462 research outputs found
Born's rule from measurements of classical signals by threshold detectors which are properly calibrated
- Author
- Publication venue
- 'Informa UK Limited'
- Publication date
- 20/07/2011
- Field of study
The very old problem of the statistical content of quantum mechanics (QM) is
studied in a novel framework. The Born's rule (one of the basic postulates of
QM) is derived from theory of classical random signals. We present a
measurement scheme which transforms continuous signals into discrete clicks and
reproduces the Born's rule. This is the sheme of threshold type detection.
Calibration of detectors plays a crucial role.Comment: The problem of double clicks is resolved; hence, one can proceed in
purely wave framework, i.e., the wave-partcile duality has been resolved in
favor of the wave picture of prequantum realit
Strain-induced Evolution of Electronic Band Structures in a Twisted Graphene Bilayer
- Author
- A Altland
- A Isacsson
- A Luican
- AF Young
- AH Castro Neto
- AS Mayorov
- B Nanda
- B Verberck
- B Wang
- C-H Park
- C-H Park
- D Guo
- DL Miller
- E Cerda
- E Cerda
- E Cerda
- E Marinani
- E McCann
- E-A Kim
- EY Andrei
- F de Juan
- F de Juan
- F Guinea
- F Guinea
- F Guinea
- F Guinea
- G Li
- G Semenoff
- GM Rutter
- H Yan
- H Yan
- I Brihuega
- J Hicks
- JMB Lopes dos Santos
- K Kim
- KK Gomes
- KS Novoselov
- L Meng
- L Meng
- M Killi
- M Mucha-Kruczyński
- M Sicot
- M Sicot
- M Yankowitz
- MAH Vozmediano
- N Levy
- P Ghaemi
- P San-Jose
- SM Choi
- T Gao
- T Ohta
- VH Pereira
- VM Pereira
- W Yan
- Y Zhang
- Z Li
- Z-D Chu
- ZF Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 14/03/2013
- Field of study
Here we study the evolution of local electronic properties of a twisted
graphene bilayer induced by a strain and a high curvature. The strain and
curvature strongly affect the local band structures of the twisted graphene
bilayer; the energy difference of the two low-energy van Hove singularities
decreases with increasing the lattice deformations and the states condensed
into well-defined pseudo-Landau levels, which mimic the quantization of massive
Dirac fermions in a magnetic field of about 100 T, along a graphene wrinkle.
The joint effect of strain and out-of-plane distortion in the graphene wrinkle
also results in a valley polarization with a significant gap, i.e., the
eight-fold degenerate Landau level at the charge neutrality point is splitted
into two four-fold degenerate quartets polarized on each layer. These results
suggest that strained graphene bilayer could be an ideal platform to realize
the high-temperature zero-field quantum valley Hall effect.Comment: 4 figure
Ultrastructural analysis and residual DNA evaluation of rabbit vein scaffold
- Author
- Ana Lívia de Carvalho Bovolato
- Andrei Moroz
- Bertanha M
- Bertanha M
- Crapo PM
- Elenice Deffune
- Gilbert TW
- Jaqueline de Carvalho Rinaldi
- Leonardo Nazario de Moraes
- Macchiarini P
- Marcone Lima Sobreira
- Matheus Bertanha
- Matsumura G
- Naderi H
- Nemeno-Guanzon JG
- Niu G
- Norgren L
- Olausson M
- Patricia Pintor Reis
- Patruno M
- Robinson DG
- Schaner PJ
- Schneider CA
- Seifu DG
- Song Y
- Writing GM
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Effective Rheology of Bubbles Moving in a Capillary Tube
- Author
- Abelev B
- Adam J
- Adamova D
- Adare AM
- Aggarwal MM
- Agocs AG
- Agostinelli A
- Ahammed Z
- Ahmad N
- Ahn SU
- Akindinov A
- Alaniz EC
- Aleksandrov D
- Alessandro B
- Alici A
- Alkin A
- Alme J
- Alt T
- Altini V
- Altinpinar S
- Altsybeev I
- Andrei C
- Andronic A
- Anguelov V
- Anielski J
- Anson C
- Anticic T
- Antinori F
- Antonioli P
- Aphecetche L
- Appelshauser H
- Arbor N
- Arcelli S
- Arend A
- Armesto N
- Arnaldi R
- Aronsson T
- Arsene IC
- Arslandok M
- Asryan A
- Augustinus A
- Averbeck R
- Avina EA
- Awes TC
- Aysto J
- Azmi MD
- Bach M
- Badala A
- Baek YW
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
- Baldisseri A
- Baldit A
- Ban J
- Baral RC
- Barbera R
- Bari DD
- Barile F
- Barnafoldi GG
- Barnby LS
- Barret V
- Barros GOVD
- Barroso VC
- Bartke J
- Basile M
- Bastid N
- Bathen B
- Batigne G
- Batyunya B
- Baumann C
- Bearden IG
- Beck H
- Belikov I
- Bellini F
- Bellwied R
- Belmont-Moreno E
- Bencedi G
- Beole S
- Berceanu I
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bergmann C
- Berzano D
- Betev L
- Bhasin A
- Bhati AK
- Bianchi L
- Bianchi N
- Bianchin C
- Bielcik J
- Bielcikova J
- Bjelogrlic S
- Blanco F
- Blanco F
- Blau D
- Blume C
- Boccioli M
- Bock N
- Bogdanov A
- Boggild H
- Bogolyubsky M
- Boldizsar L
- Bombara M
- Book J
- Borel H
- Borissov A
- Bornec YL
- Bose S
- Bossu F
- Botje M
- Bottger S
- Boyer B
- Braidot E
- Braun-Munzinger P
- Bregant M
- Breitner T
- Browning TA
- Broz M
- Brun R
- Bruna E
- Bruno GE
- Budnikov D
- Buesching H
- Bufalino S
- Bugaiev K
- Busch O
- Bustamante RTJ
- Buthelezi Z
- Caffarri D
- Cahuantzi MR
- Cai X
- Caines H
- Camerini P
- Carena F
- Carena W
- Carminati F
- Caro AD
- Castellanos JC
- Castro XS
- Casula EAR
- Cataldo GD
- Catanescu V
- Cavicchioli C
- Cepila J
- Cerello P
- Cervantes IM
- Chang B
- Chapeland S
- Charvet JL
- Chattopadhyay S
- Chattopadhyay S
- Chawla I
- Cherney M
- Cheshkov C
- Cheynis B
- Chiavassa E
- Chinellato DD
- Chochula P
- Chojnacki M
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Chung SU
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Coccetti F
- Colamaria F
- Colella D
- Collaboration ALICE
- Constantin P
- Contin G
- Contreras JG
- Corchero MAD
- Cormier TM
- Corral GH
- Cortese P
- Cosentino MR
- Costa F
- Cotallo ME
- Crescio E
- Crochet P
- Cuautle E
- Cunqueiro L
- Cuveland JD
- Dainese A
- Dalsgaard HH
- Danu A
- Das D
- Das I
- Das K
- Dash A
- Dash S
- Davalos AM
- De S
- Delagrange H
- Deloff A
- Demanov V
- Denes E
- Deppman A
- Diaz AC
- Dietel T
- Divia R
- Djuvsland O
- Dobrin A
- Dobrowolski T
- Dominguez I
- Don CKK
- Donigus B
- Dordic O
- Driga O
- Dubey AK
- Ducroux L
- Dupieux P
- Elia D
- Emschermann D
- Engel H
- Erasmo GD
- Erdal HA
- Espagnon B
- Estienne M
- Esumi S
- Evans D
- Eyyubova G
- Fabris D
- Faivre J
- Falchieri D
- Falco AD
- Fantoni A
- Fasel M
- Fearick R
- Fedunov A
- Fehlker D
- Feldkamp L
- Felea D
- Feofilov G
- Ferreiro EG
- Ferretti A
- Ferretti R
- Ferroli RB
- Figiel J
- Figueredo MAS
- Filchagin S
- Filho EPDO
- Filho NC
- Finogeev D
- Fionda FM
- Fiore EM
- Floris M
- Foertsch S
- Foka P
- Fokin S
- Fragiacomo E
- Fragkiadakis M
- Frankenfeld U
- Fuchs U
- Furget C
- Gaardhoje JJ
- Gagliardi M
- Gago A
- Gallio M
- Gangadharan DR
- Ganoti P
- Garabatos C
- Garcia GM
- Garcia-Solis E
- Garishvili I
- Gerhard J
- Germain M
- Geuna C
- Gheata A
- Gheata M
- Ghidini B
- Ghosh P
- Gianotti P
- Giglio CD
- Girard MF
- Girard MR
- Giubellino P
- Gladysz-Dziadus E
- Glassel P
- Godoy DAMD
- Gomez R
- Gonzalez-Trueba LH
- Gonzalez-Zamora P
- Gorbunov S
- Goswami A
- Gotovac S
- Grabski V
- Graczykowski LK
- Grajcarek R
- Grelli A
- Grigoras A
- Grigoras C
- Grigoriev V
- Grigoryan A
- Grigoryan S
- Grinyov B
- Grion N
- Gros P
- Grosse-Oetringhaus JF
- Grossiord JY
- Grosso R
- Gruttola DD
- Guber F
- Guernane R
- Guerzoni B
- Guevara PLD
- Guilbaud M
- Gulbrandsen K
- Gunji T
- Gupta A
- Gupta R
- Gutbrod H
- Gutierrez CG
- Haaland O
- Hadjidakis C
- Haiduc M
- Haller BV
- Hamagaki H
- Hamar G
- Han BH
- Hanratty LD
- Hansen A
- Harmanova Z
- Harris JW
- Hartig M
- Hasegan D
- Hatzifotiadou D
- Hayrapetyan A
- Heckel ST
- Heide M
- Helstrup H
- Herghelegiu A
- Hernandez JFC
- Herrmann N
- Hetland KF
- Hicks B
- Hille PT
- Hippolyte B
- Horaguchi T
- Hori Y
- Hristov P
- Hrivnacova I
- Huang M
- Huber S
- Humanic TJ
- Hwang DS
- Ichou R
- Ilkaev R
- Ilkiv I
- Inaba M
- Incani E
- Innocenti GM
- Innocenti PG
- Ippolitov M
- Irfan M
- Ivan C
- Ivanov A
- Ivanov M
- Ivanov V
- Ivanytskyi O
- Jacholkowski A
- Jacobs PM
- Jancurova L
- Jang HJ
- Jangal S
- Janik MA
- Janik R
- Jayarathna PHSY
- Jena S
- Jirden L
- Jones PG
- Jung H
- Jusko A
- Kaidalov AB
- Kakoyan V
- Kalcher S
- Kalinak P
- Kalisky M
- Kalliokoski T
- Kalweit A
- Kanaki K
- Kang JH
- Kaplin V
- Karampatsos LX
- Karavichev O
- Karavicheva T
- Karpechev E
- Kazantsev A
- Kebschull U
- Keidel R
- Khan MM
- Khan P
- Khan SA
- Khanzadeev A
- Kharlov Y
- Kileng B
- Kim B
- Kim DJ
- Kim DW
- Kim JH
- Kim JS
- Kim M
- Kim S
- Kim SH
- Kim T
- Kirsch S
- Kisel I
- Kiselev S
- Kisiel A
- Klay JL
- Klein J
- Klein-Bosing C
- Kliemant M
- Kluge A
- Knichel ML
- Knospe AG
- Koch K
- Kohler MK
- Kolk NVD
- Kolojvari A
- Kondratiev V
- Kondratyeva N
- Konevskikh A
- Korneev A
- Kour R
- Kowalski M
- Kox S
- Kral J
- Kralik I
- Kramer F
- Kraus I
- Krawutschke T
- Krelina M
- Kretz M
- Krivda M
- Krizek F
- Krus M
- Kryshen E
- Krzewicki M
- Kucheriaev Y
- Kuhn C
- Kuijer PG
- Kurashvili P
- Kurepin A
- Kurepin AB
- Kuryakin A
- Kushpil S
- Kushpil V
- Kvaerno H
- Kweon MJ
- Kwon Y
- Lakomov I
- Langoy R
- Lara C
- Lara CEP
- Lardeux A
- Lazzeroni C
- Lea R
- Lee KS
- Lee SC
- Leeuwen MV
- Lefevre F
- Lehnert J
- Leistam L
- Lenhardt M
- Lenti V
- Leon H
- Levai P
- Lezama EP
- Liberto SD
- Lien J
- Lietava R
- Lindal S
- Lindenstruth V
- Lippmann C
- Lisa MA
- Liu L
- Loenne PI
- Loggins VR
- Loginov V
- Lohn S
- Lohner D
- Loizides C
- Loo KK
- Lopez X
- Lovhoiden G
- Lu XG
- Luettig P
- Lunardon M
- Luo J
- Luparello G
- Luquin L
- Luzzi C
- Ma K
- Ma R
- Madagodahettige-Don DM
- Maevskaya A
- Mager M
- Mahapatra DP
- Maire A
- Majumdar AKD
- Majumdar MRD
- Mal'Kevich D
- Malaev M
- Maldonado IC
- Malinina L
- Malzacher P
- Mamonov A
- Manceau L
- Mangotra L
- Manko V
- Manso F
- Manzari V
- Mao Y
- Marchisone M
- Marco ND
- Mares J
- Margagliotti GV
- Margotti A
- Marin A
- Markert C
- Martashvili I
- Martinengo P
- Martinez MI
- Martynov Y
- Mas A
- Masciocchi S
- Masera M
- Masoni A
- Masoodi AA
- Massacrier L
- Mastromarco M
- Mastroserio A
- Matthews ZL
- Matyja A
- Mauro AD
- Mayani D
- Mayer C
- Mazer J
- Mazzoni MA
- Meddi F
- Meethaleveedu GK
- Menchaca-Rocha A
- Meres M
- Miake Y
- Milano L
- Milosevic J
- Mischke A
- Mishra AN
- Miskowiec D
- Mitu C
- Mlynarz J
- Mohanty AK
- Mohanty B
- Molina RA
- Molnar L
- Monteno M
- Montero AJR
- Montes E
- Montoya CAC
- Monzon IL
- Moon T
- Morales YC
- Morando M
- Moretto S
- Morsch A
- Muccifora V
- Mudnic E
- Muhuri S
- Muller H
- Munhoz MG
- Munoz GT
- Musa L
- Musso A
- Nandi BK
- Nania R
- Nappi E
- Nattrass C
- Naumov NP
- Navin S
- Nayak TK
- Nazarenko S
- Nazarov G
- Nedosekin A
- Nezza PD
- Nicassio M
- Nielsen BS
- Niida T
- Nikolaev S
- Nikolic V
- Nikulin S
- Nikulin V
- Nilsen BS
- Nilsson MS
- Noferini F
- Nomokonov P
- Nooren G
- Novitzky N
- Nyanin A
- Nyatha A
- Nygaard C
- Nystrand J
- Ochirov A
- Oeschler H
- Oh S
- Oh SK
- Oleniacz J
- Oppedisano C
- Orduna DC
- Ortona G
- Oskarsson A
- Ostrowski P
- Otwinowski J
- Ovrebekk G
- Oyama K
- Ozawa K
- Pachmayer Y
- Pachr M
- Padilla F
- Pagano P
- Paic G
- Painke F
- Pajares C
- Pal S
- Pal SK
- Palaha A
- Palmeri A
- Palomo LV
- Papikyan V
- Pappalardo GS
- Park WJ
- Pasquale SD
- Passfeld A
- Pastircak B
- Patalakha DI
- Paticchio V
- Pavlinov A
- Pawlak T
- Pedrosa FBDS
- Peitzmann T
- Peresunko D
- Perez JM
- Perini D
- Perrino D
- Peryt W
- Pesci A
- Peskov V
- Pestov Y
- Petracek V
- Petran M
- Petris M
- Petrov P
- Petrovici M
- Petta C
- Piano S
- Piccotti A
- Pikna M
- Pillot P
- Pinazza O
- Pinsky L
- Pitz N
- Piuz F
- Piyarathna DB
- Ploskon M
- Pluta J
- Pocheptsov T
- Pochybova S
- Podesta-Lerma PLM
- Poghosyan MG
- Polak K
- Polichtchouk B
- Pop A
- Porteboeuf-Houssais S
- Pospisil V
- Potukuchi B
- Prasad SK
- Preghenella R
- Prino F
- Pruneau CA
- Pshenichnov I
- Puchagin S
- Puddu G
- Pulvirenti A
- Punin V
- Putis M
- Putschke J
- Quercigh E
- Qvigstad H
- Rachevski A
- Rademakers A
- Radomski S
- Raiha TS
- Rak J
- Rakotozafindrabe A
- Ramello L
- Raniwala R
- Raniwala S
- Rasanen SS
- Rascanu BT
- Rathee D
- Read KF
- Real JS
- Redlich K
- Reichelt P
- Reicher M
- Renfordt R
- Reolon AR
- Reshetin A
- Rettig F
- Revol JP
- Reyes AR
- Reygers K
- Riccati L
- Ricci RA
- Richert T
- Richter M
- Riedler P
- Riegler W
- Riggi F
- Rinella GA
- Rocca PL
- Roed K
- Rohr D
- Rohrich D
- Roman VC
- Romeo GC
- Romita R
- Ronchetti F
- Rooij RD
- Rosnet P
- Rossegger S
- Rossi A
- Roukoutakis F
- Roy C
- Roy P
- Rui R
- Ryabinkin E
- Rybicki A
- Sadovsky S
- Safarik K
- Sahoo R
- Sahu PK
- Saini J
- Sakaguchi H
- Sakai S
- Sakata D
- Salazar SA
- Salgado CA
- Salzwedel J
- Sambyal S
- Samsonov V
- Sanchez EDC
- Sandor L
- Sandoval A
- Sano M
- Sano S
- Santo R
- Santoro R
- Sarkamo J
- Scapparone E
- Scarlassara F
- Scharenberg RP
- Schiaua C
- Schicker R
- Schmidt C
- Schmidt HR
- Schreiner S
- Schuchmann S
- Schukraft J
- Schutz Y
- Schwarz K
- Schweda K
- Scioli G
- Scomparin E
- Scott PA
- Scott R
- Segato G
- Selyuzhenkov I
- Senyukov S
- Seo J
- Serci S
- Serradilla E
- Sevcenco A
- Sgura I
- Shabetai A
- Shabratova G
- Shahoyan R
- Sharma N
- Sharma S
- Shigaki K
- Shimomura M
- Shtejer K
- Sibiriak Y
- Siciliano M
- Sicking E
- Siddhanta S
- Siemiarczuk T
- Silvermyr D
- Silvestre C
- Simonetti G
- Singaraju R
- Singh R
- Singha S
- Sinha BC
- Sinha T
- Sitar B
- Sitta M
- Skaali TB
- Skjerdal K
- Smakal R
- Smirnov N
- Snellings RJM
- Sogaard C
- Soltz R
- Son H
- Song J
- Song M
- Soos C
- Soramel F
- Sputowska I
- Spyropoulou-Stassinaki M
- Srivastava BK
- Stachel J
- Stan I
- Stan I
- Stefanek G
- Stefanini G
- Steinbeck T
- Steinpreis M
- Stenlund E
- Steyn G
- Stocco D
- Stolpovskiy M
- Strabykin K
- Strmen P
- Suaide AAP
- Sugitate T
- Suire C
- Sukhorukov M
- Sultanov R
- Sumbera M
- Susa T
- Szarka I
- Szostak A
- Tagridis C
- Takahashi J
- Takaki JDT
- Tauro A
- Teixido JP
- Telesca A
- Tellez AF
- Terrevoli C
- Thader J
- Thomas D
- Tieulent R
- Timmins AR
- Tlusty D
- Tobon CAM
- Toia A
- Toledo ASD
- Torii H
- Torres EL
- Toscano L
- Tosello F
- Truesdale D
- Trzaska WH
- Tsuji T
- Tumkin A
- Turrisi R
- Tveter TS
- Ulery J
- Ullaland K
- Ulrich J
- Uras A
- Urban J
- Urciuoli GM
- Usai GL
- Uysal AK
- Vajzer M
- Vala M
- Valle ZCD
- Vallero S
- Vannucci L
- Vargas A
- Vargas HL
- Varma R
- Vasileiou M
- Vasiliev A
- Vasquez MAS
- Vechernin V
- Velasquez AO
- Veldhoen M
- Venaruzzo M
- Vercellin E
- Vergara S
- Vernekohl DC
- Vernet R
- Verweij M
- Vickovic L
- Viesti G
- Vikhlyantsev O
- Vilakazi Z
- Villar EC
- Vinogradov A
- Vinogradov L
- Vinogradov Y
- Virgili T
- Viyogi YP
- Vodopyanov A
- Voloshin K
- Voloshin S
- Volpe G
- Vranic D
- Vrlakova J
- Vulpescu B
- Vyushin A
- Vyvre PV
- Wagner B
- Wagner V
- Wan R
- Wang D
- Wang M
- Wang Y
- Wang Y
- Watanabe K
- Wessels JP
- Westerhoff U
- Wiechula J
- Wikne J
- Wilde M
- Wilk A
- Wilk G
- Williams MCS
- Windelband B
- Yang H
- Yang S
- Yasnopolskiy S
- Yi J
- Yin Z
- Yokoyama H
- Yoo IK
- Yoon J
- Yu W
- Yuan X
- Yushmanov I
- Zach C
- Zampolli C
- Zaporozhets S
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zelnicek P
- Zetina LM
- Zgura IS
- Zhalov M
- Zhang X
- Zhou D
- Zhou F
- Zhou Y
- Zhu X
- Zichichi A
- Zimmermann A
- Zinovjev G
- Zoccarato Y
- Zynovyev M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 16/03/2012
- Field of study
We calculate the average volumetric flux versus pressure drop of bubbles
moving in a single capillary tube with varying diameter, finding a square-root
relation from mapping the flow equations onto that of a driven overdamped
pendulum. The calculation is based on a derivation of the equation of motion of
a bubble train from considering the capillary forces and the entropy production
associated with the viscous flow. We also calculate the configurational
probability of the positions of the bubbles.Comment: 4 pages, 1 figur
Coendangered hard-ticks: threatened or threatening?
- Author
- AA Guglielmone
- AA Guglielmone
- AD Nijhof
- Andrei Daniel Mihalca
- AO Bush
- AS Dissanaike
- B McCulloch
- BL Penzhorn
- Călin Mircea Gherman
- D Govender
- DA Windsor
- DA Windsor
- DD Colwell
- DW Brocklesby
- E Mey
- GM Mugera
- H Hoogstraal
- HP Waudby
- J de la Fuente
- J Lamoreux
- JM Diamond
- JM Pérez
- KB Wyatt
- L Beati
- L Rózsa
- LA Durden
- LP Koh
- M Nowak
- ME Fowler
- N Stork
- ND Levine
- P Willadsen
- P Willadsen
- P Široký
- R Pizzi
- RR Dunn
- RR Dunn
- SC Barker
- SM Waladde
- Vasile Cozma
- WB Nutting
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
The overwhelming majority of animal conservation projects are focused on vertebrates, despite most of the species on Earth being invertebrates. Estimates state that about half of all named species of invertebrates are parasitic in at least one stage of their development. The dilemma of viewing parasites as biodiversity or pest has been discussed by several authors. However, ticks were omitted. The latest taxonomic synopses of non-fossil Ixodidae consider valid 700 species. Though, how many of them are still extant is almost impossible to tell, as many of them are known only from type specimens in museums and were never collected since their original description. Moreover, many hosts are endangered and as part of conservation efforts of threatened vertebrates, a common practice is the removal of, and treatment for external parasites, with devastating impact on tick populations. There are several known cases when the host became extinct with subsequent coextinction of their ectoparasites. For our synoptic approach we have used the IUCN status of the host in order to evaluate the status of specifically associated hard-ticks. As a result, we propose a number of 63 coendangered and one extinct hard-tick species. On the other side of the coin, the most important issue regarding tick-host associations is vectorial transmission of microbial pathogens (i.e. viruses, bacteria, protozoans). Tick-borne diseases of threatened vertebrates are sometimes fatal to their hosts. Mortality associated with pathogens acquired from ticks has been documented in several cases, mostly after translocations. Are ticks a real threat to their coendangered host and should they be eliminated? Up to date, there are no reliable proofs that ticks listed by us as coendangered are competent vectors for pathogens of endangered animals
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Abdallah J
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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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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
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- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
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- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- 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
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
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- 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
- Alam MA
- 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
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
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- Altheimer A
- Gonzalez BA
- Alviggi MG
- Amako K
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
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- Zeitnitz C
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- Zenin O
- Zenis T
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
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- Zhemchugov A
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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
- Abdinov O
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- Mehta A
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- Melachrinos C
- Meloni F
- Meng Z
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- Milov A
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- Rosendahl PL
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- Sasaki Y
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- Schegelsky VA
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- Scherzer MI
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- Schnoor U
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- Schorlemmer ALS
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- Schroeder TV
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- Schultens MJ
- Schultes J
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
- Schwanenberger C
- Schwartzman A
- Schwegler P
- Schwemling P
- Schwienhorst R
- Schwierz R
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- Searcy J
- Sedov G
- Sedykh E
- Seidel SC
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- Seixas JM
- Sekhniaidze G
- Sekula SJ
- Selbach KE
- Seliverstov DM
- Sellden B
- Sellers G
- Seman M
- Semprini-Cesari N
- Serfon C
- Serin L
- Serkin L
- Seuster R
- Severini H
- Sfyrla A
- Shabalina E
- Shamim M
- Shan LY
- Shank JT
- Shao QTQ
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- Shatalov PB
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- Sherman D
- Sherwood P
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- Shimojima M
- Shin T
- Shiyakova M
- Shmeleva A
- Shochet MJ
- Short D
- Shrestha S
- Shulga E
- Shupe MA
- Sicho P
- Sidoti A
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- Simoniello R
- Simonyan M
- Sinervo P
- Sinev NB
- Sipica V
- Siragusa G
- Sircar A
- Sisakyan AN
- Sivoklokov SY
- Sjoelin J
- Sjursen TB
- Skinnari LA
- Skottowe HP
- Skovpen K
- Skubic P
- Slater NM
- Slavicek T
- Sliwa K
- Smakhtin V
- Smart BH
- Smestad L
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smit GVY
- Smith BC
- Smith D
- Smith KM
- Smizanska M
- Smolek K
- Snesarev AA
- Snow J
- Snow SW
- Snyder S
- Sobie R
- Sodomka J
- Soffer A
- Soh DA
- Soiovyallv V
- Solans CA
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- Soldatov EY
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- Solodkov AA
- Solovyev V
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- Stanescu-Bellu M
- Stanitzki MM
- Stapnes S
- Starchenko EA
- Stark J
- Staroba P
- Starovoitov P
- Staszewski R
- Staude A
- Stavina P
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- Steinbach P
- Steinberg P
- Stekl I
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
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- Stoicea G
- Stonjek S
- Strachota P
- Stradling AR
- Straessner A
- Strandberg J
- Strandberg S
- Strandlie A
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- Stroynowski R
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- Stumer I
- Stupak J
- Sturm P
- Styles NA
- Su D
- Subramania HS
- Subramaniam R
- Succurro A
- Sugaya Y
- Suhr C
- Suk M
- Sulin VV
- Sultansoy S
- Sumida T
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki Y
- Suzuki Y
- Svatos M
- Swedish S
- Sykora I
- Sykora T
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Taiblum N
- Takahashi Y
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Takubo Y
- Talby M
- Talyshev A
- Tamsett MC
- Tan KG
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanasijczuk AJ
- Tani K
- Tannoury N
- Tapprogge S
- Tardif D
- Tarem S
- Tarrade F
- Tartarelli GF
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- Temming KK
- Ten Kate H
- Teng PK
- Terada S
- Terashi K
- Terron J
- Testa M
- Teuscher RJ
- Therhaag JJ
- Theveneaux-Pelzer T
- Thoma S
- Thomas JP
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomsen LA
- Thomson E
- Thomson M
- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tic T
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
- Tipton P
- Tisserant S
- Todorov T
- Todorova-Nova S
- Toggerson B
- Tojo J
- Tokar S
- Tokushuku K
- Tollefson K
- Tomoto M
- Tompkins L
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- Trigger IM
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- Tripiana MF
- Triplett N
- Trischuk W
- Trocme B
- Troncon C
- Trottier-McDonald M
- True P
- Trzebinski M
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- Tsarouchas C
- Tseng JC-L
- Tsiakiris M
- Tsiareshka P
- Tsionou D
- Tsipolitis G
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsung J-W
- Tsuno S
- Tsybychev D
- Tua A
- Tudorache A
- Tudorache V
- Tuggle JM
- Tuna AN
- Turala M
- Turecek D
- Turlay E
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Tzanakos G
- Uchida K
- Ueda I
- Ueno R
- Ugland M
- Uhlenbrock M
- Uhrmacher M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Unno Y
- Urbaniec D
- Urquijo P
- Usai G
- Uslenghi M
- Vacavant L
- Vacek V
- Vachon B
- Vague FV
- Vahsen S
- Valenta J
- Valentinetti S
- Valero A
- Valkar S
- Valladolid Gallego E
- Vallecorsa S
- Valls Ferrer JA
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- Van der Deijl PC
- van der Geer R
- van der Graaf H
- van der Leeuw R
- van der Poe E
- van der Ster D
- van Eldik N
- van Gemmeren P
- van Huysduynen LH
- van Vulpen I
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vannucci F
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vassilakopoulos VI
- Vazeille F
- Vazquez JGP
- Vegni G
- Veillet JI
- Veloso F
- Veness R
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter MG
- Vinek E
- Vinogradov VB
- Virchaux M
- Virzi J
- Vitells O
- Viti M
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vokac P
- Volpi G
- Volpi M
- Volpini G
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorwerk V
- Vos M
- Voss R
- Voss TT
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wahlen H
- Wahrmund S
- Wakabayashi J
- Walch S
- Walder J
- Walker R
- Walkowiak W
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- Waller P
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- Wang C
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- Wang R
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- Wang T
- Warburton A
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- Wardrope DR
- Warsinsky M
- Washbrook A
- Wasicki C
- Watanabe I
- Watkins PM
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- Watson IJ
- Watson MF
- Watts G
- Watts S
- Waugh AT
- Waugh BM
- Weber MS
- Webster JS
- Weidberg AR
- Weigell P
- Weingarten J
- Weiser C
- Wells PS
- Wemans ADV
- Wenaus T
- Wendland D
- Wengler T
- Wengu Z
- Wenig S
- Wermes N
- Werner M
- Werner P
- Werth M
- Wessels M
- Wetter J
- Weydert C
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- White S
- Whitehead SR
- Whiteson D
- Whittington D
- Wicek F
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilhelm I
- Wilkens HG
- Will JZ
- Williams E
- Williams HH
- Willis W
- Willocoq S
- Wilson A
- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong WC
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wraight K
- Wright M
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wynne BM
- Xella S
- Xiao M
- Xie S
- Xu C
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yagci KD
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- 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
- Zerwas D
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- 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
- 01/01/2012
- 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
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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- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
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- Abolins M
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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
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