2,093 research outputs found
Deep learning for inferring cause of data anomalies
Daily operation of a large-scale experiment is a resource consuming task,
particularly from perspectives of routine data quality monitoring. Typically,
data comes from different sub-detectors and the global quality of data depends
on the combinatorial performance of each of them. In this paper, the problem of
identifying channels in which anomalies occurred is considered. We introduce a
generic deep learning model and prove that, under reasonable assumptions, the
model learns to identify 'channels' which are affected by an anomaly. Such
model could be used for data quality manager cross-check and assistance and
identifying good channels in anomalous data samples. The main novelty of the
method is that the model does not require ground truth labels for each channel,
only global flag is used. This effectively distinguishes the model from
classical classification methods. Being applied to CMS data collected in the
year 2010, this approach proves its ability to decompose anomaly by separate
channels.Comment: Presented at ACAT 2017 conference, Seattle, US
Red flags to diagnose infiltrative cardiomyopathies
Infiltrative cardiomyopathies are a group of diseases characterized by the deposition of abnormal substances in heart tissues, which leads to thickening of the walls or dilation of chambers with a secondary decrease in wall thickness and the development of diastolic, less often systolic, ventricular dysfunction. Most often, these are progressive diseases that, in the absence of adequate therapy, have an unfavorable prognosis. Clinical manifestations of infiltrative cardiac diseases are variable, which often leads to diagnostic difficulties and errors. In most cases, specific laboratory and morphological tests are required to confirm or clarify the diagnosis. Early diagnosis is critical to initiating therapy and improving patient prognosis. This article provides characteristic signs and symptoms, the so-called "red flags", making it possible to suspect infiltrative cardiomyopathies, diagnose them at an early stage and start life-saving therapy
Uterine microbiome in women with uterine scar defect after cesarean section: Prospective cohort study
Aim. To evaluate the endometrial microbiota in patients with uterine scar defect after cesarean section.
Materials and methods. The study included 80 women of reproductive age. The main group included 50 patients with a uterus scar defect due to cesarean section; the comparison group included 30 women with a competent uterus scar due to cesarean section. Patients underwent a Pipelle endometrial biopsy on days 2022 of the menstrual cycle using a double-lumen catheter that excludes sample contamination with vaginal and cervical microflora. A molecular genetic study of the endometrium was performed by real-time polymerase chain reaction using the Femoflor 16 reagent kit (DNA-Technology
Moscow). The DNA content in the specimen was measured using software and expressed in genome equivalent (GE) proportional to the number of microorganisms. The statistical data were processed using the ExŃel software package and SPSS Statistics 22.0.
Results. The study showed the following statistically significant differences: lower count of Lactobacillus spp. 2.600 (1.4303.600) GE/mL vs 3.550 (2.8004.700) GE/mL in patients of the comparison group (p=0.02); higher count of Streptococcus and Staphylococcus spp. 3.270 (3.0003.700) GE/mL and 3.450 (3.2003.600) GE/mL vs 1.030 (0.7601.700) GE/mL and 0.560 (0.1201.200) GE/mL in the comparison group, respectively (p0.00001); higher count of Enterobacteriaceae 2.700 (1.7003.300) GE/mL vs 0.950 (0.6601.120) GE/mL in the comparison group (p0.00001); higher count of Gardnerella/Prevotellabivia/Porphyromonas spp. 2.310 (0.9303.480) GE/mL vs 1.000 (0.0001.860) GE/mL (p=0.003); higher count of Peptostreptococcus spp. 0.195 (0.0001.560) GE/mL vs 0.000 (0.000-0.000) GE/mL (p=0.032); Eubacterium spp. 1.355 (0.1002.460) GE/mL vs 0.000 (0.0001.560) GE/mL (p=0.040).
Conclusion. Endometrial dysbiosis in patients with a uterus scar defect after cesarean section due to the possible effects of microorganisms can be considered one of the leading causes of the formation of a uterus scar defect in the postoperative period
A facility to Search for Hidden Particles (SHiP) at the CERN SPS
A new general purpose fixed target facility is proposed at the CERN SPS
accelerator which is aimed at exploring the domain of hidden particles and make
measurements with tau neutrinos. Hidden particles are predicted by a large
number of models beyond the Standard Model. The high intensity of the SPS
400~GeV beam allows probing a wide variety of models containing light
long-lived exotic particles with masses below (10)~GeV/c,
including very weakly interacting low-energy SUSY states. The experimental
programme of the proposed facility is capable of being extended in the future,
e.g. to include direct searches for Dark Matter and Lepton Flavour Violation.Comment: Technical Proposa
ĐĐĐ ĐĐĐĐĐĐĐĐ ĐĄĐĐĐĐ ĐĐĐĐĐŻ ĐĐĐ Đ Đ ĐĐЧĐĐĐ ĐŁ ĐĐĐŠĐĐĐĐąĐĐ ĐĄ ĐĐĐ ĐĐĐ«Đ ĐĐĐĐĐąĐĐĐĐ Đ ĐĄĐąĐĐĐąĐĐĐĐĐĐąĐĐąĐĐ ĐĐĐąĐĐĐĐ ĐĐ ĐĐąĐĐĐĐĐ ĐĐ -ĐĄĐĐĐйРĐĐĄĐĐĐĐĐ
Aim. Evaluation of proton MR spectroscopy in the diagnostics of non-alcoholic fatty liver disease.Materials and methods. 70 patients (40 men, 30 women) with non-alcoholic fatty liver disease were included in the study. Average age of patients was 42 ± 11 years. All patients were divided in two groups. The first group included patients with liver steĐ°thosis (n = 37). Patients with steatohepatitis detected by clinical data formed the second group (n = 33). All patients underwent MR spectroscopy for liver fat content evaluation in two time points (prescreening and after 6 months treatment).Results. MR spectroscopy showed fat content in patients with liver steatosis in the range from 7.5% to 58.4%, the median was 22.4% (lower and upper quartiles were 14.9% and 28.7%). After 6 months the liver fat content significantly decreased up to 1.5â43.7%, the median was 13.5% (the lower and upper quartiles were 5.54% and 18.9%). In patients with steatohepatitis the fat content calculated by MR spectroscopy ranged from 10.5% to 60%, the median was 28.8% (the lower and upper quartiles were 16.5% and 31.2%). There was no significant difference in fat content in this group after 6 months therapy (the median was 26.7%, the lower and upper quartiles were 14.2% and 28.7%, p = 0.22).Conclusion. Proton MR spectroscopy can be successfully used in patients with non-alcoholic fatty liver disease for liver fat content quantification in steatosis and steatohepatitis. MR spectroscopy can be discussed as a non-invasive biopsy alternative for dynamic evaluation during treatment.ĐŠĐ”Đ»Ń ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžŃ: ĐŸĐżŃĐ”ĐŽĐ”Đ»Đ”ĐœĐžĐ” ĐČĐŸĐ·ĐŒĐŸĐ¶ĐœĐŸŃŃĐž ĐžŃĐżĐŸĐ»ŃĐ·ĐŸĐČĐ°ĐœĐžŃ ĐżŃĐŸŃĐŸĐœĐœĐŸĐč ĐĐ -ŃпДĐșŃŃĐŸŃĐșĐŸĐżĐžĐž ĐČ ĐŽĐžĐ°ĐłĐœĐŸŃŃĐžĐșĐ” ĐœĐ”Đ°Đ»ĐșĐŸĐłĐŸĐ»ŃĐœĐŸĐč жОŃĐŸĐČĐŸĐč Đ±ĐŸĐ»Đ”Đ·ĐœĐž пДŃĐ”ĐœĐž(ĐĐĐĐĐ).ĐĐ°ŃĐ”ŃОал Đž ĐŒĐ”ŃĐŸĐŽŃ. Đ ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐ” бŃĐ»ĐŸ ĐČĐșĐ»ŃŃĐ”ĐœĐŸ 70 паŃĐžĐ”ĐœŃĐŸĐČ (40 ĐŒŃжŃĐžĐœ, 30 Đ¶Đ”ĐœŃĐžĐœ) Ń ĐĐĐĐĐ, ŃŃĐ”ĐŽĐœĐžĐč ĐČĐŸĐ·ŃĐ°ŃŃ ĐșĐŸŃĐŸŃŃŃ
ŃĐŸŃŃĐ°ĐČОл 42 ± 11 лДŃ. ĐĐ°ŃĐžĐ”ĐœŃŃ Đ±ŃлО ŃĐ°Đ·ĐŽĐ”Đ»Đ”ĐœŃ ĐœĐ° 2 ĐłŃŃппŃ. 1-Ń ĐłŃŃппа ĐČĐșĐ»ŃŃала Đ±ĐŸĐ»ŃĐœŃŃ
ŃĐŸ ŃŃДаŃĐŸĐ·ĐŸĐŒ пДŃĐ”ĐœĐž (37 ŃĐ”Đ»ĐŸĐČĐ”Đș). ĐĐŸ 2-Ń ĐłŃŃĐżĐżŃ ĐŸŃбОŃалОŃŃ ĐżĐ°ŃĐžĐ”ĐœŃŃ ŃĐŸ ŃŃДаŃĐŸĐłĐ”ĐżĐ°ŃĐžŃĐŸĐŒ, ĐČŃŃĐČĐ»Đ”ĐœĐœŃĐŒ ĐżĐŸ ĐŽĐ°ĐœĐœŃĐŒ ĐșĐ»ĐžĐœĐžŃĐ”ŃĐșĐžŃ
ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐč (33 паŃĐžĐ”ĐœŃĐ°). ĐŃĐ”ĐŒ паŃĐžĐ”ĐœŃĐ°ĐŒ ĐČŃĐżĐŸĐ»ĐœŃлаŃŃ ĐĐ -ŃпДĐșŃŃĐŸŃĐșĐŸĐżĐžŃ ĐŽĐ»Ń ĐŸĐżŃĐ”ĐŽĐ”Đ»Đ”ĐœĐžŃ ŃĐŸĐŽĐ”ŃĐ¶Đ°ĐœĐžŃ Đ¶ĐžŃĐ° ĐČ ĐżĐ”ŃĐ”ĐœĐž ĐČ ĐŽĐČŃŃ
ŃĐŸŃĐșĐ°Ń
: пДŃДЎ ĐČĐșĐ»ŃŃĐ”ĐœĐžĐ”ĐŒ ĐČ ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐ” Đž ŃĐżŃŃŃŃ 6 ĐŒĐ”Ń ĐœĐ° ŃĐŸĐœĐ” лДŃĐ”ĐœĐžŃ.РДзŃĐ»ŃŃĐ°ŃŃ. Đ 1-Đč ĐłŃŃппД паŃĐžĐ”ĐœŃĐŸĐČ ŃĐŸ ŃŃДаŃĐŸĐ·ĐŸĐŒ пДŃĐ”ĐœĐž ŃĐŸĐŽĐ”ŃĐ¶Đ°ĐœĐžĐ” жОŃĐ° ĐżĐŸ ĐŽĐ°ĐœĐœŃĐŒ ĐĐ -ŃпДĐșŃŃĐŸŃĐșĐŸĐżĐžĐž ĐœĐ°Ń
ĐŸĐŽĐžĐ»ĐŸŃŃ ĐČ ĐżŃДЎДлаŃ
ĐŸŃ 7,5 ĐŽĐŸ 58,4%, ĐŒĐ”ĐŽĐžĐ°ĐœĐ° ŃĐŸŃŃĐ°ĐČОла 22,4%, ĐœĐžĐ¶ĐœŃŃ Đž ĐČĐ”ŃŃ
ĐœŃŃ ĐșĐČĐ°ŃŃОлО â 14,9 Đž 28,7%. ĐŃĐž ŃДгОŃŃŃĐ°ŃОО ŃпДĐșŃŃĐŸĐČ ŃĐżŃŃŃŃ 6 ĐŒĐ”Ń ĐșĐŸĐœŃĐ”ĐœŃŃĐ°ŃĐžŃ Đ¶ĐžŃĐ° ĐČ ĐżĐ”ŃĐ”ĐœĐž Đ·ĐœĐ°ŃĐžĐŒĐŸ ŃĐœĐžĐ·ĐžĐ»Đ°ŃŃ, ŃĐŸŃŃĐ°ĐČĐ»Ńла ĐŸŃ 1,5 ĐŽĐŸ 43,7%, ĐŒĐ”ĐŽĐžĐ°ĐœĐ° â 13,5%, ĐœĐžĐ¶ĐœŃŃ Đž ĐČĐ”ŃŃ
ĐœŃŃ ĐșĐČĐ°ŃŃОлО â 5,54 Đž 18,9% (Ń = 0,015). ĐĐŸ 2-Đč ĐłŃŃппД паŃĐžĐ”ĐœŃĐŸĐČ ŃĐŸ ŃŃДаŃĐŸĐłĐ”ĐżĐ°ŃĐžŃĐŸĐŒ ŃĐŸĐŽĐ”ŃĐ¶Đ°ĐœĐžĐ” жОŃĐ° ĐżĐŸ ŃДзŃĐ»ŃŃĐ°ŃĐ°ĐŒ ĐĐ -ŃпДĐșŃŃĐŸŃĐșĐŸĐżĐžĐž ŃĐŸŃŃĐ°ĐČĐžĐ»ĐŸ ĐŸŃ 10,5 ĐŽĐŸ 60%, ĐŒĐ”ĐŽĐžĐ°ĐœĐ° â 28,8%, ĐœĐžĐ¶ĐœŃŃ Đž ĐČĐ”ŃŃ
ĐœŃŃ ĐșĐČĐ°ŃŃОлО â 16,5 Đž 31,2%. ĐŃĐž ĐżĐŸĐČŃĐŸŃĐœĐŸĐŒ ĐŸĐ±ŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐž ŃĐ”ŃДз 6 ĐŒĐ”Ń Đ»Đ”ŃĐ”ĐœĐžŃ ŃĐŸĐŽĐ”ŃĐ¶Đ°ĐœĐžĐ” жОŃĐ° ĐČ ĐżĐ”ŃĐ”ĐœĐž Ń ĐżĐ°ŃĐžĐ”ĐœŃĐŸĐČ ŃĐŸ ŃŃДаŃĐŸĐłĐ”ĐżĐ°ŃĐžŃĐŸĐŒ ĐŽĐŸŃŃĐŸĐČĐ”ŃĐœĐŸ ĐœĐ” ĐžĐ·ĐŒĐ”ĐœĐžĐ»ĐŸŃŃ: ĐŒĐ”ĐŽĐžĐ°ĐœĐ° 26,7%, ĐœĐžĐ¶ĐœŃŃ Đž ĐČĐ”ŃŃ
ĐœŃŃ ĐșĐČĐ°ŃŃОлО 14,2 Đž 28,7%(Ń = 0,22).ĐĐ°ĐșĐ»ŃŃĐ”ĐœĐžĐ”. ĐŃĐŸŃĐŸĐœĐœĐ°Ń ĐĐ -ŃпДĐșŃŃĐŸŃĐșĐŸĐżĐžŃ ĐŒĐŸĐ¶Đ”Ń ŃŃпДŃĐœĐŸ ĐżŃĐžĐŒĐ”ĐœŃŃŃŃŃ Ń ĐżĐ°ŃĐžĐ”ĐœŃĐŸĐČ Ń ĐĐĐĐĐ ĐŽĐ»Ń ĐșĐŸĐ»ĐžŃĐ”ŃŃĐČĐ”ĐœĐœĐŸĐč ĐŸŃĐ”ĐœĐșĐž ŃĐŸĐŽĐ”ŃĐ¶Đ°ĐœĐžŃ Đ¶ĐžŃĐ° ĐČ ĐżĐ”ŃĐ”ĐœĐž ĐżŃĐž ŃŃДаŃĐŸĐ·Đ” Đž ŃŃДаŃĐŸĐłĐ”ĐżĐ°ŃĐžŃĐ”. ĐĐ»Đ°ĐłĐŸĐŽĐ°ŃŃ ŃĐČĐŸĐ”Đč ĐœĐ”ĐžĐœĐČĐ°Đ·ĐžĐČĐœĐŸŃŃĐž ĐĐ -ŃпДĐșŃŃĐŸŃĐșĐŸĐżĐžŃ ĐŒĐŸĐ¶Đ”Ń ŃĐ°ŃŃĐŒĐ°ŃŃĐžĐČĐ°ŃŃŃŃ ĐșĐ°Đș Đ°Đ»ŃŃĐ”ŃĐœĐ°ŃĐžĐČĐ° Đ±ĐžĐŸĐżŃОО ĐżŃĐž ĐœĐ”ĐŸĐ±Ń
ĐŸĐŽĐžĐŒĐŸŃŃĐž ĐżĐŸĐČŃĐŸŃĐœŃŃ
ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžĐč ĐŽĐ»Ń ĐŸŃĐ”ĐœĐșĐž ĐŽĐžĐœĐ°ĐŒĐžĐșĐž ĐžĐ·ĐŒĐ”ĐœĐ”ĐœĐžĐč ĐœĐ° ŃĐŸĐœĐ” лДŃĐ”ĐœĐžŃ
Measurement of the CKM angle Îł from a combination of B±âDh± analyses
A combination of three LHCb measurements of the CKM angle Îł is presented. The decays B±âD K± and
B±âDϱ are used, where D denotes an admixture of D0 and D0 mesons, decaying into K+Kâ, Ï+Ïâ, K±Ïâ, K±ÏâϱÏâ, K0SÏ+Ïâ, or K0S K+Kâ ïŹnal states. All measurements use a dataset corresponding to 1.0 fbâ1 of integrated luminosity. Combining results from B±âD K± decays alone a best-ïŹt value of
Îł =72.0⊠is found, and conïŹdence intervals are set
Îł â [56.4,86.7]⊠at 68% CL,
Îł â [42.6,99.6]⊠at 95% CL.
The best-ïŹt value of Îł found from a combination of results from B±âDϱ decays alone, is Îł =18.9âŠ,
and the conïŹdence intervals
Îł â [7.4,99.2]⊠âȘ [167.9,176.4]⊠at 68% CL
are set, without constraint at 95% CL. The combination of results from B± â D K± and B± â Dϱ
decays gives a best-ïŹt value of Îł =72.6⊠and the conïŹdence intervals
Îł â [55.4,82.3]⊠at 68% CL,
Îł â [40.2,92.7]⊠at 95% CL
are set. All values are expressed modulo 180âŠ, and are obtained taking into account the effect of D0âD0
mixing
Measurement of the relative rate of prompt Ïc0, Ïc1 and Ïc2 production at âs=7TeV
Prompt production of charmonium Ïc0, Ïc1 and Ïc2 mesons is studied using proton-proton collisions at the LHC at a centre-of-mass energy of âs=7TeV. The Ïc mesons are identified through their decay to J/ÏÎł, with J/ÏâÎŒ+muâ using photons that converted in the detector. A data sample, corresponding to an integrated luminosity of 1.0fbâ1 collected by the LHCb detector, is used to measure the relative prompt production rate of Ïc1 and Ïc2 in the rapidity range 2.0<y<4.5 as a function of the J/Ï transverse momentum from 3 to 20 GeV/c. First evidence for Ïc0 meson production at a hadron collider is also presented
Study of DJ meson decays to D+Ïâ, D0Ï+ and Dâ+Ïâ final states in pp collisions
A study of D+Ïâ, D0Ï+ and Dâ+Ïâ final states is performed using pp collision data, corresponding to an integrated luminosity of 1.0 fbâ1, collected at a centre-of-mass energy of 7 TeV with the LHCb detector. The D1(2420)0 resonance is observed in the Dâ+Ïâ final state and the Dâ2(2460) resonance is observed in the D+Ïâ, D0Ï+ and Dâ+Ïâ final states. For both resonances, their properties and spin-parity assignments are obtained. In addition, two natural parity and two unnatural parity resonances are observed in the mass region between 2500 and 2800 MeV. Further structures in the region around 3000 MeV are observed in all the Dâ+Ïâ, D+Ïâ and D0Ï+ final states
Observation of an Excited Bc+ State
Using pp collision data corresponding to an integrated luminosity of 8.5 fb-1 recorded by the LHCb experiment at center-of-mass energies of s=7, 8, and 13 TeV, the observation of an excited Bc+ state in the Bc+Ï+Ï- invariant-mass spectrum is reported. The observed peak has a mass of 6841.2±0.6(stat)±0.1(syst)±0.8(Bc+) MeV/c2, where the last uncertainty is due to the limited knowledge of the Bc+ mass. It is consistent with expectations of the Bcâ(2S31)+ state reconstructed without the low-energy photon from the Bcâ(1S31)+âBc+Îł decay following Bcâ(2S31)+âBcâ(1S31)+Ï+Ï-. A second state is seen with a global (local) statistical significance of 2.2Ï (3.2Ï) and a mass of 6872.1±1.3(stat)±0.1(syst)±0.8(Bc+) MeV/c2, and is consistent with the Bc(2S10)+ state. These mass measurements are the most precise to date
Observation of associated production of a boson with a meson in the~forward region
A search for associated production of a boson with an open charm meson is
presented using a data sample, corresponding to an integrated luminosity of
of proton--proton collisions at a centre-of-mass energy
of 7\,TeV, collected by the LHCb experiment. %% Seven candidate events for
associated production of a boson with a meson and four candidate
events for a boson with a meson are observed with a combined
significance of 5.1standard deviations. The production cross-sections in the
forward region are measured to be where the first uncertainty is statistical and the
second systematic.Comment: 18 pages, 2 figure
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