Helium identification with LHCb

The identification of helium nuclei at LHCb is achieved using a method based on measurements of ionisation losses in the silicon sensors and timing measurements in the Outer Tracker drift tubes. The background from photon conversions is reduced using the RICH detectors and an isolation requirement. The method is developed using pp collision data at √(s) = 13 TeV recorded by the LHCb experiment in the years 2016 to 2018, corresponding to an integrated luminosity of 5.5 fb-1. A total of around 105 helium and antihelium candidates are identified with negligible background contamination. The helium identification efficiency is estimated to be approximately 50% with a corresponding background rejection rate of up to O(10^12). These results demonstrate the feasibility of a rich programme of measurements of QCD and astrophysics interest involving light nuclei

Curvature-bias corrections using a pseudomass method

Momentum measurements for very high momentum charged particles, such as muons from electroweak vector boson decays, are particularly susceptible to charge-dependent curvature biases that arise from misalignments of tracking detectors. Low momentum charged particles used in alignment procedures have limited sensitivity to coherent displacements of such detectors, and therefore are unable to fully constrain these misalignments to the precision necessary for studies of electroweak physics. Additional approaches are therefore required to understand and correct for these effects. In this paper the curvature biases present at the LHCb detector are studied using the pseudomass method in proton-proton collision data recorded at centre of mass energy √(s)=13 TeV during 2016, 2017 and 2018. The biases are determined using Z→μ + μ - decays in intervals defined by the data-taking period, magnet polarity and muon direction. Correcting for these biases, which are typically at the 10-4 GeV-1 level, improves the Z→μ + μ - mass resolution by roughly 18% and eliminates several pathological trends in the kinematic-dependence of the mean dimuon invariant mass

Momentum scale calibration of the LHCb spectrometer

For accurate determination of particle masses accurate knowledge of the momentum scale of the detectors is crucial. The procedure used to calibrate the momentum scale of the LHCb spectrometer is described and illustrated using the performance obtained with an integrated luminosity of 1.6 fb-1 collected during 2016 in pp running. The procedure uses large samples of J/ψ → μ + μ - and B+ → J/ψ K + decays and leads to a relative accuracy of 3 × 10-4 on the momentum scale

Intoxicação em suínos pela ingestão de sementes de Aeschynomene indica (Leg.Papilionoideae) Poisoning in swine from the ingestion of Aeschynomene indica (Leg.Papilionoideae) seeds

Relata-se um surto espontâneo de intoxicação em suínos pela ingestão de sementes de Aeschynomene indica e a reprodução da doença nessa espécie animal. O surto espontâneo ocorreu numa propriedade de criação de suínos localizada na região central do Rio Grande do Sul. Nessa propriedade havia 100 suínos (20 matrizes e 80 suínos jovens de várias categorias). Os suínos eram alimentados com uma ração feita na propriedade pela mistura de 50% farelo de milho, 25% de farelo de soja, 5% de um suplemento vitamínico-mineral de origem comercial e 20% quirera de arroz contaminada por 40% de sementes de A. indica. Embora aparentemente todos os suínos tenham recebido a mesma ração, apenas os suínos de 45 dias de idade foram afetados; as taxas de morbidade, mortalidade e letalidade foram respectivamente 25%-40%, 8,5%-20% e 25%-66%. Os sinais clínicos apareceram cerca de 24 horas após o início da administração da ração contendo sementes de A. indica e incluíam vários graus de incoordenação no andar, quedas, decúbito esternal com membros pélvicos posicionados afastados entre si, decúbito lateral e morte. Não foi possível determinar quantos suínos se recuperaram e quanto tempo levou a recuperação. Um suíno foi submetido à eutanásia e necropsiado na propriedade. A doença foi reproduzida em 5 suínos jovens (A-E) alimentados com uma ração contendo 10% (Suíno A), 15% (Suíno B) e 20% (Suínos C-E) de sementes de A. indica e em um suíno mais velho (Suíno F) que recebeu uma ração com 16,5% de sementes de A. indica. Os sinais clínicos foram semelhantes aos observados nos suínos do surto espontâneo. Os Suínos A, B e F foram submetidos à eutanásia e os Suínos C-E morreram de uma doença aguda respectivamente 16, 21 e 24 horas após o início do experimento. Os achados de necropsia incluíam acentuada hiperemia das leptomeninges em todos os suínos, grandes quantidades de sementes de A. indica no estômago e avermelhamento transmural da parede do intestino e conteúdo intestinal sanguinolento nos Suínos C-E. Um hematoma foi observado no pulmão do Suíno C. Os achados histopatológicos no encéfalo dos suínos alimentados com as maiores concentrações (20%) de sementes de A. indica (C-E) consistiram em áreas focais e simétricas de congestão, edema, hemorragia e tumefação do endotélio vascular em diversos núcleos e no córtex telencefálico. Nos Suínos A e B, que receberam menores concentrações das sementes de A. indica, e no Suíno F, caso espontâneo da doença, as alterações histológicas no encéfalo consistiam de áreas bem definidas de malacia focal simétrica; nessas áreas a neurópila normal era obliterada por numerosos macrófagos espumosos dispostos em estreita aposição, astrocitose e capilares com endotélios tumefeitos. Os focos de malacia focal simétrica em suínos intoxicados com sementes de A. indica afetavam os núcleos cerebelares e vestibulares, a substância negra, o putâmen e os núcleos mesencefálicos, oculomotor e núcleo vermelho. Esses dados indicam que a ingestão de sementes de A. indica é responsável por essa condição neurológica, que a doença pode ser fatal e que parece afetar igualmente suínos jovens e adultos. O desenlace clínico e as alterações patológicas são dependentes da dose e as lesões encefálicas progridem de danos vasculares a edema vasogênico, hemorragia e malacia.<br>A spontaneous outbreak of a neurological disease in swine caused by the ingestion of Aeschynomene indica seeds and the reproduction of the disease in the same animal species are reported. The natural outbreak occurred in a pig-raising facility in the central region of the state of Rio Grande do Sul, Brazil. On the premises there were 100 pigs (20 breeding sows and 80 young weaned pigs from several categories) that were fed a ration made by mixing 50% of corn bran, 25% of soybean bran, 5% of a commercial mix of vitamins and minerals, and 20% of broken rice contaminated with 40% of A. indica seeds. Although all pigs apparently ingested the same ration, only 45-day-old pigs were affected; morbidity, mortality and lethality rates were respectively 25%-40%, 8.5%-20%; and 25%-66%. Clinical signs appeared 24 hours after the beginning of feeding of A. indica seeds contaminated ration and included variable degrees of incoordinated gait, falls, sternal recumbency with the hind limbs in a wide base stance, lateral recumbency and death. It was not possible to ascertain how many pigs recovered nor the time frame of recovery. One pig was euthanatized and necropsied in the premises. The poisoning was reproduced in 5 young pigs (A-E) which were fed a ration containing 10% (Pig A), 15% (Pig B) and 20% (Pigs C-E) of A. indica seeds, and in one older pig (Pig F) which was fed a ration with 16.5% of A. indica seeds. Pigs A, B and F were euthanatized and Pigs C-E died of an acute disease respectively 16, 21 and 24 hours after the beginning of the experiment. Clinical signs were similar to those observed in pigs of the spontaneous outbreak. Necropsy findings included marked hyperemia of the encephalic leptomeninges of all pigs; there were large amounts of A. indica seeds in the stomach and reddening of the intestinal wall and bloody intestinal content in Pigs C-E. A hematoma was observed in the lungs of Pig C. The histopathological findings in the brain of pigs fed rations with larger concentrations (20%) of A. indica seeds (C-E) included congestion, edema and hemorrhage and swollen vascular endothelia with focal symmetrical distribution in several brain nuclei and in the telencephalic cortex. In Pigs A and B, and in Pig F, the case which received the lower dosage of the seeds of A. indica, and in the pig from the spontaneous outbreak, histopathological changes in the brain consisted of discrete focal symmetrical areas of malacia in which closely packed Gitter cells and astrocytosis, and capillaries with swollen endothelium obliterated the normal neuropil. The symmetrical malacic foci caused by the ingestion of A. indica seeds in swine affected cerebellar and vestibular nuclei, putamen, and the mesencephalic oculomotor and red nuclei. This indicates that the A. indica seeds ingestion was responsible for the neurological condition, that it may be fatal and seems to affect equally young and older swine. The clinical outcome and pathological changes were dose-dependent, and the brain lesions progressed from damaged blood vessels to vasogenic edema, hemorrhage and malacia

Measurement of the D∗D^* longitudinal polarization in B0→D∗−τ+ντB^0 \to D^{* -}\tau^+\nu_{\tau} decays

The longitudinal polarization fraction of the $D^*$ meson is measured in $B^0 \to D^{* -}\tau^+\nu_{\tau}$ decays, where the $\tau$ lepton decays to three charged pions and a neutrino, using proton-proton collision data collected by the LHCb experiment at center-of-mass energies of 7, 8 and 13 TeV and corresponding to an integrated luminosity of 5 fb$^{-1}$. The $D^*$ polarization fraction $F_L^{D^*}$ is measured in two $q^2$ regions, below and above 7 GeV$^2$/c$^4$, where $q^2$ is defined as the squared invariant mass of the $\tau\nu_{\tau}$ system. The $F_L^{D^*}$ values are measured to be $0.51 \pm 0.07 \pm 0.03$ and $0.35 \pm 0.08 \pm 0.02$ for the lower and higher $q^2$ regions, respectively. The first uncertainties are statistical and the second systematic. The average value over the whole $q^2$ range is: $$F_L^{D^*} = 0.43 \pm 0.06 \pm 0.03.$$ These results are compatible with the Standard Model predictions.The longitudinal polarization fraction of the $D^{*}$ meson is measured in $B^0\to D^{*-}\tau^{+}\nu_{\tau}$ decays, where the $\tau$ lepton decays to three charged pions and a neutrino, using proton-proton collision data collected by the LHCb experiment at center-of-mass energies of 7, 8 and 13 TeV and corresponding to an integrated luminosity of 5 fb$^{-1}$. The $D^{*}$ polarization fraction $F_{L}^{D^{*}}$ is measured in two $q^{2}$ regions, below and above 7 GeV$^{2}/c^{4}$, where $q^{2}$ is defined as the squared invariant mass of the $\tau\nu_{\tau}$ system. The $F_{L}^{D^{*}}$ values are measured to be $0.51 \pm 0.07 \pm 0.03$ and $0.35 \pm 0.08 \pm 0.02$ for the lower and higher $q^{2}$ regions, respectively. The first uncertainties are statistical and the second systematic. The average value over the whole $q^{2}$ range is: $$F_{L}^{D^{*}} = 0.43 \pm 0.06 \pm 0.03.$$ These results are compatible with the Standard Model predictions

Measurement of the D∗D^{*} longitudinal polarization in B0→D∗−τ+ντB^0\to D^{*-}\tau^{+}\nu_{\tau} decays

International audienceThe longitudinal polarization fraction of the $D^{*}$ meson is measured in $B^0\to D^{*-}\tau^{+}\nu_{\tau}$ decays, where the $\tau$ lepton decays to three charged pions and a neutrino, using proton-proton collision data collected by the LHCb experiment at center-of-mass energies of 7, 8 and 13 TeV and corresponding to an integrated luminosity of 5 fb$^{-1}$. The $D^{*}$ polarization fraction $F_{L}^{D^{*}}$ is measured in two $q^{2}$ regions, below and above 7 GeV$^{2}/c^{4}$, where $q^{2}$ is defined as the squared invariant mass of the $\tau\nu_{\tau}$ system. The $F_{L}^{D^{*}}$ values are measured to be $0.51 \pm 0.07 \pm 0.03$ and $0.35 \pm 0.08 \pm 0.02$ for the lower and higher $q^{2}$ regions, respectively. The first uncertainties are statistical and the second systematic. The average value over the whole $q^{2}$ range is: $$F_{L}^{D^{*}} = 0.43 \pm 0.06 \pm 0.03.$$ These results are compatible with the Standard Model predictions

Measurement of the D∗D^{*} longitudinal polarization in B0→D∗−τ+ντB^0\to D^{*-}\tau^{+}\nu_{\tau} decays

International audienceThe longitudinal polarization fraction of the $D^{*}$ meson is measured in $B^0\to D^{*-}\tau^{+}\nu_{\tau}$ decays, where the $\tau$ lepton decays to three charged pions and a neutrino, using proton-proton collision data collected by the LHCb experiment at center-of-mass energies of 7, 8 and 13 TeV and corresponding to an integrated luminosity of 5 fb$^{-1}$. The $D^{*}$ polarization fraction $F_{L}^{D^{*}}$ is measured in two $q^{2}$ regions, below and above 7 GeV$^{2}/c^{4}$, where $q^{2}$ is defined as the squared invariant mass of the $\tau\nu_{\tau}$ system. The $F_{L}^{D^{*}}$ values are measured to be $0.51 \pm 0.07 \pm 0.03$ and $0.35 \pm 0.08 \pm 0.02$ for the lower and higher $q^{2}$ regions, respectively. The first uncertainties are statistical and the second systematic. The average value over the whole $q^{2}$ range is: $$F_{L}^{D^{*}} = 0.43 \pm 0.06 \pm 0.03.$$ These results are compatible with the Standard Model predictions

Measurement of the D∗D^{*} longitudinal polarization in B0→D∗−τ+ντB^0\to D^{*-}\tau^{+}\nu_{\tau} decays

International audienceThe longitudinal polarization fraction of the $D^{*}$ meson is measured in $B^0\to D^{*-}\tau^{+}\nu_{\tau}$ decays, where the $\tau$ lepton decays to three charged pions and a neutrino, using proton-proton collision data collected by the LHCb experiment at center-of-mass energies of 7, 8 and 13 TeV and corresponding to an integrated luminosity of 5 fb$^{-1}$. The $D^{*}$ polarization fraction $F_{L}^{D^{*}}$ is measured in two $q^{2}$ regions, below and above 7 GeV$^{2}/c^{4}$, where $q^{2}$ is defined as the squared invariant mass of the $\tau\nu_{\tau}$ system. The $F_{L}^{D^{*}}$ values are measured to be $0.51 \pm 0.07 \pm 0.03$ and $0.35 \pm 0.08 \pm 0.02$ for the lower and higher $q^{2}$ regions, respectively. The first uncertainties are statistical and the second systematic. The average value over the whole $q^{2}$ range is: $$F_{L}^{D^{*}} = 0.43 \pm 0.06 \pm 0.03.$$ These results are compatible with the Standard Model predictions