Fossombronia bracchia Cargill (Fossombroniaceae, Marchantiophyta), a new species from Western Australia

The new species, Fossombronia bracchia, from Lesueur National Park, an area of high vascular plant endemism and species richness in southwestern Western Australia, is described and illustrated; a distribution map is provided. The new species has strong morphological similarities to the South African species F. tumida

The Migration of Australians to Bali, Indonesia: More than Retirees and Surfers

The factors underpinning the migration of Australian residents to Bali, Indonesia, and the demographic characteristics of the Australian expatriate population in Bali are examined. It is argued that in undertaking a move to Bali, Australian expatriates are employing a deliberate strategy to utilise their existing financial resources and social networks to gain a lifestyle they perceive would not be available to them if they were to remain in Australia. However, it is also argued that there is considerable diversity in the factors underpinning migration decisions. Through a survey of 236 Australians living in Bali, it was found that a complex of place-based and non-place-based factors influenced migration decisions. It was also found that some factors underpinning migration were broadly associated with phase in the life course. While the survey identified only a minor overrepresentation of Australian retirees living in Bali, given the factors that were identified as underpinning migration to Bali, and with the large baby boomer population nearing retirement, it is probable that as Australia's population ages, there will be further growth in the number and proportional share of older Australians living in Bali

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

Força de preensão manual de atletas tenistas avaliada por diferentes recomendações de teste

A avaliação da força de preensão manual (FPM) em tenistas competitivos deve ser realizada devido à assimetria que o jogador pode desenvolver. Para avaliar a FPM, profissionais utilizam dois protocolos diferentes (das Sociedades Americana e Europeia). Os objetivos deste estudo foram comparar a FPM usando a técnica do European Test of Physical Fitness Handbook (Eurofit) e da American Society of Hand Therapists (ASHT), bem como verificar a FPM entre o lado dominante/contralateral e comparar a FPM entre as idades em atletas de tênis da categoria infanto-juvenil. Participaram do estudo 137 tenistas do gênero masculino e 45 do feminino, todos com idade entre oito e 18 anos. Para avaliar a FPM, segundo as recomendações da Eurofit e ASHT, foi utilizado um dinamômetro manual (Jamar). Nenhum dos sujeitos avaliados apresentava qualquer lesão que pudesse comprometer o teste. Os resultados mostram que não há diferença na FPM entre os posicionamentos recomendados pela Eurofit e ASHT para medir a FPM independente do gênero. A curva sigmoide foi a que melhor se adequou para regressão da FPM e idade em ambos os gêneros sendo que para o masculino a FPM tem maior inclinação aos 11 anos, já para o feminino a maior inclinação é aos 10 anos. Além disso, a partir dos 14 anos, o lado dominante dos atletas masculinos apresentou maior FPM que o lado não dominante; contudo, essa assimetria não ocorreu no feminino em qualquer idade até os 18 anos