303 research outputs found
Nanotechnology in agriculture, livestock, and aquaculture in China. A review
- Author
- A Dhawan
- A Emamifar
- A Kahru
- A Kumar
- AM Alkilany
- AX Liu
- B Zhang
- BH Pan
- BQ Ma
- BX Hong
- C Cai
- C Wang
- C Wei
- C Yang
- CD Vecitis
- CE Albers
- CJ Smith
- CL Gong
- CM Nair
- CP Yao
- CY Sun
- D Mandal
- D Zhao
- DB Warheit
- DM Zhou
- DW Elliott
- DW Xiong
- E Can
- E Navarro
- EL Bradley
- FD Zhang
- FH Wang
- FJ Mongillo
- FOE
- FS Li
- FY Liu
- G Oberdorster
- G Zhang
- GP Zeng
- GQ Zhong
- H Bouwmeester
- H Zhang
- HB Huang
- HL Karlsson
- HL Liu
- HQ Xiang
- HX Zhao
- HX Zhao
- HZ Dong
- J Gao
- J Kong
- J Lan
- J Lee
- J Li
- J Liu
- J Sarkar
- J Zhu
- JB Liu
- JB Liu
- JB Ren
- JC Yu
- JG Ren
- JH Wang
- JH Wang
- JP Wilcoxon
- JQ Wen
- K Byrappa
- K Ma
- KK Jain
- L Pu
- L Song
- L Zhang
- L Zhong
- LA Mitchell
- LH Hao
- LH Wang
- Lianmeng Liu
- Ling Wang
- LL Guo
- LL Zhao
- LM Wu
- LP Yuan
- LQ Bian
- LQ Huang
- LR Jia
- LR Khot
- LS Deng
- Lu Li
- LY Ma
- M Chen
- M Chrysoehoou
- M Heinlaan
- M Khodakovskaya
- M Krrlik
- M Li
- M Li
- M O’Neill
- M Rai
- M Sharon
- M Wainwright
- M Wang
- M Zhang
- MH Park
- ML Zambrano-Zaragoza
- MQ Wang
- MS Xia
- MS Xia
- N Pugazhenthiran
- N Singh
- O Akhavan
- P Begum
- P Guo
- P Zhang
- PW Liu
- Q Long
- QH Zhou
- QJ Lai
- QY Tang
- R Nair
- R Singh
- RB Salunkhe
- RD Handy
- RH Li
- RK Sastry
- RK Shukla
- RK Shukla
- RQ Long
- RS Sonawane
- S Anandan
- S Cai
- S Kang
- S Lin
- S Mittal
- S Toyokuni
- S Vyom
- SD Sarma
- SG Kim
- SH Wang
- Shiwen Huang
- SJ Cui
- SJ Kang
- SS Shankar
- SS Yang
- SS Zhang
- SW Huang
- SX Wang
- SY Fang
- SY Jin
- T Satapanajaru
- T Yang
- TJ Hu
- V Sharma
- W Bai
- W Hu
- W Yun
- WH Lai
- WJ Wang
- WR Sun
- X Zhu
- XF Song
- XF Yang
- XJ Zhao
- XL Sun
- XL Yang
- XM Liu
- XS Zhu
- XY Wang
- XY Wang
- Y Ge
- Y Wang
- Y Zu
- YD Li
- YD Liu
- YG Yin
- YH Bai
- YJ Kim
- YM Zhu
- YP Kang
- YQ He
- YS Deng
- Yuxuan Hou
- YY Gao
- YZ Wu
- Z Zhang
- ZC Xie
- ZF Li
- ZK Lin
- ZM Zhang
- ZT You
- ZY Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Aakvaag E
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboelela M
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Ackermann A
- Adam Bourdarios C
- Adamczyk L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Aktas S
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Alegria ZL
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi F
- Algren M
- Alhroob M
- Ali B
- Ali HMJ
- Ali S
- Alibocus SW
- Aliev M
- Alimonti G
- Alkakhi W
- Allaire C
- Allbrooke BMM
- Allen JF
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
- Alves Cardoso M
- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amirie KJ
- Amor Dos Santos SP
- Amos KR
- An S
- Ananiev V
- Anastopoulos C
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Anulli F
- Aoki M
- Aoki T
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Appelt C
- Apyan A
- Arbiol Val SJ
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Assamagan K
- Astalos R
- Astrand KSV
- Atashi S
- Atkin RJ
- Atkinson M
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Auriol AD
- Austrup VA
- Avolio G
- Axiotis K
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Baer TM
- Bagnaia P
- Bahmani M
- Bahner D
- Bai K
- Bailey AJ
- Baines JT
- Baines L
- Baker OK
- Bakos E
- Bakshi Gupta D
- Balakrishnan V
- Balasubramanian R
- Baldin EM
- Balek P
- Ballabene E
- Balli F
- Baltes LM
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Bansal S
- Barak L
- Barakat M
- Barberio EL
- Barberis D
- Barbero M
- Barel MZ
- Barends KN
- Barillari T
- Barisits M-S
- Barklow T
- Baron Moreno DA
- Baron P
- Baroncelli A
- Barone G
- Barr AJ
- Barr JD
- Barreiro Guimarães da Costa J
- Barreiro F
- Barron U
- Barros Teixeira MG
- Barsov S
- Bartels F
- Bartoldus R
- Barton AE
- Bartos P
- Basan A
- Baselga M
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batool B
- Battaglia M
- Battulga D
- Bauce M
- Bauer M
- Bauer P
- Bazzano Hurrell LT
- Beacham JB
- Beau T
- Beaucamp JY
- Beauchemin PH
- Bechtle P
- Beck HP
- Becker K
- Beddall AJ
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Benchekroun D
- Bendebba F
- Benhammou Y
- Benkendorfer KC
- Beresford L
- Beretta M
- Bergeaas Kuutmann E
- Berger N
- Bergmann B
- Beringer J
- Bernardi G
- Bernius C
- Bernlochner FU
- Bernon F
- Berrocal Guardia A
- Berry T
- Berta P
- Berthold A
- Bethke S
- Betti A
- Bevan AJ
- Bhalla NK
- Bhamjee M
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhide KD
- Bhopatkar VS
- Bianchi RM
- Bianco G
- Biebel O
- Bielski R
- Biglietti M
- Billingsley CS
- Bindi M
- Bingul A
- Bini C
- Biondini A
- Birch-sykes CJ
- Bird GA
- Birman M
- Biros M
- Biryukov S
- Bisanz T
- Bisceglie E
- Biswal JP
- Biswas D
- Bjørke K
- Bloch I
- Blue A
- Blumenschein U
- Blumenthal J
- Bobrovnikov VS
- Boehler M
- Boehm B
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbély AG
- Bordulev IS
- Borecka-Bielska HM
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bossio Sola JD
- Bouaouda K
- Bouchhar N
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bouquet R
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Britton D
- Britzger D
- Brock I
- Brooijmans G
- Brost E
- Brown LM
- Bruce LE
- Bruckler TL
- Bruckman de Renstrom PA
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Brüers B
- Buanes T
- Buat Q
- Buchin D
- Buckley AG
- Bulekov O
- Bullard BA
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burlayenko O
- Burr JTP
- Burton CD
- Burzynski JC
- Busch EL
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buxo Vazquez CJ
- Buzykaev AR
- Büscher V
- Cabrera Urbán S
- Cadamuro L
- Caforio D
- Cai H
- Cai Y
- Cai Y
- Cairo VMM
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
- Calvet S
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarero Munoz D
- Camarri P
- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canbay AC
- Canonero E
- Cantero J
- Cao Y
- Capocasa F
- Capua M
- Carbone A
- Cardarelli R
- Cardenas JCJ
- Cardillo F
- Carducci G
- Carli T
- Carlino G
- Carlotto JI
- Carlson BT
- Carlson EM
- Carminati L
- Carnelli A
- Carnesale M
- Caron S
- Carquin E
- Carratta G
- Carroll AM
- Carrá S
- Carter TM
- Casado MP
- Caspar M
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cavaliere T
- Cavaliere V
- Cavalli N
- Cekmecelioglu YC
- Celebi E
- Cella S
- Celli F
- Centonze MS
- Cepaitis V
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervato B
- Cervelli A
- Cesarini G
- Cetin SA
- Chakraborty D
- Chan J
- Chan WY
- Chapman JD
- Chapon E
- Chargeishvili B
- Charlton DG
- Chatterjee M
- Chauhan C
- Che Y
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen B
- Chen H
- Chen H
- Chen J
- Chen J
- Chen M
- Chen S
- Chen SJ
- Chen X
- Chen X
- Chen Y
- Cheng CL
- Cheng HC
- Cheong S
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiedde N
- Chiodini G
- Chisholm AS
- Chitan A
- Chitishvili M
- Chizhov MV
- Choi K
- Chou Y
- Chow EYS
- Chu KL
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Cieri D
- Ciesla KM
- Cindro V
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Clark A
- Clark PJ
- Clarry C
- Clavijo Columbie JM
- Clawson SE
- Clement C
- Clercx J
- Coadou Y
- Cobal M
- Coccaro A
- Coelho Barrue RF
- Coelho Lopes De Sa R
- Coelli S
- Cole B
- Collot J
- Conde Muiño P
- Connell MP
- Connell SH
- Conroy EI
- Conventi F
- Cooke HG
- Cooper-Sarkar AM
- Cordeiro Oudot Choi A
- Corpe LD
- Corradi M
- Corriveau F
- Cortes-Gonzalez A
- Costa MJ
- Costanza F
- Costanzo D
- Cote BM
- Cowan G
- Cranmer K
- Cremonini D
- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosby JE
- Crosetti G
- Crépé-Renaudin S
- Cueto A
- Cui H
- Cui Z
- Cunningham WR
- Curcio F
- Curran JR
- Czodrowski P
- Czurylo MM
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dal Santo D
- Dallapiccola C
- Dam M
- Damp J
- Dandoy JR
- Danninger M
- Dao V
- Darbo G
- Das SJ
- Dattola F
- David C
- Davidek T
- Davis-Purcell B
- Dawson I
- Day-hall HA
- De Asmundis R
- De Biase N
- De Castro S
- De Groot N
- de Jong P
- De la Torre H
- De Maria A
- De Salvo A
- De Sanctis U
- De Santis F
- De Santo A
- De Vivie De Regie JB
- De K
- Dedovich DV
- Degens J
- Deiana AM
- Del Corso F
- Del Peso J
- Del Rio F
- Delagrange L
- Deliot F
- Delitzsch CM
- Della Pietra M
- Della Volpe D
- Dell’Acqua A
- Dell’Asta L
- Delmastro M
- Delsart PA
- Demers S
- Demichev M
- Denisov SP
- Derendarz D
- Derue F
- Dervan P
- Desch K
- Deutsch C
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Luca A
- Di Micco B
- Di Nardo R
- Diamantopoulou M
- Dias Do Vale T
- Dias FA
- Diaz Capriles FG
- Diaz MA
- Didenko M
- Diehl EB
- Diez Pardos C
- Dimitriadi C
- Dimitrievska A
- Dingfelder J
- Dinu I-M
- Dittmeier SJ
- Dittus F
- Divisek M
- Djama F
- Djobava T
- Doglioni C
- Dohnalova A
- Dolejsi J
- Dolezal Z
- Dona KM
- Donadelli M
- Dong B
- Donini J
- Dopke J
- Doria A
- Dos Santos Fernandes N
- Dougan P
- Dova MT
- Doyle AT
- Draguet MA
- Dreyer E
- Drivas-koulouris I
- Drnevich M
- Drozdova M
- du Pree TA
- Du D
- Dubinin F
- Dubovsky M
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Duden ER
- Duflot L
- Duminica I
- Dumitriu AE
- Dunford M
- Dungs S
- Dunne K
- Duperrin A
- Duran Yildiz H
- Durglishvili A
- Dwyer BL
- Dyckes GI
- Dyndal M
- Dziedzic BS
- Díez Cornell S
- Dührssen M
- Düren M
- D’amen G
- D’Amico V
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- D’Onofrio A
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- D’uffizi M
- Earnshaw ZO
- Eberwein GH
- Eckerova B
- Eggebrecht S
- Egidio Purcino De Souza E
- Ehrke LF
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- Einsweiler K
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- Ekman PA
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- El Ghazali Y
- El Jarrari H
- El Moussaouy A
- Ellajosyula V
- Ellert M
- Ellinghaus F
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- Elmsheuser J
- Elsawy M
- Elsing M
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- Enari Y
- Ene I
- Epari S
- Erland PA
- Errenst M
- Escalier M
- Escobar C
- Etzion E
- Evans G
- Evans H
- Evans LS
- Ezhilov A
- Ezzarqtouni S
- Fabbri F
- Fabbri L
- Facini G
- Fadeyev V
- Fakhrutdinov RM
- Fakoudis D
- Falciano S
- Falda Ulhoa Coelho LF
- Falke PJ
- Fallavollita F
- Faltova J
- Fan C
- Fan Y
- Fang Y
- Fanti M
- Faraj M
- Farazpay Z
- Farbin A
- Farilla A
- Farooque T
- Farrington SM
- Fassi F
- Fassouliotis D
- Faucci Giannelli M
- Fawcett WJ
- Fayard L
- Federic P
- Federicova P
- Fedin OL
- Feickert M
- Feligioni L
- Fellers DE
- Feng C
- Feng M
- Feng Z
- Fenton MJ
- Ferencz L
- Ferguson RAM
- Fernandez Luengo SI
- Fernandez Martinez P
- Fernoux MJV
- Ferrando J
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- Ferrere D
- Ferretti C
- Fiedler F
- Fiedler P
- Filipčič A
- Filmer EK
- Filthaut F
- Fiolhais MCN
- Fiorini L
- Fisher WC
- Fitschen T
- Fitzhugh PM
- Fleck I
- Fleischmann P
- Flick T
- Flores Castillo LR
- Flores Sanz De Acedo L
- Flores M
- Follega FM
- Fomin N
- Foo JH
- Formica A
- Forti AC
- Fortin E
- Fortman AW
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- Fox H
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- Francescato S
- Franchellucci S
- Franchini M
- Franchino S
- Francis D
- Franco Lima V
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- Freund WS
- Frid YY
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- Fritzsche N
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- Frost JA
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- Fujimoto M
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- Furukawa M
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- Gazis EN
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- Geyik ME
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- Giannini A
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- Gignac M
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- Gilbert AK
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- Gingrich DM
- Giordani MP
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- Godin D
- Gokturk B
- Goldfarb S
- Golling T
- Gololo MGD
- Golubkov D
- Gombas JP
- Gomes Da Silva G
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- Gomez Delegido AJ
- Gonella L
- Gongadze A
- Gonnella F
- Gonski JL
- Gonzalez Lopez R
- Gonzalez Renteria C
- Gonzalez Rodrigues MV
- Gonzalez Suarez R
- Gonzalez-Sevilla S
- González Andana RY
- González de la Hoz S
- Gonçalo R
- Goossens L
- Gorini B
- Gorini E
- Gorišek A
- Gosart TC
- Goshaw AT
- Gostkin MI
- Goswami S
- Gottardo CA
- Gotz SA
- Gouighri M
- Goumarre V
- Goussiou AG
- Govender N
- Grabowska-Bold I
- Graham K
- Gramstad E
- Grancagnolo S
- Grant CM
- Gravila PM
- Gravili FG
- Gray HM
- Greco M
- Grefe C
- Gregor IM
- Greif KT
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- Grewe SG
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- Grivaz J-F
- Gross E
- Grosse-Knetter J
- Grundy JC
- Guan L
- Gubbels C
- Guerrero Rojas JGR
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- Guescini F
- Gugel R
- Guhit JAM
- Guida A
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- Guindon S
- Guo F
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- Gurbuz S
- Gurdasani SS
- Gustavino G
- Guth M
- Gutierrez Zagazeta LF
- Gutierrez P
- Gutsche M
- Gutschow C
- Gwenlan C
- Gwilliam CB
- Haaland ES
- Haas A
- Habedank M
- Haber C
- Hadavand HK
- Hadef A
- Hadzic S
- Hagan AI
- Hahn JJ
- Haines EH
- Haleem M
- Haley J
- Hall JJ
- Hallewell GD
- Halser L
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- Hamer M
- Hamity GN
- Hampshire EJ
- Han J
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- Han YF
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- Hangal DA
- Hanif H
- Hank MD
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- Hansen PH
- Hara K
- Harada D
- Harenberg T
- Harkusha S
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- Zhemchugov A
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- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. 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 complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
Effects of alirocumab on types of myocardial infarction: insights from the ODYSSEY OUTCOMES trial
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- Abbas J
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- Abdullakutty J
- Abhyanakar AD
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- Zrazhevsky K
- Zuniga JDH
- Zurakowski A
- Zuran I
- Zweiker R
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 01/01/2019
- Field of study
Aims The third Universal Definition of Myocardial Infarction (MI) Task Force classified MIs into five types: Type 1, spontaneous; Type 2, related to oxygen supply/demand imbalance; Type 3, fatal without ascertainment of cardiac biomarkers; Type 4, related to percutaneous coronary intervention; and Type 5, related to coronary artery bypass surgery. Low-density lipoprotein cholesterol (LDL-C) reduction with statins and proprotein convertase subtilisin–kexin Type 9 (PCSK9) inhibitors reduces risk of MI, but less is known about effects on types of MI. ODYSSEY OUTCOMES compared the PCSK9 inhibitor alirocumab with placebo in 18 924 patients with recent acute coronary syndrome (ACS) and elevated LDL-C (≥1.8 mmol/L) despite intensive statin therapy. In a pre-specified analysis, we assessed the effects of alirocumab on types of MI. Methods and results Median follow-up was 2.8 years. Myocardial infarction types were prospectively adjudicated and classified. Of 1860 total MIs, 1223 (65.8%) were adjudicated as Type 1, 386 (20.8%) as Type 2, and 244 (13.1%) as Type 4. Few events were Type 3 (n = 2) or Type 5 (n = 5). Alirocumab reduced first MIs [hazard ratio (HR) 0.85, 95% confidence interval (CI) 0.77–0.95; P = 0.003], with reductions in both Type 1 (HR 0.87, 95% CI 0.77–0.99; P = 0.032) and Type 2 (0.77, 0.61–0.97; P = 0.025), but not Type 4 MI. Conclusion After ACS, alirocumab added to intensive statin therapy favourably impacted on Type 1 and 2 MIs. The data indicate for the first time that a lipid-lowering therapy can attenuate the risk of Type 2 MI. Low-density lipoprotein cholesterol reduction below levels achievable with statins is an effective preventive strategy for both MI types.For complete list of authors see http://dx.doi.org/10.1093/eurheartj/ehz299</p
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
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- Zhemchugov A
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- Zhulanov V
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Search for bottom-squark pair production in pp collision events at √s=13 TeV with hadronically decaying τ-leptons, b-jets, and missing transverse momentum using the ATLAS detector
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- Zhemchugov A
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/08/2021
- Field of study
A search for pair production of bottom squarks in events with hadronically decaying
τ
-leptons,
b
-tagged jets, and large missing transverse momentum is presented. The analyzed dataset is based on proton-proton collisions at
√
s
=
13
TeV
delivered by the Large Hadron Collider and recorded by the ATLAS detector from 2015 to 2018, and corresponds to an integrated luminosity of
139
fb
−
1
. The observed data are compatible with the expected Standard Model background. Results are interpreted in a simplified model where each bottom squark is assumed to decay into the second-lightest neutralino
˜
χ
0
2
and a bottom quark, with
˜
χ
0
2
decaying into a Higgs boson and the lightest neutralino
˜
χ
0
1
. The search focuses on final states where at least one Higgs boson decays into a pair of hadronically decaying
τ
-leptons. This allows the acceptance and thus the sensitivity to be significantly improved relative to the previous results at low masses of the
˜
χ
0
2
, where bottom-squark masses up to 850 GeV are excluded at the 95% confidence level, assuming a mass difference of 130 GeV between
˜
χ
0
2
and
˜
χ
0
1
. Model-independent upper limits are also set on the cross section of processes beyond the Standard Model
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector
- Author
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- Abhayasinghe DK
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- Xu R
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- Xu W
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- Xu Z
- Xu Z
- Yabsley B
- Yacoob S
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan J
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- Yang HJ
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- Yao W-M
- Yap YC
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- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- 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 H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 02/07/2021
- Field of study
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fb−1 of s√ = 13 TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015–2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single Z boson production, Higgs boson production and on-shell ZZ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The Z → 4ℓ branching fraction is extracted, giving a value of (4.41 ± 0.30) × 10−6. Constraints on effective field theory parameters and a model based on a spontaneously broken B − L gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information
Search for pair production of third-generation scalar leptoquarks decaying into a top quark and a τ-lepton in pp collisions at s√ = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
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- Alberghi GL
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 30/06/2021
- Field of study
A search for pair production of third-generation scalar leptoquarks decaying into a top quark and a τ-lepton is presented. The search is based on a dataset of pp collisions at s√ = 13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. Events are selected if they have one light lepton (electron or muon) and at least one hadronically decaying τ -lepton, or at least two light leptons. In addition, two or more jets, at least one of which must be identified as containing b-hadrons, are required. Six final states, defined by the multiplicity and flavour of lepton candidates, are considered in the analysis. Each of them is split into multiple event categories to simultaneously search for the signal and constrain several leading backgrounds. The signal-rich event categories require at least one hadronically decaying τ-lepton candidate and exploit the presence of energetic final-state objects, which is characteristic of signal events. No significant excess above the Standard Model expectation is observed in any of the considered event categories, and 95% CL upper limits are set on the production cross section as a function of the leptoquark mass, for different assumptions about the branching fractions into tτ and bν. Scalar leptoquarks decaying exclusively into tτ are excluded up to masses of 1.43 TeV while, for a branching fraction of 50% into tτ, the lower mass limit is 1.22 TeV
Medium-Induced Modification of Z-Tagged Charged Particle Yields in Pb+Pb Collisions at 5.02 TeV with the ATLAS Detector
- Author
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- Abhayasinghe DK
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- Carminati L
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- Zhemchugov A
- Zheng Z
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- Zhulanov V
- Zieminska D
- Zimine N
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- Ziolkowski M
- Zobernig G
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- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 19/02/2021
- Field of study
The yield of charged particles opposite to a
Z
boson with large transverse momentum (
p
T
) is measured in
260
pb
−
1
of
p
p
and
1.7
nb
−
1
of
Pb
+
Pb
collision data at 5.02 TeV per nucleon pair recorded with the ATLAS detector at the Large Hadron Collider. The
Z
boson tag is used to select hard-scattered partons with specific kinematics, and to observe how their showers are modified as they propagate through the quark-gluon plasma created in
Pb
+
Pb
collisions. Compared with
p
p
collisions, charged-particle yields in
Pb
+
Pb
collisions show significant modifications as a function of charged-particle
p
T
in a way that depends on event centrality and
Z
boson
p
T
. The data are compared with a variety of theoretical calculations and provide new information about the medium-induced energy loss of partons in a
p
T
regime difficult to measure through other channels
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
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- Buschmann E
- Bussey PJ
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- Buttinger W
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- Calafiura P
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- Chiu I
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- Zhemchugov A
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
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