Diabetes e sua descompensação crônica: um relato de experiência

Diabetic Ketoacidosis (DAC) is a complication that needs to be understood so that its warning signs are identified by health professionals and so that control measures can be taken, thus avoiding such a problem, so the aim was to understand the decompensation metabolic pathway that promotes CAD in patients with DM. This is an experience report elaborated from the analysis of intervention data and clinical evolution of a health service user who presented CAD due to decompensated DM and died even after the medical procedures. DKA is a hyperglycemic emergency that requires prompt medical intervention. In this sense, early diagnosis and treatment of DM is important because it prevents it from evolving to CAD. However, the study presented shows the opposite, since the patient was unaware that she had DM, so she did not undergo any treatment and died due to complications from DM.A Cetoacidose Diabética (CAD) é uma complicação que necessita ser compreendida para que seus sinais de alerta sejam identificados por profissionais de saúde e para que medidas de controle possam ser tomadas, evitando assim, tal problema, por isso, objetivou-se compreender a descompensação metabólica que promove a CAD em pacientes com DM. Trata-se de um relato de experiência elaborado a partir da análise dos dados de intervenção e evolução clínica de usuário de serviço de saúde que apresentou CAD por conta da DM descompensada e faleceu mesmo após as condutas médicas. A CAD é uma emergência hiperglicêmica que necessita de intervenção médica rápida. Nesse sentido, o diagnóstico precoce e tratamento da DM é importante pois impede que evolua para CAD. No entanto, o estudo apresentado mostra o oposto, visto que a paciente desconhecia que era portadora de DM, por conta disso não fez nenhum tratamento e faleceu em razão das complicações da DM

Diabetes e sua descompensação crônica: um relato de experiência

Diabetic Ketoacidosis (DAC) is a complication that needs to be understood so that its warning signs are identified by health professionals and so that control measures can be taken, thus avoiding such a problem, so the aim was to understand the decompensation metabolic pathway that promotes CAD in patients with DM. This is an experience report elaborated from the analysis of intervention data and clinical evolution of a health service user who presented CAD due to decompensated DM and died even after the medical procedures. DKA is a hyperglycemic emergency that requires prompt medical intervention. In this sense, early diagnosis and treatment of DM is important because it prevents it from evolving to CAD. However, the study presented shows the opposite, since the patient was unaware that she had DM, so she did not undergo any treatment and died due to complications from DM.A Cetoacidose Diabética (CAD) é uma complicação que necessita ser compreendida para que seus sinais de alerta sejam identificados por profissionais de saúde e para que medidas de controle possam ser tomadas, evitando assim, tal problema, por isso, objetivou-se compreender a descompensação metabólica que promove a CAD em pacientes com DM. Trata-se de um relato de experiência elaborado a partir da análise dos dados de intervenção e evolução clínica de usuário de serviço de saúde que apresentou CAD por conta da DM descompensada e faleceu mesmo após as condutas médicas. A CAD é uma emergência hiperglicêmica que necessita de intervenção médica rápida. Nesse sentido, o diagnóstico precoce e tratamento da DM é importante pois impede que evolua para CAD. No entanto, o estudo apresentado mostra o oposto, visto que a paciente desconhecia que era portadora de DM, por conta disso não fez nenhum tratamento e faleceu em razão das complicações da DM

Além do vírus: os efeitos do isolamento social na saúde mental

This article is a reflection study on the effect of social isolation on the mental health of Brazilians, with the main objective of reflecting on the psychosocial damages of isolation in the light of Emerson Merhy's theory of "live work in action". Three categories of analysis were established, history, the COVID-19 pandemic and live work in action, which demonstrate other pandemics throughout history and their proven effects, characterization of the social framework experienced by the Brazilian population during the pandemic and its effects on the mental health of individuals and description of “live work in action” and its relationship with the direction of health and the context of the pandemic. It was concluded that the need to institute severe measures of prevention and social isolation, in order to protect the physical health of individuals, generated psychosocial damage in Brazilian society, mainly anxiety and depression, since it caused drastic changes in lifestyle. , financial losses, feeling of fear and uncertainty.O presente artigo trata de um estudo de reflexão sobre o efeito do isolamento social na saúde mental dos brasileiros, tendo como objetivo principal refletir sobre os danos psicossociais do isolamento à luz da teoria do “trabalho vivo em ato” de Emerson Merhy. Estabeleceu-se três categorias de análises, histórico, a pandemia de COVID-19 e trabalho vivo em ato, tais quais demonstram outras pandemias ao longo da história e seus efeitos comprovados, caracterização do quadro social vivido pela população brasileira durante a pandemia e seus efeitos na saúde mental dos indivíduos e descrição do “trabalho vivo em ato” e sua relação com os rumos da saúde e com o contexto da pandemia. Concluiu-se que a necessidade de instituir medidas severas de prevenção e isolamento social, com o intuito de proteger a saúde física dos indivíduos, gerou na sociedade brasileira danos psicossociais, principalmente de ansiedade e depressão, posto que ocasionou em mudanças drásticas no estilo de vida, perdas financeiras, sentimento de medo e incerteza

Além do vírus: os efeitos do isolamento social na saúde mental

This article is a reflection study on the effect of social isolation on the mental health of Brazilians, with the main objective of reflecting on the psychosocial damages of isolation in the light of Emerson Merhy's theory of "live work in action". Three categories of analysis were established, history, the COVID-19 pandemic and live work in action, which demonstrate other pandemics throughout history and their proven effects, characterization of the social framework experienced by the Brazilian population during the pandemic and its effects on the mental health of individuals and description of “live work in action” and its relationship with the direction of health and the context of the pandemic. It was concluded that the need to institute severe measures of prevention and social isolation, in order to protect the physical health of individuals, generated psychosocial damage in Brazilian society, mainly anxiety and depression, since it caused drastic changes in lifestyle. , financial losses, feeling of fear and uncertainty.O presente artigo trata de um estudo de reflexão sobre o efeito do isolamento social na saúde mental dos brasileiros, tendo como objetivo principal refletir sobre os danos psicossociais do isolamento à luz da teoria do “trabalho vivo em ato” de Emerson Merhy. Estabeleceu-se três categorias de análises, histórico, a pandemia de COVID-19 e trabalho vivo em ato, tais quais demonstram outras pandemias ao longo da história e seus efeitos comprovados, caracterização do quadro social vivido pela população brasileira durante a pandemia e seus efeitos na saúde mental dos indivíduos e descrição do “trabalho vivo em ato” e sua relação com os rumos da saúde e com o contexto da pandemia. Concluiu-se que a necessidade de instituir medidas severas de prevenção e isolamento social, com o intuito de proteger a saúde física dos indivíduos, gerou na sociedade brasileira danos psicossociais, principalmente de ansiedade e depressão, posto que ocasionou em mudanças drásticas no estilo de vida, perdas financeiras, sentimento de medo e incerteza

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Two-particle Bose-Einstein correlations and their Lévy parameters in PbPb collisions at sNN\sqrt{s_\mathrm{NN}} = 5.02 TeV

Two-particle Bose-Einstein momentum correlation functions are studied for charged-hadron pairs in lead-lead collisions at a center-of-mass energy per nucleon pair of $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV. The data sample, containing 4.27$\times10^{9}$ minimum bias events corresponding to an integrated luminosity of 0.607 nb$^{-1}$, was collected by the CMS experiment in 2018. The experimental results are discussed in terms of a L\'evy-type source distribution. The parameters of this distribution are extracted as functions of particle pair average transverse mass and collision centrality. These parameters include the L\'evy index or shape parameter ($\alpha$), the L\'evy scale parameter ($R$), and the correlation strength parameter ($\lambda$). The source shape, characterized by $\alpha$, is found to be neither Cauchy nor Gaussian, implying the need for a full L\'evy analysis. Similarly to what was previously found for systems characterized by Gaussian source radii, a hydrodynamical scaling is observed for the L\'evy $R$ parameter. The $\lambda$ parameter is studied in terms of the core-halo model.Comment: Submitted to Physical Review C. All figures and tables can be found at http://cms-results.web.cern.ch/cms-results/public-results/publications/HIN-21-011 (CMS Public Pages

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s= \sqrt{s} = 5.02 TeV

The inclusive jet cross section is measured as a function of jet transverse momentum $p_{\mathrm{T}}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s} =$ 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4$\,\text{pb}^{-1}$. The jets are reconstructed with the anti-$k_{\mathrm{T}}$ algorithm using a distance parameter of $R=$ 0.4, within the rapidity interval $|y| <$ 2, and across the kinematic range 0.06 $< p_{\mathrm{T}} <$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$.The inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$

Measurement of the double-differential inclusive jet cross section in proton-proton collisions at s\sqrt{s} = 5.02 TeV

International audienceThe inclusive jet cross section is measured as a function of jet transverse momentum $p_\mathrm{T}$ and rapidity $y$. The measurement is performed using proton-proton collision data at $\sqrt{s}$ = 5.02 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 27.4 pb$^{-1}$. The jets are reconstructed with the anti-$k_\mathrm{T}$ algorithm using a distance parameter of $R$ = 0.4, within the rapidity interval $\lvert y\rvert$$\lt$ 2, and across the kinematic range 0.06 $\lt$$p_\mathrm{T}$$\lt$ 1 TeV. The jet cross section is unfolded from detector to particle level using the determined jet response and resolution. The results are compared to predictions of perturbative quantum chromodynamics, calculated at both next-to-leading order and next-to-next-to-leading order. The predictions are corrected for nonperturbative effects, and presented for a variety of parton distribution functions and choices of the renormalization/factorization scales and the strong coupling $\alpha_\mathrm{S}$