Search results for "Two band"

showing 4 items of 4 documents

Dispersal of larval and juvenile seabream: Implications for Mediterranean marine protected areas

2015

International audience; In the marine context, information about dispersal is essential for the design of networks of marine protected areas (MPAs). Generally, most of the dispersal of demersal fishes is thought to be driven by the transport of eggs and larvae in currents, with the potential contribution of dispersal in later life stages relatively minimal.Using otolith chemistry analyses, we estimate dispersal patterns across a spatial scale of approximately 180 km at both propagule (i.e. eggs and larvae) and juvenile (i.e. between settlement and recruitment) stages of a Mediterranean coastal fishery species, the two-banded seabream Diplodus vulgaris. We detected three major natal sources …

EcologyMarine protected areaJuvenileContext (language use)DispersalPropaguleTwo banded seabreamBiologybiology.organism_classificationOtolithDemersal zoneFisheryPropaguleMarine protected areasSpatial ecologyBiological dispersalDiplodus vulgarisJuvenileMarine protected area14. Life underwater[SDE.BE]Environmental Sciences/Biodiversity and EcologyEcology Evolution Behavior and SystematicsNature and Landscape ConservationBiological Conservation
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Study of high spins in $^{173}$Os

1991

High-spin states in 173Os have been studied by γγ-coincidence measurements following the 146Nd(32S, 5n)173Os reaction. Additional information has also been extracted from the reaction 144Sm(32S, 2pn)173Os. Four main sequencies have been identified as the two signature branches of the bands built on the [642]52+ and [523]52− Nilsson states. The band features have been analysed within the framework of the cranked shell model. The positive-parity band provides evidence for a v(i132)2 crossing at low frequency and a π(h112)2 and/or π(h92)2 cross In the negative-parity band the upbend starts at relatively low frequency indicating, presumably, an early v(i132)2 alignment. There is evidence for an…

Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonSpins010308 nuclear & particles physicsSHELL modelLow frequency[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesTwo band0103 physical sciencesAtomic physics010306 general physicsSignature (topology)
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Generation of robust entangled states in a non-hermitian periodically driven two-band Bose-Hubbard system

2016

A many-body Wannier-Stark system coupled to an effective reservoir is studied within a non-Hermitian approach in the presence of a periodic driving. We show how the interplay of dissipation and driving dynamically induces a subspace of states which are very robust against dissipation. We numerically probe the structure of these asymptotic states and their robustness to imperfections in the initial-state preparation and to the size of the system. Moreover, the asymptotic states are found to be strongly entangled making them interesting for further applications.

PhysicsStructure (category theory)FOS: Physical sciences02 engineering and technologyDissipation021001 nanoscience & nanotechnology01 natural sciencesHermitian matrixTwo bandRobustness (computer science)Quantum Gases (cond-mat.quant-gas)0103 physical sciencesStatistical physics010306 general physics0210 nano-technologyCondensed Matter - Quantum GasesSubspace topology
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Phase diagram of dirty two-band superconductors and observability of impurity-induced $s+is$ state

2016

We investigate the phase diagram of dirty two-band superconductors. This paper primarily focuses on the properties and observability of the time-reversal symmetry-breaking $s+is$ superconducting states, which can be generated in two-band superconductors by interband impurity scattering. We show that such states can appear in two distinct ways. First, according to a previously discussed scenario, the $s+is$ state can form as an intermediate phase at the impurity-driven crossover between $s_{\pm}$ and $s_{++}$ states. We show that there is a second scenario where domains of the $s+is$ state exists in the form of an isolated dome inside the $s_{\pm}$ domain, completely detached from the transi…

PhysicsSuperconductivityta114Condensed matter physicsCondensed Matter - SuperconductivityFOS: Physical sciencesState (functional analysis)superconductors01 natural sciences010305 fluids & plasmasSuperconductivity (cond-mat.supr-con)Two bandImpurityCondensed Matter::Superconductivity0103 physical sciencesObservability010306 general physicsphase diagramsPhase diagram
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