Critical appraisal of systematic reviews of intervention studies in periodontology using AMSTAR 2 and ROBIS tools

Systematic reviews of intervention studies are used to support treatment recommendations. The aim of this study was to assess the methodological quality and risk of bias of systematic reviews of intervention studies in in the field of periodontology using AMSTAR 2 and ROBIS.Systematic reviews of randomized and non-randomized clinical trials, published between 2019 and 2020, were searched at MedLine, Embase, Web of Science, Scopus, Cochrane Library, LILACS with no language restrictions between October 2019 to October 2020. Additionally, grey literature and hand search was performed. Paired independent reviewers screened studies, extracted data and assessed the methodological quality and risk of bias through the AMSTAR 2 and ROBIS tools.One hundred twenty-seven reviews were included. According to AMSTAR 2, the methodological quality was mainly critically low (64.6%) and low (24.4%), followed by moderate (0.8%) and high (10.2%). According to ROBIS, 90.6% were at high risk of bias, followed by 7.1% low, and 2.4% unclear risk of bias. The risk of bias decreased with the increased in the impact factor of the journal.Current systematic reviews of intervention studies in periodontics were classified as low or critically low methodological quality and high risk of bias. Both tools led to similar conclusions. Better adherence to established reporting guidelines and stricter research practices when conducting systematic reviews are needed

Study of the B−→Λc+Λˉc−K−B^{-} \to \Lambda_{c}^{+} \bar{\Lambda}_{c}^{-} K^{-} decay

The decay $B^{-} \to \Lambda_{c}^{+} \bar{\Lambda}_{c}^{-} K^{-}$ is studied in proton-proton collisions at a center-of-mass energy of $\sqrt{s}=13$ TeV using data corresponding to an integrated luminosity of 5 $\mathrm{fb}^{-1}$ collected by the LHCb experiment. In the $\Lambda_{c}^+ K^{-}$ system, the $\Xi_{c}(2930)^{0}$ state observed at the BaBar and Belle experiments is resolved into two narrower states, $\Xi_{c}(2923)^{0}$ and $\Xi_{c}(2939)^{0}$, whose masses and widths are measured to be $$m(\Xi_{c}(2923)^{0}) = 2924.5 \pm 0.4 \pm 1.1 \,\mathrm{MeV}, \\ m(\Xi_{c}(2939)^{0}) = 2938.5 \pm 0.9 \pm 2.3 \,\mathrm{MeV}, \\ \Gamma(\Xi_{c}(2923)^{0}) = \phantom{000}4.8 \pm 0.9 \pm 1.5 \,\mathrm{MeV},\\ \Gamma(\Xi_{c}(2939)^{0}) = \phantom{00}11.0 \pm 1.9 \pm 7.5 \,\mathrm{MeV},$$ where the first uncertainties are statistical and the second systematic. The results are consistent with a previous LHCb measurement using a prompt $\Lambda_{c}^{+} K^{-}$ sample. Evidence of a new $\Xi_{c}(2880)^{0}$ state is found with a local significance of $3.8\,\sigma$, whose mass and width are measured to be $2881.8 \pm 3.1 \pm 8.5\,\mathrm{MeV}$ and $12.4 \pm 5.3 \pm 5.8 \,\mathrm{MeV}$, respectively. In addition, evidence of a new decay mode $\Xi_{c}(2790)^{0} \to \Lambda_{c}^{+} K^{-}$ is found with a significance of $3.7\,\sigma$. The relative branching fraction of $B^{-} \to \Lambda_{c}^{+} \bar{\Lambda}_{c}^{-} K^{-}$ with respect to the $B^{-} \to D^{+} D^{-} K^{-}$ decay is measured to be $2.36 \pm 0.11 \pm 0.22 \pm 0.25$, where the first uncertainty is statistical, the second systematic and the third originates from the branching fractions of charm hadron decays.Comment: All figures and tables, along with any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2022-028.html (LHCb public pages

Measurement of the ratios of branching fractions R(D∗)\mathcal{R}(D^{*}) and R(D0)\mathcal{R}(D^{0})

The ratios of branching fractions $\mathcal{R}(D^{*})\equiv\mathcal{B}(\bar{B}\to D^{*}\tau^{-}\bar{\nu}_{\tau})/\mathcal{B}(\bar{B}\to D^{*}\mu^{-}\bar{\nu}_{\mu})$ and $\mathcal{R}(D^{0})\equiv\mathcal{B}(B^{-}\to D^{0}\tau^{-}\bar{\nu}_{\tau})/\mathcal{B}(B^{-}\to D^{0}\mu^{-}\bar{\nu}_{\mu})$ are measured, assuming isospin symmetry, using a sample of proton-proton collision data corresponding to 3.0 fb${ }^{-1}$ of integrated luminosity recorded by the LHCb experiment during 2011 and 2012. The tau lepton is identified in the decay mode $\tau^{-}\to\mu^{-}\nu_{\tau}\bar{\nu}_{\mu}$. The measured values are $\mathcal{R}(D^{*})=0.281\pm0.018\pm0.024$ and $\mathcal{R}(D^{0})=0.441\pm0.060\pm0.066$, where the first uncertainty is statistical and the second is systematic. The correlation between these measurements is $\rho=-0.43$. Results are consistent with the current average of these quantities and are at a combined 1.9 standard deviations from the predictions based on lepton flavor universality in the Standard Model.Comment: All figures and tables, along with any supplementary material and additional information, are available at https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2022-039.html (LHCb public pages

ATLANTIC EPIPHYTES: a data set of vascular and non-vascular epiphyte plants and lichens from the Atlantic Forest

Epiphytes are hyper-diverse and one of the frequently undervalued life forms in plant surveys and biodiversity inventories. Epiphytes of the Atlantic Forest, one of the most endangered ecosystems in the world, have high endemism and radiated recently in the Pliocene. We aimed to (1) compile an extensive Atlantic Forest data set on vascular, non-vascular plants (including hemiepiphytes), and lichen epiphyte species occurrence and abundance; (2) describe the epiphyte distribution in the Atlantic Forest, in order to indicate future sampling efforts. Our work presents the first epiphyte data set with information on abundance and occurrence of epiphyte phorophyte species. All data compiled here come from three main sources provided by the authors: published sources (comprising peer-reviewed articles, books, and theses), unpublished data, and herbarium data. We compiled a data set composed of 2,095 species, from 89,270 holo/hemiepiphyte records, in the Atlantic Forest of Brazil, Argentina, Paraguay, and Uruguay, recorded from 1824 to early 2018. Most of the records were from qualitative data (occurrence only, 88%), well distributed throughout the Atlantic Forest. For quantitative records, the most common sampling method was individual trees (71%), followed by plot sampling (19%), and transect sampling (10%). Angiosperms (81%) were the most frequently registered group, and Bromeliaceae and Orchidaceae were the families with the greatest number of records (27,272 and 21,945, respectively). Ferns and Lycophytes presented fewer records than Angiosperms, and Polypodiaceae were the most recorded family, and more concentrated in the Southern and Southeastern regions. Data on non-vascular plants and lichens were scarce, with a few disjunct records concentrated in the Northeastern region of the Atlantic Forest. For all non-vascular plant records, Lejeuneaceae, a family of liverworts, was the most recorded family. We hope that our effort to organize scattered epiphyte data help advance the knowledge of epiphyte ecology, as well as our understanding of macroecological and biogeographical patterns in the Atlantic Forest. No copyright restrictions are associated with the data set. Please cite this Ecology Data Paper if the data are used in publication and teaching events. © 2019 The Authors. Ecology © 2019 The Ecological Society of Americ

Halitose autorrelatada: prevalência, fatores associados e acurácia diagnóstica

Submitted by Rafael Paula ([email protected]) on 2019-10-11T17:35:36Z No. of bitstreams: 1 Dissertação Sandro Faria.pdf: 1099459 bytes, checksum: e913633fe53b03dd6f3fc6ada83a59bc (MD5)Approved for entry into archive by Eliane Andrade ([email protected]) on 2019-10-14T15:03:21Z (GMT) No. of bitstreams: 1 Dissertação Sandro Faria.pdf: 1099459 bytes, checksum: e913633fe53b03dd6f3fc6ada83a59bc (MD5)Made available in DSpace on 2019-10-15T11:42:54Z (GMT). No. of bitstreams: 1 Dissertação Sandro Faria.pdf: 1099459 bytes, checksum: e913633fe53b03dd6f3fc6ada83a59bc (MD5) Previous issue date: 2019-06-28A halitose autorrelatada tem sido utilizada como uma ferramenta diagnóstica importante em estudos epidemiológicos por ser de fácil avaliação e refletir a percepção do indivíduo segundo sua condição. Entretanto, a prevalência e os fatores associados variam na literatura. O objetivo deste trabalho foi avaliar a prevalência de halitose autorrelatada e seus preditores associados, bem como determinar as estimativas de acurácia de medidas autorrelatadas com avaliação clínica da halitose. Foi realizado um estudo transversal com uma amostra de 5420 indivíduos que responderam, via e-mail, um conjunto de perguntas incluindo questões abertas e fechadas sobre dados socioeconômicos e demográficos, história médica e odontológica, hábitos de higiene bucal, parâmetros de saúde bucal e medidas de auto relato para halitose, sendo: medida 1 - “Coloque a palma da mão na frente da boca e sopre. Depois desse teste, você diria que tem mau hálito?”; medida 2 - “Você já foi diagnosticado pelo seu dentista com mau hálito?”; medida 3 - “Algum membro da sua família ou amigo já lhe disse que você tem mau hálito?”. Posteriormente, foi realizado um exame clínico em uma subamostra de 159 indivíduos para determinação clínica da halitose através do método organoléptico. Os preditores de halitose autorrelatada foram determinados por meio de análises univariadas e multivariadas. Estimativas de acurácia diagnóstica do autorrelato foram avaliadas na subamostra. A prevalência da halitose autorrelatada para a medida 1 foi de 14,6% (n = 792), para a medida 2 de 4,1% (n = 221) e para medida 3 de 33,2% (n = 1799). A halitose autorrelatada esteve associada principalmente a variáveis socioeconômicas (idade, sexo, escolaridade), parâmetros de saúde bucal (sangramento gengival, infecções gengivais, saburra lingual, avaliação geral da saúde bucal) e impactos nas atividades cotidianas (ambiente familiar ou social e relação íntima). Os valores de especificidade para medidas de halitose autorrelatadas foram determinados como sendo altos para halitose clínica (escore organoléptico 2) e forte (escore organoléptico 4). No geral, combinações de medidas de autorrelato melhoraram o AROC dos modelos preditivos multivariados. Pode-se concluir que as taxas de prevalência de halitose autorreferida podem variar de acordo com a medida de autorrelato, mas no geral podem ser consideradas moderadas. Estimativas de acurácia diagnóstica foram determinadas como úteis e com boa predição para indivíduos não doentes.Self-reported halitosis has been used as an important diagnostic tool in epidemiological studies that can be easily applied, demands less time and resources to be performed, and can reflect the individual's perception of their condition. However, its prevalence and associated factors vary in the literature. The aim of this study was to evaluate the prevalence of self-reported halitosis and its associated factors, as well as to determine accuracy estimates with clinical evaluation of halitosis. A cross sectional study was conducted in a sample of 5420 individuals who answered, via e mail, a set of closed questions that addressed socioeconomic and demographic data, medical and dental history, oral hygiene habits, parameters of oral health and self reported measures of halitosis, being: measure 1 - "Put the palm of the hand in front of the mouth and blow. After that test, would you say you have bad breath? "; measure 2 - "Have you ever been diagnosed with bad breath by your dentist "; measure 3 - "Has any member of your family or friend ever told you that you have bad breath?". Subsequently, a clinical examination was performed in a subsample of 159 individuals for the clinical diagnostic of halitosis through the organoleptic method. Predictors associated with self-reported halitosis were determined by means of univariate and multivariate analyzes. Accuracy estimates of self-report were evaluated in the subsample. Prevalence of self-reported halitosis for measure 1 was of 14.6% (n = 792), for measure 2 of 4.1% (n = 221) and for measure 3 of 33.2% (n = 1799). Self-reported halitosis was mainly associated with socioeconomic variables (age, gender, educational level), parameters of oral health, (gingival bleeding, gingival infections, tongue coating general evaluation of oral health) and impacts on daily activities (family or social environment and intimate relations). The specificity values for self-reported halitosis measures were determined to be high for clinical (organoleptic score ≥2) and strong (organoleptic score ≥4) halitosis. Overall, combinations of self-reported measures improved the AROC of multivariate predictive models. It can be concluded that prevalence rates of self-reported halitosis may vary according to the self-reported measure, but can be considerate moderate. Estimates of diagnostic accuracy were determined to be useful and with good prediction for non-diseased individuals

Measurement of prompt D+D^+ and Ds+D^+_{s} production in pPbp\mathrm{Pb} collisions at sNN=5.02 \sqrt {s_{\mathrm{NN}}}=5.02\,TeV

International audienceThe production of prompt $D^+$ and $D^+_{s}$ mesons is studied in proton-lead collisions at a centre-of-mass energy of $\sqrt {s_{\mathrm{NN}}}=5.02\,$TeV. The data sample corresponding to an integrated luminosity of $(1.58\pm0.02)\mathrm{nb}^{-1}$ is collected by the LHCb experiment at the LHC. The differential production cross-sections are measured using $D^+$ and $D^+_{s}$ candidates with transverse momentum in the range of $0<p_{\mathrm{T}} <14\,\mathrm{GeV}/c$ and rapidities in the ranges of $1.5<y^*<4.0$ and $-5.0<y^*<-2.5$ in the nucleon-nucleon centre-of-mass system. For both particles, the nuclear modification factor and the forward-backward production ratio are determined. These results are compared with theoretical models that include initial-state nuclear effects. In addition, measurements of the cross-section ratios between $D^+$, $D^+_{s}$ and $D^0$ mesons are presented, providing a baseline for studying the charm hadronization in lead-lead collisions at LHC energies

Associated production of prompt J/ψJ/\psi and Υ\mathit{\Upsilon} mesons in pppp collisions at s=13 TeV\sqrt{s}=13\,\mathrm{TeV}

International audienceThe associated production of prompt $J/\psi$ and $\mathit{\mathit{\Upsilon}}$ mesons in $pp$ collisions at a centre-of-mass energy of $\sqrt{s}=13\,\mathrm{TeV}$ is studied using LHCb data, corresponding to an integrated luminosity of $4\,\mathrm{fb}^{-1}$. The measurement is performed for $J/\psi$ ($\mathit{\Upsilon}$) mesons with a transverse momentum $p_{\mathrm{T}}<10\,(30)\,\mathrm{GeV}/c$ in the rapidity range $2.0<y<4.5$. In this kinematic range, the cross-section of the associated production of prompt $J/\psi$ and $\mathit{\Upsilon}(1S)$ mesons is measured to be $133 \pm 22 \pm 7 \pm 3 \, \mathrm{pb}$, with a significance of $7.9\,\sigma$, and that of prompt $J/\psi$ and $\mathit{\Upsilon}(2S)$ mesons to be $76\pm 21 \pm 4 \pm 7 \, \mathrm{pb}$, with a significance of $4.9\,\sigma$. The first uncertainty is statistical, the second systematic, and the third due to uncertainties on the used branching fractions. This is the first observation of the associated production of $J/\psi$ and $\mathit{\Upsilon}(1S)$ in proton-proton collisions. Differential cross-sections are measured as function of variables that are sensitive to kinematic correlations between the $J/\psi$ and $\mathit{\Upsilon}(1S)$ mesons. The effective cross-sections of the associated production of prompt $J/\psi$ and $\mathit{\Upsilon}$ mesons are obtained and found to be compatible with measurements using other particle productions

Test of lepton flavour universality using B0→D∗−τ+ντB^0 \to D^{*-}\tau^+\nu_{\tau} decays with hadronic τ\tau channels

International audienceThe branching fraction $\mathcal{B}(B^0 \to D^{*-}\tau^+\nu_{\tau})$ is measured relative to that of the normalisation mode $B^0 \to D^{*-}\pi^+\pi^-\pi^+$ using hadronic $\tau^+ \to \pi^+\pi^-\pi^+(\pi^0)\bar{\nu}_{\tau}$ decays in proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the LHCb experiment, corresponding to an integrated luminosity of 2 fb$^{-1}$. The measured ratio is $\mathcal{B}(B^0 \to D^{*-}\tau^+\nu_{\tau})/\mathcal{B}(B^0 \to D^{*-}\pi^+\pi^-\pi^+)= 1.70 \pm 0.10^{+0.11}_{-0.10}$, where the first uncertainty is statistical and the second is related to systematic effects. Using established branching fractions for the $B^0 \to D^{*-}\pi^+\pi^-\pi^+$ and $B^0 \to D^{*-} \mu^+\nu_\mu$ modes, the lepton universality test, $\mathcal{R}(D^{*-}) \equiv \mathcal{B}(B^0 \to D^{*-}\tau^+\nu_{\tau})/\mathcal{B}(B^0 \to D^{*-} \mu^+\nu_\mu)$ is calculated, $$\mathcal{R}(D^{*-}) = 0.247 \pm 0.015 \pm 0.015 \pm 0.012\, ,$$ where the third uncertainty is due to the uncertainties on the external branching fractions. This result is consistent with the Standard Model prediction and with previous measurements

Observation of Cabibbo-suppressed two-body hadronic decays and precision mass measurement of the Ωc0\Omega_{c}^{0} baryon

International audienceThe first observation of the singly Cabibbo-suppressed $\Omega_{c}^{0}\to\Omega^{-}K^{+}$ and $\Omega_{c}^{0}\to\Xi^{-}\pi^{+}$ decays is reported, using proton-proton collision data at a centre-of-mass energy of $13\,{\rm TeV}$, corresponding to an integrated luminosity of $5.4\,{\rm fb}^{-1}$, collected with the LHCb detector between 2016 and 2018. The branching fraction ratios are measured to be $\frac{\mathcal{B}(\Omega_{c}^{0}\to\Omega^{-}K^{+})}{\mathcal{B}(\Omega_{c}^{0}\to\Omega^{-}\pi^{+})}=0.0608\pm0.0051({\rm stat})\pm 0.0040({\rm syst})$, $\frac{\mathcal{B}(\Omega_{c}^{0}\to\Xi^{-}\pi^{+})}{\mathcal{B}(\Omega_{c}^{0}\to\Omega^{-}\pi^{+})}=0.1581\pm0.0087({\rm stat})\pm0.0043({\rm syst})\pm0.0016({\rm ext})$. In addition, using the $\Omega_{c}^{0}\to\Omega^{-}\pi^{+}$ decay channel, the $\Omega_{c}^{0}$ baryon mass is measured to be $M(\Omega_{c}^{0})=2695.28\pm0.07({\rm stat})\pm0.27({\rm syst})\pm0.30({\rm ext})\,{\rm MeV}/c^{2}$, improving the precision of the previous world average by a factor of four