42 research outputs found
Studies of B_{s2}^{*} (5840)â° and B_{s1} (5830)â° mesons including the observation of the B_{s2}^{*} (5840)â° â Bâ°K_{s}^{0} decay in proton-proton collisions at âs = 8 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexander J
- Alhusseini M
- Ali MABM
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Angioni GLP
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arndt T
- Arneodo M
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- Asawatangtrakuldee C
- Asghar MI
- Asilar E
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- Atakisi IO
- Ather MW
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- Aushev T
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avila C
- Ayala E
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Bagliesi G
- Bahinipati S
- Baidali S
- Baillon P
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- Ball AH
- Ball F
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- Banerjee S
- Banerjee S
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- Barbagli G
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- Wulz C-E
- Wurthwein F
- Wyslouch B
- Xia F
- Xiao M
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- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
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- Yu I
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- Yumiceva F
- Yusli MN
- Zabel J
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang Z
- Zhao J
- Zhaozhong S
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zito G
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
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- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/11/2018
- Field of study
Measurements of B_{s2}^{*} (5840)â° and B_{s1} (5840)â° mesons are performed using a data sample of proton-proton collisions corresponding to an integrated luminosity of 19.6 fbâ»Âč, collected with the CMS detector at the LHC at a centre-of-mass energy of 8 TeV. The analysis studies P-wave B_{s}^{0} meson decays into B^{(*)}âșKâ» and B^{(*)}â°K_{s}^{0}, where the Bâș and Bâ° mesons are identified using the decays Bâș â J/ÏKâș and Bâ° â J/ÏK* (892)â°. The masses of the P-wave B_{s}^{0} meson states are measured and the natural width of the B_{*}^{s2} (5840)â° state is determined. The first measurement of the mass difference between the charged and neutral B* mesons is also presented. The B_{*}^{s2} (5840)â° decay to Bâ°K_{s}^{0} is observed, together with a measurement of its branching fraction relative to the B_{s2}^{*} (5840)â° â BâșKâ» decay
Suppression and azimuthal anisotropy of prompt and nonprompt J/psi production in PbPb collisions at root S-NN=2.76 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adzic P
- Afanasiev S
- Agapitos A
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Ainapanea N
- Akbiyik M
- Akchurin N
- Akgun B
- Al-Bataineh A
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Alderweireldt S
- Aleksandrov A
- Alexander J
- Ali MABM
- Alimena J
- Allen B
- Almond J
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amin N
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Anderson I
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Anelli C
- Angioni GLP
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arndt T
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asilar E
- Askew A
- Attikis A
- Aubin A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Baber M
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- Yilmaz Y
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- Yonamine R
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- Yu SS
- Yumiceva F
- Yusli MN
- Zabel J
- Zabi A
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- Zagozdzinska A
- Zakaria M
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zeinali M
- Zenoni F
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang F
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- Zhao J
- Zhokin A
- Zhukov V
- Zhukova V
- Zientek M
- Zolkapli Z
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- Zorbilmez C
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- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- Zykunov V
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/04/2017
- Field of study
The nuclear modification factor RAA and the azimuthal anisotropy coefficient v2 of prompt and nonprompt (i.e. those from decays of b hadrons) J/Ï mesons, measured from PbPb and pp collisions at sNNââââ=2.76 TeV at the LHC, are reported. The results are presented in several event centrality intervals and several kinematic regions, for transverse momenta pT>6.5 GeV/c and rapidity |y|<2.4 , extending down to pT=3 GeV/c in the 1.6<|y|<2.4 range. The v2 of prompt J/Ï is found to be nonzero, but with no strong dependence on centrality, rapidity, or pT over the full kinematic range studied. The measured v2 of nonprompt J/Ï is consistent with zero. The RAA of prompt J/Ï exhibits a suppression that increases from peripheral to central collisions but does not vary strongly as a function of either y or pT in the fiducial range. The nonprompt J/Ï RAA shows a suppression which becomes stronger as rapidity or pT increases. The v2 and RAA of open and hidden charm, and of open charm and beauty, are compared
Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullin S
- Abercrombie D
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- Acharya H
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- Agarwal G
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- Agram J-L
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- Yumiceva F
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
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- Zecchinelli AG
- Zeinali M
- Zeuner WD
- Zghiche A
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- Zorbilmez C
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- Zuolo D
- Zygala L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Since the discovery of the Higgs boson in 2012, detailed studies of its properties have been ongoing. Besides its mass, its widthârelated to its lifetimeâis an important parameter. One way to determine this quantity is to measure its off-shell production, where the Higgs boson mass is far away from its nominal value, and relating it to its on-shell production, where the mass is close to the nominal value. Here we report evidence for such off-shell contributions to the production cross-section of two Z bosons with data from the CMS experiment at the CERN Large Hadron Collider. We constrain the total rate of the off-shell Higgs boson contribution beyond the Z boson pair production threshold, relative to its standard model expectation, to the interval [0.0061,â2.0] at the 95% confidence level. The scenario with no off-shell contribution is excluded at a p-value of 0.0003 (3.6 standard deviations). We measure the width of the Higgs boson as ÎH=3.2+2.4â1.7MeV, in agreement with the standard model expectation of 4.1âMeV. In addition, we set constraints on anomalous Higgs boson couplings to W and Z boson pairs
Performance of the CMS muon trigger system in proton-proton collisions at root s=13 TeV
- Author
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- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullah WATW
- Abdullin S
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2021
- Field of study
The muon trigger system of the CMS experiment uses a combination of hardware and software to identify events containing a muon. During Run 2 (covering 2015â2018) the LHC achieved instantaneous luminosities as high as 2 Ă 1034 while delivering proton-proton collisions at â(s) = 13. The challenge for the trigger system of the CMS experiment is to reduce the registered event rate from about 40MHz to about 1kHz. Significant improvements important for the success of the CMS physics program have been made to the muon trigger system via improved muon reconstruction and identification algorithms since the end of Run 1 and throughout the Run 2 data-taking period. The new algorithms maintain the acceptance of the muon triggers at the same or even lower rate throughout the data-taking period despite the increasing number of additional proton-proton interactions in each LHC bunch crossing. In this paper, the algorithms used in 2015 and 2016 and their improvements throughout 2017 and 2018 are described. Measurements of the CMS muon trigger performance for this data-taking period are presented, including efficiencies, transverse momentum resolution, trigger rates, and the purity of the selected muon sample. This paper focuses on the single- and double-muon triggers with the lowest sustainable transverse momentum thresholds used by CMS. The efficiency is measured in a transverse momentum range from 8 to several hundred
Proton nuclear magnetic resonance relaxometry
- Publication venue
- 'Informa UK Limited'
- Publication date
- 22/12/2015
- Field of study
As advanced teaching and training in the development of cementitious materials increase, the need has emerged for an up-to-date practical guide to the field suitable for graduate students and junior and general practitioners.
This edited volume provides the cement science community with a state-of-the-art overview of analytical techniques used in cement chemistry to study the hydration and microstructure of cements. Each chapter focuses on a specific technique, not only describing the basic principles behind the technique, but also providing essential, practical details on its application to the study of cement hydration. Each chapter sets out present best practice, and draws attention to the limitations and potential experimental pitfalls of the technique. Databases that supply examples and that support the analysis and interpretation of the experimental results strengthen a very valuable ready reference
Proton nuclear magnetic resonance relaxometry
- Publication venue
- Boca Raton, FL, USA
- Publication date
- 31/10/2017
- Field of study
As advanced teaching and training in the development of cementitious materials increase, the need has emerged for an up-to-date practical guide to the field suitable for graduate students and junior and general practitioners. This edited volume provides the cement science community with a state-of-the-art overview of analytical techniques used in cement chemistry to study the hydration and microstructure of cements. Each chapter focuses on a specific technique, not only describing the basic principles behind the technique, but also providing essential, practical details on its application to the study of cement hydration. Each chapter sets out present best practice, and draws attention to the limitations and potential experimental pitfalls of the technique. Databases that supply examples and that support the analysis and interpretation of the experimental results strengthen a very valuable ready reference
Densification of C-S-H measured by H NMR relaxometry
- Publication venue
- 'American Chemical Society (ACS)'
- Publication date
- 10/01/2013
- Field of study
The nanoscale morphology of, and pore water interactions in, calcium silicate hydrate (C-S-H), the active component of cement, remain uncertain. H nuclear magnetic resonance (NMR) can fully characterize the nanoporosity of C-S-H in as-prepared material without the need for damaging sample drying. We use NMR to follow the density of C-S-H in sealed cured pastes as a function of degree of hydration (α) and water to cement ratio. We show clear evidence for C-S-H densification. The C-S-H "solid" density, exclusive of gel pore water, slightly decreases from Ï = 2.73 g/cm at α â 0.4 to 2.65 g/cmat α â 0.9 due to an increase in the number of layers in the nanocrystalline aggregates. In the same range, the C-S-H "bulk" density, including gel water, increases from around 1.8 to 2.1 g/cm. The increase corresponds to a transition from growth of low-density product containing gel pores to higher density product devoid of gel pores. We update Powers' classical model from 1947. In contrast to the single "hydrate" of Powers, NMR differentiates between C-S-H and calcium hydroxide and separates out the interlayer water within the C-S-H. It shows a clear nonlinearity in the growth of the different fractions with α. © 2012 American Chemical Society
Use of bench-top NMR to measure the density, composition and desorption isotherm of C-S-H in cement paste
- Publication venue
- 'Elsevier BV'
- Publication date
- 16/01/2019
- Field of study
H nuclear magnetic resonance (NMR), supported by a measurement of the degree of hydration using X-ray diffraction, has been used to fully characterise the nano-scale porosity and composition of calcium-silicate-hydrate (C-S-H), the active component of cement. The resultant "solid" density and composition are Ï = 2.68 g/cm; (Ca). (Si,Al)O. (HO) for an underwater cured, never-dried cement paste with an initial mix water-to-cement ratio of 0.4 after 28 days of hydration. In addition, the first pore-type resolved desorption isotherm of cement that shows the location of water as a function of relative humidity has been measured. Critical to our results is verification of the assignment of the different NMR spin-spin relaxation time components. These have been corroborated with conventional analyses. The new methodology is key to enabling design of cement pastes with lower environmental impact
Influence of silica fume on the microstructure of cement pastes: New insights from H NMR relaxometry
- Publication venue
- 'Elsevier BV'
- Publication date
- 23/06/2015
- Field of study
H NMR has been used to characterise white Portland cement paste incorporating 10 wt.% of silica fume. Samples were measured sealed throughout the hydration without sample drying. Paste compositions and C-S-H characteristics are calculated based on H NMR signal intensities and relaxation analysis. The results are compared with a similar study of plain white cement paste. While the presence of silica fume has little influence on C-S-H densities, the chemical composition is impacted. After 28 days of sealed hydration, the Ca/(Si + Al) ratio of the C-S-H is 1.33 and the H2O(Si + Al) ratio is 1.10 when 10% of silica fume is added to the white cement. A densification of the C-S-H with time is observed. There are no major changes in capillary, C-S-H gel and interlayer pore sizes for the paste containing silica fume compared to the plain white cement paste. However, the gel/interlayer water ratio increases in the silica fume blend
TERMINAL DELETION 6P23 - A CASE-REPORT
- Publication venue
- 'Wiley'
- Publication date
- 01/12/1990
- Field of study
ESCOLA PAULISTA MED SCH,DEPT PEDIAT,DISCIPLINA PUERICULTURA & PEDIAT SOCIAL,BR-04023 SĂŁo Paulo,BRAZILESCOLA PAULISTA MED SCH,DEPT PEDIAT,DISCIPLINA PUERICULTURA & PEDIAT SOCIAL,BR-04023 SĂŁo Paulo,BRAZILWeb of Scienc