1,274 research outputs found
The Hidden Hydroxide in BaNiO3 Single Crystals Grown from a KOH Flux
- Author
- Publication venue
- Publication date
- 08/06/2023
- Field of study
Hexagonal oxide perovskites with one-dimensional chains of face-sharing MO6
octahedra are of enduring interest. Specifically, the hexagonal perovskite
BaNiO3, prepared via non-ceramic approaches, acts as a highly functional
catalyst for the oxygen-evolution reaction (OER) in alkaline media, with
numerous studies focusing on this behavior, while its fundamental structural
and physical properties have been somewhat overlooked. The current work is
intiated by the observation of contrasting magnetic properties of BaNiO3
synthesized via KOH flux growth and high O2 pressure ceramic synthesis. To shed
light on this difference, we have performed a series of rigorous analyses and
found that the KOH flux-grown crystals made in open-air are actually a wet form
of BaNiO3 that can be dried upon annealing in O2 flow but will then slowly
degrade if stored under a condition where the O2 partial pressure is not high
enough. Therefore, the present work not only provides insightful information to
unveil a previously unknown aspect of the OER catalyst BaNiO3, but also rings a
bell that the hidden hydroxide principle described here may also be applied to
other hexagonal perovskite oxides prepared in wet conditions.Comment: 21 pages, 6 figure
Excess Imidacloprid Exposure Causes the Heart Tube Malformation of Chick Embryos
- Author
- Publication venue
- 'American Chemical Society (ACS)'
- Publication date
- 28/10/2016
- Field of study
As a neonicotinoid pesticide, imidacloprid is widely used to control sucking insects on agricultural planting and fleas on domestic animals. However, the extent to which imidacloprid exposure has an influence on cardiogensis in early embryogenesis is still poorly understood. In vertebrates, the heart is the first organ to be formed. In this study to address whether or not imidacloprid exposure affects early heart development, the early chick embryo has been used as an experimental model because of the accessibility of chick embryo at its early developmental stage. The results demonstrate that exposure of the early chick embryo to imidacloprid caused malformation of heart tube. Furthermore,the data reveal that down-regulation of GATA4, Nkx2.5 and BMP4 and up-regulation of Wnt3a led to aberrant cardiomyocyte differentiation. In addition, imidacloprid exposure interfered with basement membrane (BM) breakdown, E-cadherin/Laminin expression and mesoderm formation during the epithelial-mesenchymal transition (EMT) in gastrula chick embryos. Finally, the DiI-labeled cell migration trajectory indicated that imidacloprid restricted the cell migration of cardiac progenitors to primary heart field in gastrula chick embryos. A similar observation was also obtained from the cell migration assay of scratch wounds in vitro. Additionally, imidacloprid exposure negatively affected the cytoskeleton structure and expression of corresponding adhesion molecules. Taken together, these results reveal that the improper EMT, cardiac progenitor migration and differentiation are responsible for imidacloprid exposure-induced malformation of heart tube during chick embryo development
The LAMOST Survey of Background Quasars in the Vicinity of the Andromeda and Triangulum Galaxies -- II. Results from the Commissioning Observations and the Pilot Surveys
- Author
- Bai Zhong-Rui
- Chen Jian-Jun
- Chen Xiao-Yan
- Chu Jia-Ru
- Chu Yao-Quan
- Cui Xiang-Qun
- Du Bing
- Hou Yong-Hui
- Hu Hong-Zhuan
- Hu Zhong-Wen
- Huang Yang
- Huo Zhi-Ying
- Jia Lei
- Jiang Fang-Hua
- Lei Ya-Juan
- Li Ai-Hua
- Li Guang-Wei
- Li Guo-Ping
- Li Jian
- Li Xin-Nan
- Li Yan
- Li Ye-Ping
- Liu Gen-Rong
- Liu Xiao-Wei
- Liu Zhi-Gang
- Lu Qi-Shuai
- Luo A-Li
- Luo Yu
- Men Li
- Ni Ji-Jun
- Qi Yong-Jun
- Qi Zhao-Xiang
- Shi Huo-Ming
- Shi Jian-Rong
- Sun Shi-Wei
- Tang Zheng-Hong
- Tian Yuan
- Tu Liang-Ping
- Wang Dan
- Wang Feng-Fei
- Wang Gang
- Wang Jia-Ning
- Wang Lei
- Wang Shu-Qing
- Wang You
- Wang Yue-Fei
- Wei Ming-Zhi
- Wu Yue
- Xiang Mao-Sheng
- Xue Xiang-Xiang
- Yan Lin
- Yao Zheng-Qiu
- Yu Yong
- Yuan Hai-Bo
- Yuan Hui
- Zhai Chao
- Zhang En-Peng
- Zhang Hao-Tong
- Zhang Hui-Hua
- Zhang Jian-Nan
- Zhang Wei
- Zhang Yan-Xia
- Zhang Yong
- Zhang Zhen-Chao
- Zhao Gang
- Zhao Ming
- Zhao Yong-Heng
- Zhou Fang
- Zhou Xin-Lin
- Zhu Yong-Tian
- Zou Si-Cheng
- Publication venue
- 'IOP Publishing'
- Publication date
- 10/04/2013
- Field of study
We present new quasars discovered in the vicinity of the Andromeda and
Triangulum galaxies with the LAMOST during the 2010 and 2011 observational
seasons. Quasar candidates are selected based on the available SDSS, KPNO 4 m
telescope, XSTPS optical, and WISE near infrared photometric data. We present
509 new quasars discovered in a stripe of ~135 sq. deg from M31 to M33 along
the Giant Stellar Stream in the 2011 pilot survey datasets, and also 17 new
quasars discovered in an area of ~100 sq. deg that covers the central region
and the southeastern halo of M31 in the 2010 commissioning datasets. These 526
new quasars have i magnitudes ranging from 15.5 to 20.0, redshifts from 0.1 to
3.2. They represent a significant increase of the number of identified quasars
in the vicinity of M31 and M33. There are now 26, 62 and 139 known quasars in
this region of the sky with i magnitudes brighter than 17.0, 17.5 and 18.0
respectively, of which 5, 20 and 75 are newly-discovered. These bright quasars
provide an invaluable collection with which to probe the kinematics and
chemistry of the ISM/IGM in the Local Group of galaxies. A total of 93 quasars
are now known with locations within 2.5 deg of M31, of which 73 are newly
discovered. Tens of quasars are now known to be located behind the Giant
Stellar Stream, and hundreds behind the extended halo and its associated
substructures of M31. The much enlarged sample of known quasars in the vicinity
of M31 and M33 can potentially be utilized to construct a perfect astrometric
reference frame to measure the minute PMs of M31 and M33, along with the PMs of
substructures associated with the Local Group of galaxies. Those PMs are some
of the most fundamental properties of the Local Group.Comment: 26 pages, 6 figures, AJ accepte
Large-Scale Comparative Analyses of Tick Genomes Elucidate Their Genetic Diversity and Vector Capacities
- Author
- Bell-Sakyi Lesley
- Cao Wu-Chun
- Chang Qiao-Cheng
- Chen Hai-Ying
- Chen Shen-En
- Cheng Jing Xia
- Consortium Tick Genome Microbiome
- Cui Xiao-Ming
- Dai Pei-Fang
- Ding Shu-Jun
- Du Chun-Hong
- Du Lifeng
- Gao Yu-Chi
- Guo Wen-Bin
- Han Xiao-Hu
- Huang En-Jiong
- Huo Qiu-Bo
- Ji Peifeng
- Jia Na
- Jiang Bao-Gui
- Jiang Jia-Fu
- Lam Tommy Tsan-Yuk
- Li Jie
- Li Lian-Feng
- Li Wei
- Liu Jing-Ze
- Liu Tao
- Ni Xue-Bing
- Pan Yu-Sheng
- Que Teng Cheng
- Ruan Xiang-Dong
- Shao Hong-Ze
- Sheng Yue
- Shi Wenqiang
- Sun Yi
- Tian Jun-Hua
- Wang Chong-Cai
- Wang Jinfeng
- Wang Qian
- Wang Xian-Jun
- Wang Xin
- Wei Jia-Te
- Wei Wei
- Xia Luo-Yuan
- Yang Tian-Ci
- Yang Wei-Fei
- Ye Run-Ze
- Yuan Ting-Ting
- Zhan Wei
- Zhang Bing
- Zhao Fangqing
- Zhao Lin
- Zhou Ling-Guo
- Zhou Yu-Hao
- Zhu Jin-Guo
- Publication venue
- 'Elsevier BV'
- Publication date
- 03/09/2020
- Field of study
Atg7-Mediated Autophagy Is Involved in the Neural Crest Cell Generation in Chick Embryo
- Author
- A Kuma
- AJ Chalpe
- AM Lacosta
- Andrea Münsterberg
- B Levine
- B Ravikumar
- BK Hall
- C Gao
- C Zhuo
- Chang Liang
- D Henrique
- DR Cordero
- E Coucouvanis
- En-ni Chen
- G Juhasz
- G Wang
- G Wang
- Guang Wang
- IH Lee
- J Cayuso
- J Jang
- J McCredie
- JE Simkin
- Jianxin Liang
- L Hari
- L Lamalice
- L Pinsky
- Lin-rui Gao
- Liu Cao
- M Komatsu
- MA Mellen
- Manli Chuai
- ML Basch
- MR Aburto
- OO Oyedele
- PJ Fraker
- Q Yue
- RA Schneider
- RC Russell
- S Somi
- SC Chapman
- SV Hegarty
- TC Carter
- TF Gale
- WH Lu
- X Qu
- X Wu
- X Yang
- X Yang
- Xuesong Yang
- XY Wang
- Y Liu
- Yongping Bao
- Z Jia
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/04/2018
- Field of study
Autophagy plays a very important role in numerous physiological and pathological events. However, it still remains unclear whether Atg7-induced autophagy is involved in the regulation of neural crest cell production. In this study, we found the co-location of Atg7 and Pax7+ neural crest cells in early chick embryo development. Upregulation of Atg7 with unilateral transfection of full-length Atg7 increased Pax7+ and HNK-1+ cephalic and trunk neural crest cell numbers compared to either Control-GFP transfection or opposite neural tubes, suggesting that Atg7 over-expression in neural tubes could enhance the production of neural crest cells. BMP4 in situ hybridization and p-Smad1/5/8 immunofluorescent staining demonstrated that upregulation of Atg7 in neural tubes suppressed the BMP4/Smad signaling, which is considered to promote the delamination of neural crest cells. Interestingly, upregulation of Atg7 in neural tubes could significantly accelerate cell progression into the S phase, implying that Atg7 modulates cell cycle progression. However, β-catenin expression was not significantly altered. Finally, we demonstrated that upregulation of the Atg7 gene could activate autophagy as did Atg8. We have also observed that similar phenotypes, such as more HNK-1+ neural crest cells in the unilateral Atg8 transfection side of neural tubes, and the transfection with full-length Atg8-GFP certainly promote the numbers of BrdU+ neural crest cells in comparison to the GFP control. Taken together, we reveal that Atg7-induced autophagy is involved in regulating the production of neural crest cells in early chick embryos through the modification of the cell cycle
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck GA
- Beck HP
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellina F
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Beretta M
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernardet K
- Bernat P
- Bernhard R
- Bernius C
- Berry T
- Bertin A
- Bertinelli F
- Bertolucci F
- Besana MI
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biscarat C
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blazek T
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VB
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeriu OEV
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Bolnet NM
- Bona M
- Bondarenko VG
- Bondioli M
- Boonekamp M
- Boorman G
- Booth CN
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borroni S
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcic I
- Bracinik J
- Braem A
- Branchini P
- Brandenburg GW
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brelier B
- Bremer J
- Brenner R
- Bressler S
- Breton D
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
- Brown H
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- BScher V
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- Bueso XP
- Bugge L
- Buira-Clark D
- Bulekov O
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butin F
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Caballero J
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi R
- Calvet D
- Calvet S
- Camarri P
- Cambiaghi M
- Cameron D
- Camilocci ES
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepaa A
- Cantero J
- Capasso L
- Caprini I
- Caprini M
- Capriotti D
- Capua M
- Caputo R
- Caramarcu C
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron B
- Caron S
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo LRF
- Castro NF
- Cataldi G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cauz D
- Cavalcanti TP
- Cavalleri P
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cetin SA
- Cevenini F
- Chafaq A
- Chakraborty D
- Chan K
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciba K
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciobotaru MD
- Cioccaa C
- Ciocio A
- Cirilli M
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Cleland W
- Clemens JC
- Clement B
- Clement C
- Clifft RW
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coe P
- Cogan JG
- Coggeshall J
- Cogneras E
- Cojocaru CD
- Colas J
- Colijn AP
- Collaboration ATLAS
- Collard C
- Collins NJ
- Collins-Tooth C
- Collot J
- Colon G
- Coniavitis E
- Conidi MC
- Consonni M
- Consorti V
- Constantinescu S
- Conta C
- Conventi F
- Cook J
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Costin T
- Cote D
- Courneyea L
- Cowan G
- Cowden C
- Cox BE
- Cranmer K
- Cranshaw J
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Crosetti G
- Crupi R
- Cuciuc C-M
- Curatolo M
- Curtis CJ
- Curull XE
- Cwetanski P
- Czirr H
- Czyczula Z
- D'Auria S
- D'Onofrio M
- D'Orazio A
- Da Costa JBG
- Da Costa JGPF
- Da Silva PVM
- Da Via C
- Dabrowski W
- Dai T
- Dallapiccola C
- Daly CH
- Dam M
- Damazio DO
- Dameri M
- Damiani DS
- Danielsson HO
- Dannheim D
- Dao V
- Darbo G
- Darlea GL
- Daum C
- Dauvergne JP
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies E
- Davies M
- Davison AR
- Davygora Y
- Dawe E
- Dawson I
- Dawson JW
- Daya-Ishmukhametova RK
- de Asmundis R
- De Castro S
- De Cecco S
- De Graat J
- De Groot N
- De Jong P
- De la Hoz SG
- De la Taille C
- De la Torre H
- De Lima JGR
- De Lotto B
- De Mora L
- De Nooij L
- De Pedis D
- De Regie JBDV
- De Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
- De K
- Dean S
- Debbe R
- Dedovich DV
- Degenhardt J
- Dehchar M
- Del Papa C
- Del Peso J
- Del Prete T
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Porta GZ
- della Volpe D
- Delmastro M
- Delpierre P
- Delruelle N
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demirkoz B
- Deng J
- Deng W
- Denis RDS
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Devetak E
- Deviveiros PO
- Dewhurst A
- DeWilde B
- Dhaliwal S
- Dhullipudi R
- Di Ciaccio A
- Di Ciaccio L
- Di Girolamo A
- Di Girolamo B
- Di Luise S
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipio R
- Diaz MA
- Diblen F
- Diehl EB
- Dietrich J
- Dietzscha TA
- Diglio S
- Dingfelder J
- Dionisi C
- Dita P
- Dita S
- Dittus F
- Djama F
- Djobava T
- do Vale MAB
- Do ValleWemans A
- Doan TKO
- Dobbs M
- Dobinson R
- Dobos D
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- Dodd J
- Doglioni C
- Doherty T
- Dohmae T
- Doi Y
- Dolejsi J
- Dolenc I
- Dolezal Z
- Dolgoshein BA
- Donadelli M
- Donega M
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dos Anjos A
- Dos Santos DR
- Dosil M
- Dotti A
- Dova MT
- Dowell JD
- Doxiadis AD
- Doyle AT
- Drasal Z
- Drees J
- Dressnandt N
- Drevermann H
- Driouichi C
- Dris M
- Dubbert J
- Dubbs T
- Dube S
- Duchovni E
- Duckeck G
- Dudarev A
- Dudziak F
- Duehrssen M
- Duerdoth IP
- Dueren M
- Duflot L
- Dufour M-A
- Dunford M
- Duxfield R
- Dwuznik M
- Dydak F
- Ebenstein WL
- Ebke J
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- Eckweiler S
- Edmonds K
- Edwards CA
- Edwards NC
- Ehrenfeld W
- Ehrich T
- Eifert T
- Eigen G
- Einsweiler K
- Eisenhandler E
- Ekelof T
- El Kacimi M
- El Moursli RC
- Ellert M
- Elles S
- Ellinghaus F
- Ellis K
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- Elmsheuser J
- Elsing M
- Emeliyanov D
- Engelmann R
- Engl A
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- Ereditato A
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- Ernst J
- Ernst M
- Ernwein J
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- Yilmaz M
- Yoosootiniya R
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- Zhemchugov A
- Zheng S
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- Zieminska D
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- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
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- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
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- Adelman J
- Adomeit S
- Adye T
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- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
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- Allbrooke BMM
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- Allport PP
- Allwood-Spiers SE
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- De la Taille C
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- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
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- della Porta GZ
- della Volpe D
- Delmastro M
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- Deluca C
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- Demilly A
- Demirkoz B
- Denisov SP
- Derendarz D
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- Derue F
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- Deviveiros PO
- Dewhurst A
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- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Mattia A
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- Diglio S
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- Doglioni C
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- Ekelof T
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- Enari Y
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- Endner OC
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- Endo M
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- Engelmann R
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- Erdmann J
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- Errede D
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- Errede S
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- Ertel E
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- Escalier M
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- Esch H
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- Escobar C
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- Espinal Curull X
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- Esposito B
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- Etienne F
- Etienne F
- Etienvre AI
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- Etzion E
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- Evans H
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- Fabbri L
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- Facini G
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- Fakhrutdinov RM
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- Falciano S
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- Faltova J
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- Fang Y
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- Fanti M
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- Farbin A
- Farbin A
- Farilla A
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- Farooque T
- Farooque T
- Farrell S
- Farrell S
- Farrington SM
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- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
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- Fassouliotis D
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- Favareto A
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- Fayard L
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- Federic P
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- Fedin OL
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- Fedorko W
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- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
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- Feligioni L
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- Feng C
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- Feng EJ
- Feng EJ
- Feng H
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- Fenyuk AB
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- Fernando W
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- Ferrag S
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- Ferrando BMS
- Ferrando J
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- Ferrara V
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- Ferrari A
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- Ferrari P
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- Ferrari R
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- Ferretti C
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- Fiascaris M
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- Fiedler F
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- Filipcic A
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- Filipuzzi M
- Filipuzzi M
- Filthaut F
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- Fincke-Keeler M
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- Fiorini L
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- Firan A
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- Fisher MJ
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- Fitzgerald EA
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- Fleck I
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- Fleischmann P
- Fleischmann P
- Fleischmann S
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- Fletcher G
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- Floderus A
- Floderus A
- Florez Bustos AC
- Flowerdew MJ
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- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
- Fortin D
- Fournier D
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- Francavilla P
- Francavilla P
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- Franchini M
- Franchino S
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- Francis D
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- Franklin M
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- Franz S
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- Fraternali M
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- French ST
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- Gadomski S
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- Gagnon P
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- Galea C
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- Gallas EJ
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- Gallo V
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- Gallop BJ
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- Gao YS
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- Gardner RW
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- Garelli N
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- Garonne V
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- Garrido MDMC
- Gatti C
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- Gaudio G
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- Gaur B
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- Gauzzi P
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- Gavrilenko IL
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- Gaycken G
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- Gazis EN
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- Ge P
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- Gecse Z
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- Gee CNP
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- Geerts DAA
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- Geich-Gimbel C
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- Gellerstedt K
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- Gemme C
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- Gemmell A
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- Genest MH
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- Gentile S
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- George M
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- George S
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- Gerbaudo D
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- Gershon A
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- Ghazlane H
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- Ghodbane N
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- Giangiobbe V
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- Giannetti P
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- Gillam TPS
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- Gillberg D
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- Gillman AR
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- Gingrich DM
- Gingrich M
- Giokaris N
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- Giordani MP
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- Giordano R
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- Giugni D
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- Gornicki E
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- Goshaw AT
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- Gostkin MI
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- Zaidan R
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- Zaman A
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- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Search for pair-produced long-lived neutral particles decaying to jets in the ATLAS hadronic calorimeter in ppcollisions at √s=8TeV
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- zur Nedden M
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study
The ATLAS detector at the Large Hadron Collider at CERN is used to search for the decay of a scalar boson to a pair of long-lived particles, neutral under the Standard Model gauge group, in 20.3fb−1of data collected in proton–proton collisions at √s=8TeV. This search is sensitive to long-lived particles that decay to Standard Model particles producing jets at the outer edge of the ATLAS electromagnetic calorimeter or inside the hadronic calorimeter. No significant excess of events is observed. Limits are reported on the product of the scalar boson production cross section times branching ratio into long-lived neutral particles as a function of the proper lifetime of the particles. Limits are reported for boson masses from 100 GeVto 900 GeV, and a long-lived neutral particle mass from 10 GeVto 150 GeV
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
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- Charfeddine D
- Charlton DG
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- Chekulaev SV
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- Chernyatin V
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- D'Auria S
- D'Onofrio M
- da Costa JBG
- Da Costa JGPF
- Da Cunha Sargedas De Sousa MJ
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- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
- …