355 research outputs found
Fluorescence characterization of clinically-important bacteria
- Author
- B Hua
- C Estes
- D Patra
- DA Veal
- DC Shelly
- DC Shelly
- DJ Weber
- ET Smyth
- FA Manian
- Ginny Moore
- GM Palmer
- GV Chapman
- H Bhatta
- H Giana
- I Georgakoudi
- I Vermes
- J Alberts
- James P Brody
- Jan-Peter Muller
- JL Nadeau
- John M. Ward
- K Muirhead
- L Campbell
- L Leblanc
- L McNamara
- Lewis R. Dartnell
- LR Dartnell
- LR Dartnell
- LR Dartnell
- M Sohn
- M Ziegmann
- MC Layton
- MC Storrie-Lombardi
- MK Hayden
- MS Ammor
- P Cornelis
- P Diagaradjane
- PB Oldbam
- PW Stone
- QQ Zhang
- R Bhartia
- R JiJi
- R Rosenstein
- RA Rohde
- RJ Pratt
- RM Cory
- S Ammor
- S Elliott
- S Engelhart
- S Weinstein
- Tom A. Roberts
- YL Pan
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2013
- Field of study
Healthcare-associated infections (HCAI/HAI) represent a substantial threat to patient health during hospitalization and incur billions of dollars additional cost for subsequent treatment. One promising method for the detection of bacterial contamination in a clinical setting before an HAI outbreak occurs is to exploit native fluorescence of cellular molecules for a hand-held, rapid-sweep surveillance instrument. Previous studies have shown fluorescence-based detection to be sensitive and effective for food-borne and environmental microorganisms, and even to be able to distinguish between cell types, but this powerful technique has not yet been deployed on the macroscale for the primary surveillance of contamination in healthcare facilities to prevent HAI. Here we report experimental data for the specification and design of such a fluorescence-based detection instrument. We have characterized the complete fluorescence response of eleven clinically-relevant bacteria by generating excitation-emission matrices (EEMs) over broad wavelength ranges. Furthermore, a number of surfaces and items of equipment commonly present on a ward, and potentially responsible for pathogen transfer, have been analyzed for potential issues of background fluorescence masking the signal from contaminant bacteria. These include bedside handrails, nurse call button, blood pressure cuff and ward computer keyboard, as well as disinfectant cleaning products and microfiber cloth. All examined bacterial strains exhibited a distinctive double-peak fluorescence feature associated with tryptophan with no other cellular fluorophore detected. Thus, this fluorescence survey found that an emission peak of 340nm, from an excitation source at 280nm, was the cellular fluorescence signal to target for detection of bacterial contamination. The majority of materials analysed offer a spectral window through which bacterial contamination could indeed be detected. A few instances were found of potential problems of background fluorescence masking that of bacteria, but in the case of the microfiber cleaning cloth, imaging techniques could morphologically distinguish between stray strands and bacterial contamination
Ethnobotany in the Nepal Himalaya
- Author
- A Gomez-Beloz
- A Lewington
- A Storrs
- AC Hamilton
- B Heine
- BD Pandey
- BK Bishokarma
- BM Boom
- C Burlakoti
- C Jest
- C Körner
- C Stockwell
- CP Kala
- CP Kala
- CP Kala
- CP Kala
- CP Kala
- CS Olsen
- CS Olsen
- CS Silori
- CS Weckerle
- D Don
- DD Bhatt
- DD Dani
- DM Edwards
- DM Warren
- EW Davis
- GL Shrestha
- GN Njoroge
- Government of Nepal
- H Hara
- HG Wilkes
- IL Singha
- IUCN Nepal
- J Lambert
- J Lietava
- J Sacherer
- J Salick
- J Salick
- JD Farnsworth
- JF Dobremej
- JF Dobremez
- JI Cohen
- JS Singh
- K Niraula
- KK Shrestha
- KK Shrestha
- KR Bhattarai
- KR Bhattarai
- KR Rajbhandari
- KR Rajbhandari
- LN Mandar
- LR Bhatta
- M Gadgil
- M Johnston
- M Kappelle
- M Karki
- M Mikage
- MJ Balick
- ML Banerji
- ML Banerji
- MP Shiva
- MS Ali Shtayeh
- N Hanazaki
- N Wallich
- NK Bhattarai
- NK Bhattarai
- NK Bhattarai
- NK Bhattarai
- NK Bhattarai
- NK Bhattarai
- NK Bhattarai
- NN Tiwari
- NP Manandhar
- NP Manandhar
- NR Farnsworth
- NRC
- O Philips
- P Hall
- P Pohle
- P Shengji
- P Shengji
- P Shengji
- P Shengji
- P Shengji
- PM Adhikari
- PM Shrestha
- PP Sharma
- Rainer W Bussmann
- RD Girach
- RE Schultes
- Ripu M Kunwar
- RK Colwell
- RL Ford
- RM Kunwar
- RM Kunwar
- RM Kunwar
- RM Kunwar
- RM Kunwar
- RM Kunwar
- RM Kunwar
- RM Kunwar
- RP Chaudhary
- RW Bussmann
- RW Bussmann
- S Sherpa
- SB Malla
- SC Singh
- SK Ghimire
- SK Ghimire
- SK Ghimire
- SK Ghimire
- SK Kapur
- SK Uniyal
- SR Baral
- SS Samant
- T Iwashina
- T Ticktin
- TB Henfrey
- U Dhar
- U Schippmann
- VPK Nambier
- ZK Shinwari
- ZK Shinwari
- Publication venue
- BioMed Central
- Publication date
- 01/01/2008
- Field of study
<p>Abstract</p> <p>Background</p> <p>Indigenous knowledge has become recognized worldwide not only because of its intrinsic value but also because it has a potential instrumental value to science and conservation. In Nepal, the indigenous knowledge of useful and medicinal plants has roots in the remote past.</p> <p>Methods</p> <p>The present study reviews the indigenous knowledge and use of plant resources of the Nepal Himalayas along the altitudinal and longitudinal gradient. A total of 264 studies focusing on ethnobotany, ethnomedicine and diversity of medicinal and aromatic plants, carried out between 1979 and 2006 were consulted for the present analysis. In order to cross check and verify the data, seven districts of west Nepal were visited in four field campaigns.</p> <p>Results</p> <p>In contrast to an average of 21â28% ethnobotanically/ethnomedicinally important plants reported for Nepal, the present study found that up to about 55% of the flora of the study region had medicinal value. This indicates a vast amount of undocumented knowledge about important plant species that needs to be explored and documented. The richness of medicinal plants decreased with increasing altitude but the percentage of plants used as medicine steadily increased with increasing altitude. This was due to preferences given to herbal remedies in high altitude areas and a combination of having no alternative choices, poverty and trust in the effectiveness of folklore herbal remedies.</p> <p>Conclusion</p> <p>Indigenous knowledge systems are culturally valued and scientifically important. Strengthening the wise use and conservation of indigenous knowledge of useful plants may benefit and improve the living standard of poor people.</p
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
- 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 GuimarĂŁes 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
- BjĂžrke 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
- BrĂŒers 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
- BĂŒscher V
- Cabrera UrbĂĄn 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
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- 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
- CarrĂĄ 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
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- 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
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- 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
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- 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
- DellâAcqua A
- DellâAsta 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
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- Dona KM
- Donadelli M
- Dong B
- Donini J
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- Dougan P
- Dova MT
- Doyle AT
- Draguet MA
- Dreyer E
- Drivas-koulouris I
- Drobac AS
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- Duchovni E
- Duckeck G
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- Duden ER
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- 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
- DĂez Cornell S
- DĂŒhrssen M
- DĂŒlsen C
- DĂŒren M
- Dâamen G
- DâAmico V
- DâAuria S
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- DâOnofrio A
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- Earnshaw ZO
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- Eggebrecht S
- Egidio Purcino De Souza E
- Ehrke LF
- Eigen G
- Einsweiler K
- Ekelof T
- Ekman PA
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- Elmsheuser J
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- Erdmann J
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- Evans MO
- Ezhilov A
- Ezzarqtouni S
- Fabbri F
- Fabbri L
- Facini G
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- Fakhrutdinov RM
- Falciano S
- Falda Ulhoa Coelho LF
- Falke PJ
- Faltova J
- Fan C
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- Faraj M
- Farazpay Z
- Farbin A
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- Farooque T
- Farrington SM
- Fassi F
- Fassouliotis D
- Faucci Giannelli M
- Fawcett WJ
- Fayard L
- Federic P
- Federicova P
- Fedin OL
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- Fellers DE
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- Ferrere D
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- Fiedler F
- FilipÄiÄ 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
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- 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
- GarcĂa Navarro JE
- GarcĂa C
- Gardner GL
- Gardner RW
- Garelli N
- Garg D
- Garg RB
- Gargan JM
- Garner CA
- Gasiorowski SJ
- Gaspar P
- Gaudio G
- Gautam V
- Gauzzi P
- Gavrilenko IL
- Gavrilyuk A
- Gay C
- Gaycken G
- Gazis EN
- Geanta AA
- Gee CM
- Gemme C
- Genest MH
- Gentile S
- Gentry AD
- George S
- George WF
- Geralis T
- Gessinger-Befurt P
- Geyik ME
- Ghani M
- Ghneimat M
- Ghorbanian K
- Ghosal A
- Ghosh A
- Ghosh A
- Giacobbe B
- Giagu S
- Giani T
- Giannetti P
- Giannini A
- Gibson SM
- Gignac M
- Gil DT
- Gilbert AK
- Gilbert BJ
- Gillberg D
- Gilles G
- Gillwald NEK
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- Zhemchugov A
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- Zimine NI
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- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ 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 fbâ1 of proton-proton collision data recorded at a centre-of-mass energy of âs = 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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- Abusleme Hoffman AC
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- Zhemchugov A
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- Zhulanov V
- Zimine NI
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- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ 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 fbâ1 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
Measurement of the ttÂŻttÂŻ production cross section in pp collisions at âs=13 TeV with the ATLAS detector
- Author
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- Zhemchugov A
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
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- Zoccoli A
- Zoch K
- Zorbas TG
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- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- Field of study
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fbâ1 is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain b-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26+17â15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24+7â6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 ± 2.4 fb
Software Performance of the ATLAS Track Reconstruction for LHC Run 3
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- Zagazeta LF Gutierrez
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- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
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- Zhong D
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- Zhulanov V
- Zimine NI
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- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 02/04/2024
- Field of study
Charged particle reconstruction in the presence
of many simultaneous protonâproton (pp) collisions in the
LHC is a challenging task for the ATLAS experimentâs reconstruction software due to the combinatorial complexity. This
paper describes the major changes made to adapt the software
to reconstruct high-activity collisions with an average of 50 or
more simultaneous pp interactions per bunch crossing (pileup) promptly using the available computing resources. The
performance of the key components of the track reconstruction chain and its dependence on pile-up are evaluated, and
the improvement achieved compared to the previous software
version is quantified. For events with an average of 60 pp collisions per bunch crossing, the updated track reconstruction
is twice as fast as the previous version, without significant
reduction in reconstruction efficiency and while reducing the
rate of combinatorial fake tracks by more than a factor two
Performance and calibration of quark/gluon-jet taggers using 140 fbâ»Âč of pp collisions at âs=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
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- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/02/2024
- Field of study
The identification of jets originating from quarks and gluons, often referred to as quark/gluon tagging,
plays an important role in various analyses performed at the Large Hadron Collider, as Standard Model measurements and searches for new particles decaying to quarks often rely on suppressing a large gluon-induced background. This paper describes the measurement of the efficiencies of quark/gluon taggers developed within the ATLAS Collaboration, using âs=13 TeV protonâproton collision data with an integrated luminosity of 140 fb-1 collected by the ATLAS experiment. Two taggers with high performances in rejecting jets from gluon over jets from
quarks are studied: one tagger is based on requirements on the number of inner-detector tracks associated with the
jet, and the other combines several jet substructure observables using a boosted decision tree. A method is established to determine the quark/gluon fraction in data, by using quark/gluon-enriched subsamples defined by the jet
pseudorapidity. Differences in tagging efficiency between data and simulation are provided for jets with transverse
momentum between 500 GeV and 2 TeV and for multiple tagger working points
Combination of searches for heavy spin-1 resonances using 139 fbâ1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Aakvaag E
- Abbott B
- Abeling K
- Abicht NJ
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- Zaid E
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- Zakharchuk N
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- Zenger DT
- Zenin O
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- Zerwas D
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- Zhao T
- Zhao Y
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- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
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- Zhu CG
- Zhu J
- Zhu Y
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- Zhuang X
- Zhukov K
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
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- Zou W
- Zwalinski L
- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ 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 fbâ1 of proton-proton collisions at
= 13 TeV collected during 2015â2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (ÏÎœ and ÏÏ) 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
Measurements of sensor radiation damage in the ATLAS inner detector using leakage currents
- Author
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- Zhemchugov A
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- Zorbas TG
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- Zwalinski L
- Publication venue
- IOP
- Publication date
- 01/01/2021
- Field of study
Non-ionizing energy loss causes bulk damage to the silicon sensors of the ATLAS pixel and strip detectors. This damage has important implications for data-taking operations, charged-particle track reconstruction, detector simulations, and physics analysis. This paper presents simulations and measurements of the leakage current in the ATLAS pixel detector and semiconductor tracker as a function of location in the detector and time, using data collected in Run 1 (2010â2012) and Run 2 (2015â2018) of the Large Hadron Collider. The extracted fluence shows a much stronger |z|-dependence in the innermost layers than is seen in simulation. Furthermore, the overall fluence on the second innermost layer is significantly higher than in simulation, with better agreement in layers at higher radii. These measurements are important for validating the simulation models and can be used in part to justify safety factors for future detector designs and interventions.publishedVersio
Measurements of W+Wâ+ â„ 1 jet production cross-sections in pp collisions at sâ = 13 TeV with the ATLAS detector
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- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Fiducial and differential cross-section measurements of W+Wâ production in
association with at least one hadronic jet are presented. These measurements are sensitive
to the properties of electroweak-boson self-interactions and provide a test of perturbative
quantum chromodynamics and the electroweak theory. The analysis is performed using
proton-proton collision data collected at p
s = 13TeV with the ATLAS experiment, corresponding
to an integrated luminosity of 139 fbâ1. Events are selected with exactly one oppositely
charged electron-muon pair and at least one hadronic jet with a transverse momentum
of pT > 30 GeV and a pseudorapidity of |ïżœ| < 4.5. After subtracting the background
contributions and correcting for detector effects, the jet-inclusive W+Wâ+ ïżœ 1 jet fiducial
cross-section and W+Wâ+ jets differential cross-sections with respect to several kinematic
variables are measured. These measurements include leptonic quantities, such as the lepton
transverse momenta and the transverse mass of the W+Wâ system, as well as jet-related
observables such as the leading jet transverse momentum and the jet multiplicity. Limits on
anomalous triple-gauge-boson couplings are obtained in a phase space where interference
between the Standard Model amplitude and the anomalous amplitude is enhanced
- âŠ