177 research outputs found

    Reactive Desorption of CO Hydrogenation Products under Cold Pre-stellar Core Conditions

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    The astronomical gas-phase detection of simple species and small organic molecules in cold pre-stellar cores, with abundances as high as ∌\sim10−8−10−910^{-8}-10^{-9} nH_\text{H}, contradicts the generally accepted idea that at 1010 K, such species should be fully frozen out on grain surfaces. A physical or chemical mechanism that results in a net transfer from solid-state species into the gas phase offers a possible explanation. Reactive desorption, i.e., desorption following the exothermic formation of a species, is one of the options that has been proposed. In astronomical models, the fraction of molecules desorbed through this process is handled as a free parameter, as experimental studies quantifying the impact of exothermicity on desorption efficiencies are largely lacking. In this work, we present a detailed laboratory study with the goal of deriving an upper limit for the reactive desorption efficiency of species involved in the CO-H2_2CO-CH3_3OH solid-state hydrogenation reaction chain. The limit for the overall reactive desorption fraction is derived by precisely investigating the solid-state elemental carbon budget, using reflection absorption infrared spectroscopy and the calibrated solid-state band-strength values for CO, H2_2CO and CH3_3OH. We find that for temperatures in the range of 1010 to 1414 K, an upper limit of 0.24±0.020.24\pm 0.02 for the overall elemental carbon loss upon CO conversion into CH3_3OH. This corresponds with an effective reaction desorption fraction of ≀\leq0.070.07 per hydrogenation step, or ≀\leq0.020.02 per H-atom induced reaction, assuming that H-atom addition and abstraction reactions equally contribute to the overall reactive desorption fraction along the hydrogenation sequence. The astronomical relevance of this finding is discussed.Comment: 9 pages, 7 figure

    On the existence of the second Dirac operator in Riemannian space

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    We describe a Riemannian space class where the second Dirac operator arises and prove that the operator is always equivalent to a standard Dirac one. The particle state in this gravitational field is degenerate to some extent and we introduce an additional value in order to describe a particle state completely. Some supersymmetry constructions are also discussed. As an example we study all Riemannian spaces with a five-dimentional motion group and find all metrics for which the second Dirac operator exists. On the basis of our discussed examples we hypothesize about the number of second Dirac operators in Riemannian space.Comment: LaTex, 10 pages, no figure

    JUNO Conceptual Design Report

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    The Jiangmen Underground Neutrino Observatory (JUNO) is proposed to determine the neutrino mass hierarchy using an underground liquid scintillator detector. It is located 53 km away from both Yangjiang and Taishan Nuclear Power Plants in Guangdong, China. The experimental hall, spanning more than 50 meters, is under a granite mountain of over 700 m overburden. Within six years of running, the detection of reactor antineutrinos can resolve the neutrino mass hierarchy at a confidence level of 3-4σ\sigma, and determine neutrino oscillation parameters sin⁥2Ξ12\sin^2\theta_{12}, Δm212\Delta m^2_{21}, and ∣Δmee2∣|\Delta m^2_{ee}| to an accuracy of better than 1%. The JUNO detector can be also used to study terrestrial and extra-terrestrial neutrinos and new physics beyond the Standard Model. The central detector contains 20,000 tons liquid scintillator with an acrylic sphere of 35 m in diameter. ∌\sim17,000 508-mm diameter PMTs with high quantum efficiency provide ∌\sim75% optical coverage. The current choice of the liquid scintillator is: linear alkyl benzene (LAB) as the solvent, plus PPO as the scintillation fluor and a wavelength-shifter (Bis-MSB). The number of detected photoelectrons per MeV is larger than 1,100 and the energy resolution is expected to be 3% at 1 MeV. The calibration system is designed to deploy multiple sources to cover the entire energy range of reactor antineutrinos, and to achieve a full-volume position coverage inside the detector. The veto system is used for muon detection, muon induced background study and reduction. It consists of a Water Cherenkov detector and a Top Tracker system. The readout system, the detector control system and the offline system insure efficient and stable data acquisition and processing.Comment: 328 pages, 211 figure

    Grain Surface Models and Data for Astrochemistry

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    AbstractThe cross-disciplinary field of astrochemistry exists to understand the formation, destruction, and survival of molecules in astrophysical environments. Molecules in space are synthesized via a large variety of gas-phase reactions, and reactions on dust-grain surfaces, where the surface acts as a catalyst. A broad consensus has been reached in the astrochemistry community on how to suitably treat gas-phase processes in models, and also on how to present the necessary reaction data in databases; however, no such consensus has yet been reached for grain-surface processes. A team of ∌25 experts covering observational, laboratory and theoretical (astro)chemistry met in summer of 2014 at the Lorentz Center in Leiden with the aim to provide solutions for this problem and to review the current state-of-the-art of grain surface models, both in terms of technical implementation into models as well as the most up-to-date information available from experiments and chemical computations. This review builds on the results of this workshop and gives an outlook for future directions

    К ĐČĐŸĐżŃ€ĐŸŃŃƒ ĐŸ ĐČĐŸĐ·ĐŒĐŸĐ¶ĐœŃ‹Ń… ĐŒĐ”Ń…Đ°ĐœĐžĐ·ĐŒĐ°Ń… ĐŽĐ”ĐčстĐČоя Đ°ĐșŃƒĐżŃƒĐœĐșтуры про Đ»Đ”Ń‡Đ”ĐœĐžĐž Đ±ĐŸĐ»ŃŒĐœŃ‹Ń… Đ±Ń€ĐŸĐœŃ…ĐžĐ°Đ»ŃŒĐœĐŸĐč Đ°ŃŃ‚ĐŒĐŸĐč

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    The acupuncture effect mechanisms (efficacy of a single procedure and a treatment course) have been thoroughly studied with due account of neirophysical, biochemical and energetic aspects. The study was based on an integral estimation assessment of patients’ conditions (contemporary European and classic Chinese estimates) for 60 patients with a mild course of bronchial asthma and 30 patients with the pre-asthma state treated with acupuncture monotherapy.Specific aspects of the homeostasis adaptive correction have been defined. This makes it possible to recommend the acupuncture not only for treatment but for the bronchial asthma prophylaxis.ĐœĐ”Ń…Đ°ĐœĐžĐ·ĐŒŃ‹ ĐŽĐ”ĐčстĐČоя Đ°ĐșŃƒĐżŃƒĐœĐșтуры (ŃŃ„Ń„Đ”Đșты ĐŸĐŽĐœĐŸĐč ĐżŃ€ĐŸŃ†Đ”ĐŽŃƒŃ€Ń‹ Đž ĐșŃƒŃ€ŃĐŸĐČĐŸĐłĐŸ Đ»Đ”Ń‡Đ”ĐœĐžŃ) ĐžĐ·ŃƒŃ‡Đ°Đ»ĐžŃŃŒ ĐșĐŸĐŒĐżĐ»Đ”ĐșŃĐœĐŸ (ĐœĐ”ĐčŃ€ĐŸŃ„ĐžĐ·ĐžĐŸĐ»ĐŸĐłĐžŃ‡Đ”ŃĐșОД, Đ±ĐžĐŸŃ…ĐžĐŒĐžŃ‡Đ”ŃĐșОД, ŃĐœĐ”Ń€ĐłĐ”Ń‚ĐžŃ‡Đ”ŃĐșОД аспДĐșты) ĐœĐ° ĐŸŃĐœĐŸĐČĐ” ĐžĐœŃ‚Đ”ĐłŃ€Đ°Đ»ŃŒĐœĐŸĐč ĐŸŃ†Đ”ĐœĐșĐž ŃĐŸŃŃ‚ĐŸŃĐœĐžŃ (ŃĐŸĐČŃ€Đ”ĐŒĐ”ĐœĐœĐŸĐč Đ”ĐČŃ€ĐŸĐżĐ”ĐčсĐșĐŸĐč Đž ĐșлассОчДсĐșĐŸĐč ĐșотаĐčсĐșĐŸĐč) у 60 Đ±ĐŸĐ»ŃŒĐœŃ‹Ń… с лДгĐșĐžĐŒ Ń‚Đ”Ń‡Đ”ĐœĐžĐ”ĐŒ Đ±Ń€ĐŸĐœŃ…ĐžĐ°Đ»ŃŒĐœĐŸĐč Đ°ŃŃ‚ĐŒŃ‹ Đž 30 Đ±ĐŸĐ»ŃŒĐœŃ‹Ń… с ŃĐŸŃŃ‚ĐŸŃĐœĐžĐ”ĐŒ ĐżŃ€Đ”ĐŽĐ°ŃŃ‚ĐŒŃ‹ ĐČ ĐżŃ€ĐŸŃ†Đ”ŃŃĐ” ĐŒĐŸĐœĐŸŃ‚Đ”Ń€Đ°ĐżĐžĐž Đ°ĐșŃƒĐżŃƒĐœĐșŃ‚ŃƒŃ€ĐŸĐč. ĐŁŃ‚ĐŸŃ‡ĐœĐ”ĐœŃ‹ ĐŸŃĐŸĐ±Đ”ĐœĐœĐŸŃŃ‚Đž аЮаптоĐČĐœĐŸĐč ĐșĐŸŃ€Ń€Đ”Đșцоо ĐłĐŸĐŒĐ”ĐŸŃŃ‚Đ°Đ·Đ°, ĐżĐŸĐ·ĐČĐŸĐ»ŃŃŽŃ‰ĐžĐ” рДĐșĐŸĐŒĐ”ĐœĐŽĐŸĐČать Đ°ĐșŃƒĐżŃƒĐœĐșтуру ĐœĐ” Ń‚ĐŸĐ»ŃŒĐșĐŸ ĐŽĐ»Ń Đ»Đ”Ń‡Đ”ĐœĐžŃ, ĐœĐŸ Đž ĐŽĐ»Ń ĐżŃ€ĐŸŃ„ĐžĐ»Đ°ĐșтоĐșĐž Đ±Ń€ĐŸĐœŃ…ĐžĐ°Đ»ŃŒĐœĐŸĐč Đ°ŃŃ‚ĐŒŃ‹

    Identification and reconstruction of low-energy electrons in the ProtoDUNE-SP detector

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    Measurements of electrons from Îœe\nu_e interactions are crucial for the Deep Underground Neutrino Experiment (DUNE) neutrino oscillation program, as well as searches for physics beyond the standard model, supernova neutrino detection, and solar neutrino measurements. This article describes the selection and reconstruction of low-energy (Michel) electrons in the ProtoDUNE-SP detector. ProtoDUNE-SP is one of the prototypes for the DUNE far detector, built and operated at CERN as a charged particle test beam experiment. A sample of low-energy electrons produced by the decay of cosmic muons is selected with a purity of 95%. This sample is used to calibrate the low-energy electron energy scale with two techniques. An electron energy calibration based on a cosmic ray muon sample uses calibration constants derived from measured and simulated cosmic ray muon events. Another calibration technique makes use of the theoretically well-understood Michel electron energy spectrum to convert reconstructed charge to electron energy. In addition, the effects of detector response to low-energy electron energy scale and its resolution including readout electronics threshold effects are quantified. Finally, the relation between the theoretical and reconstructed low-energy electron energy spectrum is derived and the energy resolution is characterized. The low-energy electron selection presented here accounts for about 75% of the total electron deposited energy. After the addition of lost energy using a Monte Carlo simulation, the energy resolution improves from about 40% to 25% at 50~MeV. These results are used to validate the expected capabilities of the DUNE far detector to reconstruct low-energy electrons.Comment: 19 pages, 10 figure

    Low exposure long-baseline neutrino oscillation sensitivity of the DUNE experiment

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    The Deep Underground Neutrino Experiment (DUNE) will produce world-leading neutrino oscillation measurements over the lifetime of the experiment. In this work, we explore DUNE's sensitivity to observe charge-parity violation (CPV) in the neutrino sector, and to resolve the mass ordering, for exposures of up to 100 kiloton-megawatt-years (kt-MW-yr). The analysis includes detailed uncertainties on the flux prediction, the neutrino interaction model, and detector effects. We demonstrate that DUNE will be able to unambiguously resolve the neutrino mass ordering at a 3σ\sigma (5σ\sigma) level, with a 66 (100) kt-MW-yr far detector exposure, and has the ability to make strong statements at significantly shorter exposures depending on the true value of other oscillation parameters. We also show that DUNE has the potential to make a robust measurement of CPV at a 3σ\sigma level with a 100 kt-MW-yr exposure for the maximally CP-violating values \delta_{\rm CP}} = \pm\pi/2. Additionally, the dependence of DUNE's sensitivity on the exposure taken in neutrino-enhanced and antineutrino-enhanced running is discussed. An equal fraction of exposure taken in each beam mode is found to be close to optimal when considered over the entire space of interest

    Impact of cross-section uncertainties on supernova neutrino spectral parameter fitting in the Deep Underground Neutrino Experiment

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    A primary goal of the upcoming Deep Underground Neutrino Experiment (DUNE) is to measure the O(10)\mathcal{O}(10) MeV neutrinos produced by a Galactic core-collapse supernova if one should occur during the lifetime of the experiment. The liquid-argon-based detectors planned for DUNE are expected to be uniquely sensitive to the Îœe\nu_e component of the supernova flux, enabling a wide variety of physics and astrophysics measurements. A key requirement for a correct interpretation of these measurements is a good understanding of the energy-dependent total cross section σ(EÎœ)\sigma(E_\nu) for charged-current Îœe\nu_e absorption on argon. In the context of a simulated extraction of supernova Îœe\nu_e spectral parameters from a toy analysis, we investigate the impact of σ(EÎœ)\sigma(E_\nu) modeling uncertainties on DUNE's supernova neutrino physics sensitivity for the first time. We find that the currently large theoretical uncertainties on σ(EÎœ)\sigma(E_\nu) must be substantially reduced before the Îœe\nu_e flux parameters can be extracted reliably: in the absence of external constraints, a measurement of the integrated neutrino luminosity with less than 10\% bias with DUNE requires σ(EÎœ)\sigma(E_\nu) to be known to about 5%. The neutrino spectral shape parameters can be known to better than 10% for a 20% uncertainty on the cross-section scale, although they will be sensitive to uncertainties on the shape of σ(EÎœ)\sigma(E_\nu). A direct measurement of low-energy Îœe\nu_e-argon scattering would be invaluable for improving the theoretical precision to the needed level.Comment: 25 pages, 21 figure

    Snowmass Neutrino Frontier: DUNE Physics Summary

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    The Deep Underground Neutrino Experiment (DUNE) is a next-generation long-baseline neutrino oscillation experiment with a primary physics goal of observing neutrino and antineutrino oscillation patterns to precisely measure the parameters governing long-baseline neutrino oscillation in a single experiment, and to test the three-flavor paradigm. DUNE's design has been developed by a large, international collaboration of scientists and engineers to have unique capability to measure neutrino oscillation as a function of energy in a broadband beam, to resolve degeneracy among oscillation parameters, and to control systematic uncertainty using the exquisite imaging capability of massive LArTPC far detector modules and an argon-based near detector. DUNE's neutrino oscillation measurements will unambiguously resolve the neutrino mass ordering and provide the sensitivity to discover CP violation in neutrinos for a wide range of possible values of ÎŽCP. DUNE is also uniquely sensitive to electron neutrinos from a galactic supernova burst, and to a broad range of physics beyond the Standard Model (BSM), including nucleon decays. DUNE is anticipated to begin collecting physics data with Phase I, an initial experiment configuration consisting of two far detector modules and a minimal suite of near detector components, with a 1.2 MW proton beam. To realize its extensive, world-leading physics potential requires the full scope of DUNE be completed in Phase II. The three Phase II upgrades are all necessary to achieve DUNE's physics goals: (1) addition of far detector modules three and four for a total FD fiducial mass of at least 40 kt, (2) upgrade of the proton beam power from 1.2 MW to 2.4 MW, and (3) replacement of the near detector's temporary muon spectrometer with a magnetized, high-pressure gaseous argon TPC and calorimeter
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