97 research outputs found

    Daylight Saving Time and Spontaneous Deliveries: A Case–Control Study in Italy

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    (1) Background: Although the current literature shows that daylight saving time (DST) may play a role in human health and behavior, this topic has been poorly investigated with reference to Obstetrics. The aim of this case–control study was to evaluate whether DST may influence the number of spontaneous deliveries. (2) Methods: A low-risk pregnancy cohort with spontaneous onset of labor (n = 7415) was analyzed from a single Italian region for the period 2016–2018. Primary outcome was the number of spontaneous deliveries. Secondary outcomes were: gestational age at delivery, type and time of delivery, use of analgesia, birth weight, and 5-min Apgar at delivery. We compared the outcomes in the two weeks after DST (cases) to the two weeks before DST (controls). (3) Results: Data showed no significant difference between the number of deliveries occurring before and after DST (Chi-square = 0.546, p = 0.46). Vaginal deliveries at any gestational age showed no statistical difference between the two groups (Chi-square = 0.120, p = 0.73). There were no significant differences in the secondary outcomes, as well. (4) Conclusions: DST has neither a significant impact on the number of deliveries nor on the obstetric variables investigated by this study

    Partial external biliary diversion: A therapeutic alternative for Alagille syndrome. First case in Argentina

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    Antecedentes. El síndrome de Alagille es la principal forma sindrómica de colestasis intrahepática crónica caracterizada por la hipoplasia de la vía biliar intrahepática. Es un desorden multisistémico de herencia autosómica dominante con afectación de múltiples órganos. Suele ponerse de manifiesto en el período neonatal, entre el segundo y tercer mes de vida, presentándose desde casos subclínicos hasta grados graves de la enfermedad con el consecuente desarrollo de cirrosis hepática y posterior falla hepática, y está asociado con múltiples anomalías: defectos en los arcos vertebrales, facies típica, estenosis pulmonar, retardo mental e hipogonadismo. Objetivo. Presentar el primer caso clínico quirúrgico de derivación biliar externa parcial en Argentina, destacando la técnica quirúrgica y la mejoría en la calidad de vida, como alternativa a tener en cuenta en pacientes con este diagnóstico antes del desarrollo de cirrosis establecida. Resultados. Se ha demostrado que la derivación biliar externa parcial en algunos tipos de colestasis intrahepática detiene el proceso de fibrogénesis hepática, deteniendo a su vez la progresión de la enfermedad y evitando la necesidad de un trasplante cuando la cirrosis aún no se ha establecido. Discusión. Esta técnica quirúrgica permite mejorar la calidad de vida y la morbilidad asociada a la hipercolesterolemia en pacientes con síndrome de Alagille, postergando y tal vez evitando la necesidad de un trasplante hepático en el futuro.Background. Alagille's syndrome is the main syndromic chronic intrahepatic cholestasis characterized by hypoplasia of the intrahepatic bile ducts. It is a multisystem disorder of autosomal dominant inheritance with involvement of multiple organs. Usually it becomes apparent in the neonatal period, presenting as subclinical cases or severe degrees of the disease with the consequent development of liver cirrhosis and subsequent liver failure associated with multiple abnormalities: defects in the vertebral arches, typical facies, pulmonary stenosis, mental retardation and hypogonadism. Objective. To present the first case of partial external biliary diversion in Argentina, showing the surgical technique and the improvement in the quality of life, as an alternative to be considered in patients with Alagille's syndrome before the development of cirrhosis. Results. It has been shown that partial external biliary diversion can stop the process of liver fibrogenesis, halting the progression of the disease and avoiding the need for transplantation in some types of intrahepatic cholestasis when cirrhosis has not been established. Discussion. This surgical technique can improve the quality of life and morbidity associated with hypercholesterolemia in patients with Alagille's syndrome, delaying and maybe avoiding the need for liver transplantation.Fil: Rumbo, Carolina. Fundación Favaloro; ArgentinaFil: Sandi, Marcelo. Fundación Favaloro; ArgentinaFil: Padin, Juan Manuel. Fundación Favaloro; ArgentinaFil: Farinelli, Pablo. Fundación Favaloro; ArgentinaFil: Ramisch, Diego. Fundación Favaloro; ArgentinaFil: Barros Schelotto, Pablo. Fundación Favaloro; ArgentinaFil: Cabanne, Ana. Fundación Favaloro; ArgentinaFil: Garcia Herva, Dolores. Fundación Favaloro; ArgentinaFil: Trentadue, Julio. Fundación Favaloro; ArgentinaFil: Gondolesi, Gabriel Eduardo. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Fundación Favaloro; Argentin

    Solid pseudopapillary tumor of the páncreas

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    Antecedentes: la neoplasia sólida pseudopapilar del páncreas es una entidad rara, que típicamente se presenta en mujeres jóvenes. Suele presentar síntomas abdominales inespecíficos. Es un tumor maligno de bajo grado de malignidad.Objetivos: el objetivo del siguiente informe de serie de casos es presentar 9 casos tratados en un centro y realizar una revisión bibliográfica del tema.Material y métodos: estudio retrospectivo descriptivo de los casos con diagnóstico anatomopatológico de neoplasia sólida pseudopapilar en el Servicio de Cirugía General, desde febrero de 2013 hasta septiembre de 2019. Se contemplaron como variables: edad, sexo, localización del tumor, tratamiento quirúrgico realizado, tiempo operatorio, complicaciones, estancia hospitalaria y seguimiento alejado.Resultados: fueron 9 casos, todos de sexo femenino con media de edad de 30 años (rango 20 a 70 años). La localización más frecuente fue en cola de páncreas en 4 casos (45%). Todas las pacientes fueron sometidas a cirugía, con abordaje laparoscópico en el 60% de los casos (n = 5); la resección pancreática distal con preservación esplénica fue la conducta más utilizada (n = 6). Se constataron tres complicaciones, de las cuales dos fueron colecciones abdominales como consecuencia de una fístula pancreática que se abordaron por vía percutánea, y la restante fue un retardo del vaciamiento gástrico por lo cual la paciente requirió internación prolongada.Conclusión: la neoplasia sólida pseudopapilar pancreática es una enfermedad poco frecuente, maligna pero con bajo riesgo de malignidad. Presenta buena sobrevida cuando se somete a cirugía de carácter curativo; la laparoscopia es la vía de abordaje de elección en centros con experiencia.Background: Solid pseudopapillary tumor of the pancreas is a rare condition that affects young women. The most common symptom is unspecific abdominal pain. It is a malignant tumor of low malignant potential. Objective: The aim of this study is to report a case series of patients treated in a single center and perform a bibliographic review. Material and methods: We conducted a retrospective study of the cases with pathological diagnosis of solid pseudopapillary tumor of the pancreas treated in the Department of General Surgery between February 2013 and September 2019. The following variables were analyzed; age, sex, tumor location, surgical treatment, operative time, complications, length of hospital stay and long-term follow-up. Results: Nine patients were included; all of them were women with mean age of 30 years (range: 20 - 70 years). The most common location of the tumor was the tail of the pancreas (n = 4; 45%). Surgery was performed in all the cases; five cases underwent video-assisted laparoscopy and spleen-preserving distal pancreatectomy was the technique more commonly used (n = 6). Three complications were recorded: two abdominal collections due to biliary leaks were trated by percutaneous approach and the other patient presented delayed gastric emptying and required prolonged hospitalization. Conclusion: Solid pseudopapillary tumor pf the pancreas is a rare low-grade malignant neoplasm. The prognosis is favorable after surgery and laparoscopy is the preferred approach in centers with experience.Fil: Montes, Leonardo Ezequiel. Fundación Favaloro; ArgentinaFil: Alaniz, Jimena. Fundación Favaloro; ArgentinaFil: Dieguez Palacios, Andres. Fundación Favaloro; ArgentinaFil: Varela, Estanislao. Fundación Favaloro; ArgentinaFil: Lobos, Fernando D.. Fundación Favaloro; ArgentinaFil: Fernandez, Florencia M.. Fundación Favaloro; ArgentinaFil: Farinelli, Pablo. Fundación Favaloro; ArgentinaFil: Ramisch, Diego. Fundación Favaloro; ArgentinaFil: Barros Schelotto, Pablo. Fundación Favaloro; ArgentinaFil: Gondolesi, Gabriel Eduardo. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Houssay. Instituto de Medicina Traslacional, Trasplante y Bioingeniería. Fundación Favaloro. Instituto de Medicina Traslacional, Trasplante y Bioingeniería; Argentin

    Measurement of the (eta c)(1S) production cross-section in proton-proton collisions via the decay (eta c)(1S) -> p(p)over-bar

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    Observation of the B0 → ρ0ρ0 decay from an amplitude analysis of B0 → (π+π−)(π+π−) decays

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    Proton–proton collision data recorded in 2011 and 2012 by the LHCb experiment, corresponding to an integrated luminosity of 3.0 fb−1 , are analysed to search for the charmless B0→ρ0ρ0 decay. More than 600 B0→(π+π−)(π+π−) signal decays are selected and used to perform an amplitude analysis, under the assumption of no CP violation in the decay, from which the B0→ρ0ρ0 decay is observed for the first time with 7.1 standard deviations significance. The fraction of B0→ρ0ρ0 decays yielding a longitudinally polarised final state is measured to be fL=0.745−0.058+0.048(stat)±0.034(syst) . The B0→ρ0ρ0 branching fraction, using the B0→ϕK⁎(892)0 decay as reference, is also reported as B(B0→ρ0ρ0)=(0.94±0.17(stat)±0.09(syst)±0.06(BF))×10−6

    Studies of beauty baryon decays to D0ph− and Λ+ch− final states

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    Search for the lepton flavour violating decay tau(-) -> mu(-)mu(+)mu(-)

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    A search for the lepton flavour violating decay τμμ+μ\tau^-\rightarrow\mu^-\mu^+\mu^- is performed with the LHCb experiment. The data sample corresponds to an integrated luminosity of 1.0 fb1^{−1} of proton-proton collisions at a centre-of-mass energy of 7 TeV and 2.0 fb1^{−1} at 8 TeV. No evidence is found for a signal, and a limit is set at 90% confidence level on the branching fraction, B(τμμ+μ)<4.6×108\mathcal{B}(\tau^-\rightarrow\mu^-\mu^+\mu^-)<4.6\times10^{−8}.A search for the lepton flavour violating decay τ^{−} → μ^{−} μ+^{+} μ^{−} is performed with the LHCb experiment. The data sample corresponds to an integrated luminosity of 1.0 fb1^{−1} of proton-proton collisions at a centre-of-mass energy of 7 TeV and 2.0 fb1^{−1} at 8 TeV. No evidence is found for a signal, and a limit is set at 90% confidence level on the branching fraction, B(τμμ+μ)<4.6×108 \mathrm{\mathcal{B}}\left({\tau}^{-}\to {\mu}^{-}{\mu}^{+}{\mu}^{-}\right)<4.6\times {10}^{-8} .A search for the lepton flavour violating decay τμμ+μ\tau^-\to \mu^-\mu^+\mu^- is performed with the LHCb experiment. The data sample corresponds to an integrated luminosity of 1.0fb11.0\mathrm{\,fb}^{-1} of proton-proton collisions at a centre-of-mass energy of 7TeV7\mathrm{\,Te\kern -0.1em V} and 2.0fb12.0\mathrm{\,fb}^{-1} at 8TeV8\mathrm{\,Te\kern -0.1em V}. No evidence is found for a signal, and a limit is set at 90%90\% confidence level on the branching fraction, B(τμμ+μ)<4.6×108\mathcal{B}(\tau^-\to \mu^-\mu^+\mu^-) < 4.6 \times 10^{-8}

    Angular analysis of the B-0 -&gt; K*(0) e(+) e(-) decay in the low-q(2) region

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    An angular analysis of the B0K0e+eB^0 \rightarrow K^{*0} e^+ e^- decay is performed using a data sample, corresponding to an integrated luminosity of 3.0 {\mbox{fb}^{-1}}, collected by the LHCb experiment in pppp collisions at centre-of-mass energies of 7 and 8 TeV during 2011 and 2012. For the first time several observables are measured in the dielectron mass squared (q2q^2) interval between 0.002 and 1.120GeV2 ⁣/c4{\mathrm{\,Ge\kern -0.1em V^2\!/}c^4}. The angular observables FLF_{\mathrm{L}} and ATReA_{\mathrm{T}}^{\mathrm{Re}} which are related to the K0K^{*0} polarisation and to the lepton forward-backward asymmetry, are measured to be FL=0.16±0.06±0.03F_{\mathrm{L}}= 0.16 \pm 0.06 \pm0.03 and ATRe=0.10±0.18±0.05A_{\mathrm{T}}^{\mathrm{Re}} = 0.10 \pm 0.18 \pm 0.05, where the first uncertainty is statistical and the second systematic. The angular observables AT(2)A_{\mathrm{T}}^{(2)} and ATImA_{\mathrm{T}}^{\mathrm{Im}} which are sensitive to the photon polarisation in this q2q^2 range, are found to be AT(2)=0.23±0.23±0.05A_{\mathrm{T}}^{(2)} = -0.23 \pm 0.23 \pm 0.05 and ATIm=0.14±0.22±0.05A_{\mathrm{T}}^{\mathrm{Im}} =0.14 \pm 0.22 \pm 0.05. The results are consistent with Standard Model predictions.An angular analysis of the B0^{0} → K^{*}^{0} e+^{+} e^{−} decay is performed using a data sample, corresponding to an integrated luminosity of 3.0 fb1^{−1}, collected by the LHCb experiment in pp collisions at centre-of-mass energies of 7 and 8 TeV during 2011 and 2012. For the first time several observables are measured in the dielectron mass squared (q2^{2}) interval between 0.002 and 1.120 GeV2^{2} /c4^{4}. The angular observables FL_{L} and ATRe_{T}^{Re} which are related to the K^{*}^{0} polarisation and to the lepton forward-backward asymmetry, are measured to be FL_{L} = 0.16 ± 0.06 ± 0.03 and ATRe_{T}^{Re}  = 0.10 ± 0.18 ± 0.05, where the first uncertainty is statistical and the second systematic. The angular observables AT(2)_{T}^{(2)} and ATIm_{T}^{Im} which are sensitive to the photon polarisation in this q2^{2} range, are found to be AT(2)_{T}^{(2)}  = − 0.23 ± 0.23 ± 0.05 and ATIm_{T}^{Im}  = 0.14 ± 0.22 ± 0.05. The results are consistent with Standard Model predictions.An angular analysis of the B0K0e+eB^0 \rightarrow K^{*0} e^+ e^- decay is performed using a data sample, corresponding to an integrated luminosity of 3.0 {\mbox{fb}^{-1}}, collected by the LHCb experiment in pppp collisions at centre-of-mass energies of 7 and 8 TeV during 2011 and 2012. For the first time several observables are measured in the dielectron mass squared (q2q^2) interval between 0.002 and 1.120GeV2 ⁣/c4{\mathrm{\,Ge\kern -0.1em V^2\!/}c^4}. The angular observables FLF_{\mathrm{L}} and ATReA_{\mathrm{T}}^{\mathrm{Re}} which are related to the K0K^{*0} polarisation and to the lepton forward-backward asymmetry, are measured to be FL=0.16±0.06±0.03F_{\mathrm{L}}= 0.16 \pm 0.06 \pm0.03 and ATRe=0.10±0.18±0.05A_{\mathrm{T}}^{\mathrm{Re}} = 0.10 \pm 0.18 \pm 0.05, where the first uncertainty is statistical and the second systematic. The angular observables AT(2)A_{\mathrm{T}}^{(2)} and ATImA_{\mathrm{T}}^{\mathrm{Im}} which are sensitive to the photon polarisation in this q2q^2 range, are found to be AT(2)=0.23±0.23±0.05A_{\mathrm{T}}^{(2)} = -0.23 \pm 0.23 \pm 0.05 and ATIm=0.14±0.22±0.05A_{\mathrm{T}}^{\mathrm{Im}} =0.14 \pm 0.22 \pm 0.05. The results are consistent with Standard Model predictions

    Search for CP violation using T-odd correlations in D-0 -&gt; K+K-pi(+)pi(-) decays

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    A search for CPCP violation using TT-odd correlations is performed using the four-body D0K+Kπ+πD^0 \to K^+K^-\pi^+\pi^- decay, selected from semileptonic BB decays. The data sample corresponds to integrated luminosities of 1.0fb11.0\,\text{fb}^{-1} and 2.0fb12.0\,\text{fb}^{-1} recorded at the centre-of-mass energies of 7 TeV and 8 TeV, respectively. The CPCP-violating asymmetry aCPT-odda_{CP}^{T\text{-odd}} is measured to be (0.18±0.29(stat)±0.04(syst))%(0.18\pm 0.29\text{(stat)}\pm 0.04\text{(syst)})\%. Searches for CPCP violation in different regions of phase space of the four-body decay, and as a function of the D0D^0 decay time, are also presented. No significant deviation from the CPCP conservation hypothesis is found

    Measurement of CP asymmetry in B-s(0) -&gt; D-s(-/+) K--/+ decays

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    We report on measurements of the time-dependent CP violating observables in Bs0DsK±B^0_s\rightarrow D^{\mp}_s K^{\pm} decays using a dataset corresponding to 1.0 fb1^{-1} of pp collisions recorded with the LHCb detector. We find the CP violating observables Cf=0.53±0.25±0.04C_f=0.53\pm0.25\pm0.04, AfΔΓ=0.37±0.42±0.20A^{\Delta\Gamma}_f=0.37\pm0.42\pm0.20, AfˉΔΓ=0.20±0.41±0.20A^{\Delta\Gamma}_{\bar{f}}=0.20\pm0.41\pm0.20, Sf=1.09±0.33±0.08S_f=-1.09\pm0.33\pm0.08, Sfˉ=0.36±0.34±0.08S_{\bar{f}}=-0.36\pm0.34\pm0.08, where the uncertainties are statistical and systematic, respectively. We use these observables to make the first measurement of the CKM angle γ\gamma in Bs0DsK±B^0_s\rightarrow D^{\mp}_s K^{\pm} decays, finding γ\gamma = (11543+28_{-43}^{+28})^\circ modulo 180^\circ at 68% CL, where the error contains both statistical and systematic uncertainties.We report on measurements of the time-dependent CP violating observables in Bs0_{s}^{0}  → Ds_{s}^{∓} K±^{±} decays using a dataset corresponding to 1.0 fb1^{−1} of pp collisions recorded with the LHCb detector. We find the CP violating observables Cf_{f} = 0.53±0.25±0.04, AfΔΓ_{f}^{ΔΓ}  = 0.37 ± 0.42 ± 0.20, AfΔΓ=0.20±0.41±0.20 {A}_{\overline{f}}^{\varDelta \varGamma }=0.20\pm 0.41\pm 0.20 , Sf_{f} = −1.09±0.33±0.08, Sf=0.36±0.34±0.08 {S}_{\overline{f}}=-0.36\pm 0.34\pm 0.08 , where the uncertainties are statistical and systematic, respectively. Using these observables together with a recent measurement of the Bs0_{s}^{0} mixing phase −2βs_{s} leads to the first extraction of the CKM angle γ from Bs0_{s}^{0}  → Ds_{s}^{∓} K±^{±} decays, finding γ = (11543+28_{− 43}^{+ 28} )° modulo 180° at 68% CL, where the error contains both statistical and systematic uncertainties.We report on measurements of the time-dependent CP violating observables in Bs0DsK±B^0_s\rightarrow D^{\mp}_s K^{\pm} decays using a dataset corresponding to 1.0 fb1^{-1} of pp collisions recorded with the LHCb detector. We find the CP violating observables Cf=0.53±0.25±0.04C_f=0.53\pm0.25\pm0.04, AfΔΓ=0.37±0.42±0.20A^{\Delta\Gamma}_f=0.37\pm0.42\pm0.20, AfˉΔΓ=0.20±0.41±0.20A^{\Delta\Gamma}_{\bar{f}}=0.20\pm0.41\pm0.20, Sf=1.09±0.33±0.08S_f=-1.09\pm0.33\pm0.08, Sfˉ=0.36±0.34±0.08S_{\bar{f}}=-0.36\pm0.34\pm0.08, where the uncertainties are statistical and systematic, respectively. Using these observables together with a recent measurement of the Bs0B^0_s mixing phase 2βs-2\beta_s leads to the first extraction of the CKM angle γ\gamma from Bs0DsK±B^0_s \rightarrow D^{\mp}_s K^{\pm} decays, finding γ\gamma = (11543+28_{-43}^{+28})^\circ modulo 180^\circ at 68% CL, where the error contains both statistical and systematic uncertainties
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