428 research outputs found
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
- 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
- Adachi S
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- Adamek L
- Adelman J
- Adersberger M
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- Tsiskaridze V
- Tskhadadze EG
- Tsopoulou M
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
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- Urban J
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- Uysal Z
- Vacek V
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- Vaidya A
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- Valentinetti S
- Valero A
- Valery L
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- Vallier A
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- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandenbroucke M
- Vandewall ER
- Vaniachine A
- Vannicola D
- Vari R
- Varnes EW
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- Varouchas D
- Varvell KE
- Vasile ME
- Vasquez GA
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- Vazquez CJB
- Vazquez JGP
- Veatch J
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- Veloce LM
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- Venturi N
- Vera AMR
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- Verducci M
- Vergara JCR
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- Viehhauser GHA
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- Virdee GS
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- von Buddenbrock SE
- Von Toerne E
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- Vorobev K
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- Vossebeld JH
- Vozak M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Wang AM
- Wang AZ
- Wang C
- Wang F
- Wang H
- Wang J
- Wang P
- Wang Q
- Wang R
- Wang R-J
- Wang SM
- Wang W
- Wang WT
- Wang WX
- Wang Y
- Wang Z
- Wanotayaroj C
- Warburton A
- Ward CP
- Wardrope DR
- Warrack N
- Washbrook A
- Watson AT
- Watson MF
- Watts G
- Waugh BM
- Webb AF
- Webb S
- Weber C
- Weber MS
- Weber SA
- Weber SM
- Weidberg AR
- Weingarten J
- Weirich M
- Weiser C
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
- Wermes N
- Werner MD
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- 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 HH
- Williams S
- Willis C
- Willocq S
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolker R
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xiao X
- Xiotidis I
- Xu D
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- Xu L
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- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
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- Yang X
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- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye H
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- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- 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
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- 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
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- 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
Growth Hormone Promotes Hair Cell Regeneration in the Zebrafish (Danio rerio) Inner Ear following Acoustic Trauma
- Author
- A Lombarte
- A Scheepens
- AE Ellis
- AJ Hudspeth
- AJ Hudspeth
- B Avallone
- BM Ryals
- C Haddon
- C Sage
- CG Smith
- Chia-Hui Lin
- CL Render
- D Decker
- DA Gilpin
- DA Weigent
- DN Herdon
- DW Golde
- DW Roberson
- EJ Sanders
- EJ Sanders
- EJ Sanders
- EK O'Halloran
- EY Ma
- FF Casanueva
- GW Jung
- HR Brignull
- Huifang Sun
- J Bravo
- JA Calduch-Giner
- JA Calduch-Giner
- JA Harris
- JB Schuck
- JB Schuck
- JE Jones
- JE Jones
- JI Matsui
- JL Zhang
- JM Tanner
- JS McCullar
- JT Corwin
- K Beisel
- K Oshima
- KK Kaulsy
- M Bidlingmarier
- M Izumikawa
- M Kanje
- M Ullman
- MB Davidson
- ME Smith
- ME Smith
- ME Smith
- ME Warchol
- Michael E. Smith
- MJ van den Eijnden
- MN Rivolta
- N Jongkamonwiwat
- O Alo
- O Löwenstein
- OG Isaksson
- P Rotwein
- PA Pennisi
- Platt
- PP Hernandez
- PP Lefebvre
- R Fettiplace
- RR Taylor
- S Chardin
- S Harvey
- S Harvey
- S Okada
- SA Bhave
- SE Brunet-Dunand
- Silvana Allodi
- SP Gubbels
- T Matsuda
- Tresguerres
- UJ Pyati
- V Cacciafesta
- V Pandey
- W Driever
- Publication venue
- Public Library of Science
- Publication date
- 30/11/2011
- Field of study
BACKGROUND: Previous microarray analysis showed that growth hormone (GH) was significantly upregulated following acoustic trauma in the zebrafish (Danio rerio) ear suggesting that GH may play an important role in the process of auditory hair cell regeneration. Our objective was to examine the effects of exogenous and endogenous GH on zebrafish inner ear epithelia following acoustic trauma. METHODOLOGY/PRINCIPAL FINDINGS: We induced auditory hair cell damage by exposing zebrafish to acoustic overstimulation. Fish were then injected intraperitoneally with either carp GH or buffer, and placed in a recovery tank for either one or two days. Phalloidin-, bromodeoxyuridine (BrdU)-, and TUNEL-labeling were used to examine hair cell densities, cell proliferation, and apoptosis, respectively. Two days post-trauma, saccular hair cell densities in GH-treated fish were similar to that of baseline controls, whereas buffer-injected fish showed significantly reduced densities of hair cell bundles. Cell proliferation was greater and apoptosis reduced in the saccules, lagenae, and utricles of GH-treated fish one day following trauma compared to controls. Fluorescent in situ hybridization (FISH) was used to examine the localization of GH mRNA in the zebrafish ear. At one day post-trauma, GH mRNA expression appeared to be localized perinuclearly around erythrocytes in the blood vessels of the inner ear epithelia. In order to examine the effects of endogenous GH on the process of cell proliferation in the ear, a GH antagonist was injected into zebrafish immediately following acoustic trauma, resulting in significantly decreased cell proliferation one day post-trauma in all three zebrafish inner ear end organs. CONCLUSIONS/SIGNIFICANCE: Our results show that exogenous GH promotes post-trauma auditory hair cell regeneration in the zebrafish ear through stimulating proliferation and suppressing apoptosis, and that endogenous GH signals are present in the zebrafish ear during the process of auditory hair cell regeneration
Overactivation of Notch1 Signaling Induces Ectopic Hair Cells in the Mouse Inner Ear in an Age-Dependent Manner
- Author
- A Doetzlhofer
- A Morrison
- AE Kiernan
- AE Kiernan
- AE Kiernan
- AE Kiernan
- AK Groves
- AP Jadhav
- BB Millimaki
- BH Hartman
- C Puligilla
- C Woods
- CH Hwang
- CM Chen
- CM Hackney
- CS Jayasena
- DM Fekete
- DM Fekete
- EC Driver
- EL Rawlins
- EM Sweet
- EP Hatch
- H Li
- H Morsli
- H Tsai
- I Breuskin
- I Jahan
- J Bok
- J Burns
- J Murata
- J Neves
- Jian Zuo
- Jie Fang
- JL Zheng
- JS Stone
- JV Brigande
- L Freyer
- LC Murtaugh
- LD Urness
- M Eddison
- M Mustapha
- MC Kelly
- ML Basch
- MM Riccomagno
- MM Riccomagno
- MS Collado
- MW Kelley
- N Daudet
- N Daudet
- N Yamamoto
- N Yamamoto
- NA Bermingham
- O Nyabi
- P Chen
- Peter K. Dearden
- PJ Lanford
- R Brooker
- S Eminli
- S Hayashi
- S Huh
- S Raft
- S Takebayashi
- SJ Jeon
- SP Gubbels
- T Hayashi
- T Hayashi
- T Kwan
- T Ohyama
- T Ohyama
- T Ohyama
- Thomas Owen
- TJ Wright
- U Pirvola
- W Pan
- Y Yu
- Z Liu
- Zhiyong Liu
- Publication venue
- Public Library of Science
- Publication date
- 20/03/2012
- Field of study
Background: During mouse inner ear development, Notch1 signaling first specifies sensory progenitors, and subsequently controls progenitors to further differentiate into either hair cells (HCs) or supporting cells (SCs). Overactivation of NICD (Notch1 intracellular domain) at early embryonic stages leads to ectopic HC formation. However, it remains unclear whether such an effect can be elicited at later embryonic or postnatal stages, which has important implications in mouse HC regeneration by reactivation of Notch1 signaling. Methodology/Principal Findings: We performed comprehensive in vivo inducible overactivation of NICD at various developmental stages. In CAG CreER+; Rosa26-NICD loxp/+ mice, tamoxifen treatment at embryonic day 10.5 (E10.5) generated ectopic HCs in the non-sensory regions in both utricle and cochlea, whereas ectopic HCs only appeared in the utricle when tamoxifen was given at E13. When tamoxifen was injected at postnatal day 0 (P0) and P1, no ectopic HCs were observed in either utricle or cochlea. Interestingly, Notch1 signaling induced new HCs in a non-cell-autonomous manner, because the new HCs did not express NICD. Adjacent to the new HCs were cells expressing the SC marker Sox10 (either NICD+ or NICDnegative). Conclusions/Significance: Our data demonstrate that the developmental stage determines responsiveness of embryonic otic precursors and neonatal non-sensory epithelial cells to NICD overactivation, and that Notch 1 signaling in the wild type, postnatal inner ear is not sufficient for generating new HCs. Thus, our genetic mouse model is suitable to test additiona
Moderators of the longitudinal relationship between the perceived physical environment and outside play in children: the KOALA birth cohort study
- Author
- A Page
- B Giles-Corti
- C Bernaards
- Carel Thijs
- CD Klinker
- CJ Riddoch
- CL Addy
- D Ding
- D Kim
- D Rosenberg
- Dave Van Kann
- Dick Ettema
- E Cremers
- EE Wickel
- EF Sleddens
- G Maldonado
- H Little
- HL Burdette
- I Bakker
- I Kummeling
- J Gubbels
- J Veitch
- JC Kimiecik
- JC Spence
- Jessica Gubbels
- JF Sallis
- JG Ross
- JM Dempsey
- JO Fisher
- JO Fisher
- JS Gubbels
- JS Gubbels
- K Davison
- K Van der Horst
- KA Kirtland
- L Schaefer
- LF Berkman
- LH McNeill
- LL Birch
- M Aarts
- MR Stone
- N Darling
- N Humpel
- N Statistics
- P Blatchford
- P Gordon-Larsen
- P Tucker
- RL Mackett
- RR Pate
- Sanne de Vries
- SD Holloway
- SE Barlow
- SG Trost
- SG Trost
- SI De Vries
- SP Kremers
- SPJ Kremers
- Stef PJ Kremers
- Swantje Schmidt
- T Hinkley
- T Pikora
- T Remmers
- Teun Remmers
- TM DiLorenzo
- V Cleland
- WH Brown
- WHO
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
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
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asawatavonvanich T
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Ayoub MK
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Banerjee S
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro F
- Barron U
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Belfkir M
- Bell AS
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Berthold A
- Bertram IA
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bhattacharya DS
- Bhattarai P
- Bi R
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz N
- Biglietti M
- Billoud TR
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker E
- Boumediene D
- Bourdarios CA
- Boutle SK
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Bruschi M
- Bruscino N
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher V
- Bugge MK
- Bulekov O
- Bullard BA
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
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- Calvente Lopez S
- Calvet D
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- Carlson BT
- Carlson EM
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- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
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- Catmore JR
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- Cheremushkina E
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- Chevalerias TJA
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- Chiu I
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- Cinca D
- Cindro V
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- Zemaityte G
- Zeng JC
- Zenin O
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- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou MS
- 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
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- 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
Search for bottom-squark pair production in pp collision events at √s=13 TeV with hadronically decaying τ-leptons, b-jets, and missing transverse momentum using the ATLAS detector
- Author
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- Abbott B
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- Zhemchugov A
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- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/08/2021
- Field of study
A search for pair production of bottom squarks in events with hadronically decaying
τ
-leptons,
b
-tagged jets, and large missing transverse momentum is presented. The analyzed dataset is based on proton-proton collisions at
√
s
=
13
TeV
delivered by the Large Hadron Collider and recorded by the ATLAS detector from 2015 to 2018, and corresponds to an integrated luminosity of
139
fb
−
1
. The observed data are compatible with the expected Standard Model background. Results are interpreted in a simplified model where each bottom squark is assumed to decay into the second-lightest neutralino
˜
χ
0
2
and a bottom quark, with
˜
χ
0
2
decaying into a Higgs boson and the lightest neutralino
˜
χ
0
1
. The search focuses on final states where at least one Higgs boson decays into a pair of hadronically decaying
τ
-leptons. This allows the acceptance and thus the sensitivity to be significantly improved relative to the previous results at low masses of the
˜
χ
0
2
, where bottom-squark masses up to 850 GeV are excluded at the 95% confidence level, assuming a mass difference of 130 GeV between
˜
χ
0
2
and
˜
χ
0
1
. Model-independent upper limits are also set on the cross section of processes beyond the Standard Model
Search for dark matter in events with missing transverse momentum and a Higgs boson decaying into two photons 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
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- Yildiz HD
- Yin P
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- Zaitsev AM
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- Zakharchuk N
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- Zanzi D
- Zeissner S
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- Zemaityte G
- Zeng JC
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- Zerradi S
- Zerwas D
- Zgubic M
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- Zhang G
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- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhou M
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- Zhu CG
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- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zoccoli A
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- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/10/2021
- Field of study
A search for dark-matter particles in events with large missing transverse momentum and a Higgs boson candidate decaying into two photons is reported. The search uses 139 fb−1 of proton-proton collision data collected at s√ = 13 TeV with the ATLAS detector at the CERN LHC between 2015 and 2018. No significant excess of events over the Standard Model predictions is observed. The results are interpreted by extracting limits on three simplified models that include either vector or pseudoscalar mediators and predict a final state with a pair of dark-matter candidates and a Higgs boson decaying into two photons
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- 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
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
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- Zakareishvili T
- Zakharchuk N
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- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
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- Zhang L
- Zhang L
- Zhang M
- Zhang R
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- Zhang X
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- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhou M
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- Zhu C
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- 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
Performance of the upgraded PreProcessor of the ATLAS Level-1 Calorimeter Trigger
- Author
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- Yigitbasi E
- Yildiz H Duran
- Yorita K
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- Zahreddine J
- Zaitsev AM
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- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
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- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- 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 NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2020
- Field of study
The PreProcessor of the ATLAS Level-1 Calorimeter Trigger prepares the analogue trigger signals sent from the ATLAS calorimeters by digitising, synchronising, and calibrating them to reconstruct transverse energy deposits, which are then used in further processing to identify event features. During the first long shutdown of the LHC from 2013 to 2014, the central components of the PreProcessor, the Multichip Modules, were replaced by upgraded versions that feature modern ADC and FPGA technology to ensure optimal performance in the high pile-up environment of LHC Run 2. This paper describes the features of the newMultichip Modules along with the improvements to the signal processing achieved.ANPCyTYerPhI, ArmeniaAustralian Research CouncilBMWFW, AustriaAustrian Science Fund (FWF)Azerbaijan National Academy of Sciences (ANAS)SSTC, BelarusNational Council for Scientific and Technological Development (CNPq)Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (FAPESP)Natural Sciences and Engineering Research Council of CanadaCanada Foundation for InnovationNational Natural Science Foundation of China (NSFC)Departamento Administrativo de Ciencia, Tecnología e Innovación ColcienciasMinistry of Education, Youth & Sports - Czech Republic
Czech Republic GovernmentCzech Republic GovernmentDNRF, DenmarkDanish Natural Science Research CouncilCentre National de la Recherche Scientifique (CNRS)CEA-DRF/IRFU, FranceFederal Ministry of Education & Research (BMBF)Max Planck SocietyGreek Ministry of Development-GSRTRGC and Hong Kong SAR, ChinaIsrael Science FoundationBenoziyo Center, IsraelIstituto Nazionale di Fisica Nucleare (INFN)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)
Japan Society for the Promotion of ScienceCNRST, MoroccoRCN, NorwayPortuguese Foundation for Science and TechnologyMNE/IFA, RomaniaMES of RussiaMESTD, SerbiaMSSR, SlovakiaSlovenian Research Agency - SloveniaMIZS, SloveniaSpanish GovernmentSRC, SwedenWallenberg Foundation, SwedenSNSF Geneva, SwitzerlandMinistry of Science and Technology, TaiwanMinistry of Energy & Natural Resources - TurkeyScience & Technology Facilities Council (STFC)United States Department of Energy (DOE)National Science Foundation (NSF)BCKDF, CanadaCANARIE, CanadaCRC, CanadaEuropean Research Council (ERC)European Union (EU)French National Research Agency (ANR)German Research Foundation (DFG)Alexander von Humboldt FoundationGreek NSRF, GreeceBSF-NSF, IsraelGerman-Israeli Foundation for Scientific Research and DevelopmentLa Caixa Banking Foundation, SpainCERCA Programme Generalitat de Catalunya, SpainPROMETEO, SpainGenT Programmes Generalitat Valenciana, SpainGoran Gustafssons Stiftelse, SwedenRoyal Society of LondonLeverhulme TrustNRC, CanadaCERNANID, ChileChinese Academy of SciencesMinistry of Science and Technology, ChinaSRNSFG, GeorgiaHGF, GermanyNetherlands Organization for Scientific Research (NWO)
Netherlands GovernmentMinistry of Science and Higher Education, PolandNCN, PolandNRCKI, Russia FederationJINRDST/NRF, South AfricaSERI, Geneva, SwitzerlandCantons of Bern and Geneva, SwitzerlandCompute Canada, CanadaHorizon 2020Marie Sklodowska-Curie ActionsEuropean Cooperation in Science and Technology (COST)EU-ESF, Greec
Two-particle azimuthal correlations in photonuclear ultraperipheral Pb plus Pb collisions at 5.02 TeV with ATLAS
- 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
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- 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
- Akbiyik M
- 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
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aparo MA
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
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- Asai K
- Asai S
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- Asimakopoulou EM
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- Assahsah J
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- Astigarraga MEP
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- Ayoub MK
- Azuelos G
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- Bahrasemani H
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- Zeitnitz C
- Zemaityte G
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- Zhemchugov A
- Zheng Z
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/07/2021
- Field of study
Two-particle long-range azimuthal correlations are measured in photonuclear collisions using
1.7
nb
−
1
of 5.02 TeV
Pb
+
Pb
collision data collected by the ATLAS experiment at the CERN Large Hadron Collider. Candidate events are selected using a dedicated high-multiplicity photonuclear event trigger, a combination of information from the zero-degree calorimeters and forward calorimeters, and from pseudorapidity gaps constructed using calorimeter energy clusters and charged-particle tracks. Distributions of event properties are compared between data and Monte Carlo simulations of photonuclear processes. Two-particle correlation functions are formed using charged-particle tracks in the selected events, and a template-fitting method is employed to subtract the nonflow contribution to the correlation. Significant nonzero values of the second- and third-order flow coefficients are observed and presented as a function of charged-particle multiplicity and transverse momentum. The results are compared with flow coefficients obtained in proton-proton and proton-lead collisions in similar multiplicity ranges, and with theoretical expectations. The unique initial conditions present in this measurement provide a new way to probe the origin of the collective signatures previously observed only in hadronic collision
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