273 research outputs found

    Scalaron the mighty: producing dark matter and baryon asymmetry at reheating

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    In R^2-inflation scalaron slow roll is responsible for the inflationary stage, while its oscillations reheat the Universe. We find that the same scalaron decays induced by gravity can also provide the dark matter production and leptogenesis. With R^2-term and three Majorana fermions added to the Standard Model, we arrive at the phenomenologically complete theory capable of simultaneously explaining neutrino oscillations, inflation, reheating, dark matter and baryon asymmetry of the Universe. Besides the seesaw mechanism in neutrino sector, we use only gravity, which solves all the problems by exploiting scalaron.Comment: 13 pages; v2: minor corrections; v3: 14 pages, journal versio

    Free scalar dark matter candidates in R^2-inflation: the light, the heavy and the superheavy

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    Gravity takes care of both inflation and subsequent reheating in Starobinsky's R^2-model. The latter is due to inflaton gravitation decays dominated by scalar particle production. It is tempting to suggest that dark matter particles are also produced in this process. Since free scalars being too hot cannot serve as viable dark matter (Phys.Lett.B700:157-162,2011), we further study the issue considering two options: scalars with non-minimal coupling to gravity and superheavy scalars generated at inflationary stage. We found that the first option allows for viable warm or cold dark matter if scalar mass exceeds 0.8 MeV. The second option implies supercold dark matter with particle mass 10^16 GeV, which production is saturated at the end of inflation when inflaton-dependent scalar mass rapidly changes and violates adiabaticity. Similar result holds for superheavy fermion dark matter.Comment: 15 pages, 3 figures; journal versio

    ĐąĐ”Ń€ĐŒĐžŃ‡Đ”ŃĐșая гДлОĐč-ĐșĐžŃĐ»ĐŸŃ€ĐŸĐŽĐœĐ°Ń ŃĐŒĐ”ŃŃŒ ĐČ Đ»Đ”Ń‡Đ”Đ±ĐœĐŸĐŒ Đ°Đ»ĐłĐŸŃ€ĐžŃ‚ĐŒĐ” Đ±ĐŸĐ»ŃŒĐœŃ‹Ń… с COVID-19

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    Background. The paper discusses the use of a thermal helium-oxygen mixture (t-ĐĐ”/О2 ), a novel technology, in treating patients with the 2019-nCoV acute respiratory disease (COVID-19) who develop life-threatening respiratory failure. Aim to evaluate the safety and efficacy of t-ĐĐ”/О2 inhalation combined with standard therapy in the treatment of acute respiratory failure in patients with COVID-19. Materials and Methods. This was a single-center, randomized, prospective study of 70 patients with COVID-19. All patients were divided into two groups: in Group 1 (n = 38) patients received t-He/О2 in addition to the standard COVID-19 treatment; and in Group 2 (n = 32) patients were given the standard treatment in accordance with the Clinical Treatment Guidelines for patients with COVID-19, developed by the Ministry of Health of the Russian Federation. The male/female ratio was 18/20 in Group 1 and 18/14 in Group 2. The mean age of the patients in the study was 53.5 years (43; 62): 56 years (42; 64) in Group 1 and 52 years (43; 66) in Group 2. All patients had computed tomography (CT) signs of lung injury: ground-glass opacities and areas of consolidation. SARS-CoV-2 RNA was detected in 30 Group 1 patients and 28 Group 2 patients. The patients were matched by sex, age, body mass index (BMI), area of pulmonary involvement, and laboratory findings. All patients provided voluntary informed consent to participate in the study and signed a consent form. Results. Inhalation of thermal helium-oxygen mixture combined with standard therapy did not cause any procedure-related side effects in any of the patients. The following changes were observed in all patients: pO2 /FiO2 , SpO2 , and lymphocyte counts increased, C-reactive protein (CRP) levels decreased, and D-dimer and ferritin levels returned to normal. In Group 1 statistically significant changes in the above-mentioned parameters were seen within three days, while in Group 2 the same changes were observed between Days 7 and 10 of treatment. In Group 1 patients cleared SARS-CoV-2 within 4872 hours after initiation of inhalation, which was confirmed by polymerase chain reaction (PCR), and in Group 2 virus elimination was achieved within 72168 hours. Conclusion. The addition of inhalation of a thermal gas mixture of helium and oxygen (t-He/О2 ) to the standard therapy for patients with SARS-CoV-2 infection, CT signs of pneumonia (grades ĐĄT2 or CT3), and acute respiratory failure improves gas exchange, contributes to a more rapid virus elimination, and indirectly reduces inflammation.ĐžĐ±ĐŸŃĐœĐŸĐČĐ°ĐœĐžĐ”. В прДЎстаĐČĐ»Đ”ĐœĐœĐŸĐč Ń€Đ°Đ±ĐŸŃ‚Đ” Ń€Đ”Ń‡ŃŒ ĐżĐŸĐčЎДт ĐŸ ĐœĐŸĐČĐŸĐč Ń‚Đ”Ń…ĐœĐŸĐ»ĐŸĐłĐžĐž ĐżŃ€ĐžĐŒĐ”ĐœĐ”ĐœĐžŃ Ń‚Đ”Ń€ĐŒĐžŃ‡Đ”ŃĐșĐŸĐłĐŸ ĐłĐ”Đ»ĐžŃ Đž ĐșĐžŃĐ»ĐŸŃ€ĐŸĐŽĐ° (t-ĐĐ”/О2 ) ĐČ Đ»Đ”Ń‡Đ”ĐœĐžĐž Đ±ĐŸĐ»ŃŒĐœŃ‹Ń… с ĐČĐžŃ€ŃƒŃĐœŃ‹ĐŒ Đ·Đ°Đ±ĐŸĐ»Đ”ĐČĐ°ĐœĐžĐ”ĐŒ ĐĄOVID-19 ĐœĐ° ŃŃ‚Đ°ĐżĐ” разĐČотоя Đ¶ĐžĐ·ĐœĐ”ŃƒĐłŃ€ĐŸĐ¶Đ°ŃŽŃ‰Đ”ĐłĐŸ ŃĐžĐœĐŽŃ€ĐŸĐŒĐ° ĐŽŃ‹Ń…Đ°Ń‚Đ”Đ»ŃŒĐœĐŸĐč ĐœĐ”ĐŽĐŸŃŃ‚Đ°Ń‚ĐŸŃ‡ĐœĐŸŃŃ‚Đž. ĐŠĐ”Đ»ŃŒ ĐžĐ·ŃƒŃ‡ĐžŃ‚ŃŒ Đ±Đ”Đ·ĐŸĐżĐ°ŃĐœĐŸŃŃ‚ŃŒ Đž ŃŃ„Ń„Đ”ĐșтоĐČĐœĐŸŃŃ‚ŃŒ ĐžĐœĐłĐ°Đ»ŃŃ†ĐžĐŸĐœĐœĐŸĐč тДрапОО t-ĐĐ”/О2 ĐČ Đ»Đ”Ń‡Đ”ĐœĐžĐž ĐŸŃŃ‚Ń€ĐŸĐč ĐŽŃ‹Ń…Đ°Ń‚Đ”Đ»ŃŒĐœĐŸĐč ĐœĐ”ĐŽĐŸŃŃ‚Đ°Ń‚ĐŸŃ‡ĐœĐŸŃŃ‚Đž ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ Ń ĐĄOVID-19 ĐœĐ° Ń„ĐŸĐœĐ” ŃŃ‚Đ°ĐœĐŽĐ°Ń€Ń‚ĐœĐŸĐč тДрапОО. ĐœĐ°Ń‚Đ”Ń€ĐžĐ°Đ»Ń‹ Đž ĐŒĐ”Ń‚ĐŸĐŽŃ‹. В ĐŸĐŽĐœĐŸŃ†Đ”ĐœŃ‚Ń€ĐŸĐČĐŸĐ” Ń€Đ°ĐœĐŽĐŸĐŒĐžĐ·ĐžŃ€ĐŸĐČĐ°ĐœĐœĐŸĐ” ĐżŃ€ĐŸŃĐżĐ”ĐșтоĐČĐœĐŸĐ” ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐ” Đ±Ń‹Đ»ĐŸ ĐČĐșĐ»ŃŽŃ‡Đ”ĐœĐŸ 70 ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ Ń COVID-19. ĐŸĐ°Ń†ĐžĐ”ĐœŃ‚Ń‹ былО Ń€Đ°Đ·ĐŽĐ”Đ»Đ”ĐœŃ‹ ĐœĐ° ĐŽĐČĐ” группы: ĐČ ĐżĐ”Ń€ĐČĐŸĐč (n = 38) ĐČ ŃŃ‚Đ°ĐœĐŽĐ°Ń€Ń‚ĐœŃ‹Đč ĐżŃ€ĐŸŃ‚ĐŸĐșĐŸĐ» Đ»Đ”Ń‡Đ”ĐœĐžŃ COVID-19 была ĐČĐșĐ»ŃŽŃ‡Đ”ĐœĐ° Ń‚Đ”Ń€Đ°ĐżĐžŃ t-ĐĐ”/О2 ; ĐČĐŸ ĐČŃ‚ĐŸŃ€ĐŸĐč (n = 32) ĐżŃ€ĐŸĐČĐŸĐŽĐžĐ»Đ°ŃŃŒ ŃŃ‚Đ°ĐœĐŽĐ°Ń€Ń‚ĐœĐ°Ń Ń‚Đ”Ń€Đ°ĐżĐžŃ ĐČ ŃĐŸĐŸŃ‚ĐČДтстĐČОО с ĐșĐ»ĐžĐœĐžŃ‡Đ”ŃĐșĐžĐŒĐž рДĐșĐŸĐŒĐ”ĐœĐŽĐ°Ń†ĐžŃĐŒĐž ĐœĐžĐœĐ·ĐŽŃ€Đ°ĐČĐ° Đ ĐŸŃŃĐžĐž ĐŽĐ»Ń Đ±ĐŸĐ»ŃŒĐœŃ‹Ń… с COVID. В пДрĐČĐŸĐč ĐłŃ€ŃƒĐżĐżĐ” ŃĐŸĐŸŃ‚ĐœĐŸŃˆĐ”ĐœĐžĐ” ĐŒŃƒĐ¶Ń‡ĐžĐœŃ‹/Đ¶Đ”ĐœŃ‰ĐžĐœŃ‹ 18/20, Đ° ĐČĐŸ ĐČŃ‚ĐŸŃ€ĐŸĐč 18/14. ĐĄŃ€Đ”ĐŽĐœĐžĐč ĐČĐŸĐ·Ń€Đ°ŃŃ‚ ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ ĐČ ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐž ŃĐŸŃŃ‚Đ°ĐČĐ»ŃĐ» 53,5 ĐłĐŸĐŽĐ° (43 ĐłĐŸĐŽĐ° ĐŒŃƒĐ¶Ń‡ĐžĐœŃ‹; 62 ĐłĐŸĐŽĐ° Đ¶Đ”ĐœŃ‰ĐžĐœŃ‹), ĐČ ĐżĐ”Ń€ĐČĐŸĐč ĐłŃ€ŃƒĐżĐżĐ” 56 лДт (42 Đž 64 ĐłĐŸĐŽĐ° ŃĐŸĐŸŃ‚ĐČДтстĐČĐ”ĐœĐœĐŸ), ĐČĐŸ ĐČŃ‚ĐŸŃ€ĐŸĐč 52 ĐłĐŸĐŽĐ° (43 Đž 66 лДт). ĐŁ ĐČсДх ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ ĐžĐŒĐ”Đ»ĐžŃŃŒ Кб-ĐżŃ€ĐžĐ·ĐœĐ°ĐșĐž ĐżĐŸŃ€Đ°Đ¶Đ”ĐœĐžŃ лДгĐșох ĐżĐŸ топу ĐŒĐ°Ń‚ĐŸĐČĐŸĐłĐŸ стДĐșла, участĐșĐž ĐșĐŸĐœŃĐŸĐ»ĐžĐŽĐ°Ń†ĐžĐž. йДст РНК ĐșĐŸŃ€ĐŸĐœĐ°ĐČоруса SARS-CoV-2 ĐżĐŸĐ»ĐŸĐ¶ĐžŃ‚Đ”Đ»ŃŒĐœŃ‹Đč ĐČ ĐżĐ”Ń€ĐČĐŸĐč ĐłŃ€ŃƒĐżĐżĐ” у 30 ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ, ĐČĐŸ ĐČŃ‚ĐŸŃ€ĐŸĐč у 28. ĐŸĐ°Ń†ĐžĐ”ĐœŃ‚Ń‹ ŃĐŸĐżĐŸŃŃ‚Đ°ĐČĐžĐŒŃ‹ ĐżĐŸ ĐżĐŸĐ»Ńƒ, ĐČĐŸĐ·Ń€Đ°ŃŃ‚Ńƒ, ĐžĐœĐŽĐ”Đșсу ĐŒĐ°ŃŃŃ‹ тДла (ИМб), ĐżĐ»ĐŸŃ‰Đ°ĐŽĐž ĐżĐŸŃ€Đ°Đ¶Đ”ĐœĐžŃ Đ»Đ”ĐłĐŸŃ‡ĐœĐŸĐč ĐżĐ°Ń€Đ”ĐœŃ…ĐžĐŒŃ‹, Đ»Đ°Đ±ĐŸŃ€Đ°Ń‚ĐŸŃ€ĐœŃ‹ĐŒ ĐŽĐ°ĐœĐœŃ‹ĐŒ. Đ’ŃĐ”ĐŒĐž ĐżĐ°Ń†ĐžĐ”ĐœŃ‚Đ°ĐŒĐž Đ±Ń‹Đ»ĐŸ ĐżĐŸĐŽĐżĐžŃĐ°ĐœĐŸ ĐžĐœŃ„ĐŸŃ€ĐŒĐžŃ€ĐŸĐČĐ°ĐœĐœĐŸĐ” ĐŽĐŸĐ±Ń€ĐŸĐČĐŸĐ»ŃŒĐœĐŸĐ” ŃĐŸĐłĐ»Đ°ŃĐžĐ” ĐœĐ° ŃƒŃ‡Đ°ŃŃ‚ĐžĐ” ĐČ ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐž. Đ Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Ń‹. ВслДЎстĐČОД ĐżŃ€ĐžĐŒĐ”ĐœĐ”ĐœĐžŃ Ń‚Đ”Ń€ĐŒĐžŃ‡Đ”ŃĐșĐŸĐč гДлОĐč-ĐșĐžŃĐ»ĐŸŃ€ĐŸĐŽĐœĐŸĐč ŃĐŒĐ”ŃĐž ĐœĐ° Ń„ĐŸĐœĐ” ŃŃ‚Đ°ĐœĐŽĐ°Ń€Ń‚ĐœĐŸĐč тДрапОО ĐœĐž у ĐŸĐŽĐœĐŸĐłĐŸ ĐżĐ°Ń†ĐžĐ”ĐœŃ‚Đ° ĐŸĐ±ŃŠĐ”ĐșтоĐČĐœŃ‹Ń… ĐżĐŸĐ±ĐŸŃ‡ĐœŃ‹Ń… ŃŃ„Ń„Đ”ĐșŃ‚ĐŸĐČ, сĐČŃĐ·Đ°ĐœĐœŃ‹Ń… с ĐżŃ€ĐŸŃ†Đ”ĐŽŃƒŃ€ĐŸĐč, ĐœĐ” ĐČыяĐČĐ»Đ”ĐœĐŸ. ĐŁ ĐČсДх ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ ĐŸĐ±ĐœĐ°Ń€ŃƒĐ¶Đ”ĐœŃ‹ ŃĐ»Đ”ĐŽŃƒŃŽŃ‰ĐžĐ” ĐžĐ·ĐŒĐ”ĐœĐ”ĐœĐžŃ: ĐżĐŸĐČŃ‹ŃˆĐ”ĐœĐžĐ” pО2 /FiO2, SpO2 Đž ŃƒŃ€ĐŸĐČĐœŃ Đ»ĐžĐŒŃ„ĐŸŃ†ĐžŃ‚ĐŸĐČ, ŃĐœĐžĐ¶Đ”ĐœĐžĐ” ĐșĐŸĐœŃ†Đ”ĐœŃ‚Ń€Đ°Ń†ĐžĐž ĐĄ-рДаĐșтоĐČĐœĐŸĐłĐŸ бДлĐșĐ°, ĐČĐŸŃŃŃ‚Đ°ĐœĐŸĐČĐ»Đ”ĐœĐžĐ” ŃƒŃ€ĐŸĐČĐœĐ”Đč Д-ĐŽĐžĐŒĐ”Ń€Đ°, Ń„Đ”Ń€Ń€ĐžŃ‚ĐžĐœĐ°. Это ĐżŃ€ĐžĐ·ĐœĐ°ĐșĐž статОстОчДсĐșĐž Đ·ĐœĐ°Ń‡ĐžĐŒĐŸ ĐžĐ·ĐŒĐ”ĐœĐžĐ»ĐžŃŃŒ ĐČ ĐżĐ”Ń€ĐČĐŸĐč ĐłŃ€ŃƒĐżĐżĐ” ĐČ Ń‚Đ”Ń‡Đ”ĐœĐžĐ” 3 сут, Ń‚ĐŸĐłĐŽĐ° ĐșĐ°Đș ĐČĐŸ ĐČŃ‚ĐŸŃ€ĐŸĐč ĐłŃ€ŃƒĐżĐżĐ” ĐœĐ° 710-Đ” сут тДрапОО. Đ­Đ»ĐžĐŒĐžĐœĐ°Ń†ĐžŃ ĐČоруса SARS-CoV-2 ĐČ ĐżĐ”Ń€ĐČĐŸĐč ĐłŃ€ŃƒĐżĐżĐ” ĐżŃ€ĐŸĐžŃŃ…ĐŸĐŽĐžĐ»Đ° ĐČ Ń‚Đ”Ń‡Đ”ĐœĐžĐ” 4872 ч ĐŸŃ‚ ĐŒĐŸĐŒĐ”ĐœŃ‚Đ° ĐœĐ°Ń‡Đ°Đ»Đ° ĐžĐœĐłĐ°Đ»ŃŃ†ĐžĐž, Ń‡Ń‚ĐŸ ĐżĐŸĐŽŃ‚ĐČĐ”Ń€Đ¶ĐŽĐ°Đ»ĐŸŃŃŒ ĐŒĐ”Ń‚ĐŸĐŽĐŸĐŒ ПЩР, Đ° ĐČĐŸ ĐČŃ‚ĐŸŃ€ĐŸĐč ĐČ Ń‚Đ”Ń‡Đ”ĐœĐžĐ” 72168 ч. ЗаĐșĐ»ŃŽŃ‡Đ”ĐœĐžĐ”. ВĐșĐ»ŃŽŃ‡Đ”ĐœĐžĐ” ĐžĐœĐłĐ°Đ»ŃŃ†ĐžĐč Ń‚Đ”Ń€ĐŒĐžŃ‡Đ”ŃĐșĐŸĐč ĐłĐ°Đ·ĐŸĐČĐŸĐč ŃĐŒĐ”ŃĐž ĐłĐ”Đ»ĐžŃ с ĐșĐžŃĐ»ĐŸŃ€ĐŸĐŽĐŸĐŒ (t-ĐĐ”/О2 ) ĐČ ŃŃ‚Đ°ĐœĐŽĐ°Ń€Ń‚ĐœŃƒŃŽ тДрапОю ĐżĐ°Ń†ĐžĐ”ĐœŃ‚ĐŸĐČ, ĐżĐ”Ń€Đ”ĐœĐŸŃŃŃ‰ĐžŃ… ĐžĐœŃ„Đ”ĐșŃ†ĐžĐŸĐœĐœĐŸĐ” Đ·Đ°Đ±ĐŸĐ»Đ”ĐČĐ°ĐœĐžĐ”, ĐČŃ‹Đ·ĐČĐ°ĐœĐœĐŸĐ” SARS-CĐŸV-2, c Кб-ĐżŃ€ĐžĐ·ĐœĐ°ĐșĐ°ĐŒĐž ĐżĐœĐ”ĐČĐŒĐŸĐœĐžĐž (Кб2, Кб3), с ĐŸŃŃ‚Ń€ĐŸĐč ĐŽŃ‹Ń…Đ°Ń‚Đ”Đ»ŃŒĐœĐŸĐč ĐœĐ”ĐŽĐŸŃŃ‚Đ°Ń‚ĐŸŃ‡ĐœĐŸŃŃ‚ŃŒŃŽ ŃƒĐ»ŃƒŃ‡ŃˆĐ°Đ”Ń‚ ĐłĐ°Đ·ĐŸĐŸĐ±ĐŒĐ”Đœ, ŃĐżĐŸŃĐŸĐ±ŃŃ‚ĐČŃƒĐ”Ń‚ усĐșĐŸŃ€Đ”ĐœĐžŃŽ ŃĐ»ĐžĐŒĐžĐœĐ°Ń†ĐžĐž ĐČоруса Đž ĐŸĐżĐŸŃŃ€Đ”ĐŽĐŸĐČĐ°ĐœĐœĐŸ ĐżĐŸĐČŃ‹ŃˆĐ°Đ”Ń‚ ĐżŃ€ĐŸŃ‚ĐžĐČĐŸĐČĐŸŃĐżĐ°Đ»ĐžŃ‚Đ”Đ»ŃŒĐœŃ‹Đč ŃŃ„Ń„Đ”Đșт

    Search for displaced vertices arising from decays of new heavy particles in 7 TeV pp collisions at ATLAS

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    We present the results of a search for new, heavy particles that decay at a significant distance from their production point into a final state containing charged hadrons in association with a high-momentum muon. The search is conducted in a pp-collision data sample with a center-of-mass energy of 7 TeV and an integrated luminosity of 33 pb^-1 collected in 2010 by the ATLAS detector operating at the Large Hadron Collider. Production of such particles is expected in various scenarios of physics beyond the standard model. We observe no signal and place limits on the production cross-section of supersymmetric particles in an R-parity-violating scenario as a function of the neutralino lifetime. Limits are presented for different squark and neutralino masses, enabling extension of the limits to a variety of other models.Comment: 8 pages plus author list (20 pages total), 8 figures, 1 table, final version to appear in Physics Letters

    Measurement of the polarisation of W bosons produced with large transverse momentum in pp collisions at sqrt(s) = 7 TeV with the ATLAS experiment

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    This paper describes an analysis of the angular distribution of W->enu and W->munu decays, using data from pp collisions at sqrt(s) = 7 TeV recorded with the ATLAS detector at the LHC in 2010, corresponding to an integrated luminosity of about 35 pb^-1. Using the decay lepton transverse momentum and the missing transverse energy, the W decay angular distribution projected onto the transverse plane is obtained and analysed in terms of helicity fractions f0, fL and fR over two ranges of W transverse momentum (ptw): 35 < ptw < 50 GeV and ptw > 50 GeV. Good agreement is found with theoretical predictions. For ptw > 50 GeV, the values of f0 and fL-fR, averaged over charge and lepton flavour, are measured to be : f0 = 0.127 +/- 0.030 +/- 0.108 and fL-fR = 0.252 +/- 0.017 +/- 0.030, where the first uncertainties are statistical, and the second include all systematic effects.Comment: 19 pages plus author list (34 pages total), 9 figures, 11 tables, revised author list, matches European Journal of Physics C versio

    Observation of a new chi_b state in radiative transitions to Upsilon(1S) and Upsilon(2S) at ATLAS

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    The chi_b(nP) quarkonium states are produced in proton-proton collisions at the Large Hadron Collider (LHC) at sqrt(s) = 7 TeV and recorded by the ATLAS detector. Using a data sample corresponding to an integrated luminosity of 4.4 fb^-1, these states are reconstructed through their radiative decays to Upsilon(1S,2S) with Upsilon->mu+mu-. In addition to the mass peaks corresponding to the decay modes chi_b(1P,2P)->Upsilon(1S)gamma, a new structure centered at a mass of 10.530+/-0.005 (stat.)+/-0.009 (syst.) GeV is also observed, in both the Upsilon(1S)gamma and Upsilon(2S)gamma decay modes. This is interpreted as the chi_b(3P) system.Comment: 5 pages plus author list (18 pages total), 2 figures, 1 table, corrected author list, matches final version in Physical Review Letter

    Measurement of the inclusive isolated prompt photon cross-section in pp collisions at sqrt(s)= 7 TeV using 35 pb-1 of ATLAS data

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    A measurement of the differential cross-section for the inclusive production of isolated prompt photons in pp collisions at a center-of-mass energy sqrt(s) = 7 TeV is presented. The measurement covers the pseudorapidity ranges |eta|<1.37 and 1.52<=|eta|<2.37 in the transverse energy range 45<=E_T<400GeV. The results are based on an integrated luminosity of 35 pb-1, collected with the ATLAS detector at the LHC. The yields of the signal photons are measured using a data-driven technique, based on the observed distribution of the hadronic energy in a narrow cone around the photon candidate and the photon selection criteria. The results are compared with next-to-leading order perturbative QCD calculations and found to be in good agreement over four orders of magnitude in cross-section.Comment: 7 pages plus author list (18 pages total), 2 figures, 4 tables, final version published in Physics Letters

    Measurement of D*+/- meson production in jets from pp collisions at sqrt(s) = 7 TeV with the ATLAS detector

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    This paper reports a measurement of D*+/- meson production in jets from proton-proton collisions at a center-of-mass energy of sqrt(s) = 7 TeV at the CERN Large Hadron Collider. The measurement is based on a data sample recorded with the ATLAS detector with an integrated luminosity of 0.30 pb^-1 for jets with transverse momentum between 25 and 70 GeV in the pseudorapidity range |eta| < 2.5. D*+/- mesons found in jets are fully reconstructed in the decay chain: D*+ -> D0pi+, D0 -> K-pi+, and its charge conjugate. The production rate is found to be N(D*+/-)/N(jet) = 0.025 +/- 0.001(stat.) +/- 0.004(syst.) for D*+/- mesons that carry a fraction z of the jet momentum in the range 0.3 < z < 1. Monte Carlo predictions fail to describe the data at small values of z, and this is most marked at low jet transverse momentum.Comment: 10 pages plus author list (22 pages total), 5 figures, 1 table, matches published version in Physical Review

    Search for scalar top quark pair production in natural gauge mediated supersymmetry models with the ATLAS detector in pp collisions at sqrt(s) = 7 TeV

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    The results of a search for pair production of the lighter scalar partners of top quarks in 2.05 fb-1 of pp collisions at sqrt(s) =7 TeV using the ATLAS experiment at the LHC are reported. Scalar top quarks are searched for in events with two same flavour opposite-sign leptons (electrons or muons) with invariant mass consistent with the Z boson mass, large missing transverse momentum and jets in the final state. At least one of the jets is identified as originating from a b-quark. No excess over Standard Model expectations is found. The results are interpreted in the framework of R-parity conserving, gauge mediated Supersymmetry breaking `natural' scenarios, where the neutralino is the next-to-lightest supersymmetric particle. Scalar top quark masses up to 310 GeV are excluded for the lightest neutralino mass between 115 GeV and 230 GeV at 95% confidence level, reaching an exclusion of the scalar top quark mass of 330 GeV for the lightest neutralino mass of 190 GeV. Scalar top quark masses below 240 GeV are excluded for all values of the lightest neutralino mass above the Z boson mass.Comment: 7 pages plus author list (20 pages total), 4 figures, 1 table, matches published PLB versio
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