342 research outputs found
Using Optical Coherence Tomography to Characterize the Crack Morphology of Ceramic Glaze and Jade
Three billion new trees in the EUβs biodiversity strategy:low ambition, but better environmental outcomes?
The EU Biodiversity strategy aims to plant 3 billion trees by 2030, in order to improve ecosystem restoration and biodiversity. Here, we compute the land area that would be required to support this number of newly planted trees by taking account of different tree species and planting regimes across the EU member states. We find that 3 billion trees would require a total land area of between 0.81 and 1.37 Mha (avg. 1.02 Mha). The historic forest expansion in the EU since 2010 was 2.44 Mha, meaning that despite 3 billion trees sounding like a large number this target is considerably lower than historic afforestation rates within the EU, i.e. only 40% of the past trend. Abandoned agricultural land is often proposed as providing capacity for afforestation. We estimate agricultural abandoned land areas from the HIstoric Land Dynamics Assessment+ database using two time thresholds (abandonment since 2009 or 2014) to identify potential areas for tree planting. The area of agricultural abandoned land was 2.6 Mha (potentially accommodating 7.2 billion trees) since 2009 and 0.2 Mha (potentially accommodating 741 million trees) since 2014. Our study highlights that sufficient space could be available to meet the 3 billion tree planting target from abandoned land. However, large-scale afforestation beyond abandoned land could have displacement effects elsewhere in the world because of the embodied deforestation in the import of agricultural crops and livestock. This would negate the expected benefits of EU afforestation. Hence, the EUβs relatively low ambition on tree planting may actually be better in terms of avoiding such displacement effects. We suggest that tree planting targets should be set at a level that considers physical ecosystem dynamics as well as socio-economic conditions.</p
The XMM-Newton Slew view of IGRJ17361-4441: a transient in the globular cluster NGC 6388
IGRJ17361-4441 is a hard transient recently observed by the INTEGRAL
satellite. The source, close to the center of gravity of the globular cluster
NGC 6388, quickly became the target of follow-up observations conducted by the
Chandra, Swift/XRT and RXTE observatories. Here, we concentrate in particular
on a set of observations conducted by the XMM-Newton satellite during two
slews, in order to get the spectral information of the source and search for
spectral variations. The spectral parameters determined by the recent
XMM-Newton slew observations were compared to the previously known results. The
maximum unabsorbed -ray flux in the 0.5-10 keV band as detected by the
XMM-Newton slew observations is erg cm
s, i.e. consistent with that observed by the Swift/XRT satellite 15 days
earlier. The spectrum seems to be marginally consistent () with that derived from the previous high energy observation.Comment: Accepted for publication on New Astronomy, 2012. A sentence about the
globular cluster 47 Tuc was partially rewritten to avoid confusio
Adsorption-desorption kinetics in nanoscopically confined oligomer films under shear
The method of molecular dynamics computer simulations is employed to study oligomer melts confined in ultra-thin films and subjected to shear. The focus is on the self-diffusion of oligomers near attractive surfaces and on their desorption, together with the effects of increasing energy of adsorption and shear. It is found that the mobility of the oligomers near an attractive surface is strongly decreased. Moreover, although shearing the system forces the chains to stretch parallel to the surfaces and thus increase the energy of adsorption per chain, flow also promotes desorption. The study of chain desorption kinetics reveals the molecular processes responsible for the enhancement of desorption under shear. They involve sequences of conformations starting with a desorbed tail and proceeding in a very fast, correlated, segment-by-segment manner to the desorption of the oligomers from the surfaces.
Spin Transistor and Quantum Spin Hall Effects in CdBxF2-x - p-CdF2 - CdBxF2-x Sandwich Nanostructures
Planar CdBxF2-x - p-CdF2 - CdBxF2-x sandwich nanostructures prepared on the
surface of the n-type CdF2 bulk crystal are studied to register the spin
transistor and quantum spin Hall effects. The current-voltage characteristics
of the ultra-shallow p+-n junctions verify the CdF2 gap, 7.8 eV, and the
quantum subbands of the 2D holes in the p-type CdF2 quantum well confined by
the CdBxF2-x delta-barriers. The temperature and magnetic field dependencies of
the resistance, specific heat and magnetic susceptibility demonstrate the high
temperature superconductor properties for the CdBxF2-x delta-barriers. The
value of the superconductor energy gap, 102.06 meV, determined by the tunneling
spectroscopy method appears to be in a good agreement with the relationship
between the zero-resistance supercurrent in superconductor state and the
conductance in normal state at the energies of the 2D hole subbands. The
results obtained are evidence of the important role of the multiple Andreev
reflections in the creation of the high spin polarization of the 2D holes in
the edged channels of the sandwich device. The high spin hole polarization in
the edged channels is shown to identify the mechanism of the spin transistor
and quantum spin Hall effects induced by varying the top gate voltage, which is
revealed by the first observation of the Hall quantum conductance staircase.Comment: 5 pages, 9 figure
ΠΠΎΠ»ΠΈΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΡΡΡ ΡΠ·ΡΠΊΠΎΠ²ΠΎΠΉ Π΅Π΄ΠΈΠ½ΠΈΡΡ Π² ΡΠΎΡΠΌΠ°ΡΠ΅ Π΄Π²ΡΡΠ·ΡΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΠ½ΡΠ΅ΠΊΡΡΠ°
ΠΡΠ΅Π΄Π»ΠΎΠΆΠ΅Π½Π½ΡΠΉ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π» ΠΏΠΎΠΊΠ°Π·ΡΠ²Π°Π΅Ρ Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·Ρ ΡΡΠ½ΠΊΡΠΈΠΉ ΡΠ·ΡΠΊΠ° Π½Π° ΠΏΡΠΈΠΌΠ΅ΡΠ΅ Π½Π°ΠΈΠΌΠ΅Π½ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΡΠ΅Π΄ΠΏΡΠΈΡΡΠΈΠΉ ΠΊΠΎΠ½ΠΊΡΠ΅ΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠΎΡΠΈΠ»Ρ Π΄Π΅ΡΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ - ΠΊΠ°ΡΠ΅ ΠΈ ΡΠ΅ΡΡΠΎΡΠ°Π½ΠΎΠ² Π’ΠΎΠΌΡΠΊΠ°. ΠΠΎΠΊΠ°Π·Π°Π½Π° ΠΈΡ
Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·Ρ, ΠΊΠ°ΠΊ ΠΎΡΠ½ΠΎΠ²Π° ΠΏΠΎΠ»ΠΈΡΡΠ½ΠΊΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΡΡΠΈ ΡΠ·ΡΠΊΠΎΠ²ΠΎΠΉ Π΅Π΄ΠΈΠ½ΠΈΡΡ. ΠΠ½ΡΠ΅ΡΠΏΡΠ΅ΡΠΈΡΠΎΠ²Π°Π½Π½ΡΠ΅ ΡΠ·ΡΠΊΠΎΠ²ΡΠ΅ ΡΡΠ΅Π΄ΡΡΠ²Π°, ΠΊΠΎΡΠΎΡΡΠ΅ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½Ρ Π² Π½Π°Π·Π²Π°Π½ΠΈΡΡ
Π² ΡΠΎΡΠΌΠ°ΡΠ΅ Π΄Π²ΡΡΠ·ΡΡΠ½ΠΎΠ³ΠΎ ΠΊΠΎΠ½ΡΠ΅ΠΊΡΡΠ°
Processing and mechanical properties of magnesium-lithium composites containing steel fibers
Deformation-processed metal-metal composites (DMMC) of Mg-Li alloys containing steel reinforcing fibers were prepared by infiltrating a preform of steel wool with the molten matrix. The Li content was varied to control the crystal structure of the matrix; Mg-4 wt pct Li is hexagonal close packed (hcp), while Mg-12 wt pct Li is body-centered cubic (bcc). The low carbon steel used as the reinforcing fiber is essentially bcc. The hcp/bcc and bcc/bcc composites were subsequently deformed by rolling and by extrusion/swaging and mechanically tested to relate the tensile strength of the composites to true deformation strain. The hcp/bcc composites had limited formability at temperatures up to 400 Β°C, while the bcc/bcc composites had excellent formability during sheet rolling at room temperature but limited formability during swaging at room temperature. The tensile strengths of the hcp/bcc composite rod and the bcc/bcc composite sheet and rod increased moderately with deformation, though less than predicted from rule-of-mixtures (ROM) calculations. This article presents the experimental data for these DMMC materials and comments on the possible effect of texture development in the matrix and fiber phases on the deformation characteristics of the composite material
United classification of cosmic gamma-ray bursts and their counterparts
United classification of gamma-ray bursts and their counterparts is
established on the basis of measured characteristics: photon energy E and
emission duration T. The founded interrelation between the mentioned
characteristics of events consists in that, as the energy increases, the
duration decreases (and vice versa). The given interrelation reflects the
nature of the phenomenon and forms the E-T diagram, which represents a natural
classification of all observed events in the energy range from 10E9 to 10E-6 eV
and in the corresponding interval of durations from about 10E-2 up to 10E8 s.
The proposed classification results in the consequences, which are principal
for the theory and practical study of the phenomenon.Comment: Keywords Gamma rays: burst
The 3D Structure of N132D in the LMC: A Late-Stage Young Supernova Remnant
We have used the Wide Field Spectrograph (WiFeS) on the 2.3m telescope at
Siding Spring Observatory to map the [O III] 5007{\AA} dynamics of the young
oxygen-rich supernova remnant N132D in the Large Magellanic Cloud. From the
resultant data cube, we have been able to reconstruct the full 3D structure of
the system of [O III] filaments. The majority of the ejecta form a ring of
~12pc in diameter inclined at an angle of 25 degrees to the line of sight. We
conclude that SNR N132D is approaching the end of the reverse shock phase
before entering the fully thermalized Sedov phase of evolution. We speculate
that the ring of oxygen-rich material comes from ejecta in the equatorial plane
of a bipolar explosion, and that the overall shape of the SNR is strongly
influenced by the pre-supernova mass loss from the progenitor star. We find
tantalizing evidence of a polar jet associated with a very fast oxygen-rich
knot, and clear evidence that the central star has interacted with one or more
dense clouds in the surrounding ISM.Comment: Accepted for Publication in Astrophysics & Space Science, 18pp, 8
figure
Magnetic fields in supernova remnants and pulsar-wind nebulae
We review the observations of supernova remnants (SNRs) and pulsar-wind
nebulae (PWNe) that give information on the strength and orientation of
magnetic fields. Radio polarimetry gives the degree of order of magnetic
fields, and the orientation of the ordered component. Many young shell
supernova remnants show evidence for synchrotron X-ray emission. The spatial
analysis of this emission suggests that magnetic fields are amplified by one to
two orders of magnitude in strong shocks. Detection of several remnants in TeV
gamma rays implies a lower limit on the magnetic-field strength (or a
measurement, if the emission process is inverse-Compton upscattering of cosmic
microwave background photons). Upper limits to GeV emission similarly provide
lower limits on magnetic-field strengths. In the historical shell remnants,
lower limits on B range from 25 to 1000 microGauss. Two remnants show
variability of synchrotron X-ray emission with a timescale of years. If this
timescale is the electron-acceleration or radiative loss timescale, magnetic
fields of order 1 mG are also implied. In pulsar-wind nebulae, equipartition
arguments and dynamical modeling can be used to infer magnetic-field strengths
anywhere from about 5 microGauss to 1 mG. Polarized fractions are considerably
higher than in SNRs, ranging to 50 or 60% in some cases; magnetic-field
geometries often suggest a toroidal structure around the pulsar, but this is
not universal. Viewing-angle effects undoubtedly play a role. MHD models of
radio emission in shell SNRs show that different orientations of upstream
magnetic field, and different assumptions about electron acceleration, predict
different radio morphology. In the remnant of SN 1006, such comparisons imply a
magnetic-field orientation connecting the bright limbs, with a non-negligible
gradient of its strength across the remnant.Comment: 20 pages, 24 figures; to be published in SpSciRev. Minor wording
change in Abstrac
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