135 research outputs found
Approaches in biotechnological applications of natural polymers
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- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2016
- Field of study
Natural polymers, such as gums and mucilage, are biocompatible, cheap, easily available and non-toxic materials of native origin. These polymers are increasingly preferred over synthetic materials for industrial applications due to their intrinsic properties, as well as they are considered alternative sources of raw materials since they present characteristics of sustainability, biodegradability and biosafety. As definition, gums and mucilages are polysaccharides or complex carbohydrates consisting of one or more monosaccharides or their derivatives linked in bewildering variety of linkages and structures. Natural gums are considered polysaccharides naturally occurring in varieties of plant seeds and exudates, tree or shrub exudates, seaweed extracts, fungi, bacteria, and animal sources. Water-soluble gums, also known as hydrocolloids, are considered exudates and are pathological products; therefore, they do not form a part of cell wall. On the other hand, mucilages are part of cell and physiological products. It is important to highlight that gums represent the largest amounts of polymer materials derived from plants. Gums have enormously large and broad applications in both food and non-food industries, being commonly used as thickening, binding, emulsifying, suspending, stabilizing agents and matrices for drug release in pharmaceutical and cosmetic industries. In the food industry, their gelling properties and the ability to mold edible films and coatings are extensively studied. The use of gums depends on the intrinsic properties that they provide, often at costs below those of synthetic polymers. For upgrading the value of gums, they are being processed into various forms, including the most recent nanomaterials, for various biotechnological applications. Thus, the main natural polymers including galactomannans, cellulose, chitin, agar, carrageenan, alginate, cashew gum, pectin and starch, in addition to the current researches about them are reviewed in this article.. }To the Conselho Nacional de Desenvolvimento Cientfíico e Tecnológico (CNPq) for fellowships (LCBBC and MGCC) and the Coordenação de Aperfeiçoamento de Pessoal de Nvíel Superior (CAPES) (PBSA). This study was supported by the Portuguese Foundation for Science and Technology (FCT) under the scope of the strategic funding of UID/BIO/04469/2013 unit, the Project RECI/BBB-EBI/0179/2012 (FCOMP-01-0124-FEDER-027462) and COMPETE 2020 (POCI-01-0145-FEDER-006684) (JAT)
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Pan-cancer analysis of whole genomes
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- Xia
- Xiang
- Xiong
- xo Abeshouse
- xp Benz
- xp Edwards
- xr Ghori
- xs Gundem
- Xue
- xv Luxton
- xw McDermott
- xy Visakorpi
- xz Whitaker
- Y. -E. ot
- Y. -J. k
- Y. -J. xn
- Y. abp
- Y. ae
- Y. ae
- Y. ae
- Y. ae
- Y. ai
- Y. aj
- Y. al
- Y. bk
- Y. dg
- Y. dy
- Y. ef
- Y. ep
- Y. ez
- Y. ff
- Y. fr
- Y. fv
- Y. fv
- Y. gl
- Y. hl
- Y. hq
- Y. hq
- Y. ia
- Y. kq
- Y. lw
- Y. nh
- Y. nk
- Y. nz
- Y. rg
- Y. rj
- Y. rm
- Y. S. jf
- Y. uz
- Y. vr
- Y. wt
- Y. yc
- ya Al-Ahmadie
- Yachida
- Yamaguchi
- Yamaguchi T. N. k
- Yamamoto
- Yamaue
- Yang
- Yang
- Yang
- Yang
- Yang
- Yao
- Yaspo
- Yates
- Yau
- yb Ally
- yd Cherniack
- yd Lai
- yd Schadendorf
- ye Auman
- ye Umbricht
- Yellapantula
- Yellapantula
- yh Bathe
- yj Baylin
- Yoon
- Yu
- Yu
- Yu
- Yuan
- Yugawa
- z ah
- Z. ej
- Z. ep
- Z. fr
- Z. hv
- Z. hy
- Z. jq
- Z. kt
- Z. oe
- Zaikova
- Zapatka
- zd Gershenwald
- Zenklusen
- Zeps
- zf Ghossein
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang H. b
- Zhao
- Zheng
- Zhou
- Zhou
- Zhu
- Zhu
- zi zj
- zm Jayaseelan
- Zou
- Zou
- zt Kim
- zw Lewis
- Ó. A. th
- Ø. sk
- Publication venue
- Publication date
- 11/12/2019
- Field of study
Cancer is driven by genetic change, and the advent of massively parallel sequencing has enabled systematic documentation of this variation at the whole-genome scale(1-3). Here we report the integrative analysis of 2,658 whole-cancer genomes and their matching normal tissues across 38 tumour types from the Pan-Cancer Analysis of Whole Genomes (PCAWG) Consortium of the International Cancer Genome Consortium (ICGC) and The Cancer Genome Atlas (TCGA). We describe the generation of the PCAWG resource, facilitated by international data sharing using compute clouds. On average, cancer genomes contained 4-5 driver mutations when combining coding and non-coding genomic elements; however, in around 5% of cases no drivers were identified, suggesting that cancer driver discovery is not yet complete. Chromothripsis, in which many clustered structural variants arise in a single catastrophic event, is frequently an early event in tumour evolution; in acral melanoma, for example, these events precede most somatic point mutations and affect several cancer-associated genes simultaneously. Cancers with abnormal telomere maintenance often originate from tissues with low replicative activity and show several mechanisms of preventing telomere attrition to critical levels. Common and rare germline variants affect patterns of somatic mutation, including point mutations, structural variants and somatic retrotransposition. A collection of papers from the PCAWG Consortium describes non-coding mutations that drive cancer beyond those in the TERT promoter(4); identifies new signatures of mutational processes that cause base substitutions, small insertions and deletions and structural variation(5,6); analyses timings and patterns of tumour evolution(7); describes the diverse transcriptional consequences of somatic mutation on splicing, expression levels, fusion genes and promoter activity(8,9); and evaluates a range of more-specialized features of cancer genomes(8,10-18).Peer reviewe
Dijet Resonance Search with Weak Supervision Using root S=13 TeV pp Collisions in the ATLAS Detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
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- Alonso F
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- Alviggi MG
- Amaral Coutinho Y
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- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 25/09/2020
- Field of study
This Letter describes a search for narrowly resonant new physics using a machine-learning anomaly
detection procedure that does not rely on signal simulations for developing the analysis selection. Weakly
supervised learning is used to train classifiers directly on data to enhance potential signals. The targeted
topology is dijet events and the features used for machine learning are the masses of the two jets. The
resulting analysis is essentially a three-dimensional search A → BC, for mA ∼ OðTeVÞ, mB; mC ∼
Oð100 GeVÞ and B, C are reconstructed as large-radius jets, without paying a penalty associated with
a large trials factor in the scan of the masses of the two jets. The full run 2 ffiffi
s p ¼ 13 TeV pp collision
dataset of 139 fb−1 recorded by the ATLAS detector at the Large Hadron Collider is used for the search.
There is no significant evidence of a localized excess in the dijet invariant mass spectrum between 1.8 and
8.2 TeV. Cross-section limits for narrow-width A, B, and C particles vary with mA, mB, and mC. For
example, when mA ¼ 3 TeV and mB ≳ 200 GeV, a production cross section between 1 and 5 fb is
excluded at 95% confidence level, depending on mC. For certain masses, these limits are up to 10 times
more sensitive than those obtained by the inclusive dijet search. These results are complementary to the
dedicated searches for the case that B and C are standard model boson
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector
- Author
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- Miller LS
- Milosavljevic MV
- Milov A
- Milstead DA
- Minaenko AA
- Minashvili IA
- Mince L
- Mincer A
- Mindur B
- Mineev M
- Minegishi Y
- Mino Y
- Miotto GL
- Mir LM
- Mironova M
- Mitani T
- Mitrevski J
- Mitsou VA
- Mittal M
- Miu O
- Miucci A
- Miyagawa PS
- Mizukami A
- Mjornmark JU
- Mkrtchyan T
- Mlynarikova M
- Moa T
- Mobius S
- Mochizuki K
- Moder P
- Mogg P
- Mohamed ATA
- Mohapatra S
- Moles-Valls R
- Monig K
- Monnier E
- Montalbano A
- Montella M
- Monticelli F
- Monzani S
- Morales AR
- Morales FAJ
- Morange N
- Moreira De Carvalho AL
- Moreno Llacer M
- Moreno Martinez C
- Moreno D
- Morettini P
- Morgenstern M
- Morgenstern S
- Mori D
- Morii M
- Morinaga M
- Morisbak V
- Morley AK
- Mornacchi G
- Morris AP
- Morvaj L
- Moschovakos P
- Moser B
- Mosidze M
- Moskalets T
- Moskvitina P
- Moss J
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- Muanza S
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- Muenstermann D
- Muino PC
- Mullier GA
- Mungo DP
- Munoz Martinez JL
- Murin P
- Murray WJ
- Murrone A
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- Muskinja M
- Mwewa C
- Myagkov AG
- Myers AA
- Myers G
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- Myska M
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- Nag AN
- Nagai K
- Nagano K
- Nagasaka Y
- Nagle JL
- Nagy E
- Nairz AM
- Nakahama Y
- Nakamura K
- Nakamura T
- Nanjo H
- Napolitano F
- Narayan R
- Naryshkin I
- Naseri M
- Naumann T
- Navarro G
- Navarro LB
- Nechaeva PY
- Nechansky F
- Neep TJ
- Negri A
- Negrini M
- Nellist C
- Nelson C
- Nelson ME
- Nemecek S
- Nessi M
- Neubauer MS
- Neuhaus F
- Neumann M
- Newhouse R
- Newman PR
- Ng CW
- Ng YS
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- Nguyen HDN
- Nibigira E
- Nickerson RB
- Nicolaidou R
- Nielsen DS
- Nielsen J
- Niemeyer M
- Nikiforou N
- Nikolaenko V
- Nikolic-Audit I
- Nikolopoulos K
- Nilsson P
- Nindhito HR
- Nisati A
- Nishu N
- Nisius R
- Nitsche I
- Nitta T
- Nobe T
- Noel DL
- Noguchi Y
- Nomidis I
- Nomura MA
- Nordberg M
- Novak J
- Novak T
- Novgorodova O
- Novotny R
- Nozka L
- Ntekas K
- Nurse E
- O'Connor K
- O'Keefe MW
- O'Neil DC
- O'neill AP
- O'Shea V
- Oakham FG
- Ocariz J
- Ochi A
- Ochoa I
- Ochoa-Ricoux JP
- Oda S
- Odaka S
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- Ogrodnik A
- Oh A
- Ohm CC
- Oide H
- Oishi R
- Ojeda ML
- Okawa H
- Okazaki Y
- Okumura Y
- Olariu A
- Oleiro Seabra LF
- Olivares Pino SA
- Oliveira MVS
- Oliver JL
- Olsson MJR
- Olszewski A
- Olszowska J
- Onofre A
- Onyisi PUE
- Oppen H
- Oreglia MJ
- Orellana GE
- Orestano D
- Orlando N
- Orr RS
- Ospanov R
- Otero Y Garzon G
- Otono H
- Ott PS
- Ottino GJ
- Ouchrif M
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- Ouraou A
- Outschoorn VIM
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- Owen M
- Owen RE
- Ozcan VE
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- Pacalt J
- Pacey HA
- Pachal K
- Pacheco Pages A
- Padilla Aranda C
- Palacino G
- Palazzo S
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- Pani P
- Panizzo G
- Paolozzi L
- Papadatos C
- Papageorgiou K
- Parajuli S
- Paramonov A
- Paraskevopoulos C
- Pardos CD
- Parida B
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- Parker MA
- Parodi F
- Parrish EW
- Parsons JA
- Parzefall U
- Pascual JAG
- Pascuzzi VR
- Pasner JMP
- Pasquali F
- Pasqualucci E
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- Pastor ET
- Pastore F
- Pasuwan P
- Pataraia S
- Pater JR
- Pathak A
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- Pearkes J
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- Pena JJ
- Penc O
- Peng C
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- Perego MM
- Pereira Peixoto AP
- Pereira RA
- Perepelitsa D
- Perini L
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- Perrella S
- Perrevoort A
- Peters K
- Peters RFY
- Petersen BA
- Petersen TC
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- Pettersson NE
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- Peyaud A
- Pezoa R
- Pezzotti L
- Pham T
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- Phipps MW
- Piacquadio G
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- Picazio A
- Pickles RH
- Piegaia R
- Pietreanu D
- Pilcher JE
- Pilkington AD
- Pinamonti M
- Pineda AS
- Pinfold JL
- Pinto JVDF
- Pitt M
- Pizzimento L
- Pizzini A
- Pleier M-A
- Plesanovs V
- Pleskot V
- Plotnikova E
- Podberezko P
- Poettgen R
- Poggi R
- Poggioli L
- Pogrebnyak I
- Pohl D
- Pokharel I
- Polesello G
- Poley A
- Policicchio A
- Polifka R
- Polini A
- Pollard CS
- Polychronakos V
- Ponce JMI
- Ponomarenko D
- Pontecorvo L
- Popa S
- Popeneciu GA
- Portales L
- Pospisil S
- Potamianos K
- Potrap IN
- Potter CJ
- Potti H
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- Poveda J
- Powell TD
- Pownall G
- Pozo Astigarraga ME
- Prades Ibanez A
- Pralavorio P
- Prapa MM
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- Proffitt ML
- Proklova N
- Prokofiev K
- Prokoshin F
- Protopopescu S
- Proudfoot J
- Przybycien M
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- Quintero DMP
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- Rahal G
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- Ran K
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- Rauch DM
- Rauscher F
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- Ravina B
- Ravinovich I
- Rawling JH
- Raymond M
- Read AL
- Readioff NP
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- Rebuzzi DM
- Redlinger G
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- Reikher D
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- Rej A
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- Renardi A
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- Rendel MB
- Rennie AG
- Renous DS
- Renteria CG
- Resconi S
- Resseguie ED
- Rettie S
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- Reynolds E
- Rezanova OL
- Reznicek P
- Ricci E
- Richter R
- Richter S
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- Ridel M
- Rieck P
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- Rimoldi A
- Rimoldi M
- Rinaldi L
- Rinn TT
- Ripellino G
- Riu I
- Rivadeneira P
- Rizatdinova F
- Rizvi E
- Rizzi C
- Robertson SH
- Robin M
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- Robson A
- Rocchi A
- Roda C
- Rodriguez Bosca S
- Rodriguez AR
- Roe S
- Roggel J
- Rohne O
- Rohrig R
- Rojas RA
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- Roland CPA
- Roloff J
- Romaniouk A
- Romano M
- Rompotis N
- Ronzani M
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- Rosati S
- Rosin G
- Rosser BJ
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- Rossi LP
- Rossini L
- Rosten R
- Rotaru M
- Rottler B
- Rousseau D
- Rovelli G
- Roy A
- Roy D
- Rozanov A
- Rozas AJ
- Rozen Y
- Ruan X
- Ruggeri TA
- Ruhr F
- Ruiz-Martinez A
- Rummler A
- Rurikova Z
- Rusakovich NA
- Russell HL
- Rustige L
- Rutherfoord JP
- Ruttinger EM
- Rybar M
- Rybkin G
- Rye EB
- Ryzhov A
- Sabater Iglesias JA
- Sabatini P
- Sabetta L
- Sacerdoti S
- Sadrozinski HF-W
- Sadykov R
- Saenz SRP
- Safdari M
- Saha P
- Saha S
- Sahinsoy M
- Sahu A
- Saimpert M
- Saito M
- Saito T
- Sakamoto H
- Salamani D
- Salamanna G
- Salnikov A
- Salt J
- Salvador Salas A
- Salvatore D
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- Salzburger A
- Samani BS
- Samarati J
- Sammel D
- Sampsonidis D
- Sampsonidou D
- Sanchez CAS
- Sanchez FJM
- Sanchez J
- Sanchez LP
- Sandaker H
- Sander CO
- Sanderswood IG
- Sandhoff M
- Sandoval C
- Sankey DPC
- Sannino M
- Sano Y
- Sansoni A
- Santoni C
- Santos H
- Santpur SN
- Santra A
- Santurio EV
- Saoucha KA
- Sapronov A
- Saraiva JG
- Sasaki O
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- Sauerburger F
- Sauvan E
- Savard P
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- Sayago Galvan I
- Sbarra C
- Sbrizzi A
- Scanlon T
- Schaarschmidt J
- Schacht P
- Schaefer D
- Schaefer L
- Schafer U
- Schaffer AC
- Schaile D
- Schamberger RD
- Schanet E
- Scharf C
- Scharmberg N
- Schegelsky VA
- Scheirich D
- Schenck F
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- Schiavi C
- Schildgen LK
- Schillaci ZM
- Schioppa EJ
- Schioppa M
- Schleicher KE
- Schlenker S
- Schmidt-Sommerfeld KR
- Schmieden K
- Schmitt C
- Schmitt S
- Schoeffel L
- Schoening A
- Scholer PG
- Schopf E
- Schott M
- Schouwenberg JFP
- Schovancova J
- Schramm S
- Schroeder F
- Schroeder TV
- Schulte A
- Schultz-Coulon H-C
- Schumacher M
- Schumm BA
- Schune P
- Schwartzman A
- Schwarz TA
- Schwemling P
- Schwienhorst R
- Sciandra A
- Sciolla G
- Scuri F
- Scutti F
- Scyboz LM
- Sebastiani CD
- Sedlaczek K
- Seema P
- Seidel SC
- Seiden A
- Seidlitz BD
- Seiss T
- Seitz C
- Seixas JM
- Sekhniaidze G
- Sekula SJ
- Semprini-Cesari N
- Sen S
- Serfon C
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- Serkin L
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- Sevova S
- Sforza F
- Sfyrla A
- Shabalina E
- Shahinian JD
- Shaikh NW
- Shan LY
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- Sharma A
- Sharma AS
- Shatalov PB
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- Shaw SM
- Shehade M
- Shen Y
- Sherman AD
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- Shimogama Y
- Shimojima M
- Shinner JD
- Shipsey IPJ
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- Shiyakova M
- Shlomi J
- Shmeleva A
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- Shope DR
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- Shrif EM
- Shroff MJ
- Shulga E
- Sicho P
- Sickles AM
- Sidiropoulou O
- Sidoti A
- Siegert F
- Silva M
- Silverstein SB
- Simion S
- Simoniello R
- Simpson-allsop CJ
- Simsek S
- Sinervo P
- Sinetckii V
- Singh S
- Sinha S
- Sioli M
- Siral I
- Sivoklokov SY
- Sjolin J
- Skaf A
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith EA
- Smith HA
- Smizanska M
- Smolek K
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- Snesarev AA
- Snoek HL
- Snyder IM
- Snyder S
- Sobie R
- Soffer A
- Sogaard A
- Sohns F
- Sola JDB
- Soldatov EY
- Soldevila U
- Solis AL
- Solodkov AA
- Soloshenko A
- Solovyanov O
- Solovyev V
- Sommer P
- Son H
- Sonay A
- Song W
- Song WY
- Sopczak A
- Sopio AL
- Sopkova F
- Sottocornola S
- Soualah R
- Soukharev AM
- South D
- Spagnolo S
- Spalla M
- Spangenberg M
- Spano F
- Sperlich D
- Spieker TM
- Spigo G
- Spina M
- Spiteri DP
- Spousta M
- Stabile A
- Stamas BL
- Stamen R
- Stamenkovic M
- Stampekis A
- Stanecka E
- Stanislaus B
- Stanitzki MM
- Stankaityte M
- Stapf B
- Starchenko EA
- Stark GH
- Stark J
- Staroba P
- Starovoitov P
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- Steinhebel AL
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- Stewart GA
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- Stolarski M
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- Straessner A
- Strandberg J
- Strandberg S
- Strauss M
- Strebler T
- Strizenec P
- Strohmer R
- Strom DM
- Stroynowski R
- Strubig A
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Su D
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- Suarez NB
- Suarez RG
- Sulin VV
- Sullivan MJ
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
- Sun X
- Suster CJE
- Sutton MR
- Suzuki S
- Svatos M
- Swiatlowski M
- Swift SP
- Swirski T
- Sydorenko A
- Sykora I
- Sykora M
- Sykora T
- Ta D
- Tackmann K
- Taenzer J
- Taffard A
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- Tagiev E
- Taibah RHM
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- Talyshev AA
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- Tarem S
- Tariq K
- Tarna G
- Tartarelli GF
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- Tasevsky M
- Tassi E
- Tateno G
- Tayalati Y
- Taylor AJ
- Taylor GN
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- Tee AS
- Tehrani FS
- Teixeira-Dias P
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- Teoh JJ
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- Terron J
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- Theveneaux-Pelzer T
- Thomas DW
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- Thorpe EJ
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
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- Tisserant S
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- Trofymov A
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- Tsirigotis A
- Tsiskaridze V
- Tskhadadze EG
- Tsopoulou M
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tuna AN
- Turchikhin S
- Turgeman D
- Turner RJ
- Turra R
- Tuts PM
- Tzamarias S
- Tzovara E
- Uchida K
- Ukegawa F
- Unal G
- Unal M
- Undrus A
- Unel G
- Ungaro FC
- Unno Y
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- Urban J
- Usai G
- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
- Vafeiadis T
- Vaidya A
- Valderanis C
- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Valls Ferrer JA
- Van Daalen TR
- Van Gemmeren P
- Van Stroud S
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vannicola D
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Varvell KE
- Vasile ME
- Vasquez GA
- Vazeille F
- Vazquez Furelos D
- Vazquez CJB
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Vera AMR
- Verbytskyi A
- Vercesi V
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vernieri C
- Verschuuren PJ
- Verzini MJA
- Vetterli MC
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
- Villaplana Perez M
- Villhauer EM
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vogel M
- Vokac P
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- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
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- Vranjes N
- Vrba V
- Vu NK
- Vuillermet R
- Vukotic I
- Wada S
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Wakasa R
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Wang AM
- Wang AZ
- Wang C
- Wang C
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- Wanotayaroj C
- Warburton A
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- Ward RJ
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- Webb AF
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- Wei Y
- Weidberg AR
- Weingarten J
- Weirich M
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- Wells PS
- Wenaus T
- Wendland B
- Wengler T
- Wenig S
- Wermes N
- Wessels M
- Weston TD
- Whalen K
- Wharton AM
- White A
- White AS
- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
- Williams DM
- Williams HH
- Williams S
- Willocq S
- Windischhofer PJ
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolker R
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Wongel AF
- Woods NL
- Worm SD
- Wosiek BK
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wuerzinger J
- Wyatt TR
- Wynne BM
- Xella S
- Xiang J
- Xiao X
- Xie X
- Xiotidis I
- Xu D
- Xu H
- Xu H
- Xu L
- Xu R
- Xu T
- Xu W
- Xu Y
- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan J
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang X
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 02/07/2021
- Field of study
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fb−1 of s√ = 13 TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015–2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single Z boson production, Higgs boson production and on-shell ZZ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The Z → 4ℓ branching fraction is extracted, giving a value of (4.41 ± 0.30) × 10−6. Constraints on effective field theory parameters and a model based on a spontaneously broken B − L gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information
Search for pair production of third-generation scalar leptoquarks decaying into a top quark and a τ-lepton in pp collisions at s√ = 13 TeV with the ATLAS detector
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Zemaityte G
- Zeng JC
- Zenin O
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- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
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- Ziolkowski M
- Zobernig G
- Zoccoli A
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- Zorbas TG
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- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 30/06/2021
- Field of study
A search for pair production of third-generation scalar leptoquarks decaying into a top quark and a τ-lepton is presented. The search is based on a dataset of pp collisions at s√ = 13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. Events are selected if they have one light lepton (electron or muon) and at least one hadronically decaying τ -lepton, or at least two light leptons. In addition, two or more jets, at least one of which must be identified as containing b-hadrons, are required. Six final states, defined by the multiplicity and flavour of lepton candidates, are considered in the analysis. Each of them is split into multiple event categories to simultaneously search for the signal and constrain several leading backgrounds. The signal-rich event categories require at least one hadronically decaying τ-lepton candidate and exploit the presence of energetic final-state objects, which is characteristic of signal events. No significant excess above the Standard Model expectation is observed in any of the considered event categories, and 95% CL upper limits are set on the production cross section as a function of the leptoquark mass, for different assumptions about the branching fractions into tτ and bν. Scalar leptoquarks decaying exclusively into tτ are excluded up to masses of 1.43 TeV while, for a branching fraction of 50% into tτ, the lower mass limit is 1.22 TeV
Search for long-lived, massive particles in events with a displaced vertex and a muon with large impact parameter in pp collisions at root s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Acharya BS
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- Alberghi GL
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- Aleksandrov IN
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- Caltabiano A
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- Cameron D
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- Carlson BT
- Carminati L
- Carney RMD
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- Castillo Gimenez V
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- Castro NF
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- Daubney T
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- de Andrade Filho LM
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- de Lima DEF
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- de Renstrom PAB
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- Zeissner S
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- Zemaityte G
- Zeng JC
- Zenin O
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/08/2020
- Field of study
A search for long-lived particles decaying into hadrons and at least one muon is presented. The analysis selects events that pass a muon or missing-transverse-momentum trigger and contain a displaced muon track and a displaced vertex. The analyzed dataset of proton-proton collisions at
√
s
=
13 TeV
was collected with the ATLAS detector and corresponds to
136
fb
−
1. The search employs dedicated reconstruction techniques that significantly increase the sensitivity to long-lived particle decays that occur in the ATLAS inner detector. Background estimates for Standard Model processes and instrumental effects are extracted from data. The observed event yields are compatible with those expected from background processes. The results are presented as limits at 95% confidence level on model-independent cross sections for processes beyond the Standard Model, and interpreted as exclusion limits in scenarios with pair production of long-lived top squarks that decay via a small
R
-parity-violating coupling into a quark and a muon. Top squarks with masses up to 1.7 TeV are excluded for a lifetime of 0.1 ns, and masses below 1.3 TeV are excluded for lifetimes between 0.01 ns and 30 ns
Properties of jet fragmentation using charged particles measured with the ATLAS detector in pp collisions at root s=13 TeV
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aperio Bella L
- Arabidze G
- Aranda CP
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/09/2019
- Field of study
This paper presents a measurement of quantities related to the formation of jets from high-energy quarks and gluons (fragmentation). Jets with transverse momentum 100 GeV 500 MeV and |η| < 2.5 are used to probe the detailed structure of the jet. The fragmentation properties of the more forward and the more central of the two leading jets from each event are studied. The data are unfolded to correct for detector resolution and acceptance effects. Comparisons with parton shower Monte Carlo generators indicate that existing models provide a reasonable description of the data across a wide range of phase space, but there are also significant differences. Furthermore, the data are interpreted in the context of quark- and gluon-initiated jets by exploiting the rapidity dependence of the jet flavor fraction. A first measurement of the charged-particle multiplicity using model-independent jet labels (topic modeling) provides a promising alternative to traditional quark and gluon extractions using input from simulation. The simulations provide a reasonable description of the quark-like data across the jet
Pt range presented in -this measurement, but the gluon-like data have systematically fewer charged particles than the simulation
Search for squarks and gluinos in final states with jets and missing transverse momentum using 139 fb−1 of s√ = 13 TeV pp collision data with the ATLAS detector
- Author
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- Aad G
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- Abdinov O
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- Zaidan R
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- Zakharchuk N
- Zalieckas J
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- Zanzi D
- Zaripovas DR
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
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- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
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- Zhu CG
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- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
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- Zobernig G
- Zoccoli A
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- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 17/02/2021
- Field of study
A search for the supersymmetric partners of quarks and gluons (squarks and gluinos) in final states containing jets and missing transverse momentum, but no electrons or muons, is presented. The data used in this search were recorded by the ATLAS experiment in proton-proton collisions at a centre-of-mass energy of s√ = 13 TeV during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. The results are interpreted in the context of various R-parity-conserving models where squarks and gluinos are produced in pairs or in association and a neutralino is the lightest supersymmetric particle. An exclusion limit at the 95% confidence level on the mass of the gluino is set at 2.30 TeV for a simplified model containing only a gluino and the lightest neutralino, assuming the latter is massless. For a simplified model involving the strong production of mass-degenerate first- and second-generation squarks, squark masses below 1.85 TeV are excluded if the lightest neutralino is massless. These limits extend substantially beyond the region of supersymmetric parameter space excluded previously by similar searches with the ATLAS detector
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- 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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- Buschmann E
- Bussey PJ
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- Butterworth JM
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- Buttinger W
- Buzatu A
- Buzykaev AR
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- Cabras G
- Caforio D
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- Cakir IT
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- Calace N
- Calafiura P
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- Chitan A
- Chiu I
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- Zahreddine J
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- Zhemchugov A
- Zheng Z
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
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