Search results for "26.30.+k"

showing 6 items of 6 documents

Relative proton and γ widths of astrophysically important states in 30S studied in the β-delayed decay of 31Ar

2013

Resonances just above the proton threshold in 30S affect the 29P(p,gamma)30S reaction under astrophysical conditions. The (p,gamma)-reaction rate is currently determined indirectly and depends on the properties of the relevant resonances. We present here a method for finding the ratio between the proton and gamma partial widths of resonances in 30S. The widths are determined from the beta-2p and beta-p-gamma decay of 31Ar, which is produced at the ISOLDE facility at the European research organization CERN. Experimental limits on the ratio between the proton and gamma partial widths for astrophysical relevant levels in 30S have been found for the first time. A level at 4688(5) keV is identif…

26.30.−k 23.40.Hc 27.30.+tAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesddc:530Experimental nuclear physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experiment
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Strong BV-extension and W1,1-extension domains

2021

We show that a bounded domain in a Euclidean space is a $W^{1,1}$-extension domain if and only if it is a strong $BV$-extension domain. In the planar case, bounded and strong $BV$-extension domains are shown to be exactly those $BV$-extension domains for which the set $\partial\Omega \setminus \bigcup_{i} \overline{\Omega}_i$ is purely $1$-unrectifiable, where $\Omega_i$ are the open connected components of $\mathbb{R}^2\setminus\overline{\Omega}$.

46E35 26B30Mathematics - Metric GeometrymatematiikkaMathematics::Complex VariablesBV-extensionFOS: MathematicsSobolev extensionMetric Geometry (math.MG)Analysis
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Mass Measurement on the rp-Process Waiting Point 72Kr

2004

The mass of one of the three major waiting points in the astrophysical rp process $^{72}$Kr was measured for the first time with the Penning trap mass spectrometer ISOLTRAP. The measurement yielded a relative mass uncertainty of $\deltam/m = 1.2\times 10–7 (\deltam$ = 8 keV). $^{73,74}$Kr, also needed for astrophysical calculations, were measured with more than 1 order of magnitude improved accuracy. We use the ISOLTRAP masses of $^{72–74}$Kr to reanalyze the role of $^{72}$Kr (T$_{1/2}$ = 17.2 s) in the rp process during x-ray bursts and conclude that $^{72}$Kr is a strong waiting point delaying the burst duration with at least 80\% of its $\beta$-decay half-life.

PhysicsNuclear and High Energy PhysicsLarge Hadron Collider26.30.+k 21.10.Dr 27.50.+e 32.10.Bi010308 nuclear & particles physicsHadronrp-process[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryPenning trap01 natural sciencesISOLTRAPnuclei with mass number 59 to 89particle trapsNuclear physicsnuclear massNucleosynthesis0103 physical sciencesNuclear fusionNuclear Physics - Experimentnucleon-nucleus reactions010306 general physicsNuclear Experimentbeta-decayNuclear Physics
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Density of Lipschitz functions in energy

2020

In this paper, we show that the density in energy of Lipschitz functions in a Sobolev space $N^{1,p}(X)$ holds for all $p\in [1,\infty)$ whenever the space $X$ is complete and separable and the measure is Radon and finite on balls. Emphatically, $p=1$ is allowed. We also give a few corollaries and pose questions for future work. The proof is direct and does not involve the usual flow techniques from prior work. It also yields a new approximation technique, which has not appeared in prior work. Notable with all of this is that we do not use any form of Poincar\'e inequality or doubling assumption. The techniques are flexible and suggest a unification of a variety of existing literature on th…

Primary 46E35 Secondary 30L99 26B30 28A12Mathematics - Classical Analysis and ODEsApplied MathematicsClassical Analysis and ODEs (math.CA)FOS: MathematicsfunktionaalianalyysiAnalysis
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Approximation by uniform domains in doubling quasiconvex metric spaces

2020

We show that any bounded domain in a doubling quasiconvex metric space can be approximated from inside and outside by uniform domains.

Pure mathematicsPrimary 30L99. Secondary 46E35 26B30Algebraic geometry01 natural sciencesDomain (mathematical analysis)funktioteoriaQuasiconvex functionMathematics::Group TheoryquasiconvexityMathematics - Metric Geometry0103 physical sciencesFOS: Mathematics0101 mathematicsuniform domainComputer Science::DatabasesMathematicsPartial differential equationFunctional analysis010102 general mathematicsMetric Geometry (math.MG)General Medicinemetriset avaruudetMetric spaceBounded functionSobolev extension010307 mathematical physicsfunktionaalianalyysi
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The Choquet and Kellogg properties for the fine topology when $p=1$ in metric spaces

2017

In the setting of a complete metric space that is equipped with a doubling measure and supports a Poincar´e inequality, we prove the fine Kellogg property, the quasi-Lindel¨of principle, and the Choquet property for the fine topology in the case p = 1. Dans un contexte d’espace m´etrique complet muni d’une mesure doublante et supportant une in´egalit´e de Poincar´e, nous d´emontrons la propri´et´e fine de Kellogg, le quasi-principe de Lindel¨of, et la propri´et´e de Choquet pour la topologie fine dans le cas p = 1. peerReviewed

Pure mathematicsProperty (philosophy)1-fine topologyGeneral MathematicsPoincaré inequalityMathematics::General Topology01 natural sciencesMeasure (mathematics)Complete metric spacefunktioteoriasymbols.namesakeMathematics - Metric GeometryFOS: Mathematics0101 mathematicsMathematicsApplied Mathematics010102 general mathematicsta111Metric Geometry (math.MG)30L99 31E05 26B30function of bounded variationfine Kellogg propertymetriset avaruudet010101 applied mathematicsMetric spacemetric measure spacequasi-Lindelöf principleChoquet propertysymbolspotentiaaliteoriaFine topology
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