223 research outputs found

    Calathus: A sample-return mission to Ceres

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    Ceres, as revealed by NASA's Dawn spacecraft, is an ancient, crater-saturated body dominated by low-albedo clays. Yet, localised sites display a bright, carbonate mineralogy that may be as young as 2 Myr. The largest of these bright regions (faculae) are found in the 92 km Occator Crater, and would have formed by the eruption of alkaline brines from a subsurface reservoir of fluids. The internal structure and surface chemistry suggest that Ceres is an extant host for a number of the known prerequisites for terrestrial biota, and as such, represents an accessible insight into a potentially habitable “ocean world”. In this paper, the case and the means for a return mission to Ceres are outlined, presenting the Calathus mission to return to Earth a sample of the Occator Crater faculae for high-precision laboratory analyses. Calathus consists of an orbiter and a lander with an ascent module: the orbiter is equipped with a high-resolution camera, a thermal imager, and a radar; the lander contains a sampling arm, a camera, and an on-board gas chromatograph mass spectrometer; and the ascent module contains vessels for four cerean samples, collectively amounting to a maximum 40 g. Upon return to Earth, the samples would be characterised via high-precision analyses to understand the salt and organic composition of the Occator faculae, and from there to assess both the habitability and the evolution of a relict ocean world from the dawn of the Solar System.The attached document is the authors’ final accepted version of the journal article provided here with a Attribution-NonCommercial-NoDerivatives 4.0 International (CC BY-NC-ND 4.0) Creative Commons Licence. You are advised to consult the publisher’s version if you wish to cite from it.

    Adsorbed Natural Gas Tank feeded with Liquid Natural Gas

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    This paper present the idea of a natural gas reservoir, which uses technology of gas storage by adsorption on activated carbon. Such reservoir can be feeded with Liquid Natural Gas. The framework of article includes theoretical principals of gas-solid physical adsorption, and explains most important concepts associated with it. Moreover, concept of such tank and working regime is presented. Selected subject is very promising in the field of natural gas storage, although this is still a niche issue. Lack of universal models of gases physical adsorption made it very difficult to predict the runs of processes occurring in the proposed reservoir, which is why this project was based on models confirmed during in the earlier studies

    Cryogenic Safety - HSE seminar

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    Cryogenic process pipelines are part of the basic subsystem used in installations for fundamental research in physics, as well as in industrial plants which use LNG or liquid nitrogen. The significant increase in importance of cryogenics entails the need to explore phenomena which have direct impact in the design process of cryogenic systems and their safety systems. These aspects are of high priority due to high investment costs, mainly because of safety issues and reliability. One of the issues which requires thorough investigation is the fracture mechanics of gas pipelines in cryogenic conditions. For this subject, importance is placed not only in when the cracks begin to appear, but also in how they form and how quickly they propagate. Currently, there is a lack of reliable research in the available literature in this area. This is often raised as a significant problem for designers, because knowledge in this topic should be reflected e.g., in the sizing calculations of safety valves for the vacuum systems. This presentation includes a review of the fundamentals of pipe cracking models, the impact of this phenomenon on the safety system design process, the concept of the test stand, and the method in which these studies have been conducted. The results of this research will be able to improve the selection of safety devices in cryogenic systems

    Measurement of the Bc−B_c^- meson production fraction and asymmetry in 7 and 13 TeV pppp collisions

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    International audienceThe production fraction of the Bc- meson with respect to the sum of B- and B¯0 mesons is measured in both 7 and 13 TeV center-of-mass (c.m.) energy pp collisions produced by the Large Hadron Collider (LHC), using the LHCb detector. The rate, approximately 3.7 per mille, does not change with energy, but shows a transverse momentum dependence. The Bc--Bc+ production asymmetry is also measured and is consistent with zero within the determined statistical and systematic uncertainties of a few percent

    Observation of New Ξc0\Xi_c^0 Baryons Decaying to Λc+K−\Lambda_c^+ K^-

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    International audienceThe Λc+K- mass spectrum is studied with a data sample of pp collisions at a center-of-mass energy of 13 TeV corresponding to an integrated luminosity of 5.6  fb-1 collected by the LHCb experiment. Three Ξc0 states are observed with a large significance and their masses and natural widths are measured to be m[Ξc(2923)0]=2923.04±0.25±0.20±0.14  MeV, Γ[Ξc(2923)0]=7.1±0.8±1.8  MeV, m[Ξc(2939)0]=2938.55±0.21±0.17±0.14  MeV, Γ[Ξc(2939)0]=10.2±0.8±1.1  MeV, m[Ξc(2965)0]=2964.88±0.26±0.14±0.14  MeV, Γ[Ξc(2965)0]=14.1±0.9±1.3  MeV, where the uncertainties are statistical, systematic, and due to the limited knowledge of the Λc+ mass. The Ξc(2923)0 and Ξc(2939)0 baryons are new states. The Ξc(2965)0 state is in the vicinity of the known Ξc(2970)0 baryon; however, their masses and natural widths differ significantly

    Determination of quantum numbers for several excited charmed mesons observed in B−→D∗+π−π−B^- \to D^{*+} \pi^- \pi^- decays

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    International audienceA four-body amplitude analysis of the B-→D*+π-π- decay is performed, where fractions and relative phases of the various resonances contributing to the decay are measured. Several quasi-model-independent analyses are performed aimed at searching for the presence of new states and establishing the quantum numbers of previously observed charmed meson resonances. In particular the resonance parameters and quantum numbers are determined for the D1(2420), D1(2430), D0(2550), D1*(2600), D2(2740) and D3*(2750) states. The mixing between the D1(2420) and D1(2430) resonances is studied and the mixing parameters are measured. The dataset corresponds to an integrated luminosity of 4.7  fb-1, collected in proton-proton collisions at center-of-mass energies of 7, 8 and 13 TeV with the LHCb detector

    Constraints on the KS0→Ό+Ό−K^0_S \rightarrow \mu^+ \mu^- Branching Fraction

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    International audienceA search for the decay KS0→Ό+ÎŒ- is performed using proton-proton collision data, corresponding to an integrated luminosity of 5.6  fb-1 and collected with the LHCb experiment during 2016, 2017, and 2018 at a center-of-mass energy of 13 TeV. The observed signal yield is consistent with zero, yielding an upper limit of B(KS0→Ό+ÎŒ-)<2.2×10-10 at 90% C.L.. The limit reduces to B(KS0→Ό+ÎŒ-)<2.1×10-10 at 90% C.L. once combined with the result from data taken in 2011 and 2012

    Measurement of the Λb0→J/ψΛ\Lambda^0_b\rightarrow J/\psi\Lambda angular distribution and the Λb0\Lambda^0_b polarisation in pppp collisions

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    International audienceThis paper presents an analysis of the Λb0 {\Lambda}_b^0 → J/ψΛ angular distribution and the transverse production polarisation of Λb0 {\Lambda}_b^0 baryons in proton-proton collisions at centre-of-mass energies of 7, 8 and 13 TeV. The measurements are performed using data corresponding to an integrated luminosity of 4.9 fb−1^{−1}, collected with the LHCb experiment. The polarisation is determined in a fiducial region of Λb0 {\Lambda}_b^0 transverse momentum and pseudorapidity of 1 < pT_{T}< 20 GeV/c and 2 < η < 5, respectively. The data are consistent with Λb0 {\Lambda}_b^0 baryons being produced unpolarised in this region. The parity-violating asymmetry parameter of the Λ → pπ−^{−} decay is also determined from the data and its value is found to be consistent with a recent measurement by the BES III collaboration.[graphic not available: see fulltext

    Measurement of the electron reconstruction efficiency at LHCb

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    International audienceThe single electron track-reconstruction efficiency is determined using a sample corresponding to 1.3 fb−11.3~\mathrm{fb}^{-1}of pppp collision data recorded with the LHCb detector in 2017. This measurement exploits B+→J/ψ(e+e−)K+B^+\to J/\psi (e^+e^-)K^+ decays, where one of the electrons is fully reconstructed and paired with the kaon, while the other electron is reconstructed using only the information of the vertex detector. Despite this partial reconstruction, kinematic and geometric constraints allow the B+B^+-meson mass to be reconstructed and the signal to be well separated from backgrounds. This in turn allows the electron reconstruction efficiency to be measured by matching the partial track segment found in the vertex detector to tracks found by LHCb's regular reconstruction algorithms. The agreement between data and simulation is evaluated, and corrections are derived for simulated electrons in bins of kinematics. The presented method allows LHCb to measure branching fractions involving single electrons with a an electron reconstruction systematic uncertainty below 1%1\%

    Search for the lepton flavour violating decay B+→K+Ό−τ+B^+ \rightarrow K^+ \mu^- \tau^+ using Bs2∗0B_{s2}^{*0} decays

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    International audienceA search is presented for the lepton flavour violating decay B+^{+} → K+^{+}Ό−^{−}τ+^{+} using a sample of proton-proton collisions at centre-of-mass energies of 7, 8, and 13 TeV, collected with the LHCb detector and corresponding to a total integrated luminosity of 9 fb−1^{−1}. The τ leptons are selected inclusively, primarily via decays with a single charged particle. The four-momentum of the τ lepton is determined by using B+^{+} mesons from Bs2∗0→B+K− {B}_{s2}^{\ast 0}\to {B}^{+}{K}^{-} decays. No significant excess is observed, and an upper limit is set on the branching fractionℬ(B+^{+} → K+^{+}Ό−^{−}τ+^{+}) < 3.9 × 10−5^{−5} at 90 %  confidence level.The obtained limit is comparable to the world-best limit.[graphic not available: see fulltext
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