91 research outputs found
Authority of Bawaslu to Handle Violations of Administrative Law in Fiqh Siyasah
- Publication venue
- Fakultas Syariah UIN Sultan Maulana Hasanuddin Banten
- Publication date
- 28/06/2024
- Field of study
General Elections a process where individuals carefully choose representatives or candidates who are considered good and appropriate to their preferences. General elections are an important tool in realizing people's sovereignty, which produces people's representatives who represent the aspirations of the people, have quality, and are responsible. The research focused on three main questions: 1. What is Bawaslu's authority in resolving violations of General Election administration law? 2. What factors hinder Bawaslu's authority in addressing violations of General Election administration law? 3. What sanctions apply for violations of General Election administration law?. Library study method was used. Meanwhile, the research results explained that Bawaslu had the authority to resolve violations of general election administration law, including monitoring, handling complaints, investigating, providing recommendations, hearings, campaign assistance, and issuing guidelines. Inhibiting factors for Bawaslu in addressing violations of election administration law in Indonesia include limited resources, legal complexities, authority limitations, non-compliance by parties, political interference, restricted information access, diverse legal cultures, lack of awareness, political party involvement, and time constraints. Meanwhile, the administrative sanctions that Bawaslu could impose on violators of election administration law included cutting campaign budgets, terminating candidacy, as well as recommendations to the General Election Commission
Post Partial Nephrectomy Surveillance Imaging: an Evidence-Based Approach
- Author
- A Adamy
- A Antonelli
- A Heidenreich
- A Khalifeh
- A Zisman
- AB Stillebroer
- AC Small
- AJ Stephenson
- B Escudier
- B Ljungberg
- BC Leibovich
- CJ Weight
- CR Divgi
- DA Levy
- DC Miller
- DS Sandock
- E Mariusdottir
- HY Wang
- I Frank
- IS Gill
- J Ferlay
- JM Woldrich
- JS Lam
- K Nakatani
- KS Hafez
- Lorenzo Marconi
- M Sorbellini
- M Sun
- ME Juweid
- Michael A. Gorin
- MJ Lipsky
- Mohamad E. Allaf
- MW Kattan
- NS Majhail
- R Kumar
- R Siegel
- RJ Motzer
- S Brookman-May
- S Dabestani
- SA Poon
- SA Siddiqui
- SC Campbell
- SP Kim
- SP Povoski
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Global burden of 369 diseases and injuries in 204 countries and territories, 1990-2019: a systematic analysis for the Global Burden of Disease Study 2019
- Author
- Abbafati C
- Abbas KM
- Abbasi M
- Abbasi-Kangevari M
- Abbasifard M
- Abbastabar H
- Abd El Razek HM
- Abd El Razek MM
- Abd-Allah F
- Abdelalim A
- Abdollahi M
- Abdollahpour I
- Abdulkader RS
- Abdullah KH
- Abedi A
- Abedi P
- Abegaz KH
- Abolhassani H
- Abosetugn AE
- Aboyans V
- Abrams EM
- Abreu LG
- Abrigo MRM
- Abu Haimed AK
- Abu-Gharbieh E
- Abu-Raddad LJ
- Abualhasan A
- Abushouk AI
- Acebedo A
- Ackerman IN
- Adabi M
- Adair T
- Adamu AA
- Adebayo OM
- Adedeji IA
- Adekanmbi V
- Adelson JD
- Adeoye AM
- Adetokunboh OO
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- Ahmadi A
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- Ahmadpour E
- Ahmed MB
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- Akalu TY
- Akinyemi RO
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- Akunna CJ
- Al-Aly Z
- Al-Mekhlafi HM
- Al-Raddadi RM
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- Albertson SB
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- Alla F
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- Oiu AO
- Okunga EW
- Oladnabi M
- Olagunju AT
- Olusanya BO
- Olusanya JO
- Oluwasanu MM
- Omer MO
- Ong KL
- Ong S
- Onwujekwe OE
- Oren E
- Orji AU
- Orpana HM
- Ortega-Altamirano DV
- Ortiz A
- Osarenotor O
- Osei FB
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- Owolabi MO
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- Troeger CE
- Truelsen TC
- Tsai AC
- Tsatsakis A
- Tyrovolas S
- Uddin R
- Ullah I
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- Umeokonkwo CD
- Undurraga EA
- Unnikrishnan B
- Upadhyay E
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- Valdez PR
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- Venketasubramanian N
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- Wickramasinghe ND
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- Wondmeneh TG
- Wondmieneh AB
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- Wu A-M
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- Wu J
- Wunrow HY
- Xie Y
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- Yamagishi K
- Yaminfirooz M
- Yano Y
- Yaya S
- Yazdi-Feyzabadi V
- Yearwood JA
- Yeheyis TY
- Yeshitila YG
- Yilgwan CS
- Yilma MT
- Yip P
- Yonemoto N
- Yoon S-J
- York HW
- Younis MZ
- Younker TP
- Yousefi B
- Yousefi Z
- Yousefifard M
- Yousefinezhadi T
- Yousuf AY
- Yu C
- Yu Y
- Yuan C-W
- Yuce D
- Yusefzadeh H
- Zadey S
- Zahabi SS
- Zaidi SS
- Zaki L
- Zaki MES
- Zakzuk J
- Zamani M
- Zamanian M
- Zandian H
- Zangeneh A
- Zarafshan H
- Zastrozhin MS
- Zewdie KA
- Zhang J
- Zhang Y
- Zhang Z-J
- Zhao JT
- Zhao X-JG
- Zhao Y
- Zheleva B
- Zheng P
- Zhou M
- Zhu C
- Ziapour A
- Zimsen SRM
- Zlavog BS
- Zodpey S
- Publication venue
- 'Elsevier BV'
- Publication date
- 17/10/2020
- Field of study
Five insights from the Global Burden of Disease Study 2019
- Author
- Abbafati C
- Abbas KM
- Abbasi M
- Abbasi-Kangevari M
- Abbasifard M
- Abbastabar H
- Abd El Razek HM
- Abd El Razek MM
- Abd-Allah F
- Abdelalim A
- Abdollahi M
- Abdollahpour I
- Abdulkader RS
- Abdullah KH
- Abedi A
- Abedi P
- Abegaz KH
- Abolhassani H
- Abosetugn AE
- Aboyans V
- Abrams EM
- Abreu LG
- Abrigo MRM
- Abu Haimed AK
- Abu-Gharbieh E
- Abu-Raddad LJ
- Abualhasan A
- Abushouk AI
- Acebedo A
- Ackerman IN
- Adabi M
- Adair T
- Adamu AA
- Adebayo OM
- Adedeji IA
- Adekanmbi V
- Adelson JD
- Adeoye AM
- Adetokunboh OO
- Adham D
- Advani SM
- Afarideh M
- Afshari M
- Afshin A
- Agardh EE
- Agarwal G
- Agasthi P
- Agesa KM
- Aghaali M
- Aghamir SMK
- Agrawal A
- Ahmad T
- Ahmadi A
- Ahmadi K
- Ahmadi M
- Ahmadieh H
- Ahmadpour E
- Ahmed MB
- Aji B
- Akalu TY
- Akinyemi RO
- Akinyemiju T
- Akombi B
- Akunna CJ
- Al-Aly Z
- Al-Mekhlafi HM
- Al-Raddadi RM
- Alahdab F
- Alam K
- Alam N
- Alam S
- Alam T
- Alanezi FM
- Alanzi TM
- Albertson SB
- Alcalde-Rabanal JE
- Alema NM
- Alemu BW
- Alemu YM
- Alhabib KF
- Alhassan RK
- Ali M
- Ali S
- Alicandro G
- Alijanzadeh M
- Alinia C
- Alipour V
- Alizade H
- Aljunid SM
- Alla F
- Allebeck P
- Almadi MAH
- Almasi A
- Almasi-Hashiani A
- Almasri NA
- Almulhim AM
- Alonso J
- Altirkawi KA
- Alumran AK
- Alvis-Guzman N
- Alvis-Zakzuk NJ
- Amare AT
- Amare B
- Amini S
- Amini-Rarani M
- Aminorroaya A
- Amiri F
- Amit AML
- Amugsi DA
- Amul GGH
- Anbesu EW
- Ancuceanu R
- Anderlini D
- Anderson JA
- Andrei CL
- Andrei T
- Androudi S
- Angus C
- Anjomshoa M
- Ansari F
- Ansari I
- Ansari-Moghaddam A
- Antonazzo IC
- Antonio CAT
- Antony CM
- Antriyandarti E
- Anvari D
- Anwer R
- Appiah SCY
- Arab-Zozani M
- Arabloo J
- Aravkin AY
- Arba AAK
- Aremu O
- Ariani F
- Aripov T
- Armoon B
- Arnlov J
- Arowosegbe OO
- Aryal KK
- Arzani A
- Asaad M
- Asadi-Aliabadi M
- Asadi-Pooya AA
- Asgari S
- Asghari B
- Ashbaugh C
- Assmus M
- Atafar Z
- Athari SS
- Atnafu DD
- Atout MMW
- Atre SR
- Atteraya MS
- Ausloos F
- Ausloos M
- Avila-Burgos L
- Avokpaho EFGA
- Ayano G
- Ayanore MA
- Aynalem GL
- Aynalem YA
- Ayza MA
- Azari S
- Azarian G
- Azene ZN
- Azhar G
- Azzopardi PS
- Babaee E
- Badawi A
- Badiye AD
- Bagherzadeh M
- Bagli E
- Bahrami MA
- Baig AA
- Bairwa M
- Bakhshaei MH
- Bakhtiari A
- Bakkannavar SM
- Balachandran A
- Balakrishnan S
- Balalla S
- Balassyano S
- Baldasseroni A
- Bali AO
- Ball K
- Ballew SH
- Balzi D
- Banach M
- Bandpei MAM
- Banerjee SK
- Banik PC
- Bannick MS
- Bante AB
- Bante SA
- Baraki AG
- Barboza MA
- Barker-Collo SL
- Barnighausen TW
- Barrero LH
- Barthelemy CM
- Barua L
- Barzegar A
- Basaleem H
- Bassat Q
- Basu S
- Baune BT
- Bayati M
- Baye BA
- Bazmandegan G
- Becker JS
- Bedi N
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- Benziger CP
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- Bhutta ZA
- Bibi S
- Bicer BK
- Biehl MH
- Bijani A
- Bikbov B
- Bilano V
- Bin Sayeed MS
- Bin Zaman S
- Biondi A
- Birihane BM
- Bisanzio D
- Bisignano C
- Biswas RK
- Bitew H
- Bjorge T
- Bockarie MJ
- Bohlouli S
- Bohluli M
- Bojia HA
- Bolla SR
- Boloor A
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- Borges G
- Borzi AM
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- Bose D
- Bosetti C
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- Boufous S
- Bourne R
- Brady OJ
- Braithwaite D
- Brauer M
- Brayne C
- Breitborde NJK
- Breitner S
- Brenner H
- Breusov AV
- Briant PS
- Briggs AM
- Briko AN
- Briko NI
- Britton GB
- Brugha T
- Bryazka D
- Buchbinder R
- Bumgarner BR
- Burkart K
- Burnett RT
- Busse R
- Butt ZA
- Caetano dos Santos FL
- Cahill LE
- Cahuana-Hurtado L
- Cai T
- Callender CSKH
- Camera LA
- Campos-Nonato IR
- Cao J
- Car J
- Car LT
- Cardenas R
- Carreras G
- Carrero JJ
- Carvalho F
- Castaldelli-Maia JM
- Castaneda-Orjuela CA
- Castelpietra G
- Castle CD
- Castro E
- Castro F
- Catala-Lopez F
- Causey K
- Cederroth CR
- Cercy KM
- Cerin E
- Chalek J
- Chandan JS
- Chang AR
- Chang AY
- Chang J-C
- Chang K-L
- Charan J
- Charlson FJ
- Chattu VK
- Chaturvedi S
- Cherbuin N
- Chimed-Ochir O
- Chin KL
- Chirinos-Caceres JL
- Cho DY
- Choi J-YJ
- Christensen H
- Chu D-T
- Chung MT
- Chung S-C
- Cicuttini FM
- Ciobanu LG
- Cirillo M
- Cislaghi B
- Classen TKD
- Cohen AJ
- Collins EL
- Comfort H
- Compton K
- Conti S
- Cooper OR
- Corso B
- Cortesi PA
- Costa VM
- Cousin E
- Cowden RG
- Cowie BC
- Cromwell EA
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- Cross DH
- Cross M
- Crowe CS
- Cruz JA
- Cummins S
- Cunningham M
- D'Amico E
- da Silva DD
- Dahlawi SMA
- Dai H
- Dai H
- Damasceno AAM
- Damiani G
- Dandona L
- Dandona R
- Daneshpajouhnejad P
- Dangel WJ
- Danielsson A-K
- Dargan PI
- Darshan BB
- Darwesh AM
- Daryani A
- Das Gupta R
- Das Neves J
- Das JK
- Dash AP
- Davey G
- Davila-Cervantes CA
- Davis AC
- Davitoiu DV
- Davletov K
- De Leo D
- De Neve J-W
- Dean FE
- DeCleene NK
- Deen A
- Defo BK
- Degenhardt L
- DeLang M
- Dellavalle RP
- Demeke FM
- Demoz GT
- Demsie DG
- Denova-Gutierrez E
- Dereje ND
- Deribe K
- Dervenis N
- Desai R
- Desalew A
- Dessie GA
- Deuba K
- Dharmaratne SD
- Dhungana GP
- Dianatinasab M
- Diaz D
- Dichgans M
- Didarloo A
- Dingels ZV
- Dippenaar IN
- Dirac MA
- Djalalinia S
- Do HT
- Dokova K
- Doku DT
- Dolecek C
- Dolgert AJ
- Dorostkar F
- Doshi CP
- Doshi PP
- Doshmangir L
- Douiri A
- Doxey MC
- Doyle KE
- Driscoll TR
- Dubljanin E
- Dunachie SJ
- Duncan BB
- Duraes AR
- Eagan AW
- Ebrahimi H
- Edvardsson D
- Effiong A
- Ehrlich JR
- El Nahas N
- El Sayed I
- El Tantawi M
- El-Jaafary SI
- Elbarazi I
- Elgendy IY
- Elhabashy HR
- Elsharkawy A
- Elyazar IRF
- Emamian MH
- Emmons-Bell S
- Erskine HE
- Eshrati B
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- Eskandarieh S
- Esmaeilnejad S
- Esmaeilzadeh F
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- Estep K
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- Etisso AE
- Ezekannagha O
- Fanzo J
- Farag T
- Farahmand M
- Faraj A
- Faraon EJA
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- Faridnia R
- Farinha CSES
- Farioli A
- Faris PS
- Faro A
- Faruque M
- Farzadfar F
- Fattahi N
- Fazaeli AA
- Fazlzadeh M
- Feigin VL
- Feldman R
- Fereshtehnejad S-M
- Fernandes E
- Ferrara G
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- Ferrari AJ
- Ferreira ML
- Feyissa GT
- Filip I
- Fischer F
- Fisher JL
- Fitzgerald R
- Flohr C
- Flor LS
- Foigt NA
- Folayan MO
- Fomenkov AA
- Force LM
- Fornari C
- Forooshani ZSD
- Foroutan M
- Fox JT
- Francis JM
- Frank TD
- Franklin RC
- Freitas M
- Fu W
- Fukumoto T
- Fukutaki K
- Fuller JE
- Fullman N
- Furtado JM
- Gad MM
- Gaidhane AM
- Gakidou E
- Galles NC
- Gallus S
- Gamkrelidze A
- Garcia-Basteiro AL
- Gardner WM
- Geberemariyam BS
- Gebrehiwot AM
- Gebremedhin KB
- Gebremeskel GG
- Gebremeskel LG
- Gebresillassie BM
- Gebreslassie AAAA
- Gela JD
- Geramo YCD
- Geremew A
- Gesesew HA
- Gething PW
- Gezae KE
- Ghadimi M
- Ghadiri K
- Ghaffarifar F
- Ghafourifard M
- Ghajar A
- Ghamari F
- Ghashghaee A
- Ghiasvand H
- Ghith N
- Gholamian A
- Ghosh R
- Giampaoli S
- Gilani SA
- Gill PS
- Gill TK
- Gillum RF
- Ginawi IA
- Ginindza TG
- Gitimoghaddam M
- Giussani G
- Glagn M
- Glushkova EV
- Gnedovskaya EV
- Godinho MA
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- Golechha M
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- Gopalani SV
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- Gorman TM
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- Goudarzi H
- Goudarzian AH
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- Goulart BNG
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- Grosso G
- Gubari MIM
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- Gugnani HC
- Guimaraes ALS
- Guimaraes RA
- Guled RA
- Gultie T
- Guo G
- Guo Y
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- Hachinski V
- Haddock B
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- Hafiz A
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- Haile LM
- Haile TG
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- Haj-Mirzaian A
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- Halvaei I
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- Hamilton EB
- Hammer MS
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- Han H
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- Hanif A
- Hankey GJ
- Hanson SW
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- Harvey JD
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- Hashemian M
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- Hassanipour S
- Hassankhani H
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- Publication venue
- Publication date
- 01/01/2020
- Field of study
The Global Burden of Diseases, Injuries, and Risk Factors Study (GBD) 2019 provides a rules-based synthesis of the available evidence on levels and trends in health outcomes, a diverse set of risk factors, and health system responses. GBD 2019 covered 204 countries and territories, as well as first administrative level disaggregations for 22 countries, from 1990 to 2019. Because GBD is highly standardised and comprehensive, spanning both fatal and non-fatal outcomes, and uses a mutually exclusive and collectively exhaustive list of hierarchical disease and injury causes, the study provides a powerful basis for detailed and broad insights on global health trends and emerging challenges. GBD 2019 incorporates data from 281 586 sources and provides more than 3.5 billion estimates of health outcome and health system measures of interest for global, national, and subnational policy dialogue. All GBD estimates are publicly available and adhere to the Guidelines on Accurate and Transparent Health Estimate Reporting. From this vast amount of information, five key insights that are important for health, social, and economic development strategies have been distilled. These insights are subject to the many limitations outlined in each of the component GBD capstone papers.Peer reviewe
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta G
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-Bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexakhin V
- Alexander J
- Alhusseini M
- Ali MAB Md
- Alimena J
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- Alvarez Fernandez A
- Alvarez JD Ruiz
- Alverson G
- Alves FL
- Alves GA
- Alyari M
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- Ambrogi F
- Amendola C
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- Amsler C
- Anagnostou G
- Anampa K Hurtado
- Anderson D
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- Andreev Yu
- Andrews MB
- Androsov K
- Angioni GL Pinna
- Antonelli L
- Antropov I
- Antunovic Z
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- Auffray E
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- Autermann C
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- Avila C
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- Azarkin M
- Azhgirey I
- Aziz T
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- Azzolini V
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search for the production of a pair of top squarks at the LHC is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar, because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with 35.9 fb(-1) of proton-proton collisions at a centre-of-mass energy of root s = 13 TeV, collected by the CMS detector in 2016, using events containing one electron-muon pair with opposite charge. The search is based on a precise estimate of the top quark pair background, and the use of the M-T2 variable, which combines the transverse mass of each lepton and the missing transverse momentum. No excess of events is found over the standard model predictions. Exclusion limits are placed at 95% confidence level on the production of top squarks up to masses of 208 GeV for models with a mass difference between the top squark and the lightest neutralino close to that of the top quark.Peer reviewe
Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-Bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexander J
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- Ali MAB Md
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- Alvarez Fernandez A
- Alvarez JD Ruiz
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- Andreev Yu
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search for dark matter produced in association with top quarks in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. The data set used corresponds to an integrated luminosity of 35.9 fb(-1) recorded with the CMS detector at the LHC. Whereas previous searches for neutral scalar or pseudoscalar mediators considered dark matter production in association with a top quark pair only, this analysis also includes production modes with a single top quark. The results are derived from the combination of multiple selection categories that are defined to target either the single top quark or the top quark pair signature. No significant deviations with respect to the standard model predictions are observed. The results are interpreted in the context of a simplified model in which a scalar or pseudoscalar mediator particle couples to a top quark and subsequently decays into dark matter particles. Scalar and pseudoscalar mediator particles with masses below 290 and 300 GeV, respectively, are excluded at 95% confidence level, assuming a dark matter particle mass of 1 GeV and mediator couplings to fermions and dark matter particles equal to unity.Peer reviewe
Search for Higgs boson pair production in the gamma gamma b(b)over-bar final state in pp collisions at root s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Acosta M Vazquez
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggarwal A
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-bataineh A
- Albajar C
- Albergo S
- Albert A
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- Alcaraz Maestre J
- Alda Junior WL
- Aleksandrov A
- Alexander J
- Ali MAB Md
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- Alvarez Fernandez A
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- Alves FL
- Alves GA
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- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search is presented for the production of a pair of Higgs bosons, where one decays into two photons and the other one into a bottom quark-antiquark pair. The analysis is performed using proton-proton collision data at root s = 13 TeV recorded in 2016 by the CMS detector at the LHC, corresponding to an integrated luminosity of 35.9 fb(-1) . The results are in agreement with standard model (SM) predictions. In a search for resonant production, upper limits are set on the cross section for new spin-0 or spin-2 particles. For the SM-like nonresonant production hypothesis, the data exclude a product of cross section and branching fraction larger than 2.0 fb at 95% confidence level (CL), corresponding to about 24 times the SM prediction. Values of the effective Higgs boson self-coupling K X are constrained to be within the range -11 < K-lambda < 17 at 95% CL, assuming all other Higgs boson couplings are at their SM value. The constraints on K-lambda, are the most restrictive to date. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state with two bquarks and two tau leptons in proton-proton collisions at root s=13 TeV The CMS Collaboration
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullah Wan WAT
- Abdullin S
- Abdulsalam A
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- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for an exotic decay of the Higgs boson to a pair of light pseudoscalar bosons is performed for the first time in the final state with two b quarks and two tau leptons. The search is motivated in the context of models of physics beyond the standard model (SM), such as two Higgs doublet models extended with a complex scalar singlet (2HDM + S), which include the next-to-minimal supersymmetric SM (NMSSM). The results are based on a data set of proton-proton collisions corresponding to an integrated luminosity of 35.9 fb(-1), accumulated by the CMS experiment at the LHC in 2016 at a center-of-mass energy of 13 TeV. Masses of the pseudoscalar boson between 15 and 60 GeVare probed, and no excess of events above the SM expectation is observed. Upper limits between 3 and 12% are set on the branching fraction B(h -> aa -> 2 tau 2b) assuming the SM production of the Higgs boson. Upper limits are also set on the branching fraction of the Higgs boson to two light pseudoscalar bosons in different 2HDM + S scenarios. Assuming the SM production cross section for the Higgs boson, the upper limit on this quantity is as low as 20% for a mass of the pseudoscalar of 40 GeV in the NMSSM. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
Search for the X(5568) State Decaying into B-s(0)pi(+/-) in Proton-Proton Collisions at root s=8 TeV
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- Publication venue
- Publication date
- 01/01/2017
- Field of study
A search for resonancelike structures in the B-s(0)pi(+/-) invariant mass spectrum is performed using proton-proton collision data collected by the CMS experiment at the LHC at root s = 8 TeV, corresponding to an integrated luminosity of 19.7 fb(-1). The B-s(0) mesons are reconstructed in the decay chain B-s(0) -> J/Psi phi, with J/Psi -> mu(+) mu(-) and phi -> K+K-. The B-s(0)pi(+/-) invariant mass distribution shows no statistically significant peaks for different selection requirements on the reconstructed B-s(0) and pi(+/-) candidates. Upper limits are set on the relative production rates of the X(5568) and B-s(0) states times the branching fraction of the decay X(5568)(+/-) -> B-s(0)pi(+/-). In addition, upper limits are obtained as a function of the mass and the natural width of possible exotic states decaying into B-s(0)pi(+/-).Peer reviewe
Measurement of inclusive very forward jet cross sections in proton-lead collisions at \sqrt{sNN} = 5:02 TeV
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- Zenaiev O
- Zenz SC
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- Zevi Della Porta G
- Zeyrek M
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2019
- Field of study
Measurements of differential cross sections for inclusive very forward jet production in proton-lead collisions as a function of jet energy are presented. The data were collected with the CMS experiment at the LHC in the laboratory pseudorapidity range −6.6 < η < −5.2. Asymmetric beam energies of 4 TeV for protons and 1.58 TeV per nucleon for Pb nuclei were used, corresponding to a center-of-mass energy per nucleon pair of \sqrt{sNN} = 5:02 TeV. Collisions with either the proton (p+Pb) or the ion (Pb+p) traveling towards the negative η hemisphere are studied. The jet cross sections are unfolded to stable-particle level cross sections with p_{T} ≳ 3 GeV, and compared to predictions from various Monte Carlo event generators. In addition, the cross section ratio of p+Pb and Pb+p data is presented. The results are discussed in terms of the saturation of gluon densities at low fractional parton momenta. None of the models under consideration describes all the data over the full jet-energy range and for all beam configurations. Discrepancies between the differential cross sections in data and model predictions of more than two orders of magnitude are observed
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