The upper Permian Zechstein Limestone carbonates in the south-western part of the Polish Zechstein basin contain small quantities of organic matter (usually less than 0.1
wt% TOC) and have poor ...hydrocarbon potential. In contrast, the Kupferschiefer shales have excellent hydrocarbon potential with TOC as high as 10.8
wt%, predominantly algal type II kerogen. Generally, thermal maturity of the organic matter is 0.6–0.9% vitrinite reflectance, while locally, is as high as 1.45%. The Kimmerian and Laramian tectonic events significantly influenced the regional burial and thermal history. The main subsidence of the Kupferschiefer–Zechstein Limestone complex took place during the Late Permian–Late Triassic period, with additional burial during the Jurassic and Late Cretaceous. Hydrocarbon generation from the Kupferschiefer source rocks occurred from Middle Triassic to Late Jurassic times, reaching maximum rates during the Jurassic. The Cretaceous subsidence had only a minor influence on the maturity and transformation of organic matter. Expulsion started between Late Triassic (in the western part of the study area) and Early Jurassic (in the eastern part), then ceased by the Late Jurassic–Early Cretaceous erosion. The total amount of generated and expelled hydrocarbons from source rocks was small because their thickness was limited. Therefore, Kupferschiefer shales cannot be considered as source rocks for liquid hydrocarbons, but may be a potential source for gas accumulated in the Zechstein Limestone and Rotliegend reservoirs.
Acute ischaemic stroke is a devastating postoperative complication that significantly impacts upon a patient's quality of life. Endovascular retrieval of thromboembolic material from proximal ...cerebral arteries by mechanical thrombectomy is the new standard of care for patients presenting with a proximal artery occlusion. We report the case of a patient developing an acute ischaemic stroke following pulmonary lobectomy, who was transferred to the regional neurosciences unit, despite the absence of an established referral pathway, to undergo mechanical thrombectomy, with significant prognostic neurological benefit. We would advocate all cardiothoracic centres identify their regional neurosciences unit and initiate discussion to establish a referral pathway.
MCORD - MPD Cosmic Ray Detector a new features Bielewicz, M.; Milewicz-Zalewska, M.; Grodzicka-Kobylka, M. ...
EPJ Web of Conferences,
2019, Letnik:
204
Journal Article, Conference Proceeding
Recenzirano
Odprti dostop
The main detector system at the Nuclotron-based Ion Collider fAcility (NICA) located in Dubna, Russia is the Multi-Purpose Detector (MPD). For better calibration reason, the MPD needs an additional ...trigger system for an off-beam calibration of MPD sub-detectors and for rejection (veto) of cosmic muons. The system should also be useful for practical astrophysics observations of cosmic showers. The consortium NICA-PL group defines goals and basic assumptions for the MPD Cosmic Ray Detector (MCORD). This article describes the conceptual design and simulation plans of the MCORD detector based on plastic scintillators with SiPM photodetectors and electronic digital system based on the MicroTCA crate.
The Nuclotron-based Ion Collider fAcility (NICA) is under construction at the Joint Institute for Nuclear Research (JINR), with commissioning of the facility expected in late 2022. The Multi-Purpose ...Detector (MPD) has been designed to operate at NICA and its components are currently in production. The detector is expected to be ready for data taking with the first beams from NICA. This document provides an overview of the landscape of the investigation of the QCD phase diagram in the region of maximum baryonic density, where NICA and MPD will be able to provide significant and unique input. It also provides a detailed description of the MPD set-up, including its various subsystems as well as its support and computing infrastructures. Selected performance studies for particular physics measurements at MPD are presented and discussed in the context of existing data and theoretical expectations.
We report measurements of Υ meson production in p + p, d + Au, and Au+Au collisions using the STAR detector at RHIC. We compare the Υ yield to the measured cross section in p + p collisions in order ...to quantify any modifications of the yield in cold nuclear matter using d + Au data and in hot nuclear matter using Au+Au data separated into three centrality classes. Our p + p measurement is based on three times the statistics of our previous result. We obtain a nuclear modification factor for Upsilon (1S + 2S + 3S) in the rapidity range |y| < 1 in d + Au collisions of RdAu = 0.79 ± 0.24(stat.) ± 0.03(syst.) ± 0.10(p + p syst.). A comparison with models including shadowing and initial state parton energy loss indicates the presence of additional cold-nuclear matter suppression. Similarly, in the top 10% most-central Au + Au collisions, we measure a nuclear modification factor of R AA = 0.49 ±0.1(stat.) ±0.02(syst.) ±0.06(p + p syst.), which is a larger suppression factor than that seen in cold nuclear matter. Our results are consistent with complete suppression of excited-state Upsilon mesons in Au + Au collisions. The additional suppression in Au + Au is consistent with the level expected in model calculations that include the presence of a hot, deconfined Quark–Gluon Plasma. However, understanding the suppression seen in d + Au is still needed before any definitive statements about the nature of the suppression in Au + Au can be made.
Identified charged pion, kaon, and proton spectra are used to explore the system size dependence of bulk freeze-out properties in Cu+Cu collisions at {radical}s{sub NN} = 200 and 62.4 GeV. The data ...are studied with hydrodynamically motivated blast-wave and statistical model frameworks in order to characterize the freeze-out properties of the system. The dependence of freeze-out parameters on beam energy and collision centrality is discussed. Using the existing results from Au + Au and pp collisions, the dependence of freeze-out parameters on the system size is also explored. This multidimensional systematic study furthers our understanding of the QCD phase diagram revealing the importance of the initial geometrical overlap of the colliding ions. The analysis of Cu+Cu collisions expands the system size dependence studies from Au+Au data with detailed measurements in the smaller system. The systematic trends of the bulk freeze-out properties of charged particles is studied with respect to the total charged particle multiplicity at midrapidity, exploring the influence of initial state effects.
We report the first measurements of the moments--mean (M), variance (σ(2)), skewness (S), and kurtosis (κ)--of the net-charge multiplicity distributions at midrapidity in Au+Au collisions at seven ...energies, ranging from sqrtsNN=7.7 to 200 GeV, as a part of the Beam Energy Scan program at RHIC. The moments are related to the thermodynamic susceptibilities of net charge, and are sensitive to the location of the QCD critical point. We compare the products of the moments, σ(2)/M, Sσ, and κσ(2), with the expectations from Poisson and negative binomial distributions (NBDs). The Sσ values deviate from the Poisson baseline and are close to the NBD baseline, while the κσ(2) values tend to lie between the two. Within the present uncertainties, our data do not show nonmonotonic behavior as a function of collision energy. These measurements provide a valuable tool to extract the freeze-out parameters in heavy-ion collisions by comparing with theoretical models.
PDF
