26 research outputs found
Operation and performance of the ATLAS Tile Calorimeter in Run 1
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouelfadl 
- 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
- Akerstedt H
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- 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 
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor 
- 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
- Arce ATH
- Ardell RE
- Arduh FA
- Argos FC
- Arguin J-
- Argyropoulos S
- Armadans R
- 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
- Astigarraga ME
- Atkin RJ
- Atkinson M
- Atlay NB
- Auerbach B
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Álvarez Piqueras D
- Åkesson TPA
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahilo JJL
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M
- Barkeloo J
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro Guimarães da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batlamous S
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becker M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Bell AS
- Bella G
- Bellagamba L
- Bellerive A
- Bello FA
- Bellomo M
- Belotskiy K
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Benekos N
- Benhammou Y
- Benhar Noccioli E
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Bergsten LJ
- Beringer J
- Berlendis S
- Bernard NR
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertram IA
- Besjes GJ
- Bessidskaia Bylund O
- Bessner M
- Besson N
- Bethani A
- Bethke S
- 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
- Bini C
- Biondi S
- Bisanz T
- 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
- Bostanabad M
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt A
- Brandt G
- Brandt O
- Braren F
- Bratzler U
- 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
- Brost E
- Broughton JH
- Brown H
- Bruckman de Renstrom PA
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Bugge MK
- Bulekov O
- Bullock D
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burka K
- Burke S
- Burmeister I
- Burr JTP
- Busato E
- Buschmann E
- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bührer F
- Büscher D
- Büscher V
- Cabras G
- Cabrera Urbán S
- Caforio D
- Cai H
- Cairo VMM
- Cakir I
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarri P
- Cameron D
- Caminal 
- 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
- Carrá S
- Carrillo-Montoya GD
- 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
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan WS
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chau CC
- Chavez Barajas CA
- Che S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen CH
- Chen H
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y
- 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 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
- Ciaccio A
- Ciaccio L
- Cinca D
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Clark A
- Clark MR
- Clark PJ
- Clement C
- Clemente WK
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Coimbra AEC
- Colasurdo L
- Cole B
- Colijn AP
- Collot J
- Conde Muiño P
- Coniavitis E
- Connell SH
- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar AM
- Cormier F
- Cormier KJR
- Corradi M
- Correia AM
- Corrigan EE
- Corriveau F
- Cortes-Gonzalez A
- Costa MJ
- Costanzo D
- Cottin G
- Cowan G
- Cox BE
- Crane J
- Cranmer K
- Crawley SJ
- Creager RA
- Cree G
- Crescioli F
- Crépé-Renaudin S
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cuhadar Donszelmann T
- Cukierman AR
- Cunha 
- Curatolo M
- Cúth J
- Czekierda S
- Czodrowski P
- Da Via C
- Da 
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallaire F
- Dallapiccola C
- Dam M
- Damp J
- Dandoy JR
- Daneri MF
- Dang NP
- Dann ND
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dartsi O
- Dattagupta A
- Daubney T
- Davey W
- David C
- Davidek T
- Davis DR
- Davydov Y
- Dawe E
- Dawson I
- De Asmundis R
- De Benedetti A
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- De Lorenzi F
- De Maria A
- De Moura 
- De Pedis D
- De Salvo A
- De Sanctis U
- De Santo A
- De Vasconcelos Corga K
- De Vivie 
- De 
- De 
- De K
- Debenedetti C
- Dedovich DV
- Dehghanian N
- Del Gaudio M
- Del Peso J
- Delgado A
- Delgove D
- Deliot F
- Delitzsch CM
- Della Pietra M
- Della Volpe D
- Dell’Acqua A
- Dell’Asta L
- Delmastro M
- Delporte C
- Delsart PA
- DeMarco DA
- Demers S
- Demichev M
- Denisov SP
- Denysiuk D
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Dette K
- Devesa MR
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Di 
- Diaconu C
- Diamond M
- Dias 
- Dias FA
- Diaz LP
- Diaz MA
- Dickinson J
- Diehl EB
- Dietrich J
- Dimitrievska A
- Dingfelder J
- Dittus F
- Díez Cornell S
- Djama F
- Djobava T
- Djuvsland JI
- Do 
- Do 
- Dobre M
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Donadelli M
- Donato C
- Donini J
- Dopke J
- Doria A
- Dortz O
- Dos 
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Dreyer T
- Dris M
- Du Y
- Duarte-Campderros J
- Dubinin F
- Dubreuil A
- Duchovni E
- Duckeck G
- Ducourthial A
- Ducu OA
- Duda D
- Dudarev A
- Dudder AC
- Duffield EM
- Duflot L
- Dumancic M
- Dumitriu AE
- Duncan AK
- Dunford M
- Duperrin A
- Duran 
- Durglishvili A
- Duschinger D
- Dutta B
- Duvnjak D
- Dührssen M
- Dülsen C
- Düren M
- Dyndal M
- Dysch S
- Dziedzic BS
- D’amen G
- D’Auria S
- D’Eramo L
- D’onofrio A
- D’Onofrio M
- Eckardt C
- Ecker KM
- Edgar RC
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Kosseifi R
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Enari Y
- Ennis JS
- Epland MB
- Erdmann J
- Ereditato A
- Errede S
- Escalier M
- Escobar C
- Esposito B
- Estrada 
- Etienvre AI
- Etzion E
- Evans H
- Ezhilov A
- Ezzi M
- Fabbri F
- Fabbri L
- Fabiani V
- Facini G
- Faisca 
- Fakhrutdinov RM
- Falciano S
- Falke PJ
- Falke S
- Faltova J
- Fang Y
- Fanti M
- Farbin A
- Farilla A
- Farina EM
- Farooque T
- Farrell S
- Farrington SM
- Farthouat P
- Fassi F
- Fassnacht P
- Fassouliotis D
- Faucci Giannelli M
- Favareto A
- Fawcett WJ
- Fayard L
- Fedin OL
- Fedorko W
- Feickert M
- Feigl S
- Feligioni L
- Feng C
- Feng EJ
- Feng M
- Fenton MJ
- Fenyuk AB
- Feremenga L
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
- Ferreira de Lima DE
- Ferrer A
- Ferrere D
- Ferretti C
- Fiedler F
- Filipčič A
- Filthaut F
- Finelli KD
- Fiolhais MCN
- Fiorini L
- Fischer C
- Fisher WC
- Flaschel N
- Fleck I
- Fleischmann P
- Fletcher RRM
- Flick T
- Flierl BM
- Flores Castillo LR
- Flores LM
- Fomin N
- Forcolin GT
- Formica A
- Forti AC
- Foster AG
- Fournier D
- Fox H
- Förster FA
- Fracchia S
- Francavilla P
- Franchini M
- Franchino S
- Francis D
- Franconi L
- Franklin M
- Frate M
- Fraternali M
- Freeborn D
- Fressard-Batraneanu SM
- Freund B
- Freund WS
- Froidevaux D
- Frost JA
- Fukunaga C
- Furelos D
- Fusayasu T
- Fuster J
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gach GP
- Gadatsch S
- Gadow P
- Gagliardi G
- Gagnon LG
- Galea C
- Galhardo B
- Gallas EJ
- Gallop BJ
- Gallus P
- Galster G
- Gamboa 
- Gan KK
- Ganguly S
- Gao Y
- Gao YS
- Garcia RF
- Garcia-Sciveres M
- García Navarro JE
- García Pascual JA
- García C
- Gardner RW
- Garelli N
- Garonne V
- Gasnikova K
- Gaudiello A
- Gaudio G
- Gavrilenko IL
- Gavrilyuk A
- Gay C
- Gaycken G
- Gazis EN
- Gee CNP
- Geisen J
- Geisen M
- Geisler MP
- Gellerstedt K
- Gemme C
- Genest MH
- Geng C
- Gentile S
- Gentsos C
- George S
- Gerbaudo D
- Gessner G
- Ghasemi 
- Ghasemi S
- Ghneimat M
- Giacobbe B
- Giagu S
- Giangiacomi N
- Giannetti P
- Gibson SM
- Gignac M
- Gillberg D
- Gilles G
- Gingrich DM
- Giordani MP
- Giorgi FM
- Giraud PF
- Girolamo A
- Giromini P
- Giugliarelli G
- Giugni D
- Giuli F
- Giulini M
- Gkaitatzis S
- Gkialas I
- Gkougkousis EL
- Gkountoumis P
- Gladilin LK
- Glasman C
- Glatzer J
- Glaysher PCF
- Glazov A
- Goblirsch-Kolb M
- Godlewski J
- Goldfarb S
- Golling T
- Golubkov D
- Gomes A
- Gomes AS
- Goncalves Gama R
- Gonçalo R
- Gonella G
- Gonella L
- Gongadze A
- Goni R
- Gonnella F
- Gonski JL
- Gonzalez 
- Gonzalez B
- Gonzalez-Sevilla S
- González de la Hoz S
- Goossens L
- Gorbounov PA
- Gordon HA
- Gorini B
- Gorini E
- Gorišek A
- Goshaw AT
- Gostkin MI
- Gottardo CA
- Goudet CR
- Goujdami D
- Goussiou AG
- Gouveia EDM
- Govender N
- Goy C
- Gozani E
- Gössling C
- Grabowska-Bold I
- Gradin POJ
- Graham EC
- Gramling J
- Gramstad E
- Grancagnolo S
- Gratchev V
- Gravila PM
- Gray C
- Gray HM
- Greenwood ZD
- Grefe C
- Gregersen K
- Gregor IM
- Grenier P
- Grevtsov K
- Griffiths J
- Grillo AA
- Grimm K
- Grinstein S
- Gris P
- Grivaz J-
- Groh S
- Gross E
- Grosse-Knetter J
- Grossi GC
- Grout ZJ
- Grud C
- Grummer A
- Guan L
- Guan W
- Guenther J
- Guerguichon A
- Guescini F
- Guest D
- Gugel R
- Gui B
- Guillemin T
- Guindon S
- Guirriec E
- Gul U
- Gumpert C
- Guo J
- Guo W
- Guo Y
- Guo Z
- Gupta DB
- Gupta R
- Gurbuz S
- Gurriana L
- Gustavino G
- Gutelman BJ
- Gutierrez P
- Gutschow C
- Guyot C
- Guzik MP
- Gwenlan C
- Gwilliam CB
- Haas A
- Haber C
- Hadavand HK
- Haddad N
- Hadef A
- Hageböck S
- Hagihara M
- Hakobyan H
- Haleem M
- Haley J
- Halladjian G
- Hallewell GD
- Hamacher K
- Hamal P
- Hamano K
- Hamilton A
- Hamity GN
- Han K
- Han L
- Han S
- Hanagaki K
- Hance M
- Handl DM
- Haney B
- Hankache R
- Hanke P
- Hansen E
- Hansen JB
- Hansen JD
- Hansen MC
- Hansen PH
- Hara K
- Hard AS
- Harenberg T
- Harkusha S
- Harrison PF
- Hartmann NM
- Hasegawa Y
- Hasib A
- Hassani S
- Haug S
- Hauser R
- Hauswald L
- Havener LB
- Havranek M
- Hawkes CM
- Hawkings RJ
- Hayden D
- Hayes C
- Hays CP
- Hays JM
- Hayward HS
- Haywood SJ
- Heath MP
- Hedberg V
- Heelan L
- Heer S
- Heidegger KK
- Heilman J
- Heim S
- Heim T
- Heinemann B
- Heinrich JJ
- Heinrich L
- Heinz C
- Hejbal J
- Helary L
- Held A
- Hellesund S
- Hellman S
- Helsens C
- Henderson RCW
- Heng Y
- Henkelmann S
- Henriques 
- Herbert GH
- Herde H
- Herget V
- Hernandez CM
- Hernandez D
- Hernández Jiménez Y
- Herr H
- Herten G
- Hertenberger R
- Hervas L
- Herwig TC
- Hesketh GG
- Hessey NP
- Hetherly JW
- Higashino S
- Higón-Rodriguez E
- Hildebrand K
- Hill E
- Hill JC
- Hill KK
- Hiller KH
- Hillier SJ
- Hils M
- Hinchliffe I
- Hirose M
- Hirschbuehl D
- Hiti B
- Hladik O
- Hlaluku DR
- Hoad X
- Hobbs J
- Hod N
- Hodgkinson MC
- Hoecker A
- Hoeferkamp MR
- Hoenig F
- Hohn D
- Hohov D
- Holmes TR
- Holzbock M
- Homann M
- Honda S
- Honda T
- Hong TM
- Hooberman BH
- Hopkins WH
- Horii Y
- Horn P
- Horton AJ
- Horyn LA
- Hostachy J-
- Hostiuc A
- Hou S
- Hoummada A
- Howarth J
- Hoya J
- Hönle A
- Hrabovsky M
- Hrdinka J
- Hristova I
- Hrivnac J
- Hrynevich A
- Hryn’ova T
- Hsu PJ
- Hsu S-
- Hu Q
- Hu S
- Huang Y
- Hubacek Z
- Hubaut F
- Huebner M
- Huegging F
- Huffman TB
- Hughes EW
- Huhtinen M
- Hunter RFH
- Huo P
- Hupe AM
- Hurwitz M
- Huseynov N
- Huston J
- Huth J
- Hyneman R
- Iacobucci G
- Iakovidis G
- Ibragimov I
- Iconomidou-Fayard L
- Idrissi Z
- Iengo P
- Ignazzi R
- Igonkina O
- Iguchi R
- Iizawa T
- Ikegami Y
- Ikeno M
- Iliadis D
- Ilic N
- Iltzsche F
- Infante CMV
- Introzzi G
- Iodice M
- Iordanidou K
- Ippolito V
- Isacson MF
- Ishijima N
- Ishino M
- Ishitsuka M
- Issever C
- Istin S
- Ito F
- Iturbe Ponce JM
- Iuppa R
- Ivina A
- Iwasaki H
- Izen JM
- Izzo V
- Jabbar S
- Jacka P
- Jackson P
- Jacobs RM
- Jain V
- Jakobi KB
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- Zur 
- Zwalinski L
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The Tile Calorimeter is the hadron calorimeter covering the central region of the ATLAS experiment at the Large Hadron Collider. Approximately 10,000 photomultipliers collect light from scintillating tiles acting as the active material sandwiched between slabs of steel absorber. This paper gives an overview of the calorimeter’s performance during the years 2008–2012 using cosmic-ray muon events and proton–proton collision data at centre-of-mass energies of 7 and 8TeV with a total integrated luminosity of nearly 30 fb−1. The signal reconstruction methods, calibration systems as well as the detector operation status are presented. The energy and time calibration methods performed excellently, resulting in good stability of the calorimeter response under varying conditions during the LHC Run 1. Finally, the Tile Calorimeter response to isolated muons and hadrons as well as to jets from proton–proton collisions is presented. The results demonstrate excellent performance in accord with specifications mentioned in the Technical Design Report
Search for heavy neutral Higgs bosons produced in association with b-quarks and decaying into b-quarks at root s=13 TeV with the ATLAS detector
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- Yigitbasi E
- Yildiz HD
- Yorita K
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- Yuen SPY
- Zabinski B
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- Zahreddine J
- Zaitsev AM
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- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeiner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
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- Zhang F
- Zhang G
- Zhang G
- Zhang H
- Zhang J
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- Zhang L
- Zhang M
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 13/08/2020
- Field of study
A search for heavy neutral Higgs bosons produced in association with one or two
b
-quarks and decaying to
b
-quark pairs is presented using
27.8
fb
−
1
of
√
s
=
13
TeV
proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider during 2015 and 2016. No evidence of a signal is found. Upper limits on the heavy neutral Higgs boson production cross section times its branching ratio to
b
¯
b
are set, ranging from 4.0 to 0.6 pb at 95% confidence level over a Higgs boson mass range of 450 to 1400 GeV. Results are interpreted within the two-Higgs-doublet model and the minimal supersymmetric Standard Model
Search for excited electrons singly produced in proton–proton collisions at \sqrt{s} = 13 TeV with the ALAS experiment at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- 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
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- 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
- Arabidze G
- Aranda CP
- Araque JP
- Araya ST
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
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- Zhemchugov A
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- Zobernig G
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- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2019
- Field of study
A search for excited electrons produced in pp collisions at s√ = 13 TeV via a contact interaction qq¯→ee∗ is presented. The search uses 36.1 fb −1 of data collected in 2015 and 2016 by the ATLAS experiment at the Large Hadron Collider. Decays of the excited electron into an electron and a pair of quarks ( eqq¯ ) are targeted in final states with two electrons and two hadronic jets, and decays via a gauge interaction into a neutrino and a W boson ( νW ) are probed in final states with an electron, missing transverse momentum, and a large-radius jet consistent with a hadronically decaying W boson. No significant excess is observed over the expected backgrounds. Upper limits are calculated for the pp→ee∗→eeqq¯ and pp→ee∗→eνW production cross sections as a function of the excited electron mass me∗ at 95% confidence level. The limits are translated into lower bounds on the compositeness scale parameter Λ of the model as a function of me∗ . For me∗<0.5 TeV , the lower bound for Λ is 11 TeV . In the special case of me∗=Λ , the values of me∗<4.8 TeV are excluded. The presented limits on Λ are more stringent than those obtained in previous searches
Combination of searches for heavy resonances decaying into bosonic and leptonic final states using 36 fb−1 of proton-proton collision data at √s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
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- Yildiz HD
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- Yuen SPY
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- Zaidan R
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- Zhao P
- Zhao X
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- Zhao Z
- Zhemchugov A
- Zhong D
- Zhou B
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- Zhou L
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- Zhou N
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- Zhu CG
- Zhu H
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- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
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- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zur Nedden M
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 26/09/2018
- Field of study
Searches for new heavy resonances decaying into different pairings of W,Z, or Higgs bosons, as well as directly into leptons, are presented using a data sample corresponding to 36.1 fb−1 of pp collisions at √s=13 TeV
collected during 2015 and 2016 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting bosonic decay modes in the qqqq, ννqq, ℓνqq, ℓℓqq, ℓνℓν,
ℓℓνν, ℓνℓℓ, ℓℓℓℓ, qqbb, ννbb, ℓνbb, and ℓℓbb final states are combined, searching for a narrow-width resonance. Likewise, analyses selecting the leptonic ℓν and ℓℓ final states are also combined. These two sets of analyses are then further combined. No significant deviation from the Standard Model predictions is observed. Three benchmark models are tested: a model predicting the existence of a new heavy scalar singlet, a simplified model predicting a heavy vector-boson triplet, and a bulk Randall-Sundrum model with a heavy spin-2 Kaluza-Klein excitation of the graviton. Cross section limits are set at the 95% confidence level using an asymptotic approximation and are compared with predictions for the benchmark models. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The data exclude a heavy vector-boson triplet with mass below 5.5 TeV in a weakly coupled scenario and 4.5 TeV in a strongly coupled scenario, as well as a Kaluza-Klein graviton with mass below 2.3 TeV
Search for the HH → b b ¯ b b ¯ process via vector-boson fusion production using proton-proton collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alvarez Piqueras D
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
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- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
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- Anelli CR
- Angelidakis S
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- Zhemchugov A
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- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- Journal of High Energy Physics
- Publication date
- 01/01/2020
- Field of study
Abstract: A search for Higgs boson pair production via vector-boson fusion (VBF) in the bb¯bb¯ final state is carried out with the ATLAS experiment using 126 fb−1 of proton- proton collision data delivered at s = 13 TeV by the Large Hadron Collider. This search is sensitive to VBF production of additional heavy bosons that may decay into Higgs boson pairs, and in a non-resonant topology it can constrain the quartic coupling between the Higgs bosons and vector bosons. No significant excess relative to the Standard Model expectation is observed, and limits on the production cross-section are set at the 95% confidence level for a heavy scalar resonance in the context of an extended Higgs sector, and for non-resonant Higgs boson pair production. Interpretation in terms of the coupling between a Higgs boson pair and two vector bosons is also provided: coupling values normalised to the Standard Model expectation of κ2V 2.90 are excluded at the 95% confidence level in data
Bottle-grade polyethylene furanoate from ring-opening polymerisation of cyclic oligomers
- Author
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- 'Springer Science and Business Media LLC'
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Elucidation of non-intentionally added substances migrating from polyester-polyurethane lacquers using automated LC-HRMS data processing
- Author
- A Schaefer
- AG Harrison
- ALM Nasser
- B Lim
- Bruno Le Bizec
- C Bignardi
- C Bignardi
- C Kuhl
- C Nerin
- CA Smith
- D Jenke
- D-J Kim
- E Bradley
- E Canellas
- EL Bradley
- Elsa Omer
- European Food Safety Authority
- Gaud Dervilly-Pinel
- Gérald Remaud
- H Milon
- Hélène Germon
- J-M Besnoin
- JJL Bryant
- KA Barnes
- LW Sumner
- M Biedermann
- M Hoppe
- M Vaclavikova
- MJ Martínez-Bueno
- Paul Hill
- R Cariou
- R Paseiro-Cerrato
- R Tautenhahn
- Ronan Cariou
- S Úbeda
- Yann Guitton
- ZW Wicks
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Trauma and Stressor-Related Disorders 2: Adjustment Disorders
- Author
- A Kugaya
- A Maercker
- AF Schatzberg
- American Psychiatric Association
- American Psychiatric Association
- American Psychiatric Association
- American Psychiatric Association
- BS Runeson
- C Brezinka
- C Nardi
- CF Reynolds
- D Razavi
- D Spiegel
- D Spiegel
- D Spiegel
- D Spiegel
- DS Charney
- EH Uhlenhuth
- EI Gonzalez-Jaimes
- F Cohen
- FI Fawzy
- G Maina
- G Portzky
- G Pozzi
- G Spalletta
- H Baumeister
- H Fabrega Jr
- H Selye
- HP Volz
- HS Andersen
- J Kim
- JC Markowitz
- JJ Strain
- JJ Strain
- JJL Klink van der
- JJL Klink van der
- JM Havenaar
- JN Despland
- JP Perez-Jimenez
- JW Stewart
- L Arborelius
- L For-Wey
- L Grassi
- L Kryzhanovskaya
- LL Judd
- M Ansseau
- M Bourin
- M Frankel
- M Kellermann
- M Kovacs
- M Pelkonen
- ME Faulstich
- MG Wise
- MJ Friedman
- MJ Sullivan
- MK Popkin
- N Nguyen
- NC Andreasen
- NC Andreasen
- O Giotakos
- P Casey
- P Casey
- P Casey
- P Foster
- PB Rosenberg
- PE Sifneos
- PK True
- PR Slavney
- R Jones
- R Shaner
- RA Bryant
- RS Dunman
- S Chess
- S DeWit
- S Powell
- S Pulimood
- S Shima
- S Snyder
- SA Newell
- SM Southwick
- SM Southwick
- T Akechi
- TE Oxman
- U Schnyder
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for supersymmetry in final states with charm jets and missing transverse momentum in 13 TeV pp collisions with the ATLAS detector
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- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
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- Zu Theenhausen HM
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
A search for supersymmetric partners of top quarks decaying as t~1→c\upchi~01 and supersymmetric partners of charm quarks decaying as c~1→c\upchi~01 , where \upchi~01 is the lightest neutralino, is presented. The search uses 36.1 fb−1 pp collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS experiment at the Large Hadron Collider and is performed in final states with jets identified as containing charm hadrons. Assuming a 100% branching ratio to c\upchi~01 , top and charm squarks with masses up to 850 GeV are excluded at 95% confidence level for a massless lightest neutralino. For mt~1,c~1−m\upchi~01 < 100 GeV, top and charm squark masses up to 500 GeV are excluded
Search for the Higgs boson produced in association with a vector boson and decaying into two spin-zero particles in the H \u2192 aa \u2192 4b channel in pp collisions at 1as=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
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- Winston OJ
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- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu M
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xu D
- 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
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yue X
- Yuen SPY
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang D
- Zhang DF
- 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 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
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
A search for exotic decays of the Higgs boson into a pair of spin-zero particles, H \u2192 aa, where the a-boson decay sin to b-quarks promptly or with a mean proper lifetime c\u3c4a up to 6 mm and has a mass in the range of 20\u201360 GeV, is presented. The search is performed in events where the Higgs boson is produced in association with a W or Z boson, giving rise to a signature of one or two charged leptons (electrons or muons) and multiple jets from b-quark decays. The analysis is based on the dataset of proton-proton collisions at s 1a=13 TeV recorded in 2015 and 2016 by the ATLAS detector at the CERN Large Hadron Collider, corresponding to an integrated luminosity of 36.1 fb 121. No significant excess of events above the Standard Model background prediction is observed, and 95% confidence-level upper limits are derived for the production cross-sections for pp \u2192 WH, ZH and their combination, times the branching ratio of the decay chain H \u2192 aa \u2192 4b. For a-bosons which decay promptly, the upper limit on the combination of cross-sections for WH and ZH times the branching ratio of H \u2192 aa \u2192 4b ranges from 3.0 pb for ma = 20 GeV to 1.3 pb for ma = 60 GeV, assuming that the ratio of WH to ZH cross-sections follows the Standard Model prediction. For a-bosons with longer proper lifetimes, the most stringent limits are 1.8 pb and 0.68 pb, respectively, at c\u3c4a 3c 0.4 mm