159 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
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- Adelman J
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- Argyropoulos S
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- Arutinov D
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- Asman B
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- Yamazaki T
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- Zevi Della Porta G
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- Zhao Z
- Zhemchugov A
- Zhong J
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- 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
Scanpath analysis of expertise and culture in teacher gaze in real-world classrooms
- Author
- A Batki
- A Böckler
- A McCarthy
- A Senju
- AS Palincsar
- B Sherin
- C Wolff
- CD Frith
- CE Wolff
- D McNeill
- DC Berliner
- DC Berliner
- DE Hewes
- DF Feldon
- DJ Palmer
- DW-L Wu
- E Erdfelder
- EM Reingold
- FK Leung
- FK Leung
- G Committeri
- G Csibra
- G Csibra
- G Hofstede
- G Leinhardt
- GP Sackett
- H Akechi
- H Cheng
- H Haider
- HF Chua
- J Alston
- J Bédard
- J Holler
- J König
- J Ristic
- JG Elliott
- JJ Bartko
- JJ Merriënboer Van
- JL Fleiss
- JM Franchak
- JM Henderson
- JR Landis
- JR Searle
- K Ericsson
- K Humphrey
- KA Ericsson
- KS Cortina
- L Arnold
- L-F Zhang
- L-F Zhang
- LC Langavant De
- M Freeth
- M Hanley
- M Tomasello
- M Tomasello
- M Yang
- N Bogert van den
- N Zhou
- NA McIntyre
- Nora A. McIntyre
- P Chassy
- R Bakeman
- RC Pianta
- RC Pianta
- RE Nisbett
- RJ Sternberg
- RJ Sternberg
- RM Allen
- RM Foerster
- S Baron-Cohen
- S Brandt
- SH Cheon
- ST Fiske
- T Farroni
- T Farroni
- T Foulsham
- T Foulsham
- T Gog van
- T Wubbels
- Tom Foulsham
- VI Levenshtein
- YS Choi
- Z Wozniaková
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 05/01/2018
- Field of study
Humans are born to learn by understanding where adults look. This is likely to extend into the classroom, making teacher gaze an important topic for study. Expert teacher gaze has mainly been investigated in the laboratory, and has focused mostly on one cognitive process: teacher attentional (i.e., information-seeking) gaze. No known research has made direct cultural comparisons of teacher gaze or successfully found expert–novice differences outside Western settings. Accordingly, we conducted a real-world study of expert teacher gaze across two cultural settings, exploring communicative (i.e., information-giving) as well as attentional gaze. Forty secondary school teachers wore eye-tracking glasses, with 20 teachers (10 expert; 10 novice) from the UK and 20 teachers (10 expert; 10 novice) from Hong Kong. We used a novel eye-tracking scanpath analysis to ascertain the importance of expertise and culture, individually and as a combination. Attentional teacher scanpaths were significantly more similar within than across expertise and expertise + culture sub-groups; communicative scanpaths were significantly more similar within than across expertise and culture. Detailed analysis suggests that (1) expert teachers refer back to students constantly through focused gaze during both attentional and communicative gaze and that (2) expert teachers in Hong Kong scan students more than experts do in the UK
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
- 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
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- 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 Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- 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
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlas Collaboration
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
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- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Bakshi Gupta D
- Baldin EM
- Balek P
- Balli F
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- Benchekroun D
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- Berta P
- Bertella C
- Bertoli G
- Bertram IA
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- Bessidskaia Bylund O
- Bessner M
- Besson N
- Bethani A
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- Betti A
- Bevan AJ
- Beyer J
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
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- Biswal JP
- Bittrich C
- Bjergaard DM
- Black JE
- Black KM
- Blair RE
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blunier D
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Boscherini D
- Bosman M
- Bossio Sola JD
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bozson AJ
- Bracinik J
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- Brandt A
- Brandt G
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- Brau B
- Brau JE
- Breaden Madden WD
- Brendlinger K
- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
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- Broughton JH
- Bruckman De Renstrom PA
- Bruncko D
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- Bruno S
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
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- Buehrer F
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- Bullock D
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
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- Burke S
- Burmeister I
- Burr JTP
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- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Büscher D
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- Cabras G
- Cabrera Urbán S
- Caforio D
- Cai H
- Cairo VMM
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
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- Calvet D
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- Camarda S
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- Cameron D
- Caminal Armadans R
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Cano Bret M
- Cantero J
- Cao T
- Cao Y
- Capeans Garrido MDM
- Caprini I
- Caprini M
- Capua M
- Carbone RM
- Cardarelli R
- Cardillo FC
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carrá S
- Casadei D
- Casado MP
- Casha AF
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
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- Cavaliere V
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- Ceradini F
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- Cerri A
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- Cetin SA
- Chafaq A
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- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chau CC
- Chavez Barajas CA
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- Chelkov GA
- Chelstowska MA
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- Chen H
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- Chen X
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- Chen Y-H
- 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 I
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Christodoulou V
- Chu MC
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
- Cinca D
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Clark A
- Clark MR
- Clark PJ
- Clement C
- Coadou Y
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- Coccaro A
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- Coimbra AEC
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- Collot J
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- Connell SH
- Connelly IA
- Constantinescu S
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- Cooper-Sarkar AM
- Cormier F
- Cormier KJR
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- Mizukami A
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- Mkrtchyan T
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- Naryshkin I
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- Prokoshin F
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- Ristić B
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- Rusakovich NA
- Russell HL
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- Rybar M
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- Ryu S
- Ryzhov A
- Rzehorz GF
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- Sapronov A
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- Schwienhorst R
- Schäfer U
- Sciandra A
- Sciolla G
- Scornajenghi M
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- Sebastiani CD
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- Sekhon K
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- Shabalina E
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- Shaikh NW
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- Shaw SM
- Shcherbakova A
- Shen Y
- Sherafati N
- Sherman AD
- Sherwood P
- Shi L
- Shimizu S
- Shimmin CO
- Shimojima M
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shoaleh Saadi D
- Shochet MJ
- Shojaii S
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- Siragusa G
- Siral I
- Sivoklokov SY
- Sjölin J
- Skinner MB
- Skubic P
- Slater M
- Slavicek T
- Slawinska M
- Sliwa K
- Slovak R
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov N
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith JW
- Smith MNK
- Smith RW
- Smizanska M
- Smolek K
- Snesarev AA
- Snyder IM
- Snyder S
- Sobie R
- Soffa AM
- Soffer A
- Soh DA
- Sokhrannyi G
- Solans Sanchez CA
- Solar M
- Soldatov EY
- Soldevila U
- Solodkov AA
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
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- Sopczak A
- Sopkova F
- Sosa D
- Sotiropoulou CL
- Sottocornola S
- Soualah R
- Soukharev AM
- South D
- Sowden BC
- Spagnolo S
- Spalla M
- Spangenberg M
- Spanò F
- Sperlich D
- Spettel F
- Spieker TM
- Spighi R
- Spigo G
- Spiller LA
- Spiteri DP
- Spousta M
- Stabile A
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- Starovoitov P
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- Svatos M
- Swiatlowski M
- Swift SP
- Sydorenko A
- Sykora I
- Sykora T
- Sánchez J
- Søgaard A
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- Taenzer J
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- Tahirovic E
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- Talyshev AA
- Tanaka J
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- Tarek Abouelfadl Mohamed A
- Tarem S
- Tarna G
- Tartarelli GF
- Tas P
- Tasevsky M
- Tashiro T
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- Tayalati Y
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- Thomsen LA
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- Tian Y
- Ticse Torres RE
- Tikhomirov VO
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- Todt S
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- Tokushuku K
- Tokár S
- Tolley E
- Tomiwa KG
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- Torrence E
- Torres H
- Torró Pastor E
- Tosciri C
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- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
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- Tulbure TT
- Tuna AN
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- Turgeman D
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- Ucchielli G
- Ueda I
- Ughetto M
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- Unel G
- Ungaro FC
- Unno Y
- Uno K
- Urban J
- Urquijo P
- Urrejola P
- Usai G
- Usui J
- Vacavant L
- Vacek V
- Vachon B
- Vadla KOH
- Vaidya A
- Valderanis C
- Valdes Santurio E
- Valente M
- Valentinetti S
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- Vallance RA
- Vallier A
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- Valéry L
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- Van Gemmeren P
- Van Nieuwkoop J
- Van Vulpen I
- Van Woerden MC
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vari R
- Varnes EW
- Varni C
- Varol T
- Varouchas D
- Vartapetian A
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- Vazeille F
- Vazquez Furelos D
- Vazquez Schroeder T
- Veatch J
- Vecchio V
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Venturi M
- Venturi N
- Vercesi V
- Verducci M
- Vergel Infante CM
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vetterli MC
- Viaux Maira N
- Viazlo O
- Vichou I
- Vickey Boeriu OE
- Vickey T
- Viehhauser GHA
- Viel S
- Vigani L
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter MG
- Vinogradov VB
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vlachos S
- Vogel M
- Vokac P
- Volpi G
- Von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vranjes Milosavljevic M
- Vranjes N
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- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahlberg H
- Wahrmund S
- Wakamiya K
- Walbrecht VM
- Walder J
- Walker R
- Walkowiak W
- Wallangen V
- Wang AM
- Wang C
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- Wanotayaroj C
- Warburton A
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- Weidberg AR
- Weinert B
- Weingarten J
- Weirich M
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- Wengler T
- Wenig S
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- Werner MD
- Werner P
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- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
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- White MJ
- White R
- Whiteson D
- Whitmore BW
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wiglesworth C
- Wiik-Fuchs LAM
- Wildauer A
- Wilk F
- Wilkens HG
- Wilkins LJ
- Williams HH
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- Willis C
- Willocq S
- Wilson JA
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Woźniak KW
- Wraight K
- Wu M
- Wu SL
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- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
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- Xu H
- Xu L
- Xu T
- Xu W
- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamanaka T
- Yamane F
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yue X
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zerwas D
- Zgubič M
- Zhang D
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- Zhang F
- Zhang G
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- Zhang J
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- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
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
- Abraham NL
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- Zemaityte G
- Zemla A
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- Zeng Q
- Zenin O
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- Zhemchugov A
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- 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
Performance of the ATLAS muon trigger in pp collisions at [Formula: see text] TeV
- Author
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- Abbott B
- Abdallah J
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- Zhemchugov A
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- Åkesson TP
- Åsman B
- Ženiš T
- Publication venue
- Publication date
- 01/03/2015
- Field of study
The performance of the ATLAS muon trigger system is evaluated with proton-proton collision data collected in 2012 at the Large Hadron Collider at a centre-of-mass energy of 8 TeV. It is primarily evaluated using events containing a pair of muons from the decay of [Formula: see text] bosons. The efficiency of the single-muon trigger is measured for muons with transverse momentum [Formula: see text] GeV, with a statistical uncertainty of less than 0.01 % and a systematic uncertainty of 0.6 %. The [Formula: see text] range for efficiency determination is extended by using muons from decays of [Formula: see text] mesons, [Formula: see text] bosons, and top quarks. The muon trigger shows highly uniform and stable performance. The performance is compared to the prediction of a detailed simulation
Recommended from our members
Search for Dark Matter Produced in Association with a Higgs Boson Decaying to bb[over ¯] Using 36 fb^{-1} of pp Collisions at sqrt[s]=13 TeV 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
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- 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
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amundsen G
- Anastopoulos C
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- Andari N
- Andeen T
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- 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
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
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- Armbruster AJ
- Armitage LJ
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- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
- Astalos R
- Atkinson M
- ATLAS Collaboration
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- Avolio G
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- Ayoub MK
- Azuelos G
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- Bachacou H
- Bachas K
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- Bahrasemani H
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- Barkeloo JT
- Barklow T
- Barlow N
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- Zhemchugov A
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- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Ženiš T
- Živković L
- Publication venue
- Phys Rev Lett
- Publication date
- 03/11/2017
- Field of study
Several extensions of the standard model predict associated production of dark-matter particles with a Higgs boson. Such processes are searched for in final states with missing transverse momentum and a Higgs boson decaying to a bb[over ¯] pair with the ATLAS detector using 36.1 fb^{-1} of pp collisions at a center-of-mass energy of 13 TeV at the LHC. The observed data are in agreement with the standard model predictions and limits are placed on the associated production of dark-matter particles and a Higgs boson
Monitoring and data quality assessment of the ATLAS liquid argon calorimeter
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
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- Acharya BS
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- Publication venue
- Publication date
- 01/01/2014
- Field of study
The liquid argon calorimeter is a key component of the ATLAS detector installed at the CERN Large Hadron Collider. The primary purpose of this calorimeter is the measurement of electron and photon kinematic properties. It also provides a crucial input for measuring jets and missing transverse momentum. An advanced data monitoring procedure was designed to quickly identify issues that would affect detector performance and ensure that only the best quality data are used for physics analysis. This article presents the validation procedure developed during the 2011 and 2012 LHC data-taking periods, in which more than 98% of the proton-proton luminosity recorded by ATLAS at a centre-of-mass energy of 7-8 TeV had calorimeter data quality suitable for physics analysis
Search for Higgs and Z Boson Decays to J/ψγ and ϒ(nS)γ with the ATLAS Detector.
- Author
- (ATLAS Collaboration)
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- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdinov O
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- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou C
- Zhou L
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zurzolo G
- Zwalinski L
- Åkesson TPA
- Åsman B
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
A search for the decays of the Higgs and Z bosons to J/ψγ and ϒ(nS)γ (n=1,2,3) is performed with pp collision data samples corresponding to integrated luminosities of up to 20.3 fb^{-1} collected at sqrt[s]=8 TeV with the ATLAS detector at the CERN Large Hadron Collider. No significant excess of events is observed above expected backgrounds and 95% C.L. upper limits are placed on the branching fractions. In the J/ψγ final state the limits are 1.5×10^{-3} and 2.6×10^{-6} for the Higgs and Z boson decays, respectively, while in the ϒ(1S,2S,3S)γ final states the limits are (1.3,1.9,1.3)×10^{-3} and (3.4,6.5,5.4)×10^{-6}, respectively.We acknowledge the support of ANPCyT,
Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI,
Canada; CERN; CONICYT, Chile; CAS, MOST and
NSFC, China; COLCIENCIAS, Colombia; MSMT CR,MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; EPLANET, ERC and NSRF, European Union; IN2P3-CNRS, CEA-DSM/ IRFU, France; GNSF, Georgia; BMBF, DFG, HGF,
MPG and AvH Foundation, Germany; GSRT and
NSRF, Greece; ISF, MINERVA, GIF, I-CORE and
Benoziyo Center, Israel; INFN, Italy; MEXT and JSPS,
Japan; CNRST, Morocco; FOM and NWO, Netherlands;BRF and RCN, Norway; MNiSW and NCN, Poland;GRICES and FCT, Portugal; MNE/IFA, Romania; MES of Russia and ROSATOM, Russian Federation; JINR;MSTD, Serbia; MSSR, Slovakia; ARRS and MIZŠ, Slovenia; DST/NRF, South Africa; MINECO, Spain;SRC and Wallenberg Foundation, Sweden; SER, SNSF and Cantons of Bern and Geneva, Switzerland; NSC,Taiwan; TAEK, Turkey; STFC, the Royal Society and Leverhulme Trust, United Kingdom; DOE and NSF, United States of America
Search for flavour-changing neutral current top-quark decays t → qZ in proton-proton collisions at \sqrt{s} = 13 TeV 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
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- Zhemchugov A
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- Zobernig G
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- zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/07/2018
- Field of study
A search for flavour-changing neutral-current processes in top-quark decays is presented. Data collected with the ATLAS detector from proton-proton collisions at the Large Hadron Collider at a centre-of-mass energy of s√=13 TeV, corresponding to an integrated luminosity of 36.1 fb−1, are analysed. The search is performed using top-quark pair events, with one top quark decaying through the t → qZ (q = u, c) flavour-changing neutral-current channel, and the other through the dominant Standard Model mode t → bW. Only Z boson decays into charged leptons and leptonic W boson decays are considered as signal. Consequently, the final-state topology is characterized by the presence of three isolated charged leptons (electrons or muons), at least two jets, one of the jets originating from a b-quark, and missing transverse momentum from the undetected neutrino. The data are consistent with Standard Model background contributions, and at 95% confidence level the search sets observed (expected) upper limits of 1.7 × 10−4 (2.4 × 10−4) on the t → uZ branching ratio and 2.4 × 10−4 (3.2 × 10−4) on the t → cZ branching ratio, constituting the most stringent limits to date.
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General Didactics and Instructional Design: eyes like twins A transatlantic dialogue about similarities and differences, about the past and the future of two sciences of learning and teaching
- Author
- A Gruschka
- A Helmke
- AL Brown
- AS Gibbons
- B Bichelmeyer
- B Hudson
- BS Bloom
- C Bereiter
- C Errey
- CM Reigeluth
- CM Reigeluth
- D Jonassen
- D Leigh
- D Ritchie
- DA Norman
- DE Berlyne
- DE Broadbent
- DE Stokes
- DH Andrews
- DH Fretwell
- DH Jonassen
- DMA Sluijsmans
- DP Ausubel
- E Boling
- E Chartier
- E Kiel
- E König
- E Terhart
- EC Garbarino
- F Schott
- FK Sarfo
- FR Dinter
- FW Kron
- GA Miller
- GB Semb
- GL Hunter
- H Aebli
- H Borko
- H Ebbinghaus
- H Stachowiak
- HM Niegemann
- HW Thomas
- J Dolch
- J Gordon
- J Pieters
- J Sweller
- J Sweller
- J Sweller
- J Wedman
- J Willis
- JB Black
- JJG van Merriënboer
- JJG van Merriënboer
- JJG van Merriënboer
- JL Kolodner
- JS Brown
- JS Bruner
- JS Bruner
- JW Pellegrino
- K Wilber
- K Zierer
- K Zierer
- K Zierer
- K-H Flechsig
- KH Arnold
- KU Smith
- L Tyson
- LE Winer
- LM Stolurow
- LP Lysaught
- M Bönsch
- M Hannafin
- M Liu
- M Molenda
- M Scardamalia
- M Tessmer
- MA Meyer
- MC Wittrock
- MD Merrill
- MD Merrill
- MD Merrill
- NM Seel
- NM Seel
- NM Seel
- NM Seel
- NM Seel
- NM Seel
- O Willmann
- P Parrish
- PA Kirschner
- PL Smith
- R Bromme
- R Glaser
- R Lehrer
- R Lehrer
- RA Kaufman
- RA Kaufman
- RA Reiser
- RC Schank
- RD Tennyson
- RF Kenny
- RF Mager
- RJ Spiro
- RK Atkinson
- RM Gagné
- RM Gagné
- RM Gagné
- RM Morgan
- RM Morgan
- RN Shambaugh
- S Farnham-Diggory
- S Magliaro
- S Tripp
- SA Schrock
- SK Reed
- TF Meijman
- TJ Bastiaens
- TJ Shuell
- TS Kuhn
- TW Adorno
- U Hanke
- V Goel
- W Dick
- W Dick
- W Dick
- W Herzog
- W Jank
- W Klafki
- W Nicklis
- WH Bruford
- WJ Rothwell
- YB Kafai
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
- …