Search results for "Experimental nuclear physics"

showing 10 items of 42 documents

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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X(5) critical-point symmetries in 138Gd

2011

International audience; The lifetimes of low-lying transitions in 138Gd have been measured using the recoil-distance Doppler-shift technique. The resultant reduced transition probabilities have been compared to X(5) critical-point calculations to assess the potential 'phase-transitional' behaviour of 138Gd. The X(5) symmetry describes the first order 'phase transition' between sphericity, U(5) and an axially deformed nuclear shape, SU(3). Although a high degree of correspondence is observed between the experimental and theoretical excitation energies, the large uncertainties of the experimental B(E2) values cannot preclude contributions from either vibrational or rotational modes of excitat…

PhysicsHistory010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]First order01 natural sciencesCritical point (mathematics)Computer Science ApplicationsEducationBohr modelSphericityKokeellinen ydinfysiikka21.10.Tg Lifetimes widths 27.60.+j 90(less-than-or-equal-to)A(less-than-or-equal-to)149 21.65.-f Nuclear matter 23.20.-g Electromagnetic transitions 21.10.Re Collective levels 21.60.Ev Collective modelssymbols.namesakeQuantum mechanics0103 physical sciencesHomogeneous spacesymbolsExperimental nuclear physics010306 general physicsHamiltonian (quantum mechanics)Axial symmetryExcitation
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Pushing the Limits: Nuclear Structure of Heavy Elements

2012

Throughout the history of nuclear structure studies, searches for new phenomena have been carried out at the extremes. These extremes can be described in terms of nuclear excitation energy, spin, or in terms of proton or neutron number through the production of exotic nuclei far from stability. One extreme which has always been a centre for activity is that of mass and proton number - the desire to create new chemical elements and understand their nuclear structure. New elements up to proton number Z=118 have been created in the laboratory, but by nature these experiments cannot provide extensive information concerning nuclear structure. The extremely small production cross sections only al…

PhysicsHistoryProtonField (physics)010308 nuclear & particles physicsNuclear TheoryNuclear structure01 natural sciencesComputer Science ApplicationsEducationKokeellinen ydinfysiikkaNuclear physicsNeutron number0103 physical sciencesAtomic numberExperimental nuclear physics010306 general physicsNuclear ExperimentExcitationSpin-½
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The next generation nuclear instruments: AGATA and NEDA, and nuclear structure studies near N=Z line

2017

The first part of this thesis is devoted to the development of a large array of neutron detectors NEDA (NEutron Detector Array) and their conceptual design using Monte-Carlo simulations. Prior to the development of NEDA, the neutron detection with liquid scintillators is discussed in Chapter 2. In Chapter 3, the design criteria and simulations of NEDA are discussed. NEDA aims to build a neutron detector array with high efficiency, based on liquid scintillators. NEDA will be coupled to the high-purity γ-ray detector arrays, like AGATA, EXOGAM, to be used as a trigger or complementary detector in the contemporary nuclear physics experiments, which aim to investigate the structure of the exoti…

PhysicsNeutron DetectionDetectorsNEDANuclear Structure220806 - DETECTORES DE PARTICULASExperimental Nuclear PhysicsLiquid Scintillator Detectors220719 - ESTRUCTURA NUCLEAR220717 - REACCION NUCLEAR Y DISPERSIONNuclear ExperimentAGATAGe Semiconductor DetectorsNuclear InstrumentationNuclear Physics
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In-beam spectroscopy with intense ion beams: Evidence for a rotational structure in246Fm

2012

The rotational structure of ${}^{246}$Fm has been investigated using in-beam $\ensuremath{\gamma}$-ray spectroscopic techniques. The experiment was performed using the JUROGAMII germanium detector array coupled to the gas-filled recoil ion transport unit (RITU) and the gamma recoil electron alpha tagging (GREAT) focal plane detection system. Nuclei of ${}^{246}$Fm were produced using a 186 MeV beam of ${}^{40}$Ar impinging on a ${}^{208}$Pb target. The JUROGAMII array was fully instrumented with Tracking Numerical Treatment 2 Dubna (TNT2D) digital acquisition cards. The use of digital electronics and a rotating target allowed for unprecedented beam intensities of up to 71 particle-nanoamper…

PhysicsNuclear and High Energy Physicsta114010308 nuclear & particles physics23.20.−g 24.10.Eq 21.10.Re 27.90.+b[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Tracking (particle physics)01 natural sciencesRecoil electronKokeellinen ydinfysiikkaSemiconductor detectorIonRecoilCardinal pointNuclear magnetic resonance0103 physical sciencesNuclear Physics - ExperimentExperimental nuclear physicsAtomic physicsNuclear Experiment010306 general physicsSpectroscopyBeam (structure)Physical Review C
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Recoil-decay tagging study of 205Fr

2012

The nucleus 205Fr has been studied through γ -ray and electron spectroscopy using the recoil-decay tagging technique. The resulting level scheme presents a spherical structure built on the 9/2− ground state and a rotational structure on top of a short-lived isomer. The isomer, with a spin and parity of 13/2+ and a half-life of 80(20) ns, de-excites by an M2 transition directly to the 9/2− ground state. Another, longer-lived, isomer, with a half-life of 1.15(4) ms, has also been found and assigned a spin and parity of 1/2+. Transitions populating and de-exciting this isomer have been observed as well. peerReviewed

PhysicsNuclear physicsNuclear and High Energy PhysicsRecoilta114010308 nuclear & particles physics0103 physical sciencesExperimental nuclear physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]010306 general physics01 natural sciences23.20.Lv 23.35.+g 27.80.+w 29.30.KvKokeellinen ydinfysiikkaPhysical review C
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Transition probability studies in 175Au

2013

Transition probabilities have been measured between the low-lying yrast states in 175Au by employing the recoil distance Doppler-shift method combined with the selective recoil-decay tagging technique. Reduced transition probabilities and magnitudes of transition quadrupole moments have been extracted from measured lifetimes allowing dramatic changes in nuclear structure within a low excitation-energy range to probed. The transition quadrupole moment data are discussed in terms of available systematics as a function of atomic number and aligned angular momentum. peerReviewed

Physics::Atomic PhysicsExperimental Nuclear Physics
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Identification of new transitions feeding the high-spin isomers in $^{139}$Nd and $^{140}$Nd nuclei

2013

The population of the high-spin isomers in 139Nd and 140Nd was investigated using the 96Zr(48Ca,xn) reaction and the JUROGAM + RITU + GREAT setup employing the recoil decay tagging technique. Three transitions feeding the 23/2+ isomer in 139Nd and two transitions feeding the 20+ isomer in 140Nd were identified. The newly observed transitions allowed the excitation energy of the isomer to be established in 139Nd and to assign configurations to the states and bands deexcited by the observed transitions in both nuclei. peerReviewed

[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ComputingMilieux_MISCELLANEOUSExperimental Nuclear Physics
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The detection efficiency of the clover Ge-detectors array at the RITU-GREAT facility

2015

Absolute detection efficiency depending upon its position along the beam line is determined for three germanium detectors, that are part of the GREAT spectrometer at the RITU separator focal plane. The efficiency is determined for an energy range from 80 keV to 1400 keV for all three detectors as an array and also individually using digital electronics. The optimal position for the detector array has been defined for two configurations of the GREAT spectrometer: with planar detector and without it. The obtained results have been compared with three references: a simulation prepared especially for this setup by another student, a previous study that was carried out by applying analogue elect…

clover detectorsPhysics::Instrumentation and DetectorsGe-detectorsspektrometritexperimental nuclear physicsRITUGREATgamma-spectroscopydetction efficiencyydinfysiikka
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Reassigning the shapes of the 0+ states in the 186Pb nucleus

2022

Across the physics disciplines, the 186Pb nucleus is the only known system, where the two first excited states, together with the ground state, form a triplet of zero-spin states assigned with prolate, oblate and spherical shapes. Here we report on a precision measurement where the properties of collective transitions in 186Pb were determined in a simultaneous in-beam γ-ray and electron spectroscopy experiment employing the recoil-decay tagging technique. The feeding of the 0+2 state and the interband 2+2→2+1 transition have been observed. We also present direct measurement of the energies of the electric monopole transitions from the excited 0+ states to the 0+ ground state. In contrast to…

experimental nuclear physicslyijyhiukkasfysiikkaydinfysiikkaphysics3100
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