Search results for "PACS"

showing 10 items of 141 documents

Precise branching ratios to unbound 12C states from 12N and 12B β-decays

2009

6 pages, 2 tables, 4 figures.--PACS nrs.: 21.45.-v; 23.40.-s; 27.20.+n; 21.60.De.--Printed version published Aug 3, 2009

branching ratiosPhysicsNuclear and High Energy PhysicsChiral perturbation theory[PACS] β decayBranching fractionNuclear shell model[PACS] Ab initio methods[PACS] β decay; double β decay; electron and muon captureAlpha particleFew-body systems[PACS] Few-body systemselectron and muon capturedouble β decay6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Double beta decayExcited stateAtomic physics[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Nucleonbeta-decayC12
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Macroscopic persistent currents in YBa2Cu3O7

1988

Persistent currents in polycrystalline YBa2Cu3O7 rings have been investigated by measuring the spatial distribution of the magnetic flux trapped in field-cooled samples. The results unambiguously show that macroscopic persistent ring currents exist. The critical current density depends very sensitively on the sample quality, reachingj c ≈250 A/cm2 at 77 K for our best samples.

chemistry.chemical_classificationMaterials scienceHigh-temperature superconductivityCondensed matter physicspacs:68.35.JaPersistent currentCondensed Matter PhysicsRing (chemistry)Magnetic fluxElectronic Optical and Magnetic Materialslaw.inventionSample qualitychemistrypacs:67.70.+nlawCondensed Matter::Superconductivityddc:530General Materials ScienceCrystalliteCritical currentpacs:61.12.ExInorganic compoundZeitschrift f�r Physik B Condensed Matter
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Experimental evidence for a liquid-liquid crossover in deeply cooled confined water.

2014

International audience; In this work we investigate, by means of elastic neutron scattering, the pressure dependence of mean square displacements (MSD) of hydrogen atoms of deeply cooled water confined in the pores of a three-dimensional disordered SiO 2 xerogel; experiments have been performed at 250 and 210 K from atmospheric pressure to 1200 bar. The " pressure anomaly " of supercooled water (i.e., a mean square displacement increase with increasing pressure) is observed in our sample at both temperatures; however, contrary to previous simulation results and to the experimental trend observed in bulk water, the pressure effect is smaller at lower (210 K) than at higher (250 K) temperatur…

liquid-liquid transitionPhase transitionPACS: 64.70.Ja 64.70.pm 25.40.DnMaterials scienceNeutron diffractionGeneral Physics and AstronomyThermodynamicsNeutron scatteringSettore FIS/03 - Fisica Della MateriaPhase TransitionNuclear magnetic resonanceWater Movementsglass transitionElastic neutron scattering[PHYS.COND]Physics [physics]/Condensed Matter [cond-mat]SupercoolingElastic neutron scattering; calorimetry; glass transition; liquid-liquid transitionAtmospheric pressure[SDV.BBM.BS]Life Sciences [q-bio]/Biochemistry Molecular Biology/Structural Biology [q-bio.BM]Calorimetry Differential ScanningWaterSilicon DioxideSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Cold Temperature[SDV.BBM.BS]Life Sciences [q-bio]/Biochemistry Molecular Biology/Biomolecules [q-bio.BM]Neutron DiffractionModels ChemicalGlass transitioncalorimetryHydrophobic and Hydrophilic InteractionsAmbient pressureBar (unit)HydrogenPhysical review letters
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Interactions of membranes with coarse-grain proteins: a comparison

2012

We study the interactions between lipid bilayers and rigid transmembrane proteins by Monte Carlo simulations of generic coarse-grain models. Different popular protein models are considered and compared with each other, and key parameters such as the hydrophobicity and the hydrophobic mismatch are varied systematically. Furthermore, the properties of the membrane are manipulated by applying different tensions. The response of the membrane to the insertion of single proteins is found to be mostly generic and independent of the choice of the protein model. Likewise, the orientational distributions of single proteins depend mainly on the hydrophobic mismatch and the hydrophobicity of the protei…

pacs:87.16.D; 87.15.K; 02.70.Uu; 87.14CcPhysicsNucleationGeneral Physics and AstronomyInterbilayer forces in membrane fusion530Transmembrane proteinHydrophobic mismatchMembraneLattice proteinBiophysicsddc:530Lipid bilayerHydrophobicity scalesNew Journal of Physics
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The Interconnecting Hairpin Extension "Arm": An Essential Allosteric Element of Phytochrome Activity

2023

In red-light sensing phytochromes, isomerization of the bilin chromophore triggers structural and dynamic changes across multiple domains, ultimately leading to control of the output module (OPM) activity. In between, a hairpin structure, "arm", extends from an interconnecting domain to the chromophore region. Here, by removing this protein segment in a bacteriophytochrome from Deinococcus radiodurans (DrBphP), we show that the arm is crucial for signal transduction. Crystallographic, spectroscopic, and biochemical data indicate that this variant maintains the properties of DrBphP in the resting state. Spectroscopic data also reveal that the armless systems maintain the ability to respond t…

phytochromesoluviestintäphotosensorallostery92-11histidine kinanasephotoreceptorthermal stabilityreseptorit (biokemia)87.1592-05structure and functionproteiinitvalokemia87.14 2000 MSCprotein structurePACSsignal transduction
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8-parameter solutions of fifth order to the Johnson equation

2019

We give different representations of the solutions of the Johnson equation with parameters. First, an expression in terms of Fredholm determinants is given; we give also a representation of the solutions written as a quotient of wronskians of order 2N. These solutions of order N depend on 2N − 1 parameters. When one of these parameters tends to zero, we obtain N order rational solutions expressed as a quotient of two polyno-mials of degree 2N (N +1) in x, t and 4N (N +1) in y depending on 2N −2 parameters. Here, we explicitly construct the expressions of the rational solutions of order 5 depending on 8 real parameters and we study the patterns of their modulus in the plane (x, y) and their …

rogue waves PACS numbers : 33Q55ratio- nal solutionswronskiansrational solutions[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]Johnson equation4710A-[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]37K104735Fg4754BdFredholm determinants
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From first to fourth order rational solutions to the Boussinesq equation

2020

Rational solutions to the Boussinesq equation are constructed as a quotient of two polynomials in x and t. For each positive integer N , the numerator is a polynomial of degree N (N + 1) − 2 in x and t, while the denominator is a polynomial of degree N (N + 1) in x and t. So we obtain a hierarchy of rational solutions depending on an integer N called the order of the solution. We construct explicit expressions of these rational solutions for N = 1 to 4.

rogue waves PACS numbers : 33Q55rational solutions[MATH.MATH-MP]Mathematics [math]/Mathematical Physics [math-ph]4710A-[MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]37K104735Fg4754BdBoussinesq equation
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ETAT TOPOLOGIQUE DE L'ESPACE TEMPS A L'ECHELLE 0

2002

We propose in this research a new solution regarding the existence and the content of the initial spacetime singularity. In the context of topological field theory we consider that the initial singularity of space-time corresponds to a zero size singular gravitational instanton characterized by a Riemannian metric configuration (++++) in dimension D = 4. Connected with some unexpected topological data corresponding to the zero scale of space-time, the initial singularity is thus not considered in terms of divergences of physical fields but can be resolved in the frame of topological field theory. We get this result from the physical observation that the pre-spacetime is in a thermal equilib…

singularité initiale[ MATH.MATH-MP ] Mathematics [math]/Mathematical Physics [math-ph]amplitude topologique PACS : 0420D04.60.-m05.45.-a[PHYS.MPHY] Physics [physics]/Mathematical Physics [math-ph]État KMSinstanton gravitationnel singulierthéorie topologique des champsinvariant de singularité04.65.+e[ PHYS.MPHY ] Physics [physics]/Mathematical Physics [math-ph][MATH.MATH-MP] Mathematics [math]/Mathematical Physics [math-ph]02.40.Xx
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Predictive models in assessment of macroinvertebrates in boreal rivers

2009

Jukka Aroviita tutki väitöskirjassaan jokien ja purojen biologisen tilan mittaamismenetelmiä. Aroviita osoitti, että ihmistoiminnan aiheuttamat biologiset muutokset voivat jäädä havaitsematta, jos eliöyhteisöjen luonnollista taustavaihtelua ei oteta kunnolla huomioon.- Tällöin vesistöjen saatetaan arvioida olevan paremmassa kunnossa kuin ne todellisuudessa ovatkaan. Muutosten tunnistamistarkkuuden tulisi olla mahdollisimman hyvä, sillä tila-arvioilla on myös juridisesti määräytyviä yhteiskunnallisia ja taloudellisia seuraamuksia, Aroviita toteaa. Vielä 1990-luvulla järvien ja jokien tilaa arvioitiin suurelta osin ihmisen näkökulmasta ja veden kemian perusteella. Nykylainsäädäntö edellyttää …

spatial scalebioassessmentpohjaeläimistöRIVPACSbiotic qualitytaxonomic completenessvirtavedetvertailuololähestymistapaennustavat mallitmacroinvertebratestypologystreamstypologiat
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Laser fluence, repetition rate and pulse duration effects on paint ablation

2006

Abstract The efficiency (mm3/(J pulse)) of laser ablation of paint was investigated with nanosecond pulsed Nd:YAG lasers (λ = 532 nm) as a function of the following laser beam parameters: pulse repetition rate (1–10,000 Hz), laser fluence (0.1–5 J/cm2) and pulse duration (5 ns and 100 ns). In our study, the best ablation efficiency (η ≅ 0.3 mm3/J) was obtained with the highest repetition rate (10 kHz) at the fluence F = 1.5 J/cm2. This ablation efficiency can be associated with heat accumulation at high repetition rate, which leads to the ablation threshold decrease. Despite the low thermal diffusivity and the low optical absorption of the paint (thermal confinement regime), the ablation th…

thermal confinement regimeMaterials sciencePACS: 81.65 Cf; 42.62 Cf; 61.82 Msmedicine.medical_treatmentGeneral Physics and Astronomy02 engineering and technology01 natural sciencesFluencelaw.invention010309 opticsOpticslaw0103 physical sciencesmedicineAbsorption (electromagnetic radiation)Laser ablationPulse (signal processing)business.industryrepetition ratePulse duration[CHIM.MATE]Chemical Sciences/Material chemistrySurfaces and InterfacesGeneral ChemistryNanosecond021001 nanoscience & nanotechnologyCondensed Matter PhysicsAblationLaserpaint strippingLaser ablationSurfaces Coatings and Filmspulse duration[ CHIM.MATE ] Chemical Sciences/Material chemistryOptoelectronics0210 nano-technologybusinessApplied Surface Science
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