484 research outputs found
No imminent quantum supremacy by boson sampling
- Author
- A Arkhipov
- A Crespi
- A Politi
- AE Lita
- AI Barvinok
- Alex Neville
- Anthony Laing
- AP Lund
- Ashley Montanaro
- C Gerry
- Chris Sparrow
- DW Berry
- Eric Johnston
- H Wang
- HJ Ryser
- J Carolan
- J Carolan
- J Huh
- J Liu
- JB Spring
- JB Spring
- JC Loredo
- JT Praestgaard
- KR Motes
- L Latmiral
- M Bentivegna
- M Bentivegna
- M Pant
- M Tillmann
- MA Broome
- MJ Bremner
- N Somaschi
- N Spagnolo
- NC Harris
- NJ Russell
- Patrick M. Birchall
- PW Shor
- RA Horn
- Raphaël Clifford
- RH Hadfield
- S Aaronson
- S Aaronson
- S Aaronson
- S Rahimi-Keshari
- WR Clements
- X Ding
- Y He
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/05/2017
- Field of study
It is predicted that quantum computers will dramatically outperform their
conventional counterparts. However, large-scale universal quantum computers are
yet to be built. Boson sampling is a rudimentary quantum algorithm tailored to
the platform of photons in linear optics, which has sparked interest as a rapid
way to demonstrate this quantum supremacy. Photon statistics are governed by
intractable matrix functions known as permanents, which suggests that sampling
from the distribution obtained by injecting photons into a linear-optical
network could be solved more quickly by a photonic experiment than by a
classical computer. The contrast between the apparently awesome challenge faced
by any classical sampling algorithm and the apparently near-term experimental
resources required for a large boson sampling experiment has raised
expectations that quantum supremacy by boson sampling is on the horizon. Here
we present classical boson sampling algorithms and theoretical analyses of
prospects for scaling boson sampling experiments, showing that near-term
quantum supremacy via boson sampling is unlikely. While the largest boson
sampling experiments reported so far are with 5 photons, our classical
algorithm, based on Metropolised independence sampling (MIS), allowed the boson
sampling problem to be solved for 30 photons with standard computing hardware.
We argue that the impact of experimental photon losses means that demonstrating
quantum supremacy by boson sampling would require a step change in technology.Comment: 25 pages, 9 figures. Comments welcom
Role of anesthesiology curriculum in improving bag-mask ventilation and intubation success rates of emergency medicine residents: a prospective descriptive study
- Author
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>Rapid and safe airway management has always been of paramount importance in successful management of critically ill and injured patients in the emergency department. The purpose of our study was to determine success rates of bag-mask ventilation and tracheal intubation performed by emergency medicine residents before and after completing their anesthesiology curriculum.</p> <p>Methods</p> <p>A prospective descriptive study was conducted at Nikoukari Hospital, a teaching hospital located in Tabriz, Iran. In a skills lab, a total number of 18 emergency medicine residents (post graduate year 1) were given traditional intubation and bag-mask ventilation instructions in a 36 hour course combined with mannequin practice. Later the residents were given the opportunity of receiving training on airway management in an operating room for a period of one month which was considered as an additional training program added to their Anesthesiology Curriculum. Residents were asked to ventilate and intubate 18 patients (Mallampati class I and ASA class I and II) in the operating room; both before and after completing this additional training program. Intubation achieved at first attempt within 20 seconds was considered successful. Successful bag-mask ventilation was defined as increase in ETCo<sub>2 </sub>to 20 mm Hg and back to baseline with a 3 L/min fresh gas-flow and the adjustable pressure limiting valve at 20 cm H<sub>2</sub>O. An attending anesthesiologist who was always present in the operating room during the induction of anesthesia confirmed the endotracheal intubation by direct laryngoscopy and capnography. Success rates were recorded and compared using McNemar, marginal homogeneity and paired t-Test tests in SPSS 15 software.</p> <p>Results</p> <p>Before the additional training program in the operating room, the participants had intubation and bag-mask ventilation success rates of 27.7% (CI 0.07-0.49) and 16.6% (CI 0-0.34) respectively. After the additional training program in the operating room the success rates increased to 83.3% (CI 0.66-1) and 88.8% (CI 0.73-1), respectively. The differences in success rates were statistically significant (P = 0.002 and P = 0.0004, respectively).</p> <p>Conclusions</p> <p>The success rate of emergency medicine residents in airway management improved significantly after completing anesthesiology rotation. Anesthesiology rotations should be considered as an essential component of emergency medicine training programs. A collateral curriculum of this nature should also focus on the acquisition of skills in airway management.</p
Stretchable Dual-Capacitor Multi-Sensor for Touch-Curvature-Pressure-Strain Sensing
- Author
- A Larmagnac
- A Morteza
- A Pantelopoulos
- A Saudabayev
- AC Myers
- B Alizadeh-Taheri
- C Harland
- D Son
- DJ Lipomi
- DP Cotton
- E Roh
- G Schwartz
- J Gubbi
- J Lee
- K Suzuki
- L Atzori
- L Gatzoulis
- M Amjadi
- M Lopez-Gordo
- N Lu
- P Salvo
- R Paradiso
- R Rahimi
- RA Potyrailo
- S Luo
- S Pandey
- S Ryu
- S Yao
- SC Mannsfeld
- T Kim
- T Yamada
- W Chen
- W Hu
- WD Hairston
- X Wu
- X Zhao
- X-F Teng
- Y Cheng
- Y-S Yu
- YR Jeong
- Z Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/09/2017
- Field of study
We introduce a new type of multi-functional capacitive sensor that can sense several different external stimuli. It is fabricated only with polydimethylsiloxane (PDMS) films and silver nanowire electrodes by using selective oxygen plasma treatment method without photolithography and etching processes. Differently from the conventional single-capacitor multi-functional sensors, our new multifunctional sensor is composed of two vertically-stacked capacitors (dual-capacitor). The unique dual-capacitor structure can detect the type and strength of external stimuli including curvature, pressure, strain, and touch with clear distinction, and it can also detect the surface-normal directionality of curvature, pressure, and touch. Meanwhile, the conventional single-capacitor sensor has ambiguity in distinguishing curvature and pressure and it can detect only the strength of external stimulus. The type, directionality, and strength of external stimulus can be determined based on the relative capacitance changes of the two stacked capacitors. Additionally, the logical flow reflected on a tree structure with its branches reaching the direction and strength of the corresponding external stimulus unambiguously is devised. This logical flow can be readily implemented in the sensor driving circuit if the dual-capacitor sensor is commercialized actually in the future
Global, regional, and national comparative risk assessment of 79 behavioural, environmental and occupational, and metabolic risks or clusters of risks, 1990-2015: a systematic analysis for the Global Burden of Disease Study 2015
- Author
- Aasvang GM
- Abajobir AA
- Abate KH
- Abbafati C
- Abbas KM
- Abd-Allah F
- Abdulle AM
- Abera SF
- Abraham B
- Abu-Raddad LJ
- Abyu GY
- Adebiyi AO
- Adedeji IA
- Ademi Z
- Adou AK
- Adsuar JC
- Afshin A
- Agardh EE
- Agarwal A
- Agrawal A
- Ajala ON
- Akinyemiju TF
- Al-Aly Z
- Alam K
- Alam NKM
- Aldhahri SF
- Aldridge RW
- Alemu ZA
- Alexander LT
- Ali R
- Alkerwi A
- Alla F
- Allebeck P
- Alsharif U
- Altirkawi KA
- Alvarez Martin E
- Alves Silveira DG
- Alvis-Guzman N
- Amare AT
- Amberbir A
- Amegah AK
- Amini H
- Ammar W
- Amrock SM
- Andersen HH
- Anderson BO
- Anderson HR
- Antonio CAT
- Anwar P
- Aquino Faraon EJ
- Arnlov J
- Artaman A
- Asayesh H
- Asghar RJ
- Assadi R
- Atique S
- Avokpaho EFGA
- Awasthi A
- Azzopardi P
- Bacha U
- Badawi A
- Baernighausen T
- Bahit MC
- Balakrishnan K
- Bans C
- Barac A
- Barber RM
- Barker-Collo SL
- Barquera S
- Barregard L
- Barrero LH
- Basu S
- Bazargan-Hejazi S
- Beardsley J
- Beatriz Heredia-Pi I
- Beatriz Lawrynowicz AE
- Bedi N
- Beghi E
- Bell ML
- Bello AK
- Bennett DA
- Bensenor IM
- Berhane A
- Bernabe E
- Betsu BD
- Beyene AS
- Bhala N
- Bhansali A
- Bhatt S
- Bhutta ZA
- Biadgilign S
- Bicer BK
- Bikbov B
- Biryukov S
- Bisanzio D
- Bjertness E
- Blore JD
- Borschmann R
- Boufous S
- Bourne RRA
- Brainin M
- Brauer M
- Brazinova A
- Breitborde NJK
- Brenner H
- Broday DM
- Brugha TS
- Brunekreef B
- Burnett R
- Butt ZA
- Cahill LE
- Caicedo AJP
- Calabria B
- Cardenas R
- Carmen Gomez-Cabrera M
- Carpenter D
- Casey DC
- Castaneda-Oquela CA
- Castillo Rivas J
- Catala-Lopez F
- Cercy K
- Chang J-C
- Charlson FJ
- Chiang PP-C
- Chibalabala M
- Chimed-Ochir O
- Chisumpa VH
- Chitheer AA
- Choi J-YJ
- Christensen H
- Christopher DJ
- Ciobanu LG
- Coates MM
- Cohen AJ
- Colquhoun SM
- Cooper LT
- Cooperrider K
- Cornaby L
- Cortinovis M
- Crump JA
- Cuevas-Nasu L
- Damasceno A
- Dandona L
- Dandona R
- Darby SC
- Dargan PI
- das Neves J
- Davis AC
- Davletov K
- De la Cruz-Gongora V
- De Leo D
- Defo BK
- Degenhardt L
- Del Gobbo LC
- del Pozo-Cruz B
- Dellavalle RP
- Deribew A
- Des Jarlais DC
- Dharmaratne SD
- Dhillon PK
- Diaz-Tome C
- Dicker D
- Dimbuene ZT
- Ding EL
- Dolores Sanchez-Nino M
- Dorsey ER
- Doyle KE
- Driscoll TR
- Duan L
- Dubey M
- Duncan BB
- Elyazar I
- Endries AY
- Ermakov SP
- Erskine HE
- Eshrati B
- Estanislao Castro R
- Esteghamati A
- Estep K
- Factors GBDR
- Fahimi S
- Farid TA
- Faro A
- Farvid MS
- Farzadfar F
- Feigin VL
- Fereshtehnejad S-M
- Fernandes JG
- Ferrari AJ
- Filipa de Castro E
- Fischer F
- Fitchett JRA
- Fleming T
- Foigt N
- Foreman K
- Forouzanfar MH
- Fowkes FGR
- Francisco Hernandez-Llanes N
- Franklin RC
- Frostad JJ
- Fuerst T
- Fullman N
- Futran ND
- Gakidou E
- Garcia-Basteiro AL
- Gebrehiwot TT
- Gebremedhin AT
- Geleijnse JM
- Gessner BD
- Gething PW
- Giref AZ
- Giroud M
- Gishu MD
- Godwin WW
- Goenka S
- Gomez-Dantes H
- Gona P
- Goodridge A
- Gopalani SV
- Gotay CC
- Goto A
- Gouda HN
- Griswold M
- Gugnani HC
- Guillemin F
- Guo Y
- Gupta R
- Gupta R
- Gutierrez RA
- Haagsma JA
- Hafezi-Nejad N
- Haile D
- Hailu GB
- Halasa YA
- Hamadeh RR
- Hamidi S
- Handal AJ
- Hankey GJ
- Hao Y
- Harb HL
- Harikrishnan S
- Hassanvand MS
- Hassen TA
- Havmoeller R
- Heydarpour P
- Hoek HW
- Hoffman HJ
- Horino M
- Horita N
- Hosgood HD
- Hoy DG
- Hsairi M
- Htet AS
- Hu G
- Huang JJ
- Husseini A
- Hutchings SJ
- Huybrechts I
- Iburg KM
- Idrisov BT
- Ileanu BV
- Inoue M
- Jacobs TA
- Jacobsen KH
- Jahanmehr N
- Jakovljevic MB
- Jansen HAFM
- Jassal SK
- Javanbakht M
- Jayatilleke AU
- Jee SH
- Jeemon P
- Jha V
- Jiang Y
- Jibat T
- Jin Y
- Johnson CO
- Jonas JB
- Kabir Z
- Kalkonde Y
- Kamal R
- Kan H
- Karch A
- Karema CK
- Karimkhani C
- Kasaeian A
- Kaul A
- Kawakami N
- Kazi DS
- Keiyoro PN
- Kemp AH
- Kengne AP
- Keren A
- Kesavachandran CN
- Khader YS
- Khan AR
- Khan EA
- Khan G
- Khang Y-H
- Khatibzadeh S
- Khera S
- Khoja TAM
- Khubchandani J
- Kiadaliri AA
- Kieling C
- Kim C-I
- Kim D
- Kimokoti RW
- Kinfu Y
- Kissoon N
- Kivipelto M
- Knibbs LD
- Kokubo Y
- Kopec JA
- Koul PA
- Koyanagi A
- Kravchenko M
- Kromhout H
- Krueger H
- Ku T
- Kuchenbecker RS
- Kuipers EJ
- Kumar GA
- Kwan GF
- Kyu HH
- Lal DK
- Lalloo R
- Lallukka T
- Lan Q
- Landon N
- Larson HJ
- Larsson A
- Latif AA
- Leasher JL
- Leigh J
- Leung J
- Levi M
- Levy TS
- Li X
- Li Y
- Liang J
- Liang X
- Lim SS
- Liu PY
- Liu S
- Lloyd BK
- Logroscino G
- Lopez AD
- Lotufo PA
- Lozano R
- Lunevicius R
- Maclntyre M
- Mahdavi M
- Mahesh PA
- Majdan M
- Majeed A
- Malekzadeh R
- Malta DC
- Manamo WAA
- Mapoma CC
- Marcenes W
- Marczak L
- Maria Haro J
- Martin RV
- Martinez-Raga J
- Masiye F
- Matsushita K
- Matzopoulos R
- Mayosi BM
- McGrath JJ
- McKee M
- Meaney PA
- Medina C
- Mehari A
- Mekonnen AB
- Melaku YA
- Memish ZA
- Mena-Rodriguez F
- Mendoza W
- Mensah GA
- Mensink GBM
- Meretoja A
- Meretoja TJ
- Mesfin YM
- Mhimbira FA
- Miller TR
- Mills EJ
- Mirarefin M
- Misganaw A
- Mock CN
- Mohammadi A
- Mohammed S
- Mokdad AH
- Mola GLD
- Monasta L
- Montanez Hernandez JC
- Montico M
- Moradi-Lakeh M
- Morawska L
- Mori R
- Mozaffarian D
- Mueller UO
- Mullany E
- Mumford JE
- Murray CJL
- Murthy GVS
- Nachega JB
- Naghavi M
- Naheed A
- Nangia V
- Nassiri N
- Neal B
- Newton JN
- Ng M
- Nguyen QL
- Nisar MI
- Norheim OF
- Norman RE
- Norrving B
- Nyakarahuka L
- Obermeyer CM
- Ogbo FA
- Oh I-H
- Oladimeji O
- Olivares PR
- Olsen H
- Olusanya BO
- Olusanya JO
- Opio JN
- Oren E
- Orozco R
- Ortiz A
- Ota E
- Pana A
- Park E-K
- Parry CD
- Parsaeian M
- Patel T
- Patil ST
- Patten SB
- Patton GC
- Pearce N
- Pereira DM
- Perico N
- Pesudovs K
- Pete PMN
- Petzold M
- Phillips MR
- Piel FB
- Pillay JD
- Plass D
- Polinder S
- Pond CD
- Pope CA
- Pope D
- Popova S
- Poulton RG
- Pourmalek F
- Prasad NM
- Qorbani M
- Quintanilla BPA
- Rabiee RHS
- Radfar A
- Rafay A
- Rahimi-Movaghar V
- Rahman M
- Rahman MHU
- Rahman SU
- Rai RK
- Rajsic S
- Raju M
- Ram U
- Rana SM
- Ranganathan K
- Rao P
- Razo Garcia CA
- Refaat AH
- Rehm CD
- Rehm J
- Reinig N
- Reitsma MB
- Remuzzi G
- Resnikoff S
- Ribeiro AL
- Ricardo Campos-Nonato I
- Rivera JA
- Rodriguez A
- Rodriguez-Ramirez S
- Rojas-Rueda D
- Rolm HS
- Roman Y
- Ronfani L
- Roshandel G
- Roth GA
- Rothenbacher D
- Roy A
- Saleh MM
- Salomon JA
- Sanabria JR
- Sanchez-Pimienta TG
- Sandar L
- Santomauro DF
- Santos IS
- Sarmiento-Suarez R
- Sartorius B
- Satpathy M
- Savic M
- Sawhney M
- Schmidhuber J
- Schmidt MI
- Schneider IJC
- Schoettker B
- Schutte AE
- Schwebel DC
- Scott JG
- Seedat S
- Sepanlou SG
- Servan-Mori EE
- Shaheen A
- Shahraz S
- Shaikh MA
- Sharma R
- She J
- Sheikhbahaei S
- Shen J
- Sheth KN
- Shi P
- Shibuya K
- Shigematsu M
- Shin M-J
- Shiri R
- Shishani K
- Shiue I
- Shrime MG
- Sigfusdottir ID
- Silva DAS
- Silverberg JI
- Simard EP
- Sindi S
- Singh A
- Singh JA
- Singh PK
- Slepak EL
- Sofia E Sa Farinha C
- Soljak M
- Soneji S
- Sorensen RJD
- Sposato LA
- Sreeramareddy CT
- Stathopoulou V
- Steckling N
- Steel N
- Stein DJ
- Stein MB
- Stockl H
- Stranges S
- Stroumpoulis K
- Sunguya BF
- Sur PJ
- Swaminathan S
- Sykes BL
- Szoeke CEI
- Tabares-Seisdedos R
- Takahashi K
- Talongwa RT
- Tanne D
- Tavakkoli M
- Taye BW
- Taylor HR
- Tedla BA
- Tefera WM
- Tegegne TK
- Tekle DY
- Terkawi AS
- Thakur JS
- Thomas BA
- Thomas ML
- Thomson AJ
- Thorne-Lyman AL
- Thrift AG
- Thurston GD
- Tillmann T
- Tobe-Gai R
- Tobollik M
- Topor-Madry R
- Topouzis F
- Towbin JA
- Tran BX
- Tsilimparis N
- Tura AK
- Tuzcu EM
- Tyrovolas S
- Ukwaja KN
- Undurraga EA
- Uneke CJ
- Uthman OA
- van Donkelaar A
- van Os J
- Varakin YY
- Vasankari T
- Veerman JL
- Venketasubramanian N
- Violante FS
- Vollset SE
- Vos T
- Wagner GR
- Wagner JA
- Waller SG
- Wang H
- Wang J
- Wang L
- Wang Y
- Weichenthal S
- Weiderpass E
- Weintraub RG
- Werdecker A
- Westerman R
- Whiteford HA
- Wijeratne T
- Wiysonge CS
- Wolfe CDA
- Won S
- Woolf AD
- Wubshet M
- Xavier D
- Xu G
- Yadav AK
- Yakob B
- Yalew AZ
- Yano Y
- Yaseri M
- Ye P
- Yip P
- Yonemoto N
- Yoon S-J
- Younis MZ
- Yu C
- Zaidi Z
- Zaki MES
- Zhao Y
- Zhou M
- Zhu J
- Zipkin B
- Zodpey S
- Zuhlke LJ
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2016
- Field of study
SummaryBackground The Global Burden of Diseases, Injuries, and Risk Factors Study 2015 provides an up-to-date synthesis of the evidence for risk factor exposure and the attributable burden of disease. By providing national and subnational assessments spanning the past 25 years, this study can inform debates on the importance of addressing risks in context. Methods We used the comparative risk assessment framework developed for previous iterations of the Global Burden of Disease Study to estimate attributable deaths, disability-adjusted life-years (DALYs), and trends in exposure by age group, sex, year, and geography for 79 behavioural, environmental and occupational, and metabolic risks or clusters of risks from 1990 to 2015. This study included 388 risk-outcome pairs that met World Cancer Research Fund-defined criteria for convincing or probable evidence. We extracted relative risk and exposure estimates from randomised controlled trials, cohorts, pooled cohorts, household surveys, census data, satellite data, and other sources. We used statistical models to pool data, adjust for bias, and incorporate covariates. We developed a metric that allows comparisons of exposure across risk factors—the summary exposure value. Using the counterfactual scenario of theoretical minimum risk level, we estimated the portion of deaths and DALYs that could be attributed to a given risk. We decomposed trends in attributable burden into contributions from population growth, population age structure, risk exposure, and risk-deleted cause-specific DALY rates. We characterised risk exposure in relation to a Socio-demographic Index (SDI). Findings Between 1990 and 2015, global exposure to unsafe sanitation, household air pollution, childhood underweight, childhood stunting, and smoking each decreased by more than 25%. Global exposure for several occupational risks, high body-mass index (BMI), and drug use increased by more than 25% over the same period. All risks jointly evaluated in 2015 accounted for 57·8% (95% CI 56·6–58·8) of global deaths and 41·2% (39·8–42·8) of DALYs. In 2015, the ten largest contributors to global DALYs among Level 3 risks were high systolic blood pressure (211·8 million [192·7 million to 231·1 million] global DALYs), smoking (148·6 million [134·2 million to 163·1 million]), high fasting plasma glucose (143·1 million [125·1 million to 163·5 million]), high BMI (120·1 million [83·8 million to 158·4 million]), childhood undernutrition (113·3 million [103·9 million to 123·4 million]), ambient particulate matter (103·1 million [90·8 million to 115·1 million]), high total cholesterol (88·7 million [74·6 million to 105·7 million]), household air pollution (85·6 million [66·7 million to 106·1 million]), alcohol use (85·0 million [77·2 million to 93·0 million]), and diets high in sodium (83·0 million [49·3 million to 127·5 million]). From 1990 to 2015, attributable DALYs declined for micronutrient deficiencies, childhood undernutrition, unsafe sanitation and water, and household air pollution; reductions in risk-deleted DALY rates rather than reductions in exposure drove these declines. Rising exposure contributed to notable increases in attributable DALYs from high BMI, high fasting plasma glucose, occupational carcinogens, and drug use. Environmental risks and childhood undernutrition declined steadily with SDI; low physical activity, high BMI, and high fasting plasma glucose increased with SDI. In 119 countries, metabolic risks, such as high BMI and fasting plasma glucose, contributed the most attributable DALYs in 2015. Regionally, smoking still ranked among the leading five risk factors for attributable DALYs in 109 countries; childhood underweight and unsafe sex remained primary drivers of early death and disability in much of sub-Saharan Africa. Interpretation Declines in some key environmental risks have contributed to declines in critical infectious diseases. Some risks appear to be invariant to SDI. Increasing risks, including high BMI, high fasting plasma glucose, drug use, and some occupational exposures, contribute to rising burden from some conditions, but also provide opportunities for intervention. Some highly preventable risks, such as smoking, remain major causes of attributable DALYs, even as exposure is declining. Public policy makers need to pay attention to the risks that are increasingly major contributors to global burden. Funding Bill & Melinda Gates Foundation
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
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- Abdallah J
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- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Khalek SA
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
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- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
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- Adye T
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- Aguilar-Saavedra JA
- Agustoni M
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MS
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- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
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- Aliev M
- Alimonti G
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- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
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- Gonzalez BA
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- Yamamura T
- Yamanaka T
- Yamazaki T
- Yamazaki Y
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- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Smit GVY
- Ye J
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
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- Youssef S
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
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- Zhemchugov A
- Zhong J
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- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fb−1 of s=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan β < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
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- Abajyan T
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- Abdallah J
- Abdelalim AA
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- Yilmaz M
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- Youssef S
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- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
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- Zenin O
- Zenis T
- Zerwas D
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- Zhemchugov A
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 23/11/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Z′ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fb−1 in the e + e − channel and 5.0 fb−1 in the μ + μ −channel. A Z ′ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal Z′ Models
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