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At least 1,531 records · Page 85

Measurement of the transverse momentum distribution of Drell–Yan lepton pairs in proton–proton collisions at √s=13 TeV with the ATLAS detector

This paper describes precision measurements of the transverse momentum $p_\mathrm {T}^{\ell \ell }$ ($\ell =e,\mu $) and of the angular variable $\phi ^{*}_{\eta }$ distributions of Drell–Yan lepton pairs in a mass range of 66–116 GeV. The analysis uses data from 36.1 fb$^{-1}$ of proton–proton collisions at a centre-of-mass energy of $\sqrt{s}=13\,$TeV collected by the ATLAS experiment at the LHC in 2015 and 2016. Measurements in electron-pair and muon-pair final states are performed in the same fiducial volumes, corrected for detector effects, and combined. Compared to previous measurements in proton–proton collisions at $\sqrt{s}=7$ and $8\,$TeV, these new measurements probe perturbative QCD at a higher centre-of-mass energy with a different composition of initial states. They reach a precision of 0.2$\%$ for the normalized spectra at low values of $p_\mathrm {T}^{\ell \ell }$. The data are compared with different QCD predictions, where it is found that predictions based on resummation approaches can describe the full spectrum within uncertainties.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Measurement of the CP-violating phase ϕ s in B$_s^0$→J/ψϕ decays in ATLAS at 13 TeV

A measurement of the B$_s^0$→J/ψϕ decay parameters using 80.5 fb -1 of integrated luminosity collected with the ATLAS detector from 13 Te proton–proton collisions at the LHC is presented. The measured parameters include the CP-violating phase ϕ s , the width difference Δ Γ s between the B$_s^0$ meson mass eigenstates and the average decay width Γ s . The values measured for the physical parameters are combined with those from 19.2fb -1 of 7 and 8 Te data, leading to the following: ϕs=-0.087±0.036(stat.)±0.021(syst.)rad ΔΓ s =0.0657±0.0043(stat.)±0.0037(syst.)ps -1 Γ s =0.6703±0.0014(stat.)±0.0018(syst.)ps -1 Results for ϕ s and Δ Γ s are also presented as 68% confidence level contours in the ϕ s –Δ Γ s plane. Furthermore the transversity amplitudes and corresponding strong phases are measured. ϕ s and Δ Γ s measurements are in agreement with the Standard Model predictions.

72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS↗

Materials Data on H24OsC8(NF3)2 by Materials Project

FFOs((CH3)4NF)2F2 crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of one difluoroosmium molecule, two hydrofluoric acid molecules, and two (CH3)4NF clusters. In each (CH3)4NF cluster, there are four inequivalent C+1.25- sites. In the first C+1.25- site, C+1.25- is bonded in a 1-coordinate geometry to four H1+ atoms. There are a spread of C–H bond distances ranging from 0.83–1.70 Å. In the second C+1.25- site, C+1.25- is bonded in a 4-coordinate geometry to four H1+ atoms. There are a spread of C–H bond distances ranging from 0.82–1.66 Å. In the third C+1.25- site, C+1.25- is bonded in a 4-coordinate geometry to one N3- and three H1+ atoms. The C–N bond length is 1.12 Å. There are a spread of C–H bond distances ranging from 1.12–1.72 Å. In the fourth C+1.25- site, C+1.25- is bonded in a distorted single-bond geometry to one N3- and three H1+ atoms. The C–N bond length is 1.55 Å. There are a spread of C–H bond distances ranging from 0.80–1.75 Å. N3- is bonded in a 2-coordinate geometry to two C+1.25- atoms. There are twelve inequivalent H1+ sites. In the first H1+ site, H1+ is bonded in a single-bond geometry to one C+1.25- atom. In the second H1+ site, H1+ is bonded in a single-bond geometry to one C+1.25- atom. In the third H1+ site, H1+ is bonded in a bent 150 degrees geometry to one C+1.25- and one F1- atom. The H–F bond length is 1.44 Å. In the fourth H1+ site, H1+ is bonded in a single-bond geometry to one C+1.25- atom. In the fifth H1+ site, H1+ is bonded in a water-like geometry to two C+1.25- atoms. In the sixth H1+ site, H1+ is bonded in a single-bond geometry to one C+1.25- atom. In the seventh H1+ site, H1+ is bonded in a single-bond geometry to one C+1.25- atom. In the eighth H1+ site, H1+ is bonded in a single-bond geometry to one C+1.25- atom. In the ninth H1+ site, H1+ is bonded in a single-bond geometry to one C+1.25- atom. In the tenth H1+ site, H1+ is bonded in a single-bond geometry to one C+1.25- atom. In the eleventh H1+ site, H1+ is bonded in a single-bond geometry to one C+1.25- atom. In the twelfth H1+ site, H1+ is bonded in a distorted L-shaped geometry to two C+1.25- atoms. F1- is bonded in a single-bond geometry to one H1+ atom.

36 MATERIALS SCIENCE↗

Materials Data on Si2Os3C12(ClO2)6 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on GeOs2C8(ClO2)4 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on OsC4ClO4 by Materials Project

OsCl(CO)4 is Cubic alpha N2-derived structured and crystallizes in the orthorhombic P2_12_12_1 space group. The structure is zero-dimensional and consists of eight chloroosmium molecules and thirty-two formaldehyde molecules.

36 MATERIALS SCIENCE↗

Materials Data on Os6C19SO19 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on OsClF8 by Materials Project

OsF6ClF2 is beta-prime cadmium gold structured and crystallizes in the triclinic P-1 space group. The structure is zero-dimensional and consists of two osmium hexafluoride molecules and two ClF2 clusters. In each ClF2 cluster, Cl is bonded in a distorted rectangular see-saw-like geometry to two equivalent F atoms. Both Cl–F bond lengths are 1.62 Å. F is bonded in a single-bond geometry to one Cl atom.

36 MATERIALS SCIENCE↗

Materials Data on Os3C10(BrO5)2 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on Sb2Os(OF7)2 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on BiOs3(CO)9 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on Ca2NiOsO6 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on Ba2NiOsO6 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on H16OsC4S4Br8N8O3 by Materials Project

OsBr6(CN2H4S)4O3Br2 crystallizes in the orthorhombic Cmcm space group. The structure is zero-dimensional and consists of eight ac1nqwuv molecules, four hexabromoosmium molecules, and four trihydrate;dihydrobromide molecules.

36 MATERIALS SCIENCE↗

Materials Data on OsN5Cl3 by Materials Project

(OsN)2N2(N2Cl)2(NCl2)2 crystallizes in the orthorhombic Pnma space group. The structure is zero-dimensional and consists of four ammonia molecules, four azanylidyneosmium molecules, four dichloramine molecules, and four N2Cl clusters. In each N2Cl cluster, N+0.20+ is bonded in a single-bond geometry to one Cl1- atom. The N–Cl bond length is 1.70 Å. Cl1- is bonded in a linear geometry to two equivalent N+0.20+ atoms.

36 MATERIALS SCIENCE↗

Materials Data on Sr2CrOsO6 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗

Materials Data on Sr2CrOsO6 by Materials Project

Computed materials data using density functional theory calculations. These calculations determine the electronic structure of bulk materials by solving approximations to the Schrodinger equation. For more information, see https://materialsproject.org/docs/calculations

36 MATERIALS SCIENCE↗