321 research outputs found
Proximate Levels and Phytochemical Contents in Selected Cereals Sold in Wukari Local Government Area of Taraba State
- Publication venue
- Global Press Hub
- Publication date
- Field of study
Research has indicated that consumption of whole grain foods can significantly reduce the risk of some chronic health conditions such as type II diabetes, cardiovascular disease, and cancer Therefore, the present study evaluated the proximate constituents and the levels of phytochemicals in rice, maize and millet procured from Wukari Local Government Area of Taraba state. Three cereal samples were procured (rice, maize and millet), air dried and analyzed for proximate and phytochemical contents using AOAC and HPLC respectively. The result for proximate analysis revealed the presence of six proximate components in their respective amounts. These were ether Original research Article 36 extract, crude protein, crude fibre, Ash, Moisture, nitrogen free extract (soluble Carbohydrates). The results of protein showed no significant difference at p ≥ 0.05 in all the samples, except millet 2 and millet 3 that showed significant difference with rice (1 to 3) and maize 1. Results of fat showed no significant difference between rice (1 to 3), maize (1 to 3) and millet 2, while millet 1 and 2 significantly differ from all the samples except millet 2. The results of fibre showed no significant difference rice (1 to 3) and millet (1 to 3), while maize (1 to 3) showed significant difference with millet 1 and rice (2 and 3) at p ≤ 0.05. There is no significant difference (p>0.05) in ash content of maize and rice samples, while millet showed significant difference at p ≤ 0.05 with rice (1 to 3) and maize (2 and 3). The results of alkaloids and tannins showed significant difference rice, maize and millet. However, there is significant difference in saponins presence in rice, maize and millet at p ≤ 0.05. There is significant difference in oxalates, phytates, tarpenes, glycosides and flavonoids present in all the samples, while phenolics showed no significant difference among all the samples. This study revealed the varying and appreciable levels of food constituents and health promoting components in sample analyzed. This indicated the nutritional qualities of the samples analyzed
Functional interface micromechanics of 11 en-bloc retrieved cemented femoral hip replacements
- Author
- Publication venue
- Informa Healthcare
- Publication date
- 01/01/2010
- Field of study
Contains fulltext :
88556.pdf (publisher's version ) (Open Access)BACKGROUND AND PURPOSE: Despite the longstanding use of micromotion as a measure of implant stability, direct measurement of the micromechanics of implant/bone interfaces from en bloc human retrievals has not been performed. The purpose of this study was to determine the stem-cement and cement-bone micromechanics of functionally loaded, en-bloc retrieved, cemented femoral hip components. METHODS: 11 fresh frozen proximal femurs with cemented implants were retrieved at autopsy. Specimens were sectioned transversely into 10-mm slabs and fixed to a loading device where functional torsional loads were applied to the stem. A digital image correlation technique was used to document micromotions at stem-cement and cement-bone interfaces during loading. RESULTS: There was a wide range of responses with stem-cement micromotions ranging from 0.0006 mm to 0.83 mm (mean 0.17 mm, SD 0.29) and cement-bone micromotions ranging from 0.0022 mm to 0.73 mm (mean 0.092 mm, SD 0.22). There was a strong (linear-log) inverse correlation between apposition fraction and micromotion at the stem-cement interface (r(2) = 0.71, p < 0.001). There was a strong inverse log-log correlation between apposition fraction at the cement-bone interface and micromotion (r(2) = 0.85, p < 0.001). Components that were radiographically well-fixed had a relatively narrow range of micromotions at the stem-cement (0.0006-0.057 mm) and cement-bone (0.0022-0.029 mm) interfaces. INTERPRETATION: Minimizing gaps at the stem-cement interface and encouraging bony apposition at the cement-bone interface would be clinically desirable. The cement-bone interface does not act as a bonded interface in actual use, even in radiographically well-fixed components. Rather, the interface is quite compliant, with sliding and opening motions between the cement and bone surfaces.1 juni 201
Vertical Heterophoria and Postural Control in Nonspecific Chronic Low Back Pain
- Author
- A Hamaoui
- A Takagi
- AE Kertesz
- AJ Harris
- AM Wong
- B Missaoui
- BF Walker
- BR Bloem
- C Marucchi
- CL Allison
- CS McCabe
- CS McCabe
- DD Price
- E Casillas Casillas
- E Jonsson
- E Matheron
- E Matheron
- E Matheron
- E Matheron
- E Matheron
- E Matheron
- E Thomas
- EM Hagen
- EO Huskisson
- Eric Matheron
- EW Cheeseman Jr
- FJ Amos
- G Ebenbichler
- G Waddell
- G Waddell
- G Waddell
- GBJ Andersson
- GK von Noorden
- HI Andersson
- HM Da Cunha
- HO Diener
- IA Stokes
- IB Suchoff
- IG Amiridis
- J Ygge
- JB Baron
- JE Doble
- JL Demer
- KD Scattergood
- KE Jones
- KM Alexander
- KM Daum
- L Hestbaek
- L Pisella
- M Scheiman
- M von Korff
- MA Huang
- MI Mientjes
- N Kapoor
- N Maniadakis
- N Ushio
- N Ushio
- N Vuillerme
- NN Byl
- NW Mok
- P Sunartpin
- Paul Gribble
- PM Gagey
- PM Gagey
- PM Gagey
- PR Croft
- PS Bergin
- R della Volpe
- R Kono
- R Mazzocchio
- R Mazzocchio
- RA Deyo
- RA Speers
- S Brumagne
- S Brumagne
- S Brumagne
- SJ Atlas
- SM Henry
- T Brandt
- T Popa
- TT Lê
- U van Rijn
- W Bles
- W Paulus
- WL Cats-Baril
- WM Paulus
- WV Padula
- WV Padula
- Y Wang
- Z Kapoula
- Zoï Kapoula
- Publication venue
- Public Library of Science
- Publication date
- 30/03/2011
- Field of study
The purpose of this study was to test postural control during quiet standing in
nonspecific chronic low back pain (LBP) subjects with vertical heterophoria (VH)
before and after cancellation of VH; also to compare with healthy subjects with,
and without VH. Fourteen subjects with LBP took part in this study. The postural
performance was measured through the center of pressure displacements with a
force platform while the subjects fixated on a target placed at either 40 or 200
cm, before and after VH cancellation with an appropriate prism. Their postural
performance was compared to that of 14 healthy subjects with VH and 12 without
VH (i.e. vertical orthophoria) studied previously in similar conditions. For LBP
subjects, cancellation of VH with a prism improved postural performance. With
respect to control subjects (with or without VH), the variance of speed of the
center of pressure was higher, suggesting more energy was needed to stabilize
their posture in quiet upright stance. Similarly to controls, LBP subjects
showed higher postural sway when they were looking at a target at a far distance
than at a close distance. The most important finding is that LBP subjects with
VH can improve their performance after prism-cancellation of their VH. We
suggest that VH reflects mild conflict between sensory and motor inputs involved
in postural control i.e. a non optimal integration of the various signals. This
could affect the performance of postural control and perhaps lead to pain.
Nonspecific chronic back pain may results from such prolonged conflict
Evaluation of anxiolytic activity of methanolic extract of Urtica urens in a mice model
- Author
- A O’Donovana
- A Rexa
- A Sevki
- American Heritage Medical Dictionary Editors
- American Psychiatric Association
- Anonymous
- Anonymus
- C Manavi
- C Pál
- C Wolfman
- E Masoumeh
- EA Carlini
- EH Uhlenhuth
- EL Houcine Bouidida
- EM Lepicard
- H Takeda
- JN Crawley
- JN Crawley
- Katim Alaoui
- Khalid Taghzouti
- L Prut
- M Lader
- MEP Seligman
- ML Novas
- Mohamed Nadjmouddine
- NW Dunham
- R Verma
- RM Perez
- RN Kishore
- S Amos
- TT Faustino
- Yahya Cherrah
- Zouhra Doukkali
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
- Adamek L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi F
- Algren M
- Alhroob M
- Ali B
- Ali HMJ
- Ali S
- Alibocus SW
- Aliev M
- Alimonti G
- Alkakhi W
- Allaire C
- Allbrooke BMM
- Allen JF
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
- Alves Cardoso M
- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amor Dos Santos SP
- Amos KR
- Ananiev V
- Anastopoulos C
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Anulli F
- Aoki M
- Aoki T
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Appelt C
- Apyan A
- Aranzabal N
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Assamagan K
- Astalos R
- Atashi S
- Atkin RJ
- Atkinson M
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Auriol AD
- Austrup VA
- Avolio G
- Axiotis K
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahmani M
- Bailey AJ
- Bailey VR
- Baines JT
- Baines L
- Bakalis C
- Baker OK
- Bakos E
- Bakshi Gupta D
- Balakrishnan V
- Balasubramanian R
- Baldin EM
- Balek P
- Ballabene E
- Balli F
- Baltes LM
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Bansal S
- Barak L
- Barakat M
- Barberio EL
- Barberis D
- Barbero M
- Barel MZ
- Barends KN
- Barillari T
- Barisits M-S
- Barklow T
- Baron Moreno DA
- Baron P
- Baroncelli A
- Barone G
- Barr AJ
- Barr JD
- Barranco Navarro L
- Barreiro Guimarães da Costa J
- Barreiro F
- Barron U
- Barros Teixeira MG
- Barsov S
- Bartels F
- Bartoldus R
- Barton AE
- Bartos P
- Basan A
- Baselga M
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Battulga D
- Bauce M
- Bauer M
- Bauer P
- Bazzano Hurrell LT
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HP
- Becker K
- Becot C
- Beddall AJ
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belyaev NL
- Benchekroun D
- Bendebba F
- Benhammou Y
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Bergeaas Kuutmann E
- Berger N
- Bergmann B
- Beringer J
- Bernardi G
- Bernius C
- Bernlochner FU
- Bernon F
- Berry T
- Berta P
- Berthold A
- Bertram IA
- Bethke S
- Betti A
- Bevan AJ
- Bhamjee M
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bianchi RM
- Bianco G
- Biebel O
- Bielski R
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondini A
- Birch-sykes CJ
- Bird GA
- Birman M
- Biros M
- Biryukov S
- Bisanz T
- Bisceglie E
- Biswal JP
- Biswas D
- Bitadze A
- Bjørke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blumenthal J
- Bobbink GJ
- Bobrovnikov VS
- Boehler M
- Boehm B
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbély AG
- Bordulev IS
- Borecka-Bielska HM
- Borgna LS
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bossio Sola JD
- Bouaouda K
- Bouchhar N
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bouquet R
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Britton D
- Britzger D
- Brock I
- Brooijmans G
- Brooks WK
- Brost E
- Brown LM
- Bruce LE
- Bruckler TL
- Bruckman de Renstrom PA
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Brüers B
- Buanes T
- Buat Q
- Buchin D
- Buckley AG
- Bulekov O
- Bullard BA
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burlayenko O
- Burr JTP
- Burton CD
- Burzynski JC
- Busch EL
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buxo Vazquez CJ
- Buzykaev AR
- Büscher V
- Cabrera Urbán S
- Cadamuro L
- Caforio D
- Cai H
- Cai Y
- Cairo VMM
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarero Munoz D
- Camarri P
- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capocasa F
- Capua M
- Carbone A
- Cardarelli R
- Cardenas JCJ
- Cardillo F
- Carli T
- Carlino G
- Carlotto JI
- Carlson BT
- Carlson EM
- Carminati L
- Carnelli A
- Carnesale M
- Caron S
- Carquin E
- Carratta G
- Carrio Argos F
- Carrá S
- Carter JWS
- Carter TM
- Casado MP
- Caspar M
- Castiglia EG
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cavaliere V
- Cavalli N
- Cavasinni V
- Cekmecelioglu YC
- Celebi E
- Celli F
- Centonze MS
- Cepaitis V
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervato B
- Cervelli A
- Cesarini G
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
- Chan WY
- Chapman JD
- Chapon E
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chauhan C
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen B
- Chen H
- Chen H
- Chen J
- Chen J
- Chen M
- Chen S
- Chen SJ
- Chen X
- Chen X
- Chen Y
- Cheng CL
- Cheng HC
- Cheong S
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiedde N
- Chiodini G
- Chisholm AS
- Chitan A
- Chitishvili M
- Chizhov MV
- Choi K
- Chomont AR
- Chou Y
- Chow EYS
- Chowdhury T
- Chu KL
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Cieri D
- Ciesla KM
- Cindro V
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark PJ
- Clavijo Columbie JM
- Clawson SE
- Clement C
- Clercx J
- Coadou Y
- Cobal M
- Coccaro A
- Coelho Barrue RF
- Coelho Lopes De Sa R
- Coelli S
- Cohen H
- Coimbra AEC
- Cole B
- Collot J
- Conde Muiño P
- Connell MP
- Connell SH
- Connelly IA
- Conroy EI
- Conventi F
- Cooke HG
- Cooper-Sarkar AM
- Cordeiro Oudot Choi A
- Cormier F
- Corpe LD
- Corradi M
- Corriveau F
- Cortes-Gonzalez A
- Costa MJ
- Costanza F
- Costanzo D
- Cote BM
- Cowan G
- Cranmer K
- Cremonini D
- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosby JE
- Crosetti G
- Crépé-Renaudin S
- Cueto A
- Cuhadar Donszelmann T
- Cui H
- Cui Z
- Cunningham WR
- Curcio F
- Czodrowski P
- Czurylo MM
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dal Santo D
- Dallapiccola C
- Dam M
- Damp J
- Dandoy JR
- Daneri MF
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Das SJ
- David C
- Davidek T
- Davis-Purcell B
- Dawson I
- Day-hall HA
- De Asmundis R
- De Biase N
- De Castro S
- De Groot N
- de Jong P
- De la Torre H
- De Maria A
- De Salvo A
- De Sanctis U
- De Santo A
- De Vivie De Regie JB
- De K
- Dedovich DV
- Degens J
- Deiana AM
- Del Corso F
- Del Peso J
- Del Rio F
- Deliot F
- Delitzsch CM
- Della Pietra M
- Della Volpe D
- Dell’Acqua A
- Dell’Asta L
- Delmastro M
- Delsart PA
- Demers S
- Demichev M
- Denisov SP
- Derendarz D
- Derue F
- Dervan P
- Desch K
- Deutsch C
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Luca A
- Di Micco B
- Di Nardo R
- Diaconu C
- Diamantopoulou M
- Dias Do Vale T
- Dias FA
- Diaz Capriles FG
- Diaz MA
- Didenko M
- Diehl EB
- Diehl L
- Diez Pardos C
- Dimitriadi C
- Dimitrievska A
- Dingfelder J
- Dinu I-M
- Dittmeier SJ
- Dittus F
- Djama F
- Djobava T
- Djuvsland JI
- Doglioni C
- Dohnalova A
- Dolejsi J
- Dolezal Z
- Dona KM
- Donadelli M
- Dong B
- Donini J
- Dopke J
- Doria A
- Dos Santos Fernandes N
- Dougan P
- Dova MT
- Doyle AT
- Draguet MA
- Dreyer E
- Drivas-koulouris I
- Drobac AS
- Drozdova M
- du Pree TA
- Du D
- Dubinin F
- Dubovsky M
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Duden ER
- Duflot L
- Dumitriu AE
- Dunford M
- Dungs S
- Dunne K
- Duperrin A
- Duran Yildiz H
- Durglishvili A
- Dwyer BL
- Dyckes GI
- Dyndal M
- Dysch S
- Dziedzic BS
- Díez Cornell S
- Dührssen M
- Dülsen C
- Düren M
- D’amen G
- D’Amico V
- D’Auria S
- D’Eramo L
- D’Onofrio A
- D’Onofrio M
- D’uffizi M
- Earnshaw ZO
- Eberwein GH
- Eckerova B
- Eggebrecht S
- Egidio Purcino De Souza E
- Ehrke LF
- Eigen G
- Einsweiler K
- Ekelof T
- Ekman PA
- El Farkh S
- El Ghazali Y
- El Jarrari H
- El Moussaouy A
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Enari Y
- Ene I
- Epari S
- Erdmann J
- Erland PA
- Errenst M
- Escalier M
- Escobar C
- Etzion E
- Evans G
- Evans H
- Evans LS
- Evans MO
- Ezhilov A
- Ezzarqtouni S
- Fabbri F
- Fabbri L
- Facini G
- Fadeyev V
- Fakhrutdinov RM
- Falciano S
- Falda Ulhoa Coelho LF
- Falke PJ
- Faltova J
- Fan C
- Fan Y
- Fang Y
- Fanti M
- Faraj M
- Farazpay Z
- Farbin A
- Farilla A
- Farooque T
- Farrington SM
- Fassi F
- Fassouliotis D
- Faucci Giannelli M
- Fawcett WJ
- Fayard L
- Federic P
- Federicova P
- Fedin OL
- Fedotov G
- Feickert M
- Feligioni L
- Fellers DE
- Feng C
- Feng M
- Feng Z
- Fenton MJ
- Fenyuk AB
- Ferencz L
- Ferguson RAM
- Fernandez Luengo SI
- Fernoux MJV
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
- Ferrere D
- Ferretti C
- Fiedler F
- Filipčič A
- Filmer EK
- Filthaut F
- Fiolhais MCN
- Fiorini L
- Fisher WC
- Fitschen T
- Fitzhugh PM
- Fleck I
- Fleischmann P
- Flick T
- Flores Castillo LR
- Flores Sanz De Acedo L
- Flores M
- Follega FM
- Fomin N
- Foo JH
- Forland BC
- Formica A
- Forti AC
- Fortin E
- Fortman AW
- Foti MG
- Fountas L
- Fournier D
- Fox H
- Francavilla P
- Francescato S
- Franchellucci S
- Franchini M
- Franchino S
- Francis D
- Franco L
- Franconi L
- Franklin M
- Frattari G
- Freegard AC
- Freund WS
- Frid YY
- Friend J
- Fritzsche N
- Froch A
- Froidevaux D
- Frost JA
- Fu Y
- Fujimoto M
- Fullana Torregrosa E
- Fung KY
- Furtado De Simas Filho E
- Furukawa M
- Fuster J
- Gabrielli A
- Gabrielli A
- Gadow P
- Gagliardi G
- Gagnon LG
- Gallas EJ
- Gallop BJ
- Gan KK
- Ganguly S
- Gao J
- Gao Y
- Garay Walls FM
- Garcia Alonso A
- Garcia Caffaro AG
- Garcia B
- Garcia-Sciveres M
- García Navarro JE
- García C
- Gardner GL
- Gardner RW
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- Zhemchugov A
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- Zhulanov V
- Zimine NI
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
Search for pair production of squarks or gluinos decaying via sleptons or weak bosons in final states with two same-sign or three leptons with the ATLAS detector
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- Abbott B
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- Abidi SH
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- Abusleme Hoffman AC
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- Zhemchugov A
- Zheng K
- Zheng X
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- Zhong D
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- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 15/02/2024
- Field of study
A search for pair production of squarks or gluinos decaying via sleptons or weak bosons is reported. The search targets a final state with exactly two leptons with same-sign electric charge or at least three leptons without any charge requirement. The analysed data set corresponds to an integrated luminosity of 139 fb−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Multiple signal regions are defined, targeting several SUSY simplified models yielding the desired final states. A single control region is used to constrain the normalisation of the WZ + jets background. No significant excess of events over the Standard Model expectation is observed. The results are interpreted in the context of several supersymmetric models featuring R-parity conservation or R-parity violation, yielding exclusion limits surpassing those from previous searches. In models considering gluino (squark) pair production, gluino (squark) masses up to 2.2 (1.7) TeV are excluded at 95% confidence level
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- Author
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- Abbott B
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- Abhayasinghe DK
- Abidi SH
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
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- Zhemchugov A
- Zheng J
- Zheng K
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- Zhong D
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- Zimine NI
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- Zoccoli A
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- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
Measurement of the energy asymmetry in t(t)over-barj production at 13 TeV with the ATLAS experiment and interpretation in the SMEFT framework
- Author
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- Zhang Z
- Zhao P
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 28/04/2022
- Field of study
A measurement of the energy asymmetry in jet-associated top-quark pair production is presented using 139fb−1
139
fb
-
1
of data collected by the ATLAS detector at the Large Hadron Collider during pp collisions at s=13TeV
s
=
13
TeV
. The observable measures the different probability of top and antitop quarks to have the higher energy as a function of the jet scattering angle with respect to the beam axis. The energy asymmetry is measured in the semileptonic ttˉ
t
t
¯
decay channel, and the hadronically decaying top quark must have transverse momentum above 350GeV
350
GeV
. The results are corrected for detector effects to particle level in three bins of the scattering angle of the associated jet. The measurement agrees with the SM prediction at next-to-leading-order accuracy in quantum chromodynamics in all three bins. In the bin with the largest expected asymmetry, where the jet is emitted perpendicular to the beam, the energy asymmetry is measured to be −0.043±0.020
-
0.043
±
0.020
, in agreement with the SM prediction of −0.037±0.003
-
0.037
±
0.003
. Interpreting this result in the framework of the Standard Model effective field theory (SMEFT), it is shown that the energy asymmetry is sensitive to the top-quark chirality in four-quark operators and is therefore a valuable new observable in global SMEFT fits
Determination of the parton distribution functions of the proton using diverse ATLAS data from pp collisions at √s = 7, 8 and 13 TeV
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- Zoccoli A
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
This paper presents an analysis at next-to-next-to-leading order in the theory of quantum chromodynamics for the determination of a new set of proton parton distribution functions using diverse measurements in pp collisions at \sqrt{s} = 7, 8 and 13 TeV, performed by the ATLAS experiment at the Large Hadron Collider, together with deep inelastic scattering data from ep collisions at the HERA collider. The ATLAS data sets considered are differential cross-section measurements of inclusive W^{±} and Z/gamma^{*} boson production, W^{±} and Z boson production in association with jets, t\bar{t} production, inclusive jet production and direct photon production. In the analysis, particular attention is paid to the correlation of systematic uncertainties within and between the various ATLAS data sets and to the impact of model, theoretical and parameterisation uncertainties. The resulting set of parton distribution functions is called ATLASpdf21
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