Search results for "[formula omitted] decay"

showing 10 items of 1452 documents

Superasymmetric fission at intermediate energy and production of neutron-rich nuclei with A < 80

1997

Abstract The yields of neutron-rich Ni, Cu, Zn, Ga and Ge-isotopes were measured in 25 MeV proton induced fission of 238 U using the ion guide-based isotope separator technique. The results indicate enhancement for superasymmetric mass division at intermediate excitation energy of the fissioning nucleus and show the potential of this reaction for the production of neutron-rich exotic nuclei around Z = 28.

Nuclear physicsPhysicsNuclear and High Energy PhysicsCold fissionCluster decayProtonIsotopeFissionNuclear fissionNuclear TheoryNeutronFission product yieldNuclear ExperimentPhysics Letters B
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Levels in104Ru populated by the ??-decay of104Tc

1978

Theβ− — andγ-activities of 18.4 min104Tc have been studied with singles and coincidence measurements. Sources were prepared by chemical separation of technetium from the fission products of thermal-neutron-induced fission of235U. A revised level scheme of104Ru up to an excitation energy of 4.26 MeV is proposed. Fromβ-γ coincidence measurements, aQβ-value of 5.62±0.07 MeV has been obtained.

Nuclear physicsPhysicsNuclear and High Energy PhysicsCold fissionFission productsCluster decayFissionNuclear fusionFission product yieldCoincidenceExcitationZeitschrift f�r Physik A Atoms and Nuclei
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Cross section systematics for the lightest Bi and Po nuclei produced in complete fusion reactions with heavy ions

2005

The production of the very neutron-deficient nuclides $^{184\ensuremath{-}192}\mathrm{Bi}$ and $^{186\ensuremath{-}192}\mathrm{Po}$ in the vicinity of the neutron midshell at N = 104 has been studied by using heavy-ion-induced complete fusion reactions in a series of experiments at the velocity filter SHIP. The cross sections for the xn and pxn evaporation channels of the $^{46}\mathrm{Ti}$+$^{144}\mathrm{Sm}$$\ensuremath{\rightarrow}^{190}\mathrm{Po}{}^{*},$$^{98}\mathrm{Mo}$+$^{92}\mathrm{Mo}$$\ensuremath{\rightarrow}^{190}\mathrm{Po}{}^{*},$$^{50,52}\mathrm{Cr}$+$^{142}\mathrm{Nd}$$\ensuremath{\rightarrow}^{192,194}\mathrm{Po}{}^{*}$, and $^{94,95}\mathrm{Mo}$+$^{93}\mathrm{Nb}$$\ensurem…

Nuclear physicsPhysicsNuclear and High Energy PhysicsCross section (physics)CrystallographyFissionNuclear fusionProduction (computer science)NeutronAlpha decayXXNuclear ExperimentIonPhysical Review C
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Study of theB−→J/ψK−π+π−decay and measurement of theB−→X(3872)K−branching fraction

2005

The authors study the decay B{sup -} {yields} J/{psi}K{sup -}{pi}{sup +}{pi}{sup -} using 117 million B{bar B} events collected at the {Upsilon}(4S) resonance with the BaBar detector at the PEP-II e{sup +}e{sup -} asymmetric-energy storage ring. They measure the branching fractions {Beta}(B{sup -} {yields} J/{psi}K{sup -} {pi}{sup +}{pi}{sup -}) = (116 {+-} 7(stat.) {+-} 9(syst.)) x 10{sup -5} and {Beta}(B{sup -} {yields} X(3872)K{sup -}) x {Beta}(X(3872) {yields} J/{psi}{pi}{sup +}{pi}{sup -}) = (1.28 {+-} 0.41) x 10{sup -5} and find the mass of the X(3872) to be 3873.4 {+-} 1.4MeV/c{sup 2}. They search for the h{sub c} narrow state in the decay B{sup -} {yields} h{sub c} K{sup -}, h{sub c…

Nuclear physicsPhysicsNuclear and High Energy PhysicsCrystallographyParticle decay010308 nuclear & particles physicsBranching fractionTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYElectron–positron annihilation0103 physical sciences010306 general physics01 natural sciencesX(3872)Physical Review D
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In-beam and decay spectroscopy of transfermium nuclei

2008

Abstract In recent years the body of experimental data on nuclei with masses A ≃ 250 has increased dramatically. Nuclei that had been out of reach for experimental studies have now become available for study through a variety of approaches, both with in-beam spectroscopic methods and through spectroscopy following the decay of isomeric states or alpha decays at the focal plane of powerful separators. This article aims to collect the currently available experimental data on nuclei between Cm ( Z = 96 ) and Db ( Z = 105 ) . The review of this data builds on the evaluations in the literature and focusses on those datasets obtained most recently.

Nuclear physicsPhysicsNuclear and High Energy PhysicsDecay schemeCardinal pointDouble beta decayExperimental dataAlpha decaySpectroscopyBeam (structure)Progress in Particle and Nuclear Physics
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β-decay ofO13

2005

The beta decay of O-13 has been studied at the IGISOL facility of the Jyvaskyla accelerator centre (Finland). By developing a low-energy isotope-separated beam of O-13 and using a modern segmented charged-particle detector array an improved measurement of the delayed proton spectrum was possible. Protons with energy up to more than 12 MeV are measured and the corresponding log(ft) values extracted. A revised decay scheme is constructed. The connection to molecular states and the shell model is discussed.

Nuclear physicsPhysicsNuclear and High Energy PhysicsDecay schemeInternal conversionProtonDouble beta decayPhysics::Accelerator PhysicsNeutronNuclear drip lineNuclear ExperimentBeta decayRadioactive decayPhysical Review C
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Note on the decay of200Au

1972

Gamma and beta rays from the decay of200Au (48.4 min) were studied employing Ge(Li) and plastic detectors in various singles and coincidence arrangements. The intensity of the β-branch to the ground state of200Hg was determined as 79%, and the disintegration energy of200Au to be asQβ=2.26 ± 0.06 MeV. A tentative spin and parity assignment of (1,2)+ is proposed for levels at 1515.2 and 1972.5 keV in 200Hg

Nuclear physicsPhysicsNuclear and High Energy PhysicsDecay schemeIsotopes of germaniumDouble beta decayBeta particleIsotopes of zirconiumAtomic physicsNuclear isomerGround stateRadioactive decayZeitschrift f�r Physik
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R-matrix analysis of theβdecays ofN12andB12

2010

The β decays of 12N and 12B have been studied at KVI and JYFL to resolve the composition of the broad and interfering 0+ and 2+ strengths in the triple-α continuum. For the first time a complete treatment of 3α decay is presented including all major breakup channels. A multilevel, many-channel R-matrix formalism has been developed for the complete description of the breakup in combination with the recently published separate analysis of angular correlations. We find that, in addition to the Hoyle state at 7.65 MeV, more than one 0+ and 2+ state is needed to reproduce the spectra. Broad 03+ and 22+ states are found between 10.5 and 12 MeV in this work. The presence of β strength up to the 12…

Nuclear physicsPhysicsNuclear and High Energy PhysicsExcited stateDouble beta decayCarbon-12Isotopes of boronAlpha particleAtomic physicsRadioactive decaySpectral lineR-matrixPhysical Review C
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Level scheme ofZr101and structure of theN=61 Sr, Zr, and Mo isotones

1995

The neutron-rich nucleus $_{40}^{101}\mathrm{Zr}_{61}$ has been studied at the isotope separator ISOLDE via the \ensuremath{\beta} decay of $^{101}\mathrm{Y}$. A detailed level scheme has been obtained from \ensuremath{\gamma}-ray singles, \ensuremath{\gamma}-\ensuremath{\gamma}-t and \ensuremath{\beta}-\ensuremath{\gamma}-t coincidence measurements. The level structure of $^{101}\mathrm{Zr}$ is similar to that of its isotone $^{103}\mathrm{Mo}$ showing that, in contrast to their Sr neighbors, the Zr isotopes do not reach maximum of deformation immediately at its onset. This result is rather well reproduced by particle-rotor coupling calculations. A level systematics for the deformed N=61 i…

Nuclear physicsPhysicsNuclear and High Energy PhysicsExcited stateIsotoneNuclear structureLevel structureAtomic physicsNuclear ExperimentRadioactive decayPhysical Review C
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First observation of excited states in the neutron deficientN=86isotones159Taand160W

2001

Nuclear physicsPhysicsNuclear and High Energy PhysicsExcited stateNeutronAlpha decayAtomic physicsPhysical Review C
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