16 research outputs found
Search for dark matter at √s=13 TeV in final states containing an energetic photon and large missing transverse momentum with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam ER
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
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- Albicocco P
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Kado M
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- Kaji T
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- Kalderon CW
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- Karastathis N
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- Karentzos E
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- Karyukhin AN
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- Knue A
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- Komori Y
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- Kostyukhin VV
- Kotwal A
- Koulouris A
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- Kourkoumelis C
- Kourlitis E
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- Zalieckas J
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- Zhemchugov A
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
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- Zobernig G
- Zoccoli
- Zou R
- Zu Theenhausena HM
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
Results of a search for physics beyond the Standard Model in events containing an energetic photon and large missing transverse momentum with the ATLAS detector at the Large Hadron Collider are reported. As the number of events observed in data, corresponding to an integrated luminosity of 36.1 fb−1 of proton–proton collisions at a centre-of-mass energy of 13 TeV, is in agreement with the Standard Model expectations, model-independent limits are set on the fiducial cross section for the production of events in this final state. Exclusion limits are also placed in models where dark-matter candidates are pair-produced. For dark-matter production via an axial-vector or a vector mediator in the s-channel, this search excludes mediator masses below 750–1200 GeV for dark-matter candidate masses below 230–480 GeV at 95% confidence level, depending on the couplings. In an effective theory of dark-matter production, the limits restrict the value of the suppression scale M∗ to be above 790 GeV at 95% confidence level. A limit is also reported on the production of a high-mass scalar resonance by processes beyond the Standard Model, in which the resonance decays to Zγ and the Z boson subsequently decays into neutrinos
A search for pair-produced resonances in four-jet final states at root s=13 TeV with the ATLAS detector
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- Zhemchugov A
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- Zibell A
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- Zimine NI
- Zimmermann C
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- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 03/04/2017
- Field of study
A search for massive coloured resonances which are pair-produced and decay into two jets is presented. The analysis uses 36.7 fb−1
−
1
of √
s
= 13 TeV pp collision data recorded by the ATLAS experiment at the LHC in 2015 and 2016. No significant deviation from the background prediction is observed. Results are interpreted in a SUSY simplified model where the lightest supersymmetric particle is the top squark, ̃
t
~
, which decays promptly into two quarks through R-parity-violating couplings. Top squarks with masses in the range 100 GeV<̃<410
100
GeV
<
m
t
~
<
410
GeV
GeV
are excluded at 95% confidence level. If the decay is into a b-quark and a light quark, a dedicated selection requiring two b-tags is used to exclude masses in the ranges 100 GeV<̃<470
100
GeV
<
m
t
~
<
470
GeV
GeV
and 480 GeV<̃<610
480
GeV
<
m
t
~
<
610
GeV
GeV
. Additional limits are set on the pair-production of massive colour-octet resonances
Measurement of single top-quark production in association with a W boson in the single-lepton channel at \sqrt{s} = 8\,\text {TeV} with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Acharya BS
- Achkar B
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- Aguilar-Saavedra JA
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- Alberghi GL
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- Aleksa M
- Aleksandrov IN
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- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Bogavac D
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- Burzynski JC
- Buscher V
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
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- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
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- Caforio D
- Cai H
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- Cakir IT
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- Calace N
- Calafiura P
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- Calderini G
- Calfayan P
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- Casha AF
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- Castillo FL
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- Cheremushkina E
- Cheu E
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- Chevalerias TJA
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- Zhemchugov A
- Zheng Z
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
The production cross-section of a top quark in association with a W boson is measured using proton–proton collisions at \sqrt{s} = 8\,\text {TeV}. The dataset corresponds to an integrated luminosity of 20.2\,\text {fb}^{-1}, and was collected in 2012 by the ATLAS detector at the Large Hadron Collider at CERN. The analysis is performed in the single-lepton channel. Events are selected by requiring one isolated lepton (electron or muon) and at least three jets. A neural network is trained to separate the tW signal from the dominant t{\bar{t}} background. The cross-section is extracted from a binned profile maximum-likelihood fit to a two-dimensional discriminant built from the neural-network output and the invariant mass of the hadronically decaying W boson. The measured cross-section is \sigma _{tW} = 26 \pm 7\,\text {pb}, in good agreement with the Standard Model expectation
Identification and rejection of pile-up jets at high pseudorapidity with the ATLAS detector
- Author
- Aaboud M
- Aad G
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- Zimine NI
- Zimmermann C
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- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
The rejection of forward jets originating from
additional proton–proton interactions (pile-up) is crucial for
a variety of physics analyses at the LHC, including Standard
Model measurements and searches for physics beyond
the Standard Model. The identification of such jets is challenging
due to the lack of track and vertex information in
the pseudorapidity range |η| > 2.5. This paper presents a
novel strategy for forward pile-up jet tagging that exploits
jet shapes and topological jet correlations in pile-up interactions.
Measurements of the per-jet tagging efficiency are
presented using a data set of 3.2 fb−1 of proton–proton collisions
at a centre-of-mass energy of 13 TeV collected with the
ATLAS detector. The fraction of pile-up jets rejected in the
range 2.5 < |η| < 4.5 is estimated in simulated events with
an average of 22 interactions per bunch-crossing. It increases
with jet transverse momentum and, for jets with transverse
momentum between 20 and 50 GeV, it ranges between 49%
and 67% with an efficiency of 85% for selecting hard-scatter
jets. A case study is performed in Higgs boson production
via the vector-boson fusion process, showing that these techniques
mitigate the background growth due to additional
proton–proton interactions, thus enhancing the reach for such
signatures
Search for new phenomena in high-mass final states with a photon and a jet from pp collisions at root s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
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- Acharya BS
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- Zobernig G
- Zoccoli A
- Zou R
- Zwalinski L
- Publication venue
- Springer Verlag
- Publication date
- 29/09/2017
- Field of study
A search is performed for new phenomena in events having a photon with high transverse momentum and a jet collected in 36.7 fb−1 of proton–proton collisions at a centre-of-mass energy of s√ = 13 TeV recorded with the ATLAS detector at the Large Hadron Collider. The invariant mass distribution of the leading photon and jet is examined to look for the resonant production of new particles or the presence of new high-mass states beyond the Standard Model. No significant deviation from the background-only hypothesis is observed and cross-section limits for generic Gaussian-shaped resonances are extracted. Excited quarks hypothesized in quark compositeness models and high-mass states predicted in quantum black hole models with extra dimensions are also examined in the analysis. The observed data exclude, at 95% confidence level, the mass range below 5.3 TeV for excited quarks and 7.1 TeV (4.4 TeV) for quantum black holes in the Arkani-Hamed–Dimopoulos–Dvali (Randall–Sundrum) model with six (one) extra dimensions
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- Author
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- Krause HF
- Kreindler JL
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- Krings JG
- Kristin J
- Kristjansson RP
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- Lam WW
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- Larivée N
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- Le Bon SD
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- Lechien JR
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- Lee JS
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- Lee S
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- Lennard CM
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- Liu CM
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- Lowery AS
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- Mariano ER
- Marple BF
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- Marseglia GL
- Marshall AH
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- Marzban S
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- Masterson L
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- Matheny KE
- Matsune S
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- Maxfield AZ
- May A
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- McKinley SH
- McMains KC
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- Melen I
- Melroy C
- Meltzer EO
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- Meltzer EO
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- Melvin TA
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- Merkley MA
- Messerklinger W
- Metson R
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- Mfuna EL
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- Middleton PG
- Miglani A
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- Miller AJ
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- Mitchell E
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- Miłoński J
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- Morrissey DK
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- Mortazavi N
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- Mostafa BE
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- Mozzanica F
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- Nagarkar DR
- Nagata Y
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- Namyslowski G
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- Newberry CI
- Newton E
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- Ngoc Ha T
- Nguyen BK
- Nguyen KL
- Nguyen T
- Nicolai P
- Nimsakul S
- Nino G
- Ninomiya T
- Nisa L
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- Nocera AL
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- Nomura K
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- Novis SJ
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- Nussenbaum B
- Nyenhuis SM
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- Oakley GM
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- Ocampo CJ
- Odat H
- Ogasawara N
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- Ohnishi T
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- Orb Q
- Ordovas‐Montanes J
- Ordovas‐Montanes J
- Organization WH
- Orlandi R
- Orlandi RR
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- Orlandi RR
- Orlandi RR
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- Orlandi RR
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- Ostovar A
- Ou J
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- Ozturan A
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- Paderno A
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- Papagiannopoulos P
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- Paramasivan S
- Parasher AK
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- Parikh A
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- Parikh SL
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- Paris G.
- Park D‐Y
- Park M
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- Park SK
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- Park SM
- Parma V
- Parsek MR
- Pasaje CF
- Pasaje CF
- Pasaje CF
- Passali D
- Passali D
- Passali D
- Passàli D
- Passàli D
- Passàli D
- Patel NA
- Patel NN
- Patel VS
- Patel ZM
- Patel ZM
- Patou J
- Patro SK
- Pauli C
- Pavlin JD
- Payne SC
- Payne SJ
- Pearlman AN
- Pearlman AN
- Peng Y
- Peng Y
- Penttila M
- Perez‐Novo CA
- Peric A
- Peric A
- Perica A
- Perić A
- Perkasa MF
- Perloff JR
- Persson EK
- Peters AT
- Peña MT
- Pfaar O
- Pfaar O
- Pfaar O
- Pham V
- Phillips KM
- Phillips KM
- Phillips KM
- Phillips KM
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- Philpott C
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- Picado C
- Piccirillo JF
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- Pimenta F
- Pincus RL
- Pinther S
- Pinto Bezerra Soter AC
- Pinto JM
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- Pipolo C
- Plebani A
- Plonk DP
- Poachanukoon O
- Poetker DM
- Poetker DM
- Poetker DM
- Poetker DM
- Poletti SC
- Ponikau JU
- Ponikau JU
- Ponikau JU
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- Porter PC
- Pothoven KL
- Prajapati DP
- Prickett KK
- Prince AA
- Principi N
- Promsopa C
- Psaltis AJ
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- Pumhirun P
- Pundir V
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- Purcell PL
- Purkey MT
- Purnell PR
- Pynnonen M
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- Qualliotine JR
- Quintanilla‐Dieck L
- Quinti I
- Qvarnberg Y
- Rabago D
- Rabago D
- Rabbe R
- Rachelefsky GS
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- Ragab A
- Ragab A
- Ragab S
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- Raghunandhan S
- Rahbar R
- Rai G
- Rains BM
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- Raithatha R
- Rajan JP
- Rajiv S
- Ramadan HH
- Ramadan HH
- Ramadan HH
- Ramadan HH.
- Ramadan HH.
- Ramakrishnan V
- Ramakrishnan VR
- Ramakrishnan VR
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- Ramakrishnan VR
- Ramakrishnan VR
- Ramakrishnan VR
- Ramakrishnan VR
- Ramanathan M
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- Rantala A
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- Rawal RB
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- Rawlings BA
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- Reddel HK
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- Reg‐entSM MIPS 2018 Reporting ‐ Quality Measures
- Reh DD
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- Revai K
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- Ricciardolo FLM
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- Rosen PL
- Rosenfeld RM
- Rosenfeld RM
- Rosenfeld RM
- Rostkowska‐Nadolska B
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- Rostkowska‐Nadolska BLM
- Rotenberg BW
- Roth M
- Rowan NR
- Rowan NR
- Rowan NR
- Rowe SM
- Rowe‐Jones JM
- Roxbury CR
- Rozsasi A
- Rudack C
- Rudmik L
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- Rudmik L
- Rudmik L
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- Saidi IS
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- Salama ER
- Salama N
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- Sawhney S
- Sawicki GS
- Saylam G
- Scadding GK
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- Scangas GA
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- Scangas GA
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- Scarpignato C
- Schaper C
- Scheinberg PA
- Schenkel E
- Schenkel EJ
- Scheuller MC
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- Schicht M
- Schlosser RJ
- Schlosser RJ
- Schlosser RJ
- Schlosser RJ
- Schlosser RJ
- Schlosser RJ
- Schmidt F
- Schneider S
- Schreiber CP
- Schubert MS
- Schwartz HJ
- Schwartz JS
- Schwarzbach HL
- Schwitzguébel AJ‐P
- Scott JR
- Scott JR
- Sedaghat AR
- Sedaghat AR
- Sedaghat AR
- Seiberling K
- Seiberling KA
- Seiberling KA
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- Sejima T
- Sella GCP
- Sener M
- Senior BA
- Senior BA
- Senturk M
- Seppanen M
- Seresirikachorn K
- Servat JJ
- Seshadri S
- Sethi DS
- Sethi N
- Sethi RKV
- Sethi S
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- Settipane RA
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- Shah GB
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- Shaikh N
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- Shanbhag S
- Shapiro AJ
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- Sharif‐Askari FS
- Sharma P
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- Sharp HJ
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- Shen J
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- Shin HW KD
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- Siedek V
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- Siegel GJ
- Sieskiewicz A
- Sikand A
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- Silva MP
- Silveira MLC
- Silverman RA
- Sindwani R
- Singhal D
- Singla G
- Sintobin I
- Sirikci A
- Sitarek P
- Siu J
- Sivaci R
- Sjogren PP
- Slavin RG
- Sleigh MA
- Sleigh MA
- Small CB
- Smith A
- Smith KA
- Smith KA
- Smith KA
- Smith KA
- Smith KA
- Smith KA
- Smith SS
- Smith SS
- Smith T
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
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- Snow DG
- Snyderman CH
- Sohn HG
- Sohn JH
- Soler ZM
- Soler ZM
- Soler ZM
- Soler ZM
- Soler ZM
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- Southwood JE
- Sowerby LJ
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- Steinke JW
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- Stentzel S
- Stern‐Shavit S
- Stevens PR
- Stevens WW
- Stevens WW
- Stevens WW
- Stevens WW
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- Stevenson DD
- Stevenson DD
- Stewart RA
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- Stokken J
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- Stolovitzky JP
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- Strauss G
- Stringer SP
- Stryjewska‐Makuch G
- Su MC
- Subramanian HN
- Succar EF
- Sugimoto I
- Sugino T
- Suh JD
- Sullivan PW
- Sultan B
- Sunadome H
- Sundaresan AS
- Sunkaraneni VS
- Suzuki S
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- Sylvester DC
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- Tabaee A
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- Tabrizi R
- Taccariello M
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- Takabayashi T
- Takabayashi T
- Takabayashi T
- Takahashi T
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- Tammemagi CM
- Tan BK
- Tan BK
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- Tan KS
- Tan KS
- Tan NC
- Tan NC
- Tan NC
- Tanaka S
- Tang C
- Tanner SB
- Tarrant BJ
- Tas M
- Taschieri S
- Taulu R
- Taulu R
- Tay TR
- Taylor MJ
- Telmesani LM
- Tesche S
- Teufelberger AR
- Tewfik MA
- Thacker NM
- Thamboo A
- Thamboo A
- Thamboo A
- Tharakan A
- Theodoraki MN
- Thilsing T
- Thomas AJ
- Thomas JK
- Thomas M
- Thomas WW
- Thulasidas P
- Tieu DD
- Tipirneni KE
- Tipirneni KE
- Tipirneni KE
- Tirelli G
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- Tirumandas M
- Tizzano M
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- Todman MS
- Tomassen P
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- Tomassen P
- Tomassen P
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- Tos M
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- Tosca MA
- Toskala E
- Tosun F
- Tournas A
- Tran Khai Hoan N
- Tripathi A
- Trompette A
- Tscopp KP
- Tsetsos N
- Turan A
- Turan A
- Turfe Z
- Turner JH
- Turner JH
- Turner JH
- Turner JH
- Turner JH
- Tyler MA
- Tyler MA
- Tyler MA
- Tyler MA
- Tzelnick S
- Ualiyeva S
- Ueda D
- Ulualp SO
- Ulualp SO
- Unlu HH
- Unsal AA
- Ural A
- Uri N
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- Vaezi MF
- Vaidyanathan S
- Vaiman M
- Vaira LA
- Vaira LA
- Valdes CJ
- Valentine R
- Valentine R
- Valentine R
- Valera FCP
- Van Bruaene N
- Van Crombruggen K
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- Van Der Veen J
- Van der Veken P
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- Varshney R
- Varvyanskaya A
- Vashishta R
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- Vceva A
- Velasquez N
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- Venekamp RP
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- Veskitkul J
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- Villari CR
- Virgin F
- Virgin FW
- Virgin FW
- Vlastarakos PV
- Vlckova I
- Vleming M
- Voegels RL
- Von Buchwald C
- Vreugdenburg TD
- Vultaggio A
- Vuralkan E
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- Wald ER
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- Wald ER.
- Walker A
- Wallwork B
- Walsh JE
- Walsh TJ
- Wan H
- Wandell GM
- Wang CS
- Wang EW
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- Wang F
- Wang F
- Wang J
- Wang JH
- Wang LF
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- Wang L‐F
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- Wang M
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- Wang PC
- Wang TT
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- Wang X
- Wang X
- Wang X
- Wasan A
- Watelet J‐B
- Watts WJ
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- Weakley J
- Weber R
- Weber R
- Wechsler ME
- Wei CC
- Wei JL
- Weinberg EA
- Weinhold B
- Weissman JD
- Weitzel EK
- Welch KC
- Welch KC
- Welch KC.
- Wellborn PS
- Wen W LW
- Wen YS
- Wentzel JL
- Weschta M
- Westman M
- Westrin KM
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- Williamson IG
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- Won HK
- Wong AYS
- Wong D
- Wong IW
- Wong IW
- Wong SJ
- Wood AJ
- Wood AJ
- Woodard T
- Woodhouse BM
- Woods CM
- Woodworth BA
- Woodworth BA
- Woodworth BA
- Woodworth BA
- Woodworth BA.
- Workman AD
- Workman AD
- Workman AD
- Workman AD
- Workman AD
- Workman AD
- Wormald PJ
- Wormald PJ
- Wright ED
- Wu AW
- Wu AW
- Wu D
- Wu D
- Wu D
- Wu J
- Wu Y‐X
- Wuister AM
- Wuokko‐Landén A
- Xia Z
- Xian M
- Xu J
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- Xu Z
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- Yan C
- Yan CH
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- Yan CH
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- Yancey KL
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- Yang C
- Yang C
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- Yayik AM
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- Yohai RA
- Yoo F
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- Yoon H
- Yoon HY
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- Young J
- Young Jang T
- Young LC
- Yousefi J
- Yu MS
- Yu X
- Yu XM
- Zabner J
- Zacharek M
- Zainine R
- Zajac AE
- Zalmanovici Trestioreanu A
- Zalmanovici Trestioreanu A
- Zariwala MA
- Zeiger J
- Zeng M
- Zeng M
- Zhai GT
- Zhang L
- Zhang ML
- Zhang N
- Zhang N
- Zhang N
- Zhang Q
- Zhang S
- Zhang S
- Zhang S
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhang Z
- Zhang Z
- Zhang Z
- Zhao CY
- Zhao K
- Zhao K
- Zhao L
- Zhao YC
- Zhao YC
- Zheng C
- Zheng Z
- Zhou B
- Zia S
- Ziegler CGK
- Zielinska‐Blizniewska H
- Zou L
- Zuckerman JD
- Zurlo JJ
- Zuskin E
- Čulig J
- Publication venue
- 'Wiley'
- Publication date
- 01/01/2021
- Field of study
Background: The 5 years since the publication of the first International Consensus Statement on Allergy and Rhinology: Rhinosinusitis (ICAR‐RS) has witnessed foundational progress in our understanding and treatment of rhinologic disease. These advances are reflected within the more than 40 new topics covered within the ICAR‐RS‐2021 as well as updates to the original 140 topics. This executive summary consolidates the evidence‐based findings of the document. Methods: ICAR‐RS presents over 180 topics in the forms of evidence‐based reviews with recommendations (EBRRs), evidence‐based reviews, and literature reviews. The highest grade structured recommendations of the EBRR sections are summarized in this executive summary. Results: ICAR‐RS‐2021 covers 22 topics regarding the medical management of RS, which are grade A/B and are presented in the executive summary. Additionally, 4 topics regarding the surgical management of RS are grade A/B and are presented in the executive summary. Finally, a comprehensive evidence‐based management algorithm is provided. Conclusion: This ICAR‐RS‐2021 executive summary provides a compilation of the evidence‐based recommendations for medical and surgical treatment of the most common forms of RS
Relationship between Vertical Wind Shear and Typhoon Intensity Change, and Development of Three-Predictor Intensity Prediction Model.
- Author
- Publication venue
- 'Meteorological Society of Japan'
- Publication date
- 01/01/2001
- Field of study
Performance of the CMS Level-1 trigger in proton-proton collisions at root s=13 TeV
- Publication venue
- Publication date
- 01/01/2020
- Field of study
At the start of Run 2 in 2015, the LHC delivered proton-proton
collisions at a center-ofmass energy of 13 TeV. During Run 2 (years
2015-2018) the LHC eventually reached a luminosity of 2.1 x 10(34)
cm(-2) s(-1), almost three times that reached during Run 1 (2009-2013)
and a factor of two larger than the LHC design value, leading to events
with up to a mean of about 50 simultaneous inelastic proton-proton
collisions per bunch crossing (pileup). The CMS Level-1 trigger was
upgraded prior to 2016 to improve the selection of physics events in the
challenging conditions posed by the second run of the LHC. This paper
describes the performance of the CMS Level-1 trigger upgrade during the
data taking period of 2016-2018. The upgraded trigger implements pattern
recognition and boosted decision tree regression techniques for muon
reconstruction, includes pileup subtraction for jets and energy sums,
and incorporates pileup-dependent isolation requirements for electrons
and tau leptons. In addition, the new trigger calculates high-level
quantities such as the invariant mass of pairs of reconstructed
particles. The upgrade reduces the trigger rate from background
processes and improves the trigger efficiency for a wide variety of
physics signals
Correlations of azimuthal anisotropy Fourier harmonics with subevent cumulants in pPb collisions at root s(NN)=8.16 TeV
- Publication venue
- Publication date
- 01/01/2021
- Field of study
Event-by-event long-range correlations of azimuthal anisotropy Fourier
coefficients (v(n)) in 8.16 TeV pPb data, collected by the CMS
experiment at the CERN Large Hadron Collider, are extracted using a
subevent four-particle cumulant technique applied to very low
multiplicity events. Each combination of four charged particles is
selected from either two, three, or four distinct subevent regions of a
pseudorapidity range from -2.4 to 2.4 of the CMS tracker, and with
transverse momentum between 0.3 and 3.0 GeV. Using the subevent cumulant
technique, correlations between v(n) of different orders are measured as
functions of particle multiplicity and compared to the standard cumulant
method without subevents over a wide event multiplicity range. At high
multiplicities, the v(2) and v(3) coefficients exhibit an
anticorrelation; this behavior is observed consistently using various
methods. The v(2) and v(4) correlation strength is found to depend on
the number of subevents used in the calculation. As the event
multiplicity decreases, the results from different subevent methods
diverge because of different contributions of noncollective or
few-particle correlations. Correlations extracted with the four-subevent
method exhibit a tendency to diminish monotonically toward the lowest
multiplicity region (about 20 charged tracks) investigated. These
findings extend previous studies to a significantly lower event
multiplicity range and establish the evidence for the onset of
long-range collective multiparticle correlations in small system
collisions
Search for W ` bosons decaying to a top and a bottom quark at root s=13 TeV in the hadronic final state
- Publication venue
- Publication date
- 01/01/2021
- Field of study
A search is performed for W ‘ bosons decaying to a top and a bottom
quark in the all-hadronic final state, in proton-proton collisions at a
center-of-mass energy of 13TeV. The analyzed data were collected by the
CMS experiment between 2016 and 2018 and correspond to an integrated
luminosity of 137fb(-1). Deep neural network algorithms are used to
identify the jet initiated by the bottom quark and the jet containing
the decay products of the top quark when the W ‘ boson from the top
quark decays hadronically. No excess above the estimated standard model
background is observed. Upper limits on the production cross sections of
W ‘ bosons decaying to a top and a bottom quark are set. Both left- and
right-handed W ‘ bosons with masses below 3.4TeV are excluded at 95%
confidence level, and the most stringent limits to date on W ‘ bosons
decaying to a top and a bottom quark in the all-hadronic final state are
obtained. (C) 2021 The Author(s). Published by Elsevier B.V