6,479 research outputs found
Improving accuracy and precision of ice core ÎŽD(CH<sub>4</sub>) analyses using methane pre-pyrolysis and hydrogen post-pyrolysis trapping and subsequent chromatographic separation
Firn and polar ice cores offer the only direct palaeoatmospheric
archive. Analyses of past greenhouse gas concentrations and their
isotopic compositions in air bubbles in the ice can help to
constrain changes in global biogeochemical cycles in the past. For
the analysis of the hydrogen isotopic composition of methane
(ÎŽD(CH<sub>4</sub>) or δ<sup>2</sup>H(CH<sub>4</sub>)) 0.5 to 1.5 kg
of ice was hitherto used. Here we present
a method to improve precision and reduce the sample amount for
ÎŽD(CH<sub>4</sub>) measurements in (ice core)
air. Pre-concentrated methane is focused in front of a high temperature
oven (pre-pyrolysis trapping), and molecular hydrogen formed by
pyrolysis is trapped afterwards (post-pyrolysis trapping), both on
a carbon-PLOT capillary at â196 °C.
Argon, oxygen, nitrogen, carbon monoxide, unpyrolysed methane and
krypton are trapped together with H<sub>2</sub> and must
be separated using a second short, cooled chromatographic column to ensure
accurate results. Pre- and post-pyrolysis trapping largely removes
the isotopic fractionation induced during chromatographic separation
and results in a narrow peak in the mass spectrometer. Air
standards can be measured with a precision better than
1‰. For polar ice samples from glacial periods, we estimate
a precision of 2.3‰ for 350 g of ice (or roughly
30 mL â at standard temperature and pressure (STP) â of air)
with 350 ppb of methane. This corresponds to recent
tropospheric air samples (about 1900 ppb CH<sub>4</sub>) of
about 6 mL (STP) or about 500 pmol of pure
CH<sub>4</sub>
The effect of activity-related meridional flow modulation on the strength of the solar polar magnetic field
We studied the effect of the perturbation of the meridional flow in the
activity belts detected by local helioseismology on the development and
strength of the surface magnetic field at the polar caps. We carried out
simulations of synthetic solar cycles with a flux transport model, which
follows the cyclic evolution of the surface field determined by flux emergence
and advective transport by near-surface flows. In each hemisphere, an
axisymmetric band of latitudinal flows converging towards the central latitude
of the activity belt was superposed onto the background poleward meridional
flow. The overall effect of the flow perturbation is to reduce the latitude
separation of the magnetic polarities of a bipolar magnetic region and thus
diminish its contribution to the polar field. As a result, the polar field
maximum reached around cycle activity minimum is weakened by the presence of
the meridional flow perturbation. For a flow perturbation consistent with
helioseismic observations, the polar field is reduced by about 18% compared to
the case without inflows. If the amplitude of the flow perturbation depends on
the cycle strength, its effect on the polar field provides a nonlinearity that
could contribute to limiting the amplitude of a Babcock-Leighton type dynamo.Comment: 16 pages, 5 figures, accepted by Ap
How to quantify deterministic and random influences on the statistics of the foreign exchange market
It is shown that prize changes of the US dollar - German Mark exchange rates
upon different delay times can be regarded as a stochastic Marcovian process.
Furthermore we show that from the empirical data the Kramers-Moyal coefficients
can be estimated.
Finally, we present an explicite Fokker-Planck equation which models very
precisely the empirical probabilitiy distributions.Comment: 3 figure
Nonconcave entropies in multifractals and the thermodynamic formalism
We discuss a subtlety involved in the calculation of multifractal spectra
when these are expressed as Legendre-Fenchel transforms of functions analogous
to free energy functions. We show that the Legendre-Fenchel transform of a free
energy function yields the correct multifractal spectrum only when the latter
is wholly concave. If the spectrum has no definite concavity, then the
transform yields the concave envelope of the spectrum rather than the spectrum
itself. Some mathematical and physical examples are given to illustrate this
result, which lies at the root of the nonequivalence of the microcanonical and
canonical ensembles. On a more positive note, we also show that the
impossibility of expressing nonconcave multifractal spectra through
Legendre-Fenchel transforms of free energies can be circumvented with the help
of a generalized free energy function, which relates to a recently introduced
generalized canonical ensemble. Analogies with the calculation of rate
functions in large deviation theory are finally discussed.Comment: 9 pages, revtex4, 3 figures. Changes in v2: sections added on
applications plus many new references; contains an addendum not contained in
published versio
Deconstructing HD 28867
The 3" pair of B9 stars, HD 28867, is one of the brightest X-ray sources in
the Taurus-Auriga star forming region. In this multi-wavelength study, we
attempt to deduce the source of the X-ray emission. We show that the East
component is the X-ray source. The East component has a near-IR excess and
displays narrow absorption lines in the optical, both of which are consistent
with a cool stellar companion. This companion is one of the brightest low mass
pre-main sequence stars in Tau-Aur; at 2 microns it and the B9 star are equally
bright. We see evidence for radial velocity variability in the cool component
of >34 km/s. It is not visible in K band speckle imaging, which constrains the
companion to lie within 14 AU of the B star.
We also report on a possible fourth member of the group, an M1 star 18" south
of HD 28867.Comment: accepted by the Astronomical Journa
Testing models for molecular gas formation in galaxies: hydrostatic pressure or gas and dust shielding?
Stars in galaxies form in giant molecular clouds that coalesce when the
atomic hydrogen is converted into molecules. There are currently two dominant
models for what property of the galactic disk determines its molecular
fraction: either hydrostatic pressure driven by the gravity of gas and stars,
or a combination of gas column density and metallicity. To assess the validity
of these models, we compare theoretical predictions to the observed atomic gas
content of low-metallicity dwarf galaxies with high stellar densities. The
extreme conditions found in these systems are optimal to distinguish the two
models, otherwise degenerate in nearby spirals. Locally, on scales <100 pc, we
find that the state of the interstellar medium is mostly sensitive to the gas
column density and metallicity rather than hydrostatic pressure. On larger
scales where the average stellar density is considerably lower, both pressure
and shielding models reproduce the observations, even at low metallicity. We
conclude that models based on gas and dust shielding more closely describe the
process of molecular formation, especially at the high resolution that can be
achieved in modern galaxy simulations or with future radio/millimeter arrays.Comment: 20 pages, 12 figures. Accepted for publication in Ap
Measurement of the Omega_c Lifetime
We present the measurement of the lifetime of the Omega_c we have performed
using three independent data samples from two different decay modes. Using a
Sigma- beam of 340 GeV/c we have obtained clean signals for the Omega_c
decaying into Xi- K- pi+ pi+ and Omega- pi+ pi- pi+, avoiding topological cuts
normally used in charm analysis. The short but measurable lifetime of the
Omega_c is demonstrated by a clear enhancement of the signals at short but
finite decay lengths. Using a continuous maximum likelihood method we
determined the lifetime to be tau(Omega_c) = 55 +13-11(stat) +18-23(syst) fs.
This makes the Omega_c the shortest living weakly decaying particle observed so
far. The short value of the lifetime confirms the predicted pattern of the
charmed baryon lifetimes and demonstrates that the strong interaction plays a
vital role in the lifetimes of charmed hadrons.Comment: 15 pages, including 7 figures; gzipped, uuencoded postscrip
Follow the foreign leader? Why following foreign incumbents is an effective electoral strategy
Previous research suggests that political parties respond to leftâright policy positions of successful foreign political parties (âforeign leadersâ). We evaluate whether this is an effective electoral strategy: specifically, do political parties gain votes in elections when they respond to successful foreign parties? We argue that parties that follow foreign leaders will arrive at policy positions closer to their own (domestic) median voter, which increases their electoral support. The analysis is based on a two-stage model specification of partiesâ vote shares and suggests that following foreign leaders is a beneficial election strategy in national election because it allows them to better identify the position of their own median voter. These findings have important implications for our understanding of political representation, partiesâ election strategies, and for policy diffusion
Military objectives in cyber warfare
This Chapter discusses the possible problems arising from the application of the principle of distinction under the law of armed conflict to cyber attacks. It first identifies when cyber attacks qualify as âattacksâ under the law of armed conflict and then examines the two elements of the definition of âmilitary objectiveâ contained in Article 52(2) of the 1977 Protocol I additional to the 1949 Geneva Conventions on the Protection of Victims of War. The Chapter concludes that this definition is flexible enough to apply in the cyber context without significant problems and that none of the challenges that characterize cyber attacks hinders the application of the principle of distinction
Search for the exotic Resonance in 340GeV/c -Nucleus Interactions
We report on a high statistics search for the resonance in
-nucleus collisions at 340GeV/c. No evidence for this resonance is
found in our data sample which contains 676000 candidates above
background. For the decay channel and the
kinematic range 0.150.9 we find a 3 upper limit for the
production cross section of 3.1 and 3.5 b per nucleon for reactions with
carbon and copper, respectively.Comment: 5 pages, 4 figures, modification of ref. 43 and 4
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