761 research outputs found
Armenian Speech Reports: Blurring the Quotative Line
Modern Eastern Armenian has two complementizers, vor and te. When used to introduce speech reports, those complementizers differ as to the discourse status of the speech event they introduce; most notably, te possesses an evidential meaning that vor lacks. Using the model of discourse update suggested in Portner (2006), I provide an analysis of te that explains its evidential properties. I also provide evidence that MEA thwarts the traditional dichotomy assumed in the literature between direct and indirect speech by allowing a form of loose quotation
A new set-up for simultaneous high-precision measurements of CO<sub>2</sub>,δ<sup>13 </sup>C-CO<sub>2</sub> and δ<sup>18</sup>O-CO2 on small ice core samples
Palaeoatmospheric records of carbon dioxide and its stable carbon isotope
composition (<i>δ</i><sup>13</sup>C) obtained from polar ice cores provide important
constraints on the natural variability of the carbon cycle. However, the
measurements are both analytically challenging and time-consuming; thus only data
exist from a limited number of sampling sites and time periods.
Additional analytical resources with high analytical precision and throughput
are thus desirable to extend the existing datasets. Moreover, consistent
measurements derived by independent laboratories and a variety of analytical
systems help to further increase confidence in the global CO<sub>2</sub> palaeo-reconstructions. Here, we describe our new set-up for simultaneous
measurements of atmospheric CO<sub>2</sub> mixing ratios and atmospheric
<i>δ</i><sup>13</sup>C and <i>δ</i><sup>18</sup>O-CO<sub>2</sub> in air extracted from ice core
samples. The centrepiece of the system is a newly designed needle cracker for
the mechanical release of air entrapped in ice core samples of 8–13 g
operated at −45 °C. The small sample size allows for high
resolution and replicate sampling schemes. In our method, CO<sub>2</sub> is
cryogenically and chromatographically separated from the bulk air and its
isotopic composition subsequently determined by continuous flow isotope ratio
mass spectrometry (IRMS). In combination with thermal conductivity
measurement of the bulk air, the CO<sub>2</sub> mixing ratio is calculated. The
analytical precision determined from standard air sample measurements over
ice is ±1.9 ppm for CO<sub>2</sub> and ±0.09 ‰
for <i>δ</i><sup>13</sup>C. In a laboratory intercomparison study with CSIRO
(Aspendale, Australia), good agreement between CO<sub>2</sub> and <i>δ</i><sup>13</sup>C
results is found for Law Dome ice core samples. Replicate analysis of these
samples resulted in a pooled standard deviation of 2.0 ppm for CO<sub>2</sub> and
0.11 ‰ for <i>δ</i><sup>13</sup>C. These numbers are good, though they are
rather conservative estimates of the overall analytical precision achieved
for single ice sample measurements. Facilitated by the small sample
requirement, replicate measurements are feasible, allowing the method
precision to be improved potentially. Further, new analytical approaches are
introduced for the accurate correction of the procedural blank and for a
consistent detection of measurement outliers, which is based on <i>δ</i><sup>18</sup>O-CO<sub>2</sub> and the exchange of oxygen between CO<sub>2</sub> and
the surrounding ice (H<sub>2</sub>O)
Rapid growth of HFC-227ea (1,1,1,2,3,3,3-Heptafluoropropane) in the atmosphere
We report the first measurements of 1,1,1,2,3,3,3-heptafluoropropane (HFC-227ea), a substitute for ozone depleting compounds, in remote regions of the atmosphere and present evidence for its rapid growth. Observed mixing ratios ranged from below 0.01 ppt in deep firn air to 0.59 ppt in the northern mid-latitudinal upper troposphere. Firn air samples collected in Greenland were used to reconstruct a history of atmospheric abundance. Year-on-year increases were deduced, with acceleration in the growth rate from 0.026 ppt per year in 2000 to 0.057 ppt per year in 2007. Upper tropospheric air samples provide evidence for a continuing growth until late 2009. Fur- thermore we calculated a stratospheric lifetime of 370 years from measurements of air samples collected on board high altitude aircraft and balloons. Emission estimates were determined from the reconstructed atmospheric trend and suggest that current "bottom-up" estimates of global emissions for 2005 are too high by more than a factor of three
Atmospheric abundance and global emissions of perfluorocarbons CF4, C2F6 and C3F8 since 1800 inferred from ice core, firn, air archive and in situ measurements
Perfluorocarbons (PFCs) are very potent and long-lived greenhouse gases in the atmosphere, released predominantly during aluminium production and semiconductor manufacture. They have been targeted for emission controls under the United Nations Framework Convention on Climate Change. Here we present the first continuous records of the atmospheric abundance of CF4 (PFC-14), C2F6 (PFC-116) and C3F8 (PFC-218) from 1800 to 2014. The records are derived from high-precision measurements of PFCs in air extracted from polar firn or ice at six sites (DE08, DE08-2, DSSW20K, EDML, NEEM and South Pole) and air archive tanks and atmospheric air sampled from both hemispheres. We take account of the age characteristics of the firn and ice core air samples and demonstrate excellent consistency between the ice core, firn and atmospheric measurements. We present an inversion for global emissions from 1900 to 2014. We also formulate the inversion to directly infer emission factors for PFC emissions due to aluminium production prior to the 1980s. We show that 19th century atmospheric levels, before significant anthropogenic influence, were stable at 34.1 ± 0.3 ppt for CF4 and below detection limits of 0.002 and 0.01 ppt for C2F6 and C3F8, respectively. We find a significant peak in CF4 and C2F6 emissions around 1940, most likely due to the high demand for aluminium during World War II, for example for construction of aircraft, but these emissions were nevertheless much lower than in recent years. The PFC emission factors for aluminium production in the early 20th century were significantly higher than today but have decreased since then due to improvements and better control of the smelting process. Mitigation efforts have led to decreases in emissions from peaks in 1980 (CF4) or early-to-mid-2000s (C2F6 and C3F8) despite the continued increase in global aluminium production; however, these decreases in emissions appear to have recently halted. We see a temporary reduction of around 15 % in CF4 emissions in 2009, presumably associated with the impact of the global financial crisis on aluminium and semiconductor production
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An interlaboratory comparison of techniques for extracting and analyzing trapped gases in ice cores
We undertook an interlaboratory comparison of techniques used to extract and analyze trapped gases in ice cores. The intercomparison included analyses of standard reference gases and samples of ice from the Greenland Ice Sheet Project 2 (GISP2) site. Concentrations of CO₂, CH₄, the δ¹⁸O of O₂, the δ¹⁵N of N₂, and the O₂/N₂, and Ar/N₂ ratios were measured in air standards and ice core sampries. The standard reference scales for CO₂ and CH₄ were consistent at the ±2% level. The δᴼ²/N₂ and δ¹⁸O of O₂ measurements showed substantial deviations between the two laboratories able to measure these ratios. The deviations are probably related to errors associated with calibration of the working standards. The δᴬʳ/N₂ and δ¹⁵N of N₂ measurements were consistent. Five laboratories analyzed the
CH₄ concentration in a 4.2-m section of the GISP2 ice core. The average of 20 discrete CH₄
measurements was 748±10 parts per billion by volume (ppbv). The standard deviation of these measurements was close to the total analytical uncertainty associated with the measurements. In all cases, those laboratories employing a dry extraction technique determined higher CH₄ values than laboratories using a wet extraction technique. The origin of this difference is unclear but may involve uncertainties associated with blank corrections. Analyses of the CO₂ concentration of trapped gases showed extreme variations which cannot be explained by analytical uncertainties alone. Three laboratories measured the [CO₂] on 21 discrete depths yielding an average value of 283±13 parts per million by volume (ppmv). In this case, the standard deviation was roughly a factor of 2 greater than the analytical uncertainties. We believe the variability in the measured [CO₂] results from impurities in the ice which may have compromised the [CO₂] of trapped gases in Greenland ice
South Atlantic intermediate water advances into the North-east Atlantic with reduced Atlantic meridional overturning circulation during the last glacial period
The Nd isotopic composition (epsilon Nd) of seawater and cold-water coral (CWC) samples from the Gulf of Cadiz and the Alboran Sea, at a depth of 280-827 m were investigated in order to constrain middepth water mass dynamics within the Gulf of Cadiz over the past 40 ka. epsilon Nd of glacial and Holocene CWC from the Alboran Sea and the northern Gulf of Cadiz reveals relatively constant values (-8.6 to -9.0 and -9.5 to -10.4, respectively). Such values are similar to those of the surrounding present-day middepth waters from the Mediterranean Outflow Water (MOW; epsilon Nd approximate to -9.4) and Mediterranean Sea Water (MSW; epsilon Nd approximate to -9.9). In contrast, glacial epsilon Nd values for CWC collected at thermocline depth (550-827 m) in the southern Gulf of Cadiz display a higher average value (-8.90.4) compared to the present-day value (-11.70.3). This implies a higher relative contribution of water masses of Mediterranean (MSW) or South Atlantic origin (East Antarctic Intermediate Water, EAAIW). Our study has produced the first evidence of significant radiogenic epsilon Nd values (approximate to -8) at 19, 23-24, and 27 ka, which are coeval with increasing iceberg discharges and a weakening of Atlantic Meridional Overturning Circulation (AMOC). Since MOW epsilon Nd values remained stable during the last glacial period, it is suggested that these radiogenic epsilon Nd values most likely reflect an enhanced northward propagation of glacial EAAIW into the eastern Atlantic Basin
Search for dark matter produced in association with bottom or top quarks in √s = 13 TeV pp collisions with the ATLAS detector
A search for weakly interacting massive particle dark matter produced in association with bottom or top quarks is presented. Final states containing third-generation quarks and miss- ing transverse momentum are considered. The analysis uses 36.1 fb−1 of proton–proton collision data recorded by the ATLAS experiment at √s = 13 TeV in 2015 and 2016. No significant excess of events above the estimated backgrounds is observed. The results are in- terpreted in the framework of simplified models of spin-0 dark-matter mediators. For colour- neutral spin-0 mediators produced in association with top quarks and decaying into a pair of dark-matter particles, mediator masses below 50 GeV are excluded assuming a dark-matter candidate mass of 1 GeV and unitary couplings. For scalar and pseudoscalar mediators produced in association with bottom quarks, the search sets limits on the production cross- section of 300 times the predicted rate for mediators with masses between 10 and 50 GeV and assuming a dark-matter mass of 1 GeV and unitary coupling. Constraints on colour- charged scalar simplified models are also presented. Assuming a dark-matter particle mass of 35 GeV, mediator particles with mass below 1.1 TeV are excluded for couplings yielding a dark-matter relic density consistent with measurements
Measurement of the W±Z boson pair-production cross section in pp collisions at √s=13TeV with the ATLAS detector
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