94 research outputs found
Unveiling a novel transient druggable pocket in BACE-1 through molecular simulations: conformational analysis and binding mode of multisite inhibitors
- Author
- A Shkurti
- AA Gorfe
- AK Ghosh
- AK Ghosh
- AK Ghosh
- B Hess
- B Laurent
- C Galdeano
- Chandra Verma
- Charles A. Laughton
- CI Bayly
- CR Søndergaard
- D Lama
- Diego Muñoz-Torrero
- DJ Selkoe
- DM Skovronsky
- DR Davies
- E Viayna
- F. Javier Luque
- FNB Edfelt
- GB McGaughey
- GR Bowman
- H Park
- HM Berman
- HM Kumalo
- I Bahar
- I Schecter
- J Wang
- J Yuan
- J-P Ryckaert
- Jordi Juárez-Jiménez
- JY Lee
- L Hong
- L Hong
- L McConlogue
- L Zhou
- LC Walker
- LJ Gutierrez
- M Cascella
- MG Kornacker
- MHM Olsson
- MI Fernández-Bachiller
- MS Wolfe
- Ornella Di Pietro
- P Camps
- P Cimermancic
- P Kacker
- P Schmidtke
- R Friedman
- R Vassar
- RT Turner III
- RT Turner III
- S Liu
- S Patel
- S Ruiz-Carmona
- SL Cole
- SL Roberds
- T Darden
- U Essmann
- V Hornak
- V Le Guilloux
- V Oleinikovas
- W Wang
- WL Jorgensen
- Y Xu
- YS Tan
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 15/05/2017
- Field of study
The critical role of BACE-1 in the formation of neurotoxic ß-amyloid peptides in the brain makes it an attractive target for an efficacious treatment of Alzheimer’s disease. However, the development of clinically useful BACE-1 inhibitors has proven to be extremely challeng- ing. In this study we examine the binding mode of a novel potent inhibitor (compound 1, with IC50 80 nM) designed by synergistic combination of two fragments—huprine and rhein— that individually are endowed with very low activity against BACE-1. Examination of crystal structures reveals no appropriate binding site large enough to accommodate 1. Therefore we have examined the conformational flexibility of BACE-1 through extended molecular dynamics simulations, paying attention to the highly flexible region shaped by loops 8–14, 154–169 and 307–318. The analysis of the protein dynamics, together with studies of pocket druggability, has allowed us to detect the transient formation of a secondary binding site, which contains Arg307 as a key residue for the interaction with small molecules, at the edge of the catalytic cleft. The formation of this druggable “floppy” pocket would enable the bind- ing of multisite inhibitors targeting both catalytic and secondary sites. Molecular dynamics simulations of BACE-1 bound to huprine-rhein hybrid compounds support the feasibility of this hypothesis. The results provide a basis to explain the high inhibitory potency of the two enantiomeric forms of 1, together with the large dependence on the length of the oligo- methylenic linker. Furthermore, the multisite hypothesis has allowed us to rationalize the inhibitory potency of a series of tacrine-chromene hybrid compounds, specifically regarding the apparent lack of sensitivity of the inhibition constant to the chemical modifications intro- duced in the chromene unit. Overall, these findings pave the way for the exploration of novel functionalities in the design of optimized BACE-1 multisite inhibitors
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
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- Ahmed A
- Ahuja S
- Aime C
- Akchurin N
- Akgun B
- Akpinar A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allen B
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- Alvarez Gonzalez B
- Alverson G
- Alves GA
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- Alyari M
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- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeinali M
- Zenaiev O
- Zeuner WD
- Zghiche A
- Zhang F
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- Zhang Z
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- Zhokin A
- Zhu DH
- Zhu RY
- Zich J
- Zielinski K
- Ziemons T
- Zientek M
- Zlebcik R
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Österberg K
- Özçelik Ö
- Široký J
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
A search for dark matter in the form of strongly interacting massive particles (SIMPs) using the CMS detector at the LHC is presented. The SIMPs would be produced in pairs that manifest themselves as pairs of jets without tracks. The energy fraction of jets carried by charged particles is used as a key discriminator to suppress efficiently the large multijet background, and the remaining background is estimated directly from data. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 16.1 fb - 1 , collected with the CMS detector in 2016. No significant excess of events is observed above the expected background. For the simplified dark matter model under consideration, SIMPs with masses up to 100 GeV are excluded and further sensitivity is explored towards higher masses
Evidence for Top Quark Production in Nucleus-Nucleus Collisions
- Author
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- Aarup Petersen H
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- Wolfe E
- Wong K
- Wong WY
- Wood D
- Woodard A
- Wozniak KA
- Wozniewski S
- Wright D
- Wu Z
- Wuchterl S
- Wulz C-E
- Wuyckens S
- Wyslouch B
- Wöhrmann C
- Würthwein F
- Xia F
- Xiao J
- Xiao M
- Xiao R
- Xie S
- Xie W
- Yagil A
- Yalvac M
- Yang UK
- Yang YC
- Yao Y
- Yates BR
- Yazgan E
- Yetkin EA
- Yi K
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- Yoo HD
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- Yu D
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- Yumiceva F
- Yusli MN
- Zabi A
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- Zahid S
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- Zhang A
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- Ziemons T
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- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2019
- Field of study
Peer reviewe
Observation of the B-s(0) -> X(3872)phi Decay
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
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- Akgun B
- Akpinar A
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- Alcaraz Maestre J
- Aldaya Martin M
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allen B
- Almond J
- Alvarez Gonzalez B
- Alverson G
- Alves GA
- Aly R
- Alyari M
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- Ambrogi F
- Amendola C
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- Amram O
- Amsler C
- Anagnostou G
- Anderson D
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- Andreev Y
- Andrews MB
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- Ang L
- Antchev G
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
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- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
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- Atakisi IO
- Atanasov I
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awan MIM
- Ayala E
- Aydogmus Sen F
- Azarkin M
- Azhgirey I
- Aziz T
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- Bagaturia I
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- Caminada L
- Campagnari C
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- Capiluppi P
- Cappati A
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- Carle A
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- Carrillo Montoya CA
- Carrillo Moreno S
- Cartiglia N
- Carvalho Antunes De Oliveira A
- Carvalho W
- Casarsa M
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- Cassese A
- Castaldi R
- Castaneda Hernandez A
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- Castro A
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- Cepaitis V
- Cepeda M
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- Chatterjee RM
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- Chauhan S
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- Chawla R
- Chazin Quero B
- Checchia P
- Chekhovsky V
- Chen C
- Chen GM
- Chen HS
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- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
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- Chiarito B
- Chinellato J
- Chistov R
- Chlebana F
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- Choudhary BC
- Choudhury S
- Chu J
- Chudasama R
- Chwalek T
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- Ciocca C
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- Cipriani M
- Ciriolo V
- Cirkovic P
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
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- Clerbaux B
- CMS Collaboration
- Cockerill DJA
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- Colaleo A
- Cole JE
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- Consuegra Rodríguez S
- Contardo D
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- Cornelis T
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- Cossutti F
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- Coubez X
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- Cranshaw DJ
- Creanza D
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- Cumalat JP
- Cummings G
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- de Trocóniz JF
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- Dimitrov A
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- Zhang S
- Zhang W
- Zhang Y
- Zhang Z
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu DH
- Zhu RY
- Ziemons T
- Zientek M
- Zlebcik R
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2020
- Field of study
Using a data sample of proton-proton collisions at root s = 13 TeV, corresponding to an integrated luminosity of 140 fb(-1) collected by the CMS experiment in 2016-2018, the B-s(0) -> X(3872)phi decay is observed. Decays into J/psi pi(+)pi(-) and K+K- are used to reconstruct, respectively, the X(3872) and phi. The ratio of the product of branching fractions B[B-s(0) -> X(3872)phi]B[X(3872) -> J/psi pi(+)pi(-)] to the product B[B-s(0) ->psi(2S)phi]B[psi(2S) -> J/psi pi(+)pi(-)] is measured to be [2.21 +/- 0.29(stat) +/- 0.17(syst)]%. The ratio B[B-s(0) -> X(3872)phi]/B[B-0 -> X(3872)K-0] is found to be consistent with one, while the ratio B[B-s(0) -> X(3872)phi]/B[B+-> X(3872)K+] is two times smaller. This suggests a difference in the production dynamics of the X(3872) in B-0 and B(0)s meson decays compared to B+. The reported observation may shed new light on the nature of the X(3872) particle.Peer reviewe
Observation of a New Excited Beauty Strange Baryon Decaying to Ξb- π+π-
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
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- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- American Physical Society
- Publication date
- 01/01/2021
- Field of study
The Ξb-π+π- invariant mass spectrum is investigated with an event sample of proton-proton collisions at s=13 TeV, collected by the CMS experiment at the LHC in 2016-2018 and corresponding to an integrated luminosity of 140 fb-1. The ground state Ξb- is reconstructed via its decays to J/ψΞ- and J/ψΛK-. A narrow resonance, labeled Ξb(6100)-, is observed at a Ξb-π+π- invariant mass of 6100.3±0.2(stat)±0.1(syst)±0.6(Ξb-) MeV, where the last uncertainty reflects the precision of the Ξb- baryon mass. The upper limit on the Ξb(6100)- natural width is determined to be 1.9 MeV at 95% confidence level. The low Ξb(6100)- signal yield observed in data does not allow a measurement of the quantum numbers of the new state. However, following analogies with the established excited Ξc baryon states, the new Ξb(6100)- resonance and its decay sequence are consistent with the orbitally excited Ξb- baryon, with spin and parity quantum numbers JP=3/2-
Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of τ Leptons in pp collisions at sqrt[s]=13 TeV
- Author
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- Aarup Petersen H
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- Lannon K
- Lariccia P
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- Lath A
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- Lattaud H
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- Laurila S
- Lawhorn JM
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- Lazarovits M
- Le Bihan A-C
- Lechner L
- Lecoq P
- Ledovskoy A
- Lee H
- Lee H
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- Lee K
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- Lee SW
- Lee Y
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- Leggat D
- Legger F
- Lehti S
- Lelas D
- Lelek A
- Lemaitre V
- Lemos DS
- Lenzi B
- Lenzi P
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- Leontsinis S
- Lesauvage A
- Lethuillier M
- Letts J
- Levchuk L
- Levin A
- Lezki S
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- León Holgado J
- Li A
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- Liao H
- Lidrych J
- Liechti SP
- Ligabue F
- Liko D
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- Lintuluoto A
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- Lista L
- Litomin A
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- Liu C
- Liu M
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- Liu Y
- Liu Z-A
- Liyanage K
- Lizzo M
- Lo Meo S
- Lo KH
- Lobanov A
- Locci E
- Loeliger A
- Lohmann W
- Lokhtin I
- Lomidze I
- Long K
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- Longo E
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- Lotfy A
- Lotti M
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- Lukasik M
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- Luo J
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- Lutton D
- Luukka P
- Lychkovskaya N
- Lyon A-M
- Lyons L
- Lyu X
- Lökös S
- Macchiolo A
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- Makarenko V
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- Meneguzzo AT
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- Metzler M
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- Mikulec I
- Mikuni VM
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- Mohammadi A
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- Mukherjee S
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- Netrakanti PK
- Neu C
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- Neutelings I
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- Newman HB
- Ngadiuba J
- Nguyen D
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- Nguyen V
- Ni H
- Nibigira E
- Nickel M
- Nicolaou C
- Niedziela J
- Niedziela M
- Nielsen C
- Nigamova A
- Nikitenko A
- Niknejad T
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- Noll D
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- Novaes SF
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- Nuzzo S
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- Obertino MM
- Obraztsov S
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- Ochando C
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- Ojalvo I
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- Olaiya E
- Olmedo Negrete M
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- Oreshkin V
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- Ozkorucuklu S
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- Padeken K
- Padley BP
- Padula SS
- Paganini P
- Paganis E
- Paganoni M
- Pak SI
- Palencia Cortezon E
- Palichik V
- Palit P
- Palla F
- Palmer C
- Panagiotou A
- Pandey S
- Pandolfi F
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- Pantaleo F
- Panwar L
- Paoletti S
- Paolucci P
- Papadimitriou V
- Papadopoulos I
- Papakrivopoulos I
- Papavergou I
- Pape L
- Paramatti R
- Paramesvaran S
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- Pashenkov A
- Paspalaki G
- Pastika N
- Pastrone N
- Pasztor G
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- Patel R
- Patterson JR
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- Paulitsch P
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- Paus C
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- Pavlov B
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- Pedraza I
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- Pellecchia A
- Pellett D
- Pelliccioni M
- Peltola T
- Pena Rodriguez KJ
- Pena C
- Penzo A
- Perelygin V
- Perera N
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- Perries S
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- Pervan N
- Pesaresi M
- Petkov P
- Petrilli A
- Petrov A
- Petrov V
- Petrow H
- Petrucciani G
- Petrushanko S
- Petyt D
- Pfeiffer A
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- Pieri M
- Pierini M
- Pigazzini S
- Pinna Angioni GL
- Pinna D
- Pinolini BS
- Piparo D
- Piperov S
- Pisano M
- Pistone C
- Pitt M
- Pitters FM
- Pitzl D
- Pivovarov G
- Polatoz A
- Polikarpov S
- Pompili A
- Pook T
- Pooth O
- Popov A
- Popov V
- Popova E
- Postiau N
- Potenza R
- Poudyal N
- Pozdnyakov A
- Pradhan R
- Presilla M
- Prieels C
- Primavera F
- Prisciandaro J
- Priyanka P
- Prokofyev O
- Prosper H
- Psallidas A
- Ptochos F
- Puerta Pelayo J
- Pugliese G
- Pujahari PR
- Puljak I
- Purohit A
- Pérez Adán D
- Pérez-Calero Yzquierdo A
- Pétré L
- Qian SJ
- Qu H
- Quach D
- Quaranta C
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- Rahatlou S
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- Raics P
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- Ramos D
- Ramón Álvarez C
- Rander J
- Rane A
- Ranieri A
- Ranjan K
- Ranken E
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- Rappoccio S
- Raspereza A
- Rastogi A
- Rath Y
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- Ratti MG
- Ratti SP
- Rauser J
- Ravera F
- Rawal N
- Raymond DM
- Razis PA
- Re V
- Reales Gutiérrez G
- Rebassoo F
- Rebello Teles P
- Redaelli N
- Redjimi R
- Redondo I
- Reed I
- Regnard S
- Regnery B
- Reichert J
- Reichmann M
- Reid ID
- Reid M
- Reimers A
- Reinsvold Hall A
- Reis T
- Reissel C
- Reitenspiess T
- Reithler H
- Rejeb Sfar H
- Rembser J
- Revering M
- Reyes-Almanza R
- Ribeiro Lopes B
- Riccardi C
- Richards A
- Richman J
- Rieger M
- Rieger O
- Rinkevicius A
- Ristic B
- Ristori L
- Rizzi A
- Robmann P
- Robutti E
- Rodozov M
- Rodrigo T
- Rodríguez Bouza V
- Roemer J
- Rogan C
- Roguljic M
- Roh Y
- Rohe T
- Rohlf J
- Roland C
- Roland G
- Rolandi G
- Romeo F
- Romero L
- Ronchese P
- Rose A
- Rosenzweig D
- Rosenzweig S
- Roskas C
- Roskes J
- Rosowsky A
- Rossi A
- Rossi AM
- Rossi B
- Rossin R
- Rotter J
- Rout PK
- Rovelli C
- Rovelli T
- Rovere M
- Roy Chowdhury S
- Roy A
- Roy D
- Roy T
- Royon C
- Ruchti R
- Rudrabhatla S
- Ruini D
- Ruiz Alvarez JD
- Ruiz-Jimeno A
- Rumerio P
- Rusack R
- Ruspa M
- Ryd A
- Rykaczewski H
- Ryu MS
- Ryutin R
- Rádl AJ
- Röwert N
- Rübenach J
- Safonov A
- Saggio A
- Sagir S
- Saha G
- Saha P
- Sahasransu AR
- Sahin MÖ
- Sahu B
- Saibel A
- Saka H
- Sakulin H
- Salazar González CA
- Salazar Ibarguen HA
- Salerno R
- Salfeld-Nebgen J
- Saltzberg D
- Salur S
- Salvatico R
- Salvini P
- Salyer K
- Samalan A
- Sanchez Cruz S
- Sanchez A
- Sanchez-Hernandez A
- Sandeep K
- Sanders S
- Santanastasio F
- Santocchia A
- Santoro A
- Sanz Becerra DA
- Saoulidou N
- Saradhy R
- Sarica U
- Sarkar S
- Sarkar T
- Sarkar U
- Sathia Narayanan BV
- Saunders M
- Sauvan JB
- Savard C
- Savin A
- Savina M
- Savitskyi M
- Savoiu D
- Savoy-Navarro A
- Savrin V
- Sawant S
- Scarfi S
- Scham M
- Scheurer V
- Schiber C
- Schieck J
- Schleper P
- Schmidt A
- Schmitt MH
- Schmitz E
- Schnepf M
- Schnetzer S
- Schroeder N
- Schröder M
- Schuh T
- Schuler SC
- Schulte JF
- Schulz J
- Schwandt J
- Schwanenberger C
- Schwarz D
- Schweiger K
- Schwick C
- Schäfer C
- Schöfbeck R
- Schütze P
- Sciacca C
- Scodellaro L
- Scott E
- Scribano A
- Sculac T
- Seez C
- Sehrawat A
- Seidel M
- Seidita R
- Seif El Nasr-Storey S
- Seith D
- Seitova D
- Seixas J
- Sekmen S
- Selivanova D
- Selvaggi G
- Selvaggi M
- Sen S
- Seo H
- Sert H
- Setti F
- Sexton-Kennedy E
- Sguazzoni G
- Shafiei N
- Shah A
- Shah MA
- Shalaev V
- Shang V
- Sharan M
- Sharma A
- Sharma A
- Sharma A
- Sharma R
- Sharma S
- Sharma V
- Sharma V
- Shchablo K
- Shchedrolosiev M
- Shchelina K
- Sheldon P
- Shepherd-Themistocleous CH
- Sheplock J
- Shi K
- Shi W
- Shi Z
- Shmatov S
- Shoaib M
- Shopova M
- Shtipliyski A
- Shukla P
- Shulha S
- Shvetsov I
- Si W
- Siado JE
- Siddireddy P
- Siikonen H
- Sikdar AK
- Sikler F
- Silva Do Amaral SM
- Silva P
- Silvestris L
- Simone FM
- Simonetto F
- Simonis HJ
- Simpson F
- Simsek AE
- Singh B
- Singh JB
- Sirois Y
- Siroli GP
- Siviero F
- Skinnari L
- Skovpen K
- Skovpen Y
- Skuja A
- Slabospitskii S
- Smirnov I
- Smirnov V
- Smith C
- Smith N
- Smith VJ
- Smith WH
- Snoeys W
- Snow GR
- Snyder C
- Sobol A
- Soffi L
- Soha A
- Sola V
- Solano A
- Soldi D
- Somalwar S
- Song D
- Sonnadara DUJ
- Sonneveld J
- Sordini V
- Sorrentino G
- Sosa Ricardo RE
- Sosnov D
- Soto Rodríguez A
- Spagnolo P
- Spalding WJ
- Spanier S
- Sperka D
- Sphicas P
- Spiegel L
- Spiga D
- Spiropulu M
- Spitzbart D
- Srimanobhas N
- Stadie H
- Stafford D
- Stahl Leiton AG
- Stahl A
- Staiano A
- Stakia A
- Stampf V
- Starling E
- Starodumov A
- Steen A
- Steggemann J
- Steinbrück G
- Stenson K
- Stepennov A
- Stephans GSF
- Stickland D
- Stojanovic M
- Stone B
- Stone R
- Stoynev S
- Strait J
- Strobbe N
- Strologas J
- Strong G
- Stuart D
- Sturdy J
- Stylianou N
- Suarez I
- Sulimov V
- Sultanov G
- Summers S
- Sun W
- Sunar Cerci D
- Sur N
- Surányi O
- Susa T
- Sutantawibul C
- Swain SK
- Swartz M
- Szillasi Z
- Szleper M
- Sznajder A
- Sánchez Navas S
- Tabarelli de Fatis T
- Tabb W
- Tadel M
- Takahashi Y
- Tali B
- Taliercio A
- Tamulaitis G
- Tani L
- Tannenwald B
- Tao J
- Tapia Takaki JD
- Tapper A
- Tarabini A
- Tatar K
- Taus R
- Tavernier S
- Tavolaro VR
- Taylor D
- Taylor L
- Tcherniaev E
- Teague D
- Tedeschi T
- Teklishyn M
- Tekten S
- Templ S
- Tenchini R
- Teodorescu L
- Terkulov A
- Teroerde M
- Terrill W
- Teryaev O
- Tews A
- Teyssier D
- Thakur S
- Thayil SA
- Theofilatos K
- Thiel M
- Thieman J
- Thom J
- Thomas L
- Thomas S
- Thomas-Wilsker J
- Tiras E
- Tishelman-Charny A
- Titov M
- Tiwari PC
- Tkaczyk S
- Tok UG
- Toldaiev O
- Tomalin IR
- Tomei TRFP
- Toms M
- Tonelli G
- Tonjes MB
- Tonon N
- Toriashvili T
- Torims T
- Tornago M
- Toropin A
- Torres Da Silva De Araujo F
- Torterotot L
- Tosi M
- Tosi S
- Touquet G
- Townsend A
- Tramontano R
- Tran NV
- Tran TT
- Trapote A
- Treille D
- Trembath-Reichert S
- Trevisani N
- Tricomi A
- Trocino D
- Trocsanyi ZL
- Tropea P
- Troshin S
- Tsamalaidze Z
- Tsatsos A
- Tsipolitis G
- Tsirou A
- Tully C
- Tumasyan A
- Tuo S
- Tuominen E
- Tuominiemi J
- Turini N
- Turkcapar S
- Tuuva T
- Tuve C
- Tytgat M
- Tyurin N
- Tziaferi E
- Uchida K
- Ujvari B
- Ulmer KA
- Ulrich R
- Uniyal R
- Uplegger L
- Urda Gómez L
- Uribe Estrada C
- Usai E
- Uvarov L
- Uzunian A
- Vaandering EW
- Vagnerini A
- Vai I
- Valencia Palomo L
- Valsecchi D
- Valuev V
- Van De Klundert M
- Van Der Linden J
- Van Doninck W
- Van Hove P
- Van Mechelen P
- Van Mulders P
- Van Onsem GP
- Van Putte S
- Van Remortel N
- Vanden Bemden M
- Vander Donckt M
- Vander Velde C
- Vanlaer P
- Varela J
- Varelas N
- Vargas Hernandez AM
- Vartak A
- Vats D
- Vazquez Valencia F
- Vazzoler F
- Veckalns V
- Veelken C
- Velasco M
- Velkovska J
- Vellidis K
- Venditti R
- Venturi A
- Verdini PG
- Veres GI
- Vermassen B
- Verwilligen P
- Veszpremi V
- Vetens W
- Viazlo O
- Vico Villalba C
- Vigilante L
- Viinikainen J
- Vila I
- Vilela Pereira A
- Viliani L
- Virdee T
- Virdi AK
- Viret S
- Vischia P
- Vit M
- Vitulo P
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vojinovic M
- Volkov A
- Volkov S
- Volobouev I
- Von Cube RF
- Vorobyev A
- Vourliotis E
- Voutilainen M
- Voytishin N
- Vámi TÁ
- Wadud MA
- Wagner SR
- Walkingshaw Pass K
- Wallny R
- Walsh R
- Waltenberger W
- Walter D
- Wamorkar T
- Wan Abdullah WAT
- Wanczyk J
- Wang B
- Wang C
- Wang D
- Wang F
- Wang H
- Wang J
- Wang J
- Wang J
- Wang L
- Wang Q
- Wang Q
- Wang S
- Wang X
- Wang Y
- Wang Z
- Wang Z
- Waqas M
- Wardle N
- Warner Z
- Wassmer M
- Watson IJ
- Wayne M
- Webb SN
- Weber HA
- Weber M
- Wei K
- Wen Y
- Wertz S
- West C
- Wezenbeek L
- Whitbeck A
- White R
- White S
- Wichmann K
- Wickramage N
- Wickramarathna DDC
- Wiedenbeck S
- Wieland S
- Wiens L
- Wightman A
- Williams A
- Williams J
- Williams T
- Willmott C
- Wilson G
- Wilson J
- Wimpenny S
- Winer BL
- Winterbottom D
- Wisecarver A
- Wissing C
- Wittich P
- Wolf R
- Wolfe E
- Wong K
- Wong WY
- Wood D
- Wozniak KA
- Wozniewski S
- Wright D
- Wu HY
- Wu Z
- Wuchterl S
- Wulz C-E
- Wunsch S
- Wyslouch B
- Würthwein F
- Xiang Y
- Xiao J
- Xiao M
- Xiao R
- Xie S
- Xie W
- Yagil A
- Yalvac M
- Yan F
- Yan X
- Yang S
- Yang S
- Yang UK
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Ye Z
- Yetkin EA
- Yi K
- Yigitbasi E
- Yohay R
- Yoo HD
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu GB
- Yu I
- Yu PR
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yumiceva F
- Yusli MN
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeinali M
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
- Zhang Y
- Zhang Z
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu DH
- Zhu RY
- Ziemons T
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
- Zou D
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
Measurements of the inclusive and differential fiducial cross sections of the Higgs boson are presented, using the τ lepton decay channel. The differential cross sections are measured as functions of the Higgs boson transverse momentum, jet multiplicity, and transverse momentum of the leading jet in the event, if any. The analysis is performed using proton-proton collision data collected with the CMS detector at the LHC at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 138 fb^{-1}. These are the first differential measurements of the Higgs boson cross section in the final state of two τ leptons. In final states with a large jet multiplicity or with a Lorentz-boosted Higgs boson, these measurements constitute a significant improvement over measurements performed in other final states
Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at root s=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Adán DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aime' C
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- Akgun B
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- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks is performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 35.9 fb(-1). The signal is characterized by a large missing transverse momentum recoiling against a bottom quark-antiquark system that has a large Lorentz boost. The number of events observed in the data is consistent with the standard model background prediction. Results are interpreted in terms of limits both on parameters of the type-2 two-Higgs doublet model extended by an additional light pseudoscalar boson a (2HDM+a) and on parameters of a baryonic Z simplified model. The 2HDM+a model is tested experimentally for the first time. For the baryonic Z model, the presented results constitute the most stringent constraints to date.Peer reviewe
A Deep Neural Network for Simultaneous Estimation of b Jet Energy and Resolution
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Adán DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmad WH
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Allen B
- Almond J
- Alonso AG
- Alvarez JDR
- Alverson G
- Alves FL
- Alves GA
- Aly R
- 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
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- Angioni GLP
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- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2020
- Field of study
We describe a method to obtain point and dispersion estimates for the energies of jets arising from b quarks produced in proton-proton collisions at an energy of s = 13 TeV at the CERN LHC. The algorithm is trained on a large sample of simulated b jets and validated on data recorded by the CMS detector in 2017 corresponding to an integrated luminosity of 41 fb - 1 . A multivariate regression algorithm based on a deep feed-forward neural network employs jet composition and shape information, and the properties of reconstructed secondary vertices associated with the jet. The results of the algorithm are used to improve the sensitivity of analyses that make use of b jets in the final state, such as the observation of Higgs boson decay to b b ¯
Search for the X(5568) State Decaying into B-s(0)pi(+/-) in Proton-Proton Collisions at root s=8 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- 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
- Aldaya Martin M
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alimena J
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- Alunni Solestizi L
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- Publication venue
- Publication date
- 01/01/2017
- Field of study
A search for resonancelike structures in the B-s(0)pi(+/-) invariant mass spectrum is performed using proton-proton collision data collected by the CMS experiment at the LHC at root s = 8 TeV, corresponding to an integrated luminosity of 19.7 fb(-1). The B-s(0) mesons are reconstructed in the decay chain B-s(0) -> J/Psi phi, with J/Psi -> mu(+) mu(-) and phi -> K+K-. The B-s(0)pi(+/-) invariant mass distribution shows no statistically significant peaks for different selection requirements on the reconstructed B-s(0) and pi(+/-) candidates. Upper limits are set on the relative production rates of the X(5568) and B-s(0) states times the branching fraction of the decay X(5568)(+/-) -> B-s(0)pi(+/-). In addition, upper limits are obtained as a function of the mass and the natural width of possible exotic states decaying into B-s(0)pi(+/-).Peer reviewe
Search for lepton flavour violating decays of a neutral heavy Higgs boson to μτ and eτ in proton-proton collisions at s√ = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullin S
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- Acharya H
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- Özçelik Ö
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2020
- Field of study
A search for lepton flavour violating decays of a neutral non-standard-model Higgs boson in the μτ and eτ decay modes is presented. The search is based on proton-proton collisions at a center of mass energy s√ = 13 TeV collected with the CMS detector in 2016, corresponding to an integrated luminosity of 35.9 fb−1. The τ leptons are reconstructed in the leptonic and hadronic decay modes. No signal is observed in the mass range 200–900 GeV. At 95% confidence level, the observed (expected) upper limits on the production cross section multiplied by the branching fraction vary from 51.9 (57.4) fb to 1.6 (2.1) fb for the μτ and from 94.1 (91.6) fb to 2.3 (2.3) fb for the eτ decay modes
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