451 research outputs found
Phenotypic Variation and Bistable Switching in Bacteria
- Author
- A Becskei
- A Becskei
- A Guerrero
- A Johnson
- A Khlebnikov
- A Khlebnikov
- A Khlebnikov
- A Lipshtat
- A Moter
- A Novick
- AE Merode van
- AE Merode van
- AE Tsong
- B Muller-Hill
- B Slutsky
- BB Magee
- BE Laue
- BF Brehm-Stecher
- BJ Haijema
- C Hadden
- C Wiuff
- CM Hull
- CM Hull
- CM Southward
- CY Lan
- D Angeli
- D Dubnau
- D Dubnau
- D Dubnau
- D Kidane
- D Sinderen van
- D Sinderen van
- DB Kearns
- DC Dooley
- DH Dean
- DR Soll
- E Korobkova
- E Kussell
- EH Rikkerink
- EJ Stewart
- EM Ozbudak
- EM Ozbudak
- ER Sumner
- EW Nester
- F Jacob
- F Joux
- F Ortega
- F Russo-Marie
- FH Cahn
- FH Kasten
- FJ Isaacs
- G Huang
- G Nebe-von-Caron
- GM Suel
- GM Suel
- H Kobayashi
- H Maamar
- H Makinoshima
- H Steinmoen
- H Steinmoen
- HB Fraser
- HM Davey
- I Golding
- I Golding
- I Hautefort
- IR Henderson
- J Casadesus
- J Hahn
- J Hahn
- J Hasty
- J Hasty
- J Holtzendorff
- J Kreth
- J Monod
- J Vidal-Mas
- J Vives-Rego
- J Zieg
- JD Chung
- JD Chung
- JD Chung
- JE Ferrell Jr
- JE Ferrell Jr
- JE Gonzalez-Pastor
- JE Lisman
- JM Abraham
- JM Anderson
- JM Pedraza
- JR Glynn Jr
- JW Veening
- K Lewis
- KA Susanna
- KP Lemon
- KZ Abshire
- L Cai
- LF Greer III
- LW Hamoen
- LW Hamoen
- M Acar
- M Albano
- M Albano
- M Albano
- M Cohn
- M Cohn
- M Lange
- M Laurent
- M Leisner
- M Santillán
- M Thattai
- M Woude van der
- MB Elowitz
- MB Elowitz
- MG Miller
- MJ Hoek van
- MR Barer
- N Chantratita
- N Friedman
- N Rosenfeld
- N Yildirim
- N Yildirim
- NC Shaner
- NC Shaner
- NE Kramer
- NQ Balaban
- P Viswanathan
- PS Swain
- R Amann
- R Carballido-Lopez
- R Thomas
- R Thomas
- RA Daniel
- RE Zordan
- RI Amann
- RJ Bennett
- RM Morgan-Kiss
- RN Singh
- RN Singh
- RP Burchard
- RP Haugland
- RY Tsien
- S Guiral
- S Hooshangi
- S Stibitz
- SB Williams
- SE Finkel
- SR Biggar
- SR Lockhart
- SR Lockhart
- SV Avery
- T Hornbaek
- T Nishino
- T Tian
- T Tolker-Nielsen
- TF Meyer
- TS Gardner
- TT Hoa
- V Sentchilo
- V Sentchilo
- WK Smits
- WK Smits
- WK Smits
- Publication venue
- Publication date
- 01/01/2008
- Field of study
Microbial research generally focuses on clonal populations. However, bacterial cells with identical genotypes frequently display different phenotypes under identical conditions. This microbial cell individuality is receiving increasing attention in the literature because of its impact on cellular differentiation, survival under selective conditions, and the interaction of pathogens with their hosts. It is becoming clear that stochasticity in gene expression in conjunction with the architecture of the gene network that underlies the cellular processes can generate phenotypic variation. An important regulatory mechanism is the so-called positive feedback, in which a system reinforces its own response, for instance by stimulating the production of an activator. Bistability is an interesting and relevant phenomenon, in which two distinct subpopulations of cells showing discrete levels of gene expression coexist in a single culture. In this chapter, we address techniques and approaches used to establish phenotypic variation, and relate three well-characterized examples of bistability to the molecular mechanisms that govern these processes, with a focus on positive feedback.
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
- Author
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- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimoto G
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Almond J
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
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- Anastopoulos C
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- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
- Author
- Aad G
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
Network analysis of depressive symptoms in Hong Kong residents during the COVID-19 pandemic
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 06/09/2021
- Field of study
In network theory depression is conceptualized as a complex network of individual symptoms that influence each other, and central symptoms in the network have the greatest impact on other symptoms. Clinical features of depression are largely determined by sociocultural context. No previous study examined the network structure of depressive symptoms in Hong Kong residents. The aim of this study was to characterize the depressive symptom network structure in a community adult sample in Hong Kong during the COVID-19 pandemic. A total of 11,072 participants were recruited between 24 March and 20 April 2020. Depressive symptoms were measured using the Patient Health Questionnaire-9. The network structure of depressive symptoms was characterized, and indices of “strength”, “betweenness”, and “closeness” were used to identify symptoms central to the network. Network stability was examined using a case-dropping bootstrap procedure. Guilt, Sad Mood, and Energy symptoms had the highest centrality values. In contrast, Concentration, Suicide, and Sleep had lower centrality values. There were no significant differences in network global strength (p = 0.259), distribution of edge weights (p = 0.73) and individual edge weights (all p values > 0.05 after Holm–Bonferroni corrections) between males and females. Guilt, Sad Mood, and Energy symptoms were central in the depressive symptom network. These central symptoms may be targets for focused treatments and future psychological and neurobiological research to gain novel insight into depression
Physiological and biochemical traits as tools to screen sensitive and resistant varieties of tomatoes exposed to salt stress
- Author
- Abbruzzese G
- Aqil Ahmad
- Bates LS
- Beauchamp CO
- Belkhodja R
- Bilal Ahmad Mir
- Bradford MM
- Breckle SW
- Chance B
- Cosgrove DJ
- Dwivedi RS
- Flordeliza FC
- Flowers TJ
- Flowers TJ
- Flowers TJ
- Foyer CH
- Frary A
- Gomez KA
- Hajjar R
- Hayat S
- Hayat S
- Hayat S
- Hernandez JA
- Hollington PA
- Hopkins WG
- Jaworski EG
- Karlidag H
- Kavi Kishor PB
- Läuchli A
- Läuchli A
- Majeau N
- Parida A
- Parida AK
- Pitann B
- Qazi Fariduddin
- Sabra A
- Santos CV
- Shahbaz M
- Shahid MA
- Shalata A
- Shen B
- Solomonson LP
- Soussi M
- Srivastava HS
- Sudhir P
- Sullivan CY
- Tabatabaei SJ
- Tiwari A
- Wang X
- Winicov I
- Yildirim E
- Yusuf M
- Zhu JK
- Zhu JK
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Unified representation of the family of L-functions
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for High-Mass Resonances Decaying to τν in pp Collisions at √s=13 TeV with the ATLAS Detector
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- Zivkovic L
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- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to τν using proton-proton collisions at √s=13 TeV produced by the Large Hadron Collider is presented. Only τ-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb−1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W′ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2–3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Measurement of differential cross sections and W + /W − cross-section ratios for W boson production in association with jets at √s =8 TeV with the ATLAS detector
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- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
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- Zhemchugov A
- Zhou B
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
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- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
This paper presents a measurement of the W boson production cross section and the W + /W − cross-section ratio, both in association with jets, in proton--proton collisions at s √ =8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb −1 . Differential cross sections for events with one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles and the missing transverse momentum in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W + /W − the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proto
Measurement of the cross section for inclusive isolated-photon production in pp collisions at √s=13TeV using the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
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- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
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- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt SC
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
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- Alshehri AA
- Alstaty MI
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amundsen G
- Anastopoulos C
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- Andari N
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- Anderson KJ
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- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
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- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
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- Klitzner FF
- Kluge E-E
- Kluit P
- Kluth S
- Kneringer E
- Knoops EBFG
- Knue A
- Kobayashi A
- Kobayashi D
- Kobayashi T
- Kobel M
- Kocian M
- Kodys P
- Koehler MK
- Koehler NM
- Koeneke K
- Koenig AC
- Koffas T
- Koffeman E
- Koi T
- Kolb M
- Koletsou I
- Kondo T
- Kondrashova N
- Kono T
- Konoplich R
- Konstantinidis N
- Konya B
- Kopeliansky R
- Koperny S
- Kopp AK
- Korcyl K
- Kordas K
- Korn A
- Korol AA
- Korolkov I
- Korolkova EV
- Kortner O
- Kortner S
- Kosek T
- Kostyukhin VV
- Kotwal A
- Koulouris A
- Kourkoumeli-Charalampidi A
- Kourkoumelis C
- Kourlitis E
- Kouskoura V
- Kowalewska AB
- Kowalewski R
- Kowalski TZ
- Kozakai C
- Kozanecki W
- Kozhin AS
- Kramarenko VA
- Kramberger G
- Krasnopevtsev D
- Krasny MW
- Krasznahorkay A
- Krauss D
- Kremer JA
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- Krizka K
- Kroeninger K
- Kroha H
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- Krstic J
- Kruchonak U
- Krueger H
- Krumnack N
- Kruse MC
- Kubota T
- Kucuk H
- Kuday S
- Kuechler JT
- Kuehn S
- Kugel A
- Kuger F
- Kuh T
- Kukhtin V
- Kukla R
- Kulchitsky Y
- Kuleshov S
- Kulinich YP
- Kuna M
- Kunigo T
- Kupco A
- Kupfer T
- Kuprash O
- Kurashige H
- Kurchaninov LL
- Kurochkin YA
- Kurth MG
- Kuutmann EB
- Kuwertz ES
- Kuze M
- Kvita J
- Kwan T
- Kyriazopoulos D
- La Rosa A
- La Rotonda L
- La Ruffa F
- Lacasta C
- Lacava F
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- Lacker H
- Lacour D
- Ladygin E
- Lafaye R
- Laforge B
- Lagouri T
- Lai S
- Lammers S
- Lampl W
- Lancon E
- Landgraf U
- Landon MPJ
- Lanfermann MC
- Lang VS
- Lange JC
- Langenberg RJ
- Lankford AJ
- Lanni F
- Lantzsch K
- Lanza A
- Lapertosa A
- Laplace S
- Laporte JF
- Lari T
- Lassnig M
- Latour BMD
- Lau TS
- Laurelli P
- Lavrijsen W
- Law AT
- Laycock P
- Lazovich T
- Lazzaroni M
- Le Dortz O
- Le Guirriec E
- Le Quilleuc EP
- Le B
- LeBlanc M
- LeCompte T
- Ledroit-Guillon F
- Lee CA
- Lee GR
- Lee L
- Lee SC
- Lefebvre B
- Lefebvre G
- Lefebvre M
- Legger F
- Leggett C
- Lei X
- Leight WA
- Leite MAL
- Leitner R
- Lellouch D
- Lemmer B
- Leney KJC
- Lenz T
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- Leonidopoulos C
- Lerner G
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- Lester CG
- Levchenko M
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- Levinson LJ
- Levy M
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- Li B
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- Li Q
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- Li S
- Li X
- Li Y
- Liang Z
- Liberti B
- Liblong A
- Lie K
- Liebal J
- Liebig W
- Limosani A
- Lin CY
- Lin K
- Lin SC
- Lin TH
- Linck RA
- Lindquist BE
- Lionti AE
- Lipeles E
- Lipniacka A
- Lisovyi M
- Liss TM
- Lister A
- Litke AM
- Liu B
- Liu H
- Liu H
- Liu J
- Liu JB
- Liu JKK
- Liu K
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- Liu M
- Liu Y
- Liu YL
- Livan M
- Llacer MM
- Lleres A
- Lloyd SL
- Lo Sterzo F
- Lo CY
- Lobodzinska EM
- Loch P
- Loebinger FK
- Loesle A
- Loew KM
- Lohse T
- Lohwasser K
- Lokajicek M
- Long BA
- Long JD
- Long RE
- Longo L
- Looper KA
- Lopez JA
- Lorenz J
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- Losel PJ
- Lou X
- Lounis A
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- Love PA
- Loyola JES
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- Lukas W
- Luminari L
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- Lundberg O
- Lutz MS
- Luzi PM
- Lynn D
- Lysak R
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- Lyu F
- Lyubushkin V
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- Ma LL
- Ma Y
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- Macchiolo A
- Macdonald CM
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- Machado Miguens J
- Madaffari D
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- Mader WF
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- Madysa N
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- Maevskiy AS
- Magerl V
- Maiani C
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- Maier T
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- Majersky O
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- Manhaes de Andrade Filho L
- Mankinen KH
- Mann A
- Manousos A
- Mansoulie B
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- Martoiu VS
- Martyniuk AC
- Marzin A
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- Mashinistov R
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- Masubuchi T
- Maurer J
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- Maximov DA
- Mazini R
- Maznas I
- Mazza SM
- Mc Fadden NC
- Mc Goldrick G
- Mc Kee SP
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- Mcfayden JA
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- McMahon SJ
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- Mellado Garcia BR
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- Mizukami A
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- Olsson MJR
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- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
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- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
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- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang D
- Zhang F
- Zhang G
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- Zhang Z
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- Zhao Z
- Zhemchugov A
- Zhou B
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- Zhou N
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- Zhu CG
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
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- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2017
- Field of study
Inclusive isolated-photon production in pp collisions at a centre-of-mass energy of 13TeVis studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 3.2fb−1. The cross section is measured as a function of the photon transverse energy above 125GeVin different regions of photon pseudorapidity. Next-to-leading-order perturbative QCD and Monte Carlo event-generator predictions are compared to the cross-section measurements and provide an adequate description of the data
Search for supersymmetry in events with four or more leptons in √s =13 TeV pp collisions with ATLAS
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
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- Zhemchugov A
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- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
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- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
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- zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
Results from a search for supersymmetry in events with four or more charged leptons (electrons, muons and taus) are presented. The analysis uses a data sample corresponding to 36.1 fb −1 of proton-proton collisions delivered by the Large Hadron Collider at s √ =13 TeV and recorded by the ATLAS detector. Four-lepton signal regions with up to two hadronically decaying taus are designed to target a range of supersymmetric scenarios that can be either enriched in or depleted of events involving the production and decay of a Z boson. Data yields are consistent with Standard Model expectations and results are used to set upper limits on the event yields from processes beyond the Standard Model. Exclusion limits are set at the 95% confidence level in simplified models of General Gauge Mediated supersymmetry, where higgsino masses are excluded up to 295 GeV. In R -parity-violating simplified models with decays of the lightest supersymmetric particle to charged leptons, lower limits of 1.46 TeV, 1.06 TeV, and 2.25 TeV are placed on wino, slepton and gluino masses, respectively
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