Errors are statistical only.

GAMMA C --> PI0 PI-Single Differential Cross SectionGAMMA C --> PI0 PI+PhotoproductionDSIG/DMExclusiveGAMMA NUCLEUS --> PI- PI0GAMMA NUCLEUS --> PI+ PI0
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