162 research outputs found
In vivo assessment of a novel biodegradable ureteral stent
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
Purpose: To perform an in vivo assessment of a newly developed biodegradable ureteral stent (BUS) produced with natural-based polymers. Methods: The BUS is based on a patented technology combining the injection process with the use of supercritical fluid technology. The study was conducted at ICVS-University of Minho (Braga, Portugal) and a total of ten domestic pigs were used. In seven animals, the experimental BUS stent was inserted, whereas in the remaining a commercially available stent was used (6-Fr Biosoft(®) duo stents, Porges Coloplast, Denmark). Post-stenting intravenous pyelogram was used to evaluate the degree of hydronephrosis. The in vivo stent degradation was measured as a function of the weight loss. Moreover, the tensile properties of the BUS were tested during in vivo degradation. After maximum 10 days, animals were killed and necropsy was performed. Tissues were compared between the stented groups as well as between the non-stented contralateral ureters and stented ureters in each group. Biocompatibility was assessed by histopathological grading. Results: In all cases, the BUS was only visible during the first 24 h on X-ray, and in all cases, the BUS was completely degraded in urine after 10 days, as confirmed on necropsy. During the degradation process, the mechanical properties of the BUS decreased, while the commercial ureteral stents remained constant. At all time-points after stent insertion, the level of hydronephrosis was minimal. Overall, animals stented with BUS had an average grade of hydronephrosis which was lower compared to the controls. The BUS showed better pathological conditions, and hence better biocompatibility when compared with commercial stents. Conclusions: Notwithstanding the limitations of the present study, the in vivo testing of our novel natural origin polymer-based BUS suggests this device to feature homogeneous degradation, good urine drainage, and high biocompatibility. Next steps will be to increase its stability and to improve the radiopacity without compromising its degradation. Ultimately, clinical studies will be required to determine the safety and feasibility of its use in humans.FCT -Fuel Cell Technologies Program(POCI-01-0145-FEDER-007038)info:eu-repo/semantics/publishedVersio
Protistan Diversity in the Arctic: A Case of Paleoclimate Shaping Modern Biodiversity?
- Author
- A Ahlberg
- A Akhmanova
- A Behnke
- A Cameron
- A Chao
- A Sluijs
- A Tripati
- A Zuendorf
- AG Fischer
- AGB Simpson
- AP Martin
- B Bodiselitsch
- B Lawley
- B Shopsin
- BF Lang
- BL Maidak
- BS Leander
- BS Leander
- C Lovejoy
- Chesley Leslin
- CJ O'Kelly
- D Posada
- DD Leipe
- DJ Lane
- DL Swofford
- DP Schrag
- ET Steenkamp
- F Voncken
- HC Jenkyns
- HJ Elwood
- J Cuny
- J Fried
- J Wuyts
- JD Thompson
- Jennifer Kasper
- JF Robison-Cox
- JL Kirschvink
- JL Kirschvink
- John Bunge
- K Moran
- KJ-A Barger
- L Medlin
- LA Amaral Zettler
- MD Johnson
- MT Suzuki
- MV Lomolino
- MW Gray
- N Lang-Unnasch
- ON Kuvardina
- P Lopez-Garcia
- P Lopez-Garcia
- P Lopez-Garcia
- PA Wilson
- PD Gingerich
- PF Hoffman
- PF Hoffman
- Rees Kassen
- RK Naviaux
- SC Dawson
- SF Altschul
- SH Hong
- SL Miller
- Slava Epstein
- SO Jeon
- SY Moon-van der Staay
- T Stoeck
- T Stoeck
- T Stoeck
- T-J Shen
- TD Kocher
- Thorsten Stoeck
- Valya Ilyin
- VP Edgcomb
- W Ludwig
- Publication venue
- Public Library of Science
- Publication date
- 15/08/2007
- Field of study
The impact of climate on biodiversity is indisputable. Climate changes over geological time must have significantly influenced the evolution of biodiversity, ultimately leading to its present pattern. Here we consider the paleoclimate data record, inferring that present-day hot and cold environments should contain, respectively, the largest and the smallest diversity of ancestral lineages of microbial eukaryotes.We investigate this hypothesis by analyzing an original dataset of 18S rRNA gene sequences from Western Greenland in the Arctic, and data from the existing literature on 18S rRNA gene diversity in hydrothermal vent, temperate sediments, and anoxic water column communities. Unexpectedly, the community from the cold environment emerged as one of the richest observed to date in protistan species, and most diverse in ancestral lineages.This pattern is consistent with natural selection sweeps on aerobic non-psychrophilic microbial eukaryotes repeatedly caused by low temperatures and global anoxia of snowball Earth conditions. It implies that cold refuges persisted through the periods of greenhouse conditions, which agrees with some, although not all, current views on the extent of the past global cooling and warming events. We therefore identify cold environments as promising targets for microbial discovery
Absorption across the nasal airway mucosa in house dust mite perennial allergic rhinitis
- Author
- Publication venue
- 'Wiley'
- Publication date
- Field of study
Evaluating the use of citizens' juries in food policy: a case study of food regulation
- Author
- A Barnes
- A Coote
- A Gutmann
- B Evoy
- B Kelly
- B Kelly
- B Swinburn
- C Bailey
- C Mitton
- C Molster
- D Ryfe
- Elizabeth House
- G Gooberman-Hill
- J Abelson
- J Abelson
- J Lenaghan
- JD Feron
- Jefferson Center
- John Coveney
- JS Dryzek
- JS Fishkin
- Julie Henderson
- K Mehta
- L Pratchett
- M Delli Carpini
- Michael Calnan
- P Elwood
- Paul Ward
- R Inglehart
- R Ireland
- R Kuper
- Rachel Ankeny
- RK Blamey
- Samantha Meyer
- State Government of Victoria
- World Health Organization
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2013
- Field of study
BACKGROUND Deliberative engagement techniques and citizens’ juries are touted as means of incorporating the public into policy decision-making, managing community expectations and increasing commitment to public health policy. This paper reports a study to examine the feasibility of citizens’ juries as a means of collecting data to inform public health policy related to food regulation through evaluation of the conduct of a citizens’ jury. METHODS A citizens’ jury was conducted with a representative sample of 17 South Australians to explore their willingness to consider the proposition that food and drink advertising and/or sponsorship should be banned at children’s sporting events. RESULTS The results showed that, in relation to the central proposition and evaluation data from the jury, opinion on the proposition remained comparatively stable. Most jurors indicated that they thought that food and drink sponsorship and/or advertising at children’s sporting events would have little or no effect on altering children’s diet and eating habits, with the proportion increasing during the jury process. Jurors were given evaluation sheets about the content of the jury and the process of the citizens’ jury to complete at the end of the session. The evaluation of the citizens’ jury process revealed positive perceptions. The majority of jurors agreed that their knowledge of the issues of food and drink sponsorship in children’s sport had increased as a result of participation in the citizens’ jury. The majority also viewed the decision-making process as fair and felt that their views were listened to. One important response in the evaluation was that all jurors indicated that, if given the opportunity, they would participate in another citizens’ jury. CONCLUSIONS The findings suggest that the citizens’ jury increased participant knowledge of the issue and facilitated reflective discussion of the proposition. Citizens’ juries are an effective means of gaining insight into public views of policy and the circumstances under which the public will consider food regulation; however a number of issues need to be considered to ensure the successful conduct of a citizens’ jury.Julie Henderson, Elizabeth House, John Coveney, Samantha Meyer, Rachel Ankeny, Paul Ward and Michael Calna
Precise determination of the mass of the Higgs boson and tests of compatibility of its couplings with the standard model predictions using proton collisions at 7 and 8 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agapitos A
- Agram JL
- Ahmad A
- Ahmad M
- Ahuja S
- Akchurin N
- Akgun B
- Akin IV
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Alderweireldt S
- Aleksandrov A
- Alexander J
- Alimena J
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anderson I
- Anderson J
- Andrea J
- Andreev V
- Andreev Y
- Androsov K
- Antonelli L
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Apyan A
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Arora S
- Asavapibhop B
- Asawatangtrakuldee C
- Asin I
- Askew A
- Aslanoglou X
- Assran Y
- Ata M
- Attikis A
- Aubin A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Baber M
- Bacchetta N
- Bachmair F
- Bachtis M
- Baden A
- Baffioni S
- Bagliesi G
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Ball AH
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Barbagli G
- Barberis E
- Barbieri R
- Bargassa P
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barth C
- Bartosik N
- Basegmez S
- Battilana C
- Bauerdick LA
- Baumgartel D
- Baus C
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Beernaert K
- Behnamian H
- Behr J
- Behrens U
- Beirão Da Cruz E Silva C
- Belforte S
- Beliy N
- Belknap DA
- Bell AJ
- Bell KW
- Bellan R
- Belloni A
- Beluffi C
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benitez JF
- Benucci L
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Bhardwaj A
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhawandeep U
- Bhowmik S
- Bialkowska H
- Bian JG
- Bianchini L
- Bianco S
- Biasini M
- Bierwagen K
- Biino C
- Bilei GM
- Bilin B
- Bilki B
- Bilmis S
- Biselloa D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodlak M
- Boimska B
- Bolla G
- Bolognesi S
- Bonacorsi D
- Bonato A
- Bondu O
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- Boos E
- Bornheim A
- Borras K
- Bortignon P
- Bortoletto D
- Bose S
- Bose T
- Botta C
- Boudoul G
- Bouhali O
- Bourilkov D
- Boutle S
- Bouvier E
- Bradmiller-Feld J
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breto G
- Breuker H
- Brew C
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Brinson J
- Brito L
- Broccolo G
- Brochero Cifuentes JA
- Brochet S
- Brodski M
- Brom JM
- Brona G
- Brooke JJ
- Brown RM
- Brownson E
- Brun H
- Bruner C
- Bruno G
- Buchmann MA
- Buchmuller O
- Bucinskaite I
- Bunichev V
- Bunin P
- Bunkowski K
- Bunn J
- Buontempo S
- Burgmeier A
- Burkett K
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- Burton D
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butz E
- Bylsma B
- Bäni L
- Böser C
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Caillol C
- Cakir A
- Calabria C
- Calamba A
- Calderon A
- Cali IA
- Calligaris L
- Calvert B
- Calvo E
- Campagnari C
- Campanini R
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- Camporesi T
- Candelise V
- Canelli MF
- Cankocak K
- Capiluppi P
- Cappello G
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- Carlsmith D
- Carlson B
- Carrillo Montoya CA
- Carrillo Moreno S
- Cartiglia N
- Carvalho W
- Carver M
- Casal B
- Casarsa M
- Casasso S
- Casimiro Linares E
- Castaldi R
- Castaneda Hernandez A
- Castello R
- Castilla-Valdez H
- Castro A
- Caudron A
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Centis Vignali M
- Cepeda M
- Cerati GB
- Cerci S
- Cerminara G
- Cerrada M
- Chabert EC
- Chakaberia I
- Chamizo Llatas M
- Chan KM
- Chang P
- Chang S
- Chang YH
- Chanon N
- Chao Y
- Chaparro Sierra LF
- Chapon E
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- Chasserat J
- Chatterjee A
- Chatterjee K
- Chatterjee RM
- Chauhan S
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- Chen HS
- Chen KF
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- Cherepanov V
- Chertok M
- Cheung HW
- Chhibra SS
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- Chiochia V
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- Choi YK
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- Choudhary BC
- Choudhury S
- Christopher G
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- Chwalek T
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- Cimmino A
- Ciocci MA
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
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- Clarida W
- Clarke C
- Clement E
- Clerbaux B
- CMS Collaboration
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- Codispoti G
- Colafranceschi S
- Colaleo A
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- Colino N
- Collard C
- Colling D
- Contardo D
- Conte E
- Contreras-Campana C
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- Cooper SI
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- Correa Martins Junior M
- Cossutti F
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- Costantini S
- Costanza F
- Couderc F
- Coughlan JA
- Courbon B
- Cousins R
- Covarelli R
- Cowden C
- Cox B
- Cox PT
- Creanza D
- Cripps N
- Cristella L
- Crucy S
- Cuevas J
- Cuffiani M
- Cumalat JP
- Curry D
- Cussans D
- Custódio A
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- d'Enterria D
- D'Hondt J
- D'imperio G
- Da Costa EM
- Da Silveira GG
- Dabrowski A
- Daci N
- Dahmes B
- Dahms T
- Dalchenko M
- Dall'Osso M
- Dallavalle GM
- Damgov J
- Danielson T
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- Dauncey P
- David A
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- de Barbaro P
- De Boer W
- De Cosa A
- De Filippis N
- De Gruttola M
- De Guio F
- De Jesus Damiao D
- De La Barca Sanchez MC
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Mattia M
- De Oliveira Martins C
- De Palma M
- De Roeck A
- de Trocóniz JF
- De Visscher S
- De Wolf EA
- Degano A
- Deiters K
- Dejardin M
- Del Re D
- Delaere C
- Delannoy AG
- Delgado Peris A
- Dell'Orso R
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- Della Ricca G
- Demaria N
- Demina R
- Demiragli Z
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- Denegri D
- Depasse P
- Dermenev A
- Descroix A
- Dewanjee RK
- Dhingra N
- Di Giovanni GP
- Di Guida S
- Di Marco E
- Di Matteo L
- Diamond B
- Diemoz M
- Dierlamm A
- Dietz C
- Dietz-Laursonn E
- Diez Pardos C
- Dildick S
- Dilsiz K
- Dimitrov A
- Dinardo ME
- Dishaw A
- Dissertori G
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- Dittmer S
- Dobrzynski L
- Dobson M
- Dobur D
- Dodd L
- Dogra S
- Dolen J
- Dolinska G
- Dominguez A
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- Domínguez Vázquez D
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- Donegà M
- Dooling S
- Dordevic M
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- Dorland T
- Dorney B
- Doroba K
- Dosselli U
- Dozen C
- Draeger AR
- Dragicevic M
- Dragoiu C
- Dremin I
- Driga O
- Drozdetskiy A
- du Pree T
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- Duarte Campderros J
- Duarte J
- Dubinin M
- Duchardt D
- Dudero PR
- Dudko L
- Dugad S
- Duggan D
- Dumanoglu I
- Dunne P
- Dupont-Sagorin N
- Duric S
- Durkin LS
- Dutta D
- Dutta S
- Dutta V
- Dünser M
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- Ecklund KM
- Eckstein D
- Edelhoff M
- Eerola P
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- Ekmedzic M
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- Eller P
- Elliott-Peisert A
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- Elmer P
- Elvira VD
- Elwood A
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erdogan Y
- Erfle J
- Ershov A
- Erö J
- Escalante Del Valle A
- Eshaq Y
- Eskut E
- Etesami SM
- Eusebi R
- Evangelou I
- Evdokimov O
- Everaerts P
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- Faulkner J
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- Favart D
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- Fehling D
- Feindt M
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- Ferapontov A
- Ferbel T
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- Fernandez Bedoya C
- Fernandez Menendez J
- Fernandez Perez Tomei TR
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- Finger M
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- Fonseca De Souza S
- Fontaine JC
- Ford WT
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- Foudas C
- Fouz MC
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- Franco Sevilla M
- Franzoni G
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- Geisler M
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- Geurts FJ
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- Guthoff M
- Gutsche O
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- Gülmez E
- Güth A
- Haas J
- Hadjiiska R
- Hadley NJ
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- Hagopian V
- Hahn KA
- Haj Ahmad W
- Hajdu C
- Halkiadakis E
- Hall G
- Hall-Wilton R
- Haller J
- Hamel de Monchenault G
- Hammad GH
- Hammer J
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- Hatakeyama K
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- Heath GP
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- Hebda P
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- Heidemann C
- Heikkilä JK
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- Henderson C
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- Heredia-de La Cruz I
- Hernandez JM
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- Horisberger R
- Horvath D
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- Höing RS
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- Iaydjiev P
- Ignatenko M
- Iiyama Y
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- Jain S
- Jandir P
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- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zeinali M
- Zenoni F
- Zenz SC
- Zeuner WD
- Zevi Della Porta G
- Zeyrek M
- Zhang F
- Zhang J
- Zhang L
- Zhokin A
- Zhu RY
- Zhukov V
- Zhukova V
- Zorbilmez C
- Zotto P
- Zou W
- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- Zvada M
- Publication venue
- Publication date
- 01/01/2014
- Field of study
Peer reviewe
Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at root s=8 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adair A
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adzic P
- Agapitos A
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Al-bataineh A
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Alderweireldt S
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alimena J
- Almond J
- Alunni Solestizi L
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Amsler C
- Anagnostou G
- Anderson D
- Anderson I
- Andrea J
- Andreev V
- Andreev Yu
- Andrews MB
- Androsov K
- Anelli C
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Arcaro D
- Arcidiacono R
- Arenton MW
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- Asawatangtrakuldee C
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- Avetisyan A
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- Awad A
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- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Baber M
- Bacchetta N
- Bachmair F
- Bachtis M
- Baden A
- Baffioni S
- Bagliesi G
- Bahinipati S
- Baillon P
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
Peer reviewe
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- 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
- 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
- Antunes De Oliveira AC
- 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 M
- Asilar E
- Askew A
- Atakisi IO
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Autermann C
- Auzinger G
- 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
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- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
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- Yu I
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- 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
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- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zito G
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- Zoi I
- Zolkapli Z
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- 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}→J/ψϕ→μ^{+}μ^{−}K^{+}K^{−} 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 7–15 GeV/c, and 0.87±0.30(stat)±0.17(syst) for 15–50 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
Constraints on anomalous HVV couplings from the production of Higgs bosons decaying to τ lepton pairs
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Acharya H
- 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
- 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
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- Almond J
- Alvarez Fernandez A
- Alverson G
- Alves FL
- Alves GA
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- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
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- Andreev Y
- Andrews MB
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- Yohay R
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- Yoo J
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- 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
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- Zhang S
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- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 04/12/2019
- Field of study
A study is presented of anomalous HVV interactions of the Higgs boson, including its CP properties. The study uses Higgs boson candidates produced mainly in vector boson fusion and gluon fusion that subsequently decay to a pair of τ leptons. The data were recorded by the CMS experiment at the LHC in 2016 at a center-of-mass energy of 13 TeV and correspond to an integrated luminosity of 35.9 fb−1. A matrix element technique is employed for the analysis of anomalous interactions. The results are combined with those from the H→4ℓ decay channel presented earlier, yielding the most stringent constraints on anomalous Higgs boson couplings to electroweak vector bosons expressed as effective cross section fractions and phases: the CP-violating parameter fa3cos(ϕa3)=(0.00±0.27)×10−3 and the CP-conserving parameters fa2cos(ϕa2)=(0.08+1.04−0.21)×10−3, fΛ1cos(ϕΛ1)=(0.00+0.53−0.09)×10−3, and fZγΛ1cos(ϕZγΛ1)=(0.0+1.1−1.3)×10−3. The current dataset does not allow for precise constraints on CP properties in the gluon fusion process. The results are consistent with standard model expectations
Measurement of the tt¯ production cross section, the top quark mass, and the strong coupling constant using dilepton events in pp collisions at √s = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Acharya H
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- Yohay R
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- Yoo J
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- Yumiceva F
- Yusli MN
- Zabi A
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- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
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- Zenz SC
- Zeuner WD
- Zeyrek M
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- Zhang A
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- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
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- Zoi I
- Zolkapli Z
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- Zuolo D
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 29/04/2019
- Field of study
A measurement of the top quark–antiquark pair production cross section σtt¯ in proton–proton collisions at a centre-of-mass energy of 13TeV is presented. The data correspond to an integrated luminosity of 35.9fb−1, recorded by the CMS experiment at the CERN LHC in 2016. Dilepton events (e ± μ ∓, μ+μ−, e+e−) 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 σtt¯=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)+0.66−0.72(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 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
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- Acosta JG
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- Ahmad A
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- Ahmed I
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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
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