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1.
Cureus ; 15(5): e39594, 2023 May.
Artigo em Inglês | MEDLINE | ID: mdl-37384079

RESUMO

Spontaneous coronary artery dissection is a rare and commonly underdiagnosed cause of acute coronary syndrome. Here, we report the case of a 36-year-old male patient who presented with an acute onset of left-sided chest pain, preceded by several hours of nausea and vomiting. Past medical history was significant for chronic marijuana use and multiple episodes of nausea and vomiting requiring multiple hospitalizations. Urinary drug screen was positive for cannabinoids only, and electrocardiography revealed an ST-segment elevation myocardial infarction. This was complicated by an episode of ventricular fibrillation that was successfully defibrillated and prompted cardiac catheterization, which revealed a coronary intraluminal filling defect and a segmental lesion, suggestive of coronary dissection. No evidence of atherosclerotic plaque was noticed. Stent placement and thrombectomy were pursued and the patient was stabilized. As cannabinoid use is gaining legality and becoming widespread, this case aims to enhance physicians' awareness of potentially life-threatening complications of its use.

2.
Sensors (Basel) ; 20(22)2020 Nov 20.
Artigo em Inglês | MEDLINE | ID: mdl-33233598

RESUMO

We measured the radiation tolerance of commercially available diamonds grown by the Chemical Vapor Deposition process by measuring the charge created by a 120 GeV hadron beam in a 50 µm pitch strip detector fabricated on each diamond sample before and after irradiation. We irradiated one group of samples with 70 MeV protons, a second group of samples with fast reactor neutrons (defined as energy greater than 0.1 MeV), and a third group of samples with 200 MeV pions, in steps, to (8.8±0.9) × 1015 protons/cm2, (1.43±0.14) × 1016 neutrons/cm2, and (6.5±1.4) × 1014 pions/cm2, respectively. By observing the charge induced due to the separation of electron-hole pairs created by the passage of the hadron beam through each sample, on an event-by-event basis, as a function of irradiation fluence, we conclude all datasets can be described by a first-order damage equation and independently calculate the damage constant for 70 MeV protons, fast reactor neutrons, and 200 MeV pions. We find the damage constant for diamond irradiated with 70 MeV protons to be 1.62±0.07(stat)±0.16(syst)× 10-18 cm2/(p µm), the damage constant for diamond irradiated with fast reactor neutrons to be 2.65±0.13(stat)±0.18(syst)× 10-18 cm2/(n µm), and the damage constant for diamond irradiated with 200 MeV pions to be 2.0±0.2(stat)±0.5(syst)× 10-18 cm2/(π µm). The damage constants from this measurement were analyzed together with our previously published 24 GeV proton irradiation and 800 MeV proton irradiation damage constant data to derive the first comprehensive set of relative damage constants for Chemical Vapor Deposition diamond. We find 70 MeV protons are 2.60 ± 0.29 times more damaging than 24 GeV protons, fast reactor neutrons are 4.3 ± 0.4 times more damaging than 24 GeV protons, and 200 MeV pions are 3.2 ± 0.8 more damaging than 24 GeV protons. We also observe the measured data can be described by a universal damage curve for all proton, neutron, and pion irradiations we performed of Chemical Vapor Deposition diamond. Finally, we confirm the spatial uniformity of the collected charge increases with fluence for polycrystalline Chemical Vapor Deposition diamond, and this effect can also be described by a universal curve.

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