185 research outputs found
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
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- Adye T
- Aefsky S
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- Agustoni M
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- Akimoto G
- Akimov AV
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- Alessandria F
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- Argyropoulos S
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- Arutinov D
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- Asman B
- Asquith L
- Assamagan K
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- ATLAS Collaboration The
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- Tsukerman II
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- Tudorache V
- Tuggle JM
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- Turk Cakir I
- Turra R
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- Tykhonov A
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- Uchida K
- Ueda I
- Ueno R
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- van Vulpen I
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- Vandelli W
- Vaniachine A
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- Varnes EW
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- von der Schmitt H
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- Weingarten J
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- Yamamura T
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- Yamauchi K
- Yamazaki T
- Yamazaki Y
- Yan Z
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- Yang UK
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- Yanush S
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- Yen AL
- Yilmaz M
- Yoosoofmiya R
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- Zeitnitz C
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- Zemla A
- Zenin O
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- Zevi Della Porta G
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- Zhao Z
- Zhemchugov A
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- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivković L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Conceptions about palliative care: literature review
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- 01/01/2008
- Field of study
Improving Cry8Ka toxin activity towards the cotton boll weevil (Anthonomus grandis)
- Author
- A Bravo
- A Sali
- Alexandre AP Firmino
- C James
- C James
- C Rausell
- Carlos R Soccol
- CF Barbas III
- CF Barbas III
- CI Wang
- CR Pigott
- Daniel J Rigden
- DJ Finney
- Djair SL Souza
- E Schnepf
- Erich YT Nakasu
- EYT Nakasu
- Gustavo R Oliveira
- H Höfte
- H Ishikawa
- H Zhao
- HM Berman
- Hudson B Ramos
- J Andris-Widhopf
- J Li
- JD Thompson
- JO Silva-Werneck
- José DA de Souza
- José E Gomes
- KIC Craveiro
- L Kiczak
- LE Fernández
- LM Kasman
- M Lassner
- M Soberon
- M Wolfsberger
- MA Scataglini
- Magda A Beneventi
- Maria CM Silva
- Maria F Grossi-de-Sa
- MF Grossi-de-Sa
- MF Grossi-de-Sa
- MM Bradford
- N Galitsky
- NA Broderick
- NN Rosic
- P Silvie
- R Staden
- RA Laskowski
- RC Edgar
- RH Maun
- S Pacheco
- S Vílchez
- SF Altschul
- SJ Wu
- SY Guo
- UK Laemmli
- Wagner A Lucena
- WFS Martins
- WGT Willats
- WPC Stemmer
- X Zhang
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>The cotton boll weevil (<it>Anthonomus grandis</it>) is a serious insect-pest in the Americas, particularly in Brazil. The use of chemical or biological insect control is not effective against the cotton boll weevil because of its endophytic life style. Therefore, the use of biotechnological tools to produce insect-resistant transgenic plants represents an important strategy to reduce the damage to cotton plants caused by the boll weevil. The present study focuses on the identification of novel molecules that show improved toxicity against the cotton boll weevil. <it>In vitro </it>directed molecular evolution through DNA shuffling and phage display screening was applied to enhance the insecticidal activity of variants of the Cry8Ka1 protein of <it>Bacillus thuringiensis</it>.</p> <p>Results</p> <p>Bioassays carried out with <it>A. grandis </it>larvae revealed that the LC<sub>50 </sub>of the screened mutant Cry8Ka5 toxin was 3.15-fold higher than the wild-type Cry8Ka1 toxin. Homology modelling of Cry8Ka1 and the Cry8Ka5 mutant suggested that both proteins retained the typical three-domain Cry family structure. The mutated residues were located mostly in loops and appeared unlikely to interfere with molecular stability.</p> <p>Conclusions</p> <p>The improved toxicity of the Cry8Ka5 mutant obtained in this study will allow the generation of a transgenic cotton event with improved potential to control <it>A. grandis</it>.</p
Evaluation of the symptoms and treatment prescribed to hospitalized patients
- Author
- Bret EP
- Caprara
- Chang VT
- Correia LA
- Davis MP
- Firmino TM
- Fontes KB
- George E
- Glare P
- Grudzen CR
- Honea N
- Kalache A
- Lau F
- Mariana da Silva Roldi
- Moritz RD
- Moritz RD
- Palma A
- Pantilat SZ
- Puntillo KA
- Rachel Duarte Moritz
- Rezende EM
- Rhondali W
- Riechelmann RP
- Sarti C
- Seow H
- Sigurdardottir KR
- Solano JP
- Spichiguer E
- Swarm RA
- Vitorelli E
- Walling AM
- Weng LC
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Search for the direct production of charginos and neutralinos in final states with tau leptons in √s=13 TeV collisions with 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
- Afik Y
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Albergh 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
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amelung C
- Amidei D
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans R Caminal
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
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- Astigarraga ME Pozo
- Atkinson M
- Atlay NB
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- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Bandyopadhyay A
- Banerjee Sw
- Bannoura AAE
- Barajas CA Chavez
- Barak L
- Barberio EL
- Barberis D
- Barbero M
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- Barkeloo JT
- Barklow T
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- Beattie MD
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- Beauchemin PH
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- Beck HC
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- Beddall A
- Beddall AJ
- Bednyakov VA
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- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behr JK
- Bell AS
- Bella G
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- Bellomo M
- Belotskiy K
- Beltramello O
- Belyaev NL
- Benary O
- Benchekroun D
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- Benhammou Y
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
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- Beretta M
- Berge D
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- Berlingen J Montejo
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- Bernlochner FU
- Berry T
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- Bertolucci F
- Bertram IA
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- Besjes GJ
- Bessner M
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- Bevan AJ
- Beyer J
- Bianchi RM
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- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bilokon H
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- Bingul A
- Bini C
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- Bittrich C
- Bjergaard DM
- Black JE
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- Blair RE
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- Bocchetta SS
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- Bogdanchikov AG
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- Boldyrev AS
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- Bomben M
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- Borisov A
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- Bossio Sola JD
- Boudreau J
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- Bouhova-Thacker EV
- Boumediene D
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- Boyd J
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- Bracinik J
- Brandt A
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- Brau B
- Brau JE
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- Buckley AG
- Budagov IA
- Buehrer F
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- Bugge MK
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- Burdin S
- Burgard CD
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- Burke S
- Burmeister I
- Burr JTP
- Busato E
- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund O Bessidskaia
- Cabrera Urban S
- Caforio D
- Cairo VM
- Cakir I Turk
- Cakir O
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- Camarda S
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- Canale V
- Cantero J
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- Capua M
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- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
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- Carra S
- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo I Santoyo
- Castillo LR Flores
- Castro NF
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- Catmore JR
- Cattai A
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- Ceradini F
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- Cerri A
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- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan WS
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chau CC
- Che S
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
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- Chen J
- Chen S
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- Chen X
- Chen Y
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Christodoulou V
- Chu MC
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
- Ciftci AK
- Cinca D
- Cindro V
- Cioara IA
- Ciocca C
- Ciocio A
- Cirotto F
- Citron ZH
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- Clark A
- Clark BL
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- Sinev NB
- Sioli M
- Siragusa G
- Siral I
- Sivoklokov S Yu
- Sjolin J
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- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
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- Smirnov Y
- Smirnova LN
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- Smizanska M
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- Soldevila U
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- Sotiropoulou CL
- Soualah R
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- Spagnolo S
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- Spano F
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- Stramaglia ME
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- Strubig A
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- Sugaya Y
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- Sulin VV
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- Sykora I
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- Ta D
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- Taffard A
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- Teng PK
- Teoh JJ
- Tepel F
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- Tikhomirov VO
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- Tsang KW
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- Tsiareshka PV
- Tsipolitis G
- Tsirintanis N
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsui KM
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Tupputi SA
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- Ucchielli G
- Ueda I
- Ughetto M
- Ukegawa F
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- Ungaro FC
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- Urban J
- Urek T Javdegrees
- Urquijo P
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- Usai G
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- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Valente M
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- Valero A
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- Vallier A
- Valls Ferrer JA
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- van Vulpen I
- van Woerden MC
- Vanadia M
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- Varouchas D
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- Vermeulen JC
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- Viazlo O
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- Vickey T
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- Villa M
- Villar DI Narrias
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vlachos S
- Vogel M
- Vokac P
- Volpi G
- von der Schmitt H
- von Toerne E
- Vorobel V
- Vorobev K
- Vos M
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- Vossebeld JH
- Vranjes N
- Vrba V
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- Vukotic I
- Wagner P
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- Wanotayaroj C
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- Weidberg AR
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- Weingarten J
- Weirich M
- Weiser C
- Weits H
- Wells PS
- Wenaus T
- Wengler T
- Wenig S
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- Werner MD
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- Weston TD
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- Whallon NL
- Wharton AM
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- Whitmore BW
- Wickens FJ
- Wiedenmann W
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- Wiglesworth C
- Wiik-Fuchs LAM
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- Wilkens HG
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- Williams S
- Willis C
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- Wilson JA
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong KH Yau
- Wong VWS
- Worm SD
- Wosiek BK
- Wotschack J
- Wozniak KW
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- Xu L
- Xu T
- Yabsley B
- Yacoob S
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamamoto S
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- 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 F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhu CG
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- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
A search for the direct production of charginos and neutralinos in final states with at least two hadronically decaying tau leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 36.1 fb−1, recorded with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13TeV.Nosignificant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of ˜χ+1 ˜χ−1 pair production and of ˜χ±1 ˜χ02 and ˜χ+1 ˜χ−1 production in simplified models where the neutralinos and charginos decay solely via intermediate left-handed staus and tau sneutrinos, and the mass of the ˜ τL state is set to be halfway between the masses of the ˜χ±1 and the ˜χ01. Chargino masses up to 630 GeV are excluded at 95% confidence level in the scenario of direct production of ˜χ+1 ˜χ−1 for a massless ˜χ01. Common ˜χ±1 and ˜χ02 masses up to 760 GeV are excluded in the case of production of ˜χ±1 ˜χ02 and ˜χ+1 ˜χ−1 assuming a massless ˜χ01. Exclusion limits for additional benchmark scenarios with large and small mass-splitting between the ˜χ±1 and the ˜χ01 are also studied by varying the ˜ τL mass between the masses of the ˜χ±1 and the ˜χ01
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
- Author
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- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
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- Zhemchugov A
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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
Search for supersymmetry in events with four or more leptons in √s =13 TeV pp collisions with ATLAS
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- Yigitbasi E
- Yildirim E
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- Yoshihara K
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- Yuen SPY
- Yusuff I
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- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zerwas D
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- Zhang M
- Zhang P
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- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zou R
- 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
Study of ordered hadron chains with 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
- Afik Y
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- 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
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- 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
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans R Caminal
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga ME Pozo
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Bandyopadhyay A
- Banerjee Sw
- Bannoura AAE
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- Zimmermann C
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- Zinonos Z
- Zinser M
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- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
The analysis of the momentum difference between charged hadrons in high-energy proton-proton collisions is performed in order to study coherent particle production. The observed correlation pattern agrees with a model of a helical QCD string fragmenting into a chain of ground-state hadrons. A threshold momentum difference in the production of adjacent pairs of charged hadrons is observed, in agreement with model predictions. The presence of low-mass hadron chains also explains the emergence of charge-combination-dependent two-particle correlations commonly attributed to Bose-Einstein interference. The data sample consists of 190 μb−1 of minimum-bias events collected with proton-proton collisions at a center-of-mass energy √s=7 TeV in the early low-luminosity data taking with the ATLAS detector at the LHC
Anatomy of the sign-problem in heavy-dense QCD
- Author
- Adam E Romero
- Aranda C Padilla
- Arjanovic MM
- Armadans R Caminal
- Astigarraga ME Pozo
- Barajas CA Chavez
- Bechtle P
- Beck HP
- Becker K
- Becker M
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- Bednyakov VA
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- Benjamin DP
- Bensinger JR
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- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
QCD at finite densities of heavy quarks is investigated
using the density-of-states method. The phase factor
expectation value of the quark determinant is calculated to
unprecedented precision as a function of the chemical potential.
Results are validated using those from a reweighting
approach where the latter can produce a significant signalto-noise
ratio. We confirm the particle–hole symmetry at low
temperatures, find a strong sign problem at intermediate values
of the chemical potential, and an inverse Silver Blaze
feature for chemical potentials close to the onset value: here,
the phase-quenched theory underestimates the density of the
full theory
Search for anomalous couplings in the W tb vertex from the measurement of double differential angular decay rates of single top quarks produced in the t-channel with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
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- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
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- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
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- Aleksa M
- Aleksandrov IN
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- Alexander G
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 13/10/2015
- Field of study
The electroweak production and subsequent decay of single top quarks is determined by the properties of the Wtb vertex. This vertex can be described by the complex parameters of an effective Lagrangian. An analysis of angular distributions of the decay products of single top quarks produced in the t -channel constrains these parameters simultaneously. The analysis described in this paper uses 4.6 fb−1 of proton-proton collision data at √s =7 TeV collected with the ATLAS detector at the LHC. Two parameters are measured simultaneously in this analysis. The fraction f 1 of decays containing transversely polarised W bosons is measured to be 0.37 ± 0.07 (stat.⊕syst.). The phase δ − between amplitudes for transversely and longitudinally polarised W bosons recoiling against left-handed b-quarks is measured to be −0.014π ± 0.036π (stat.⊕syst.). The correlation in the measurement of these parameters is 0.15. These values result in two-dimensional limits at the 95% confidence level on the ratio of the complex coupling parameters g R and V L, yielding Re[g R /V L] ∈ [−0.36, 0.10] and Im[g R /V L] ∈ [−0.17, 0.23] with a correlation of 0.11. The results are in good agreement with the predictions of the Standard Model
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