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Can information affect sensory perceptions? Evidence from a survey on Italian organic food consumers
- Author
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- Westcombe A Wardle J
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- Zanoli R Naspetti S
- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2018
- Field of study
This paper aims to investigate the influence of information on consumersâ preferences and sensory perceptions of organic food using a sample of 301 Italian organic food consumers. Consumers stated their preferences for âcore organicâ attributes, labels and information on food products and performed blind and informed tests on strawberry yoghurts and cookies. Data were analysed using descriptive analysis, Mann-Whitney U tests and Wilcoxon signed-rank test. Results revealed that consumers appreciate âcore organicâ attributes, like artisanal production and variability of sensory attributes. Comparing blind and informed tests, results showed that information affects the overall liking of products and consumersâ perception of product-specific sensory attributes. However, the influence of information on sensory perceptions depends on the product category, sensory attributes and the type of information provided
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
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- Pozzobon N
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- Safonov A
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- Spiridonov A
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- Topaksu A Kayis
- Topsis-Giotis I
- Torassa E
- Toropin A
- Torres Da Silva De Araujo F
- Tos K
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- Tsipolitis G
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- Uzunian A
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- Vadruccio D
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- Vesztergombi G
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- Vizan Garcia JM
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- Voevodina E
- Volkov A
- Volobouev I
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- Vorobiev I
- Vorobyev A
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- Yusli MN
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- Zorbilmez C
- Zotto P
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- Zucchetta A
- Zumerle G
- Zuolo D
- 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
- Alhusseini M
- Ali MAB Md
- Alimena J
- Allen B
- Almond J
- 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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- Anampa K Hurtado
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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
Mortality from gastrointestinal congenital anomalies at 264 hospitals in 74 low-income, middle-income, and high-income countries: a multicentre, international, prospective cohort study
- Author
- Abantanga FA
- Abatli SJ
- Abbas W
- Abbo O
- Abd Elmenam M
- Abd Razak RB
- Abdelbaqi R
- Abdelhady DS
- Abdelhafez MOM
- Abdelhamid SS
- Abdelmaksoud S
- Abdelmoumen R
- Abdelmutalib F
- Abdul-Mumin A
- Abduljawad FM
- Abdullah F
- Abdulraheem N
- Abdulrahman A
- Abdulsalam MA
- Abdunomonovich DA
- Abib SDCV
- Aboelela A
- Abouheba M
- Abrahamsson K
- Abu Ajwa AE
- Abu Al-saleem HSH
- Abu Alamrain AA
- Abu Bakar AH
- Abu Farha MS
- Abu Jamie N
- Abu Jamie YMK
- Abu Jayyab M
- Abu Mayaleh A
- Abu Shiha E
- Abu Za'nouneh FJ
- Abu-Nejmah F
- Abuajaila A
- Abuattaya AA
- Abubakar AM
- Abueideh A
- Abuhayyeh HA
- Abuhlega MA
- Abukhalaf S
- Abumunshar AA
- Acuna G
- Adams S
- Adamu S
- Adanan MFSBM
- Adawi I
- Adawi S
- Adawy A
- Ade-Ajayi N
- Adegboyega R
- Ademuyiwa A
- Adesanya O
- Adhiwidjaja CF
- Adofo-Ansong N
- Agboola TH
- Agelebe E
- Aguiar AA
- Aguilar FA
- Aguirre-Lopez P
- Agulham MA
- Ahmad H
- Ahmad ZAH
- Ahmed H
- Ahmed MA
- Ajai OT
- Ajao EA
- Ajiboye OS
- Ajrami Y
- Akan ME
- Akhbari M
- Akhter N
- Akova F
- Al Dammagh NM
- Al Hussein S
- Al Massry NA
- Al Quran TM
- Al-Attar HM
- Al-Halbouni L
- Al-Mamun A
- Al-Mayoof AF
- Al-Momani HM
- Al-Mouakeh A
- Al-Rayyes M
- Al-Salhi AA
- Al-Shwaikh SH
- Al-Slaibi I
- Al-Taher RN
- Al-Taher RN
- Al-Tammam H
- Alakaloko F
- Alattas K
- Alberto C
- Albozidi A
- Alcantara E
- Aldirawi MAM
- Alebbini MM
- Alfoghi M
- Algabri HNO
- Alglaib MM
- Alhamid A
- Alhamid A
- Alhassan P
- Ali H
- Ali KO
- Ali L
- Ali M
- Alijla S
- Alijla SS
- Aliwisat AH
- Aljaboo H
- Aljadidi WOFS
- Aljarad Z
- Alkali YS
- Alkareem RMA
- Almada SA
- Almadhoun W
- Almasri M
- Almeida G
- Almengar I
- Almohamady H
- Almosaibli M
- Almusleh TFH
- Alnaeri A
- Alnahhal K
- Alonso V
- Alosta HM
- Alqarajeh F
- Alqor MOI
- Alsaadi NN
- Alsaggaf A
- Alsaied A
- Alser M
- Alser OH
- Alshaikhkhalil HAA
- Alshehri A
- Altamirano PR
- Altaweel A
- Altin M
- Altokhais T
- Altomi M
- Alturki F
- Alva LRC
- Alvarez JR
- Alwadia SMS
- Alwaggaa NA
- Alzamari AAM
- Alzeer AMS
- Alzerei ST
- Alzraikat SH
- Alzubair A
- Alzughayyar TZ
- Amad M
- Amado F
- Amaechi C
- Amah CC
- Amarin JZ
- Amarin M
- Ambriz-Gonzalez G
- Ameh E
- Amoabin AA
- Anatole N
- Anatole NK
- Anaya F
- Anaya WB
- Andrade J
- Andreussi L
- Annajjar MH
- Anntinea J
- Antunes A
- Antunez-Mora A
- Anyomih TTK
- Anzelewicz S
- Appeadu-Mensah W
- Arabiat E
- Arafa MA
- Arafat H
- Aragao L
- Arancibia JAC
- Arar AS
- Arauco J
- Arbab H
- Arboleda J
- Aremo A
- Argomedo MRO
- Arnadottir H
- Arnaud AP
- Arnold M
- Arnoletto LB
- Arrmali S
- Arrmalli LA
- Arshad M
- Arthur F
- Arul S
- Ashour DA
- Ashour YS
- Aslan Y
- Aspirot A
- Assi A
- Assi MAF
- Astudillo M
- Atatri YYM
- Atta A
- Attia AM
- Aucatoma FC
- Augusto MLDS
- Avila DC
- Avile R
- Avolio L
- Awad H
- Aydin E
- Aykut M
- Aziz DAA
- Ba'baa' B
- Badr H
- Baertschiger R
- Bagbio D
- Bah A
- Bai Q
- Bai YZ
- Baistrocchi V
- Baker W
- Ballah AM
- Ballouhey Q
- Balousha AG
- Bamanga A
- Baniowda MAM
- Bao X
- Barauskas V
- Barbosa PR
- Barcelos FZ
- Baron JDJC
- Barreto JJS
- Barros BS
- Baseggio N
- Bashir F
- Bashir MK
- Bataineh ZA
- Batal MM
- Bazozi HM
- Beasley S
- Becker K
- Belesa FDA
- Beloy IC
- Beltran NS
- Ben Enbaya M
- Benaskeur Y-I
- Benavente CM
- Beres A
- Berkova K
- Bernaus M
- Berzanskis M
- Beshtawi DMS
- Besir A
- Bianchin E
- Bibas F
- Biber E
- bin Abdullah MY
- Bin Amjad M
- bin Bujarimin AS
- bin Hassan MR
- Bin Othman MY
- bin Zahari Z
- bin Zarwawi AZ
- Bischoff C
- Blain OE
- Blanc T
- Blanchet EB
- Blazquez-Gomez E
- Blom MD
- Bode C
- Bonnard A
- Boonthai A
- Borbonet D
- Borges CG
- Bouhadiba N
- Bowder A
- Bradshaw K
- Bragagnini P
- Brahmamdam P
- Bravo MN
- Bravo MRDT
- Brenner NK
- Bright BP
- Broch A
- Brunero M
- Bruxel CL
- Bsisu I
- Bucaram E
- Burgos CM
- Burks SS
- Burns K
- Butler M
- Bvulani B
- Caamal LJ
- Cai D
- Calancea C
- Calderon LO
- Calistus N
- Calle CS
- Cama J
- Camacho FRC
- Camamra K
- Cameron F
- Camp L
- Canozer A
- Caouette-Laberge L
- Carbajal LF
- Carloni ICS
- Carrasco AL
- Carrasco-Ortega C
- Carrillo I
- Casado FT
- Caseb P
- Casquero V
- Castaneda FDMD
- Castillo MN
- Cavaiuolo S
- Cekic B
- Celik M
- Centen SV
- Cepeda R
- Cesur IB
- Chan J
- Chang J
- Charras MD
- Chaudary AR
- Chaudhry MA
- Chauhan N
- Chen J
- Chen L
- Chen R
- Cheung M
- Chipalavela RF
- Chipana CLA
- Chiriboga E
- Chiroque CM
- Chitiavi SW
- Chitnis M
- Cho SH
- Choo CSC
- Chukwu I
- Chukwuemeka AL-J
- Chung JH
- Cino EL
- Cletus C
- Coghill G
- Collins N
- Comert HSY
- Contreras CS
- Coon J
- Cordonnier A
- Cordova KH
- Cornelli F
- Cornwall H
- Corona MQ
- Correa A
- Correa C
- Cortez LFG
- Cosoreanu V
- Costa EC
- Costas-Chavarri A
- Cripovich A
- Cruzado GJS
- Cunningham A
- Cury EK
- Czauderna P
- da Cunha AG
- da Silva EAD
- da Silva JAN
- da Silva KI
- Dagilyte R
- Daher AP
- Dahman NBH
- Dalek NFRA
- Dallegre MB
- Dalloul H
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- Dania B
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- Darwish A
- Darwish AS
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- de Almeida TL
- de Andrade SO
- de Fernandez y Alcazar FR
- de Fraga JCS
- de Guzman J
- de Holanda FC
- De La Cruz RR
- de Oliveira DF
- de Oliveira DP
- de Souza RF
- de Vos C
- Dedeke F
- Defago VH
- Defert C
- Delefortrie T
- Delforge X
- Dendusic N
- Derbew M
- Derks T
- Deya C
- Deyab A
- Deyl RT
- Di Siervi O
- Dias AIBDS
- Dieudonne L
- Dimatatac DM
- Djordjevic I
- do Nascimento SD
- Dogar S
- Doheim MF
- Dominguez D
- Dominguez MA
- dos Santos CS
- dos Santos MSF
- Dosselman LJ
- Douiri A
- Drah W
- Dube AM
- Duchesne C
- Duggan E
- Dure C
- Ebeido A
- Echegaray MD
- Egbuchulem IK
- Ejinkeonye EC
- Ekenze SO
- Ekwunife OH
- El Tallaa MA
- El-Ghazaly M
- Elassall GMH
- Elayeb A
- Elebute OA
- Elewaily M
- Elfiky M
- Elgammudi M
- Elghazaly SM
- Elhadi A
- Elhadi M
- Elhajjaji YA
- Elhattab A
- Elias RA
- Elisante J
- Elkaloush AA
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- Elsiraffy OO
- Elstad M
- Elzohiri M
- Elzowawi F
- Emam OS
- Emil S
- Ensar N
- Ercin S
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- Eroglu E
- Erturk N
- Eshkabilov S
- Espineda B
- Espinosa SC
- Espinoza PP
- Essa TM
- Essamilghi KAM
- Ezidiegwu US
- Ezomike UO
- Faboya OM
- Fachin C
- Fadhle MJ
- Fajardo GYP
- Faks V
- Falah EH
- Farag EM
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- Fawzy OM
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- Felix M
- Feliz E
- Ferdinando DLT
- Ferdousi T
- Fernandez JY
- Ferreira JL
- Ferreira MDSS
- Ferrer MF
- Flores IMR
- Ford K
- Fory GO
- Fouda MF
- Fouly MAN
- Fouquet-Languillat V
- Fourcade L
- Fowler KL
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- Frutos FJL
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- Gad D
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- Gadepalli S
- Gai A
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- Gallego EA
- Gallindo RM
- Galvez PC
- Gamage T
- Gao Z
- Gao ZC
- Garcia I
- Garcia M
- Garcia V
- Garcia-Aparicio L
- Gargum SA
- Gargurevich PPA
- Garnier H
- Garrett-Cox R
- Gasana G
- Gashugi IS
- Gatzinsky V
- Gavrila B
- Gavrilovska-Brzanov A
- Gee O
- Gerus S
- Geze S
- Ghabayen ATS
- Ghallab A
- Ghaly KAE
- Ghanem WH
- Ghayth S
- Ghazzawi I
- Ghorab IA
- Ghosh D
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- Giovanoni LS
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- Gohil H
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- Graneli C
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- Guimaraes P
- Guinsburg R
- Guisse C
- Guo X
- Gurgel do Amaral AC
- Gurskas P
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- Gutierrez NT
- Guzman NJT
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- Hakan N
- Halabi YA
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- Hamidovic A
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- Hammato AY
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- Hammouri AG
- Hamzah SNABH
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- Harilal S
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- Hasan S
- Hasan S
- Hasanain DK
- Hashim HHB
- Hashim I
- Hashim S
- Hassan MA
- Hassan MYM
- Hassan ZBM
- Herdan MO
- Herrera C
- Herrera L
- Hery G
- Hinojosa AS
- Hinostroza D
- Hisham I
- Hodgman E
- Honhar M
- Horacio B
- Horozic D
- Hospital SI
- Hossini SL
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- Hussain SR
- Hussein OG
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- Ibukunolu O
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- Imamoglu M
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- Jester I
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- Kayibanda E
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- Martins BMR
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- Matour BM
- Mazzuca RB
- Mbonicura JC
- Mbonisweni A
- Mccluney S
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- Milisic E
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- Moriya E
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- Muragijimana JDD
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- Mussein HM
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- Ngwenya S
- Nisar MU
- Niyukuri A
- Nkuliza D
- Nkunzimana E
- Nofal AH
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- Novotny N
- Nuntasunti W
- Nwangwu EI
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- Obianyo NE
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- Ozcelik Z
- Ozen MA
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- Palacios N
- Palomino AG
- Pandit GS
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- Pardy C
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- Paredes VS
- Parigi GB
- Parker S
- Parmentier B
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- Pasierbek M
- Pasqua N
- Patel A
- Patkowski D
- Patzer L
- Pauzi SFM
- Peraza JL
- Perez JO
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- Pesara LMH
- Petel MR
- Peycelon M
- Phannua R
- Philipo GS
- Piche N
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- Pigeolet M
- Pilkington M
- Pinar B
- Piotrowska A
- Planka L
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- Poocharoen W
- Popovic N
- Porras JD
- Portilla EF
- Pos L
- Prabhu PS
- Prat J
- Puentes MC
- Puglia P
- Puig MG
- Puligandla P
- Putruele D
- Qabaja MM
- Qadomi AB
- Qawwash A
- Qi TTH
- Qudah HA
- Quevedo LMB
- Quinteros EFD
- Quiroz NH
- Qunaibi MAF
- Qureshi T
- Qutishat H
- Qwaider YZ
- Raboe E
- Rackova T
- Radwan AS
- Raffaele A
- Raicevic M
- Raj A
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- Ramos Y
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- Raposo JW
- Rasaki A
- Rashid S
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- Raza R
- Reda A
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- Rengura C
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- Rhodes H
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- Rincon LC
- Rissmann A
- Risteski T
- Rite S
- Rivarola NI
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- Roberts CA
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- Rojas N
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- Rosas FA
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- Sahuanay VRC
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- Salha AAS
- Salim JM
- Salinas V
- Salo M
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- Samarah YA
- Samarakkody U
- Sambo YT
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- Scalabre A
- Scherl H
- Schmedding A
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- Shaheen AA
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- Shalaby A
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- Zidan M
- Zivanovic D
- Zreeg DAS
- Zurikat RO
- Zvizdic N
- Zvizdic Z
- Publication venue
- ELSEVIER SCIENCE INC
- Publication date
- 24/07/2021
- Field of study
Background: Congenital anomalies are the fifth leading cause of mortality in children younger than 5 years globally. Many gastrointestinal congenital anomalies are fatal without timely access to neonatal surgical care, but few studies have been done on these conditions in low-income and middle-income countries (LMICs). We compared outcomes of the seven most common gastrointestinal congenital anomalies in low-income, middle-income, and high-income countries globally, and identified factors associated with mortality. // Methods: We did a multicentre, international prospective cohort study of patients younger than 16 years, presenting to hospital for the first time with oesophageal atresia, congenital diaphragmatic hernia, intestinal atresia, gastroschisis, exomphalos, anorectal malformation, and Hirschsprung's disease. Recruitment was of consecutive patients for a minimum of 1 month between October, 2018, and April, 2019. We collected data on patient demographics, clinical status, interventions, and outcomes using the REDCap platform. Patients were followed up for 30 days after primary intervention, or 30 days after admission if they did not receive an intervention. The primary outcome was all-cause, in-hospital mortality for all conditions combined and each condition individually, stratified by country income status. We did a complete case analysis. // Findings: We included 3849 patients with 3975 study conditions (560 with oesophageal atresia, 448 with congenital diaphragmatic hernia, 681 with intestinal atresia, 453 with gastroschisis, 325 with exomphalos, 991 with anorectal malformation, and 517 with Hirschsprung's disease) from 264 hospitals (89 in high-income countries, 166 in middle-income countries, and nine in low-income countries) in 74 countries. Of the 3849 patients, 2231 (58·0%) were male. Median gestational age at birth was 38 weeks (IQR 36â39) and median bodyweight at presentation was 2·8 kg (2·3â3·3). Mortality among all patients was 37 (39·8%) of 93 in low-income countries, 583 (20·4%) of 2860 in middle-income countries, and 50 (5·6%) of 896 in high-income countries (p<0·0001 between all country income groups). Gastroschisis had the greatest difference in mortality between country income strata (nine [90·0%] of ten in low-income countries, 97 [31·9%] of 304 in middle-income countries, and two [1·4%] of 139 in high-income countries; pâ€0·0001 between all country income groups). Factors significantly associated with higher mortality for all patients combined included country income status (low-income vs high-income countries, risk ratio 2·78 [95% CI 1·88â4·11], p<0·0001; middle-income vs high-income countries, 2·11 [1·59â2·79], p<0·0001), sepsis at presentation (1·20 [1·04â1·40], p=0·016), higher American Society of Anesthesiologists (ASA) score at primary intervention (ASA 4â5 vs ASA 1â2, 1·82 [1·40â2·35], p<0·0001; ASA 3 vs ASA 1â2, 1·58, [1·30â1·92], p<0·0001]), surgical safety checklist not used (1·39 [1·02â1·90], p=0·035), and ventilation or parenteral nutrition unavailable when needed (ventilation 1·96, [1·41â2·71], p=0·0001; parenteral nutrition 1·35, [1·05â1·74], p=0·018). Administration of parenteral nutrition (0·61, [0·47â0·79], p=0·0002) and use of a peripherally inserted central catheter (0·65 [0·50â0·86], p=0·0024) or percutaneous central line (0·69 [0·48â1·00], p=0·049) were associated with lower mortality. // Interpretation: Unacceptable differences in mortality exist for gastrointestinal congenital anomalies between low-income, middle-income, and high-income countries. Improving access to quality neonatal surgical care in LMICs will be vital to achieve Sustainable Development Goal 3.2 of ending preventable deaths in neonates and children younger than 5 years by 2030
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
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- Abdelalim AA
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- Abdulsalam A
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- Yang UK
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- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
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- Yu D
- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
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- Zhang S
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zito G
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- 'Elsevier BV'
- Publication date
- 10/09/2019
- Field of study
The production cross sections of B_{s}^{0} mesons and charge conjugates are measured in proton-proton (pp) and PbPb collisions via the exclusive decay channel B_{s}^{0}âJ/ÏÏâÎŒ^{+}ÎŒ^{â}K^{+}K^{â} at a center-of-mass energy of 5.02 TeV per nucleon pair and within the rapidity range |y|<2.4 using the CMS detector at the LHC. The pp measurement is performed as a function of transverse momentum (p_{T}) of the B_{s}^{0} mesons in the range of 7 to 50 GeV/c and is compared to the predictions of perturbative QCD calculations. The B_{s}^{0} production yield in PbPb collisions is measured in two p_{T} intervals, 7 to 15 and 15 to 50 GeV/c, and compared to the yield in pp collisions in the same kinematic region. The nuclear modification factor (R_{AA}) is found to be 1.5±0.6(stat)±0.5(syst) for 7â15 GeV/c, and 0.87±0.30(stat)±0.17(syst) for 15â50 GeV/c, respectively. Within current uncertainties, the B_{s}^{0} results are consistent with models of strangeness enhancement, and suppression by parton energy loss, as observed for the B+ mesons
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
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- Abercrombie D
- Abu Zeid S
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- Zorbilmez C
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- Zou D
- Zucchetta A
- 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
Measurement of the ttÂŻ production cross section, the top quark mass, and the strong coupling constant using dilepton events in pp collisions at âs = 13 TeV
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
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- Yetkin EA
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- Yumiceva F
- Yusli MN
- Zabi A
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- Zahid S
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- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
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- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zobec J
- Zoi I
- Zolkapli Z
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- Zorbilmez C
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- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 29/04/2019
- Field of study
A measurement of the top quarkâantiquark pair production cross section ÏttÂŻ in protonâproton collisions at a centre-of-mass energy of 13TeV is presented. The data correspond to an integrated luminosity of 35.9fbâ1, recorded by the CMS experiment at the CERN LHC in 2016. Dilepton events (e ± ÎŒ â, ÎŒ+ÎŒâ, e+eâ) are selected and the cross section is measured from a likelihood fit. For a top quark mass parameter in the simulation of mMCt=172.5GeV the fit yields a measured cross section ÏttÂŻ=803±2(stat)±25(syst)±20(lumi)pb, in agreement with the expectation from the standard model calculation at next-to-next-to-leading order. A simultaneous fit of the cross section and the top quark mass parameter in the POWHEG simulation is performed. The measured value of mMCt=172.33±0.14(stat)+0.66â0.72(syst)GeV is in good agreement with previous measurements. The resulting cross section is used, together with the theoretical prediction, to determine the top quark mass and to extract a value of the strong coupling constant with different sets of parton distribution functions
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
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
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- Aggleton R
- Agram JL
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- Ahmad M
- Ahmad M
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- Akchurin N
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- Al-bataineh A
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- Alhusseini M
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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
Evidence for Top Quark Production in Nucleus-Nucleus Collisions
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
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- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
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- Ahuja S
- Akbiyik M
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- Akgun B
- Akpinar A
- Albajar C
- Albergo S
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- Alcaraz Maestre J
- Aldaya Martin M
- AldĂĄ JĂșnior WL
- Aleksandrov A
- Alexander J
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- Alimena J
- Alison J
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- Alvarez Gonzalez B
- Alverson G
- Alves GA
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- Amendola C
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- Amsler C
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- Anderson D
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- Andrews MB
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- Asghar MI
- Asilar E
- Askew A
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- Atakisi IO
- Atanasov I
- Ather MW
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- Ăzçelik Ă
- Publication venue
- Publication date
- 01/01/2019
- Field of study
Peer reviewe
Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at \sqrt{s} = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- 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
- Alhusseini M
- Ali MABM
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez JDR
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Angioni GLP
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arndt T
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asghar MI
- Asilar E
- Askew A
- Assran Y
- Atakisi IO
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Autermann C
- Avdeeva E
- Avery P
- Avila C
- Ayala E
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Bagaturia I
- Bagliesi G
- Bahinipati S
- Baidali S
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Ball AH
- Ball F
- Ban Y
- Band R
- Banerjee S
- Banerjee S
- Bani L
- Bansal S
- Barbagli G
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- Yusli MN
- Zabi A
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- Zanetti M
- Zarubin A
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- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2019
- Field of study
A search for nonresonant excesses in the invariant mass spectra of electron and muon pairs is presented. The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the CMS experiment in 2016, corresponding to a total integrated luminosity of 36 fb^{-1}. No significant deviation from the standard model is observed. Limits are set at 95% confidence level on energy scales for two general classes of nonresonant models. For a class of fermion contact interaction models, lower limits ranging from 20 to 32 TeV are set on the characteristic compositeness scale Î. For the Arkani-Hamed, Dimopoulos, and Dvali model of large extra dimensions, the first results in the dilepton final state at 13 TeV are reported, and values of the ultraviolet cutoff parameter Î_{T} below 6.9 TeV are excluded. A combination with recent CMS diphoton results improves this exclusion to Î_{T} below 7.7 TeV, providing the most sensitive limits to date in nonhadronic final states
- âŠ