Which factors contribute to sexual well-being? A comparative study among 17 to 20 year old boys and girls in Belgium and Ecuador

ABSTRACT Despite recognition that sexual well-being is an important part of adolescent sexual and reproductive health, a clear description of adolescent sexual well-being does not yet exist. Through six in-depth interviews and four focus group discussions with 56 young people in two distinct contexts (Belgium and Ecuador), we used the socialecological framework to identify factors influencing adolescent sexual well-being. According to respondents, the main factors that influence adolescent sexual well-being are not only situated at the individual (having knowledge and skills and being physically, sexually and mental mature and healthy) and interpersonal levels (positive attraction towards others and communication about sexuality), but at a broader societal level, including social acceptance of sex, gender and sexual diversity and its (legal) translation into comprehensive sexuality education and the ready availability of contraceptives. Our results go well beyond two existing definitions of (adolescent) sexual wellbeing to contribute to understanding and measurement from the perspective of young people themselves, adding substantively to ongoing discussion about the definition of the concep

¿Qué factores contribuyen al bienestar sexual? Un estudio comparativo entre chicos y chicas de 17 a 20 años en Bélgica y Ecuador

A pesar del reconocimiento de que el bienestar sexual es una parte importante de la salud sexual y reproductiva de los adolescentes, aún no existe una descripción clara del bienestar sexual de los adolescentes. A través de seis entrevistas en profundidad y cuatro discusiones de grupos focales con 56 jóvenes en dos contextos distintos (Bélgica y Ecuador), utilizamos el marco socioecológico para identificar los factores que influyen en el bienestar sexual de los adolescentes. Según los encuestados, los principales factores que influyen en el bienestar sexual de los adolescentes no solo se sitúan a nivel individual (tener conocimientos y habilidades y ser física, sexual y mentalmente maduro y saludable) e interpersonales (atracción positiva hacia los demás y comunicación sobre la sexualidad) , pero a un nivel social más amplio, incluida la aceptación social del sexo, el género y la diversidad sexual y su traducción (legal) en educación sexual integral y la disponibilidad inmediata de anticonceptivos. Nuestros resultados van mucho más allá de dos definiciones existentes de bienestar sexual (adolescente) para contribuir a la comprensión y medición desde la perspectiva de los propios jóvenes, lo que se suma de manera sustancial a la discusión en curso sobre la definición del concepto.Despite recognition that sexual well-being is an important part of adolescent sexual and reproductive health, a clear description of adolescent sexual well-being does not yet exist. Through six in-depth interviews and four focus group discussions with 56 young people in two distinct contexts (Belgium and Ecuador), we used the social-ecological framework to identify factors influencing adolescent sexual well-being. According to respondents, the main factors that influence adolescent sexual well-being are not only situated at the individual (having knowledge and skills and being physically, sexually and mental mature and healthy) and interpersonal levels (positive attraction towards others and communication about sexuality), but at a broader societal level, including social acceptance of sex, gender and sexual diversity and its (legal) translation into comprehensive sexuality education and the ready availability of contraceptives. Our results go well beyond two existing definitions of (adolescent) sexual well-being to contribute to understanding and measurement from the perspective of young people themselves, adding substantively to ongoing discussion about the definition of the concept

First evidence for off-shell production of the Higgs boson and measurement of its width

The first evidence for off-shell Higgs production is reported in the final state with two Z bosons decaying into either four charged leptons (muons or electrons), or two charged leptons and two neutrinos, and a measurement of the Higgs boson width is performed. Results are based on data from the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of up to 140 fb$^{-1}$. The total rate of off-shell Higgs boson production beyond the Z boson pair production threshold, relative to its standard model expectation, is constrained to the interval [0.0061, 2.0] at 95% confidence level. The scenario with no off-shell production is excluded at 99.97% confidence level (3.6 standard deviations). The width of the Higgs boson is extracted as $\Gamma_{\mathrm{H}}$ = 3.2$_{-1.7}^{+2.4}$ MeV, in agreement with the standard model expectation of 4.1 MeV. The data are also used to set new constraints on anomalous Higgs boson couplings to W and Z boson pairs

First evidence for off-shell production of the Higgs boson and measurement of its width

The first evidence for off-shell Higgs production is reported in the final state with two Z bosons decaying into either four charged leptons (muons or electrons), or two charged leptons and two neutrinos, and a measurement of the Higgs boson width is performed. Results are based on data from the CMS experiment at the LHC at a center-of-mass energy of 13 TeV, corresponding to an integrated luminosity of up to 140 fb$^{-1}$. The total rate of off-shell Higgs boson production beyond the Z boson pair production threshold, relative to its standard model expectation, is constrained to the interval [0.0061, 2.0] at 95% confidence level. The scenario with no off-shell production is excluded at 99.97% confidence level (3.6 standard deviations). The width of the Higgs boson is extracted as $\Gamma_{\mathrm{H}}$ = 3.2$_{-1.7}^{+2.4}$ MeV, in agreement with the standard model expectation of 4.1 MeV. The data are also used to set new constraints on anomalous Higgs boson couplings to W and Z boson pairs

Azimuthal correlations in Z+jets events in proton-proton collisions at s\sqrt{s} = 13 TeV

The production of Z bosons associated with jets is measured in pp collisions at $\sqrt{s}=$ 13 TeV with data recorded with the CMS experiment at the LHC corresponding to an integrated luminosity of 36.3 fb$^{-1}$. The multiplicity of jets with transverse momentum $p_{\mathrm{T}} >$ 30 GeV is measured for different regions of the Z boson's $p_{\mathrm{T}}(\mathrm{Z})$, from lower than 10 GeV to higher than 100 GeV. The azimuthal correlation $\Delta \phi$ between the Z boson and the leading jet, as well as the correlations between the two leading jets are measured in three regions of $p_{\mathrm{T}}(\mathrm{Z})$. The measurements are compared with several predictions at leading and next-to-leading orders, interfaced with parton showers. Predictions based on transverse-momentum dependent parton distributions and corresponding parton showers give a good description of the measurement in the regions where multiple parton interactions and higher jet multiplicities are not important. The effects of multiple parton interactions are shown to be important to correctly describe the measured spectra in the low $p_{\mathrm{T}}(\mathrm{Z})$ regions.The production of Z bosons associated with jets is measured in $\text {p}\text {p}$ collisions at $\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V}$ with data recorded with the CMS experiment at the LHC corresponding to an integrated luminosity of 36.3$\,\text {fb}^{-1}$. The multiplicity of jets with transverse momentum $p_{\textrm{T}} > 30\,\text {Ge}\hspace{-.08em}\text {V}$ is measured for different regions of the Z boson’s $p_{\textrm{T}} (\text {Z })$, from lower than 10$\,\text {Ge}\hspace{-.08em}\text {V}$ to higher than 100$\,\text {Ge}\hspace{-.08em}\text {V}$. The azimuthal correlation $\varDelta \phi$ between the Z boson and the leading jet, as well as the correlations between the two leading jets are measured in three regions of $p_{\textrm{T}} (\text {Z })$. The measurements are compared with several predictions at leading and next-to-leading orders, interfaced with parton showers. Predictions based on transverse-momentum dependent parton distributions and corresponding parton showers give a good description of the measurement in the regions where multiple parton interactions and higher jet multiplicities are not important. The effects of multiple parton interactions are shown to be important to correctly describe the measured spectra in the low $p_{\textrm{T}} (\text {Z })$ regions.The production of Z bosons associated with jets is measured in pp collisions at $\sqrt{s}$ = 13 TeV with data recorded with the CMS experiment at the LHC corresponding to an integrated luminosity of 36.3 fb$^{-1}$. The multiplicity of jets with transverse momentum $p_\mathrm{T}$$\gt$ 30 GeV is measured for different regions of the Z boson's $p_\mathrm{T}$(Z), from lower than 10 GeV to higher than 100 GeV. The azimuthal correlation $\Delta \phi$ between the Z boson and the leading jet, as well as the correlations between the two leading jets are measured in three regions of $p_\mathrm{T}$(Z). The measurements are compared with several predictions at leading and next-to-leading orders, interfaced with parton showers. Predictions based on transverse-momentum dependent parton distributions and corresponding parton showers give a good description of the measurement in the regions where multiple parton interactions and higher jet multiplicities are not important. The effects of multiple parton interactions are shown to be important to correctly describe the measured spectra in the low $p_\mathrm{T}$(Z) regions

Observation of electroweak W+W− pair production in association with two jets in proton-proton collisions at <math altimg="si1.svg"><msqrt><mrow><mi>s</mi></mrow></msqrt><mo linebreak="goodbreak" linebreakstyle="after">=</mo><mn>13</mn><mspace width="0.2em"/><mtext>TeV</mtext></math>

International audienceAn observation is reported of the electroweak production of a W+W− pair in association with two jets, with both W bosons decaying leptonically. The data sample corresponds to an integrated luminosity of 138fb−1 of proton-proton collisions at s=13TeV, collected by the CMS detector at the CERN LHC. Events are selected by requiring exactly two opposite-sign leptons (electrons or muons) and two jets with large pseudorapidity separation and high dijet invariant mass. Events are categorized based on the flavor of the final-state leptons. A signal is observed with a significance of 5.6 standard deviations (5.2 expected) with respect to the background-only hypothesis. The measured fiducial cross section is 10.2±2.0fb and this value is consistent with the standard model prediction of 9.1±0.6fb

Constraints on anomalous Higgs boson couplings to vector bosons and fermions from the production of Higgs bosons using the ττ\tau\tau final state

A study of anomalous couplings of the Higgs boson to vector bosons and fermions is presented. The data were recorded by the CMS experiment at a center-of-mass energy of pp collisions at the LHC of 13 TeV and correspond to an integrated luminosity of 138 fb$^{-1}$. The study uses Higgs boson candidates produced mainly in gluon fusion or electroweak vector boson fusion at the LHC that subsequently decay to a pair of $\tau$ leptons. Matrix-element and machine-learning techniques were employed in a search for anomalous interactions. The results are combined with those from the four-lepton and two-photon decay channels to yield the most stringent constraints on anomalous Higgs boson couplings to date. The pure CP-odd scenario of the Higgs boson coupling to gluons is excluded at 2.4 standard deviations. The results are consistent with the standard model predictions.A study of anomalous couplings of the Higgs boson to vector bosons and fermions is presented. The data were recorded by the CMS experiment at a center-of-mass energy of pp collisions at the LHC of 13 TeV and correspond to an integrated luminosity of 138  fb-1. The study uses Higgs boson candidates produced mainly in gluon fusion or electroweak vector boson fusion at the LHC that subsequently decay to a pair of τ leptons. Matrix-element and machine-learning techniques were employed in a search for anomalous interactions. The results are combined with those from the four-lepton and two-photon decay channels to yield the most stringent constraints on anomalous Higgs boson couplings to date. The pure CP-odd scenario of the Higgs boson coupling to gluons is excluded at 2.4 standard deviations. The results are consistent with the standard model predictions.A study of anomalous couplings of the Higgs boson to vector bosons and fermions is presented. The data were recorded by the CMS experiment at a center-of-mass energy of pp collisions at the LHC of 13 TeV and correspond to an integrated luminosity of 138 fb$^{-1}$. The study uses Higgs boson candidates produced mainly in gluon fusion or electroweak vector boson fusion at the LHC that subsequently decay to a pair of $\tau$ leptons. Matrix-element and machine-learning techniques were employed in a search for anomalous interactions. The results are combined with those from the four-lepton and two-photon decay channels to yield the most stringent constraints on anomalous Higgs boson couplings to date. The pure $CP$-odd scenario of the Higgs boson coupling to gluons is excluded at 2.4 standard deviations. The results are consistent with the standard model predictions

Azimuthal correlations in Z +jets events in proton–proton collisions at s=13 TeV\sqrt{s} = 13\,\text {Te}\hspace{-.08em}\text {V}

The production of Z bosons associated with jets is measured in $\text {p}\text {p}$ collisions at $\sqrt{s}=13\,\text {Te}\hspace{-.08em}\text {V}$ with data recorded with the CMS experiment at the LHC corresponding to an integrated luminosity of 36.3$\,\text {fb}^{-1}$. The multiplicity of jets with transverse momentum $p_{\textrm{T}} > 30\,\text {Ge}\hspace{-.08em}\text {V}$ is measured for different regions of the Z boson’s $p_{\textrm{T}} (\text {Z })$, from lower than 10$\,\text {Ge}\hspace{-.08em}\text {V}$ to higher than 100$\,\text {Ge}\hspace{-.08em}\text {V}$. The azimuthal correlation $\varDelta \phi$ between the Z boson and the leading jet, as well as the correlations between the two leading jets are measured in three regions of $p_{\textrm{T}} (\text {Z })$. The measurements are compared with several predictions at leading and next-to-leading orders, interfaced with parton showers. Predictions based on transverse-momentum dependent parton distributions and corresponding parton showers give a good description of the measurement in the regions where multiple parton interactions and higher jet multiplicities are not important. The effects of multiple parton interactions are shown to be important to correctly describe the measured spectra in the low $p_{\textrm{T}} (\text {Z })$ regions

Search for a massive scalar resonance decaying to a light scalar and a Higgs boson in the four b quarks final state with boosted topology

International audienceWe search for new massive scalar particles X and Y through the resonant process X→YH→bb¯bb¯, where H is the standard model Higgs boson. Data from CERN LHC proton-proton collisions are used, collected at a centre-of-mass energy of 13 TeV in 2016–2018 and corresponding to an integrated luminosity of 138fb−1. The search is performed in mass ranges of 0.9–4 TeV for X and 60–600 GeV for Y, where both Y and H are reconstructed as Lorentz-boosted single large-area jets. The results are interpreted in the context of the next-to-minimal supersymmetric standard model and also in an extension of the standard model with two additional singlet scalar fields. The 95% confidence level upper limits for the production cross section vary between 0.1 and 150 fb depending on the X and Y masses, and represent a significant improvement over results from previous searches