1,356 research outputs found
Bats Use Magnetite to Detect the Earth's Magnetic Field
- Author
- AJ Kalmijn
- CV Mora
- DA Bazylinski
- E Batschelet
- ER Buchler
- G Fleissner
- G Kramer
- HG Wallraff
- HG Wallraff
- JB Phillips
- JC Diaz-Ricci
- JL Gould
- JL Kirschvink
- JL Kirschvink
- JL Kirschvink
- JL Kirschvink
- JL Kirschvink
- JL Kirschvink
- JL Kirschvink
- Joseph L. Kirschvink
- KJ Lohmann
- KJ Lohmann
- Martin Wikelski
- MJM Leask
- MM Walker
- MM Walker
- P Light
- P Thalau
- PJ Nemec
- R Wiltschko
- R Wiltschko
- RA Holland
- RA Holland
- RA Holland
- RC Beason
- RC Beason
- RE Wegner
- Richard A. Holland
- RP Blakemore
- RP Blakemore
- RP Blakemore
- S Marhold
- Sarah Frances Brosnan
- TC Williams
- TE Dennis
- TH Flemming
- Thomas G. Doak
- TP Quinn
- U Munro
- W Wiltschko
- W Wiltschko
- W Wiltschko
- W Wiltschko
- W Wiltschko
- WP Irwin
- WW Cochran
- Y Wang
- Publication venue
- Publication date
- 01/01/2008
- Field of study
While the role of magnetic cues for compass orientation has been confirmed in numerous animals, the mechanism of detection is still debated. Two hypotheses have been proposed, one based on a light dependent mechanism, apparently used by birds and another based on a “compass organelle” containing the iron oxide particles magnetite (Fe3O4). Bats have recently been shown to use magnetic cues for compass orientation but the method by which they detect the Earth's magnetic field remains unknown. Here we use the classic “Kalmijn-Blakemore” pulse re-magnetization experiment, whereby the polarity of cellular magnetite is reversed. The results demonstrate that the big brown bat Eptesicus fuscus uses single domain magnetite to detect the Earths magnetic field and the response indicates a polarity based receptor. Polarity detection is a prerequisite for the use of magnetite as a compass and suggests that big brown bats use magnetite to detect the magnetic field as a compass. Our results indicate the possibility that sensory cells in bats contain freely rotating magnetite particles, which appears not to be the case in birds. It is crucial that the ultrastructure of the magnetite containing magnetoreceptors is described for our understanding of magnetoreception in animals
Prime movers : mechanochemistry of mitotic kinesins
- Author
- A Blangy
- A Groen
- A Hutterer
- A Jannasch
- A Karabay
- A Toso
- A Yildiz
- AA Levesque
- AB Asenjo
- AC Groen
- AE Butterfield
- AF Huxley
- AF Straight
- AJ Roberts
- AM Mulder
- AM Saunders
- Andrew McAinsh
- AS Kashina
- AS Khalil
- B Gigant
- B Owens
- B Wickstead
- BH Kwok
- BH Kwok
- BJ Grant
- BT Schaar
- C Antonio
- C Hentrich
- C Peters
- C Thiede
- C Wandke
- CA Watts
- CC Leduc
- CE Walczak
- CJ Lawrence
- CK Hu
- CL Parke
- CL Rieder
- CL Rieder
- CM Whitehead
- CTC Friel
- CV Sindelar
- CV Sindelar
- D Vanneste
- D Vanneste
- DA Compton
- E Doménech
- E Karsenti
- E Vladimirou
- EG Sturgill
- ER Hildebrandt
- FJ Kull
- FJ Kull
- G Fink
- GC Rogers
- GJ Brouhard
- GJ Gorbsky
- GJPL Kops
- H Aizawa
- H Boleti
- H Drechsler
- H Funabiki
- H Yardimci
- HS Sardar
- HS Sardar
- HYK Kaan
- I Brust-Mascher
- I Brust-Mascher
- I Minoura
- IM Crevel
- IM-TC Crevel
- J Espeut
- J Helenius
- J Roostalu
- J Roostalu
- J Rosenblatt
- J Stumpff
- J Stumpff
- J Stumpff
- J Yajima
- JC Cochran
- JC Gatlin
- JC Waters
- JM Scholey
- JPI Welburn
- JR Aist
- JR Cooper
- JR McIntosh
- JRJ Stout
- JS Allingham
- JS Weinger
- K Hahlen
- K Jaqaman
- K Kaseda
- K Kaseda
- K Samejima
- KE Gascoigne
- KJ Verhey
- KS Burbank
- KW Wood
- KW Wood
- KY Lee
- L Wordeman
- LC Kapitein
- LC Kapitein
- LN Weaver
- LR Sproul
- M Braun
- M Braun
- M Glotzer
- M Joshi
- M Kikkawa
- M Klejnot
- M Mishima
- M Nishiyama
- M Wagenbach
- MA Hoyt
- MA Seeger
- MC Alonso
- ME Douglas
- ME Tanenbaum
- ME Tanenbaum
- ME Tanenbaum
- MI Mayr
- MJ Korneev
- ML Gupta
- MT Valentine
- MT Valentine
- N Gudimchuk
- N Hirokawa
- N Hirokawa
- N Joseph
- NF Endres
- NJ Carter
- NJ Ganem
- OO Rath
- P Bieling
- Q Chang
- R Nitta
- R Nunes Bastos
- R Uehara
- RB Case
- RD Vale
- Robert A. Cross
- S Acar
- S Cai
- S Cane
- S Debonis
- S Diez
- S Dumont
- S Highsmith
- S Inoué
- S Oh
- S Rice
- S Rice
- S Shastry
- SF Bakhoum
- SS Rosenfeld
- SS Rosenfeld
- SW Grill
- T Krzysiak
- T Maney
- T Surrey
- TJ Mitchison
- TJ Mitchison
- TM Kapoor
- TT Ogawa
- V Fridman
- V Magidson
- V Mountain
- V Varga
- VV Bormuth
- W Saunders
- WW Wang
- X Su
- X Su
- Y Du
- Y Kim
- Y Kurasawa
- Y Oguchi
- Y Zhai
- YF Dufrene
- YM Lee
- YY Okada
- Z Yang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 21/03/2014
- Field of study
Mitotic spindles are self-organizing protein machines that harness teams of multiple force generators to drive chromosome segregation. Kinesins are key members of these force-generating teams. Different kinesins walk directionally along dynamic microtubules, anchor, crosslink, align and sort microtubules into polarized bundles, and influence microtubule dynamics by interacting with microtubule tips. The mechanochemical mechanisms of these kinesins are specialized to enable each type to make a specific contribution to spindle self-organization and chromosome segregation
Ratio of the Isolated Photon Cross Sections at \sqrt{s} = 630 and 1800 GeV
- Author
- Abazov VM
- Abbott B
- Abdesselam A
- Abolins M
- Abramov V
- Acharya BS
- Adams DL
- Adams M
- Ahmed SN
- Alexeev GD
- Alton A
- Alves GA
- Amos N
- Anderson EW
- Arnoud Y
- Avila C
- Baarmand MM
- Babintsev VV
- Babukhadia L
- Bacon TC
- Baden A
- Baldin B
- Balm PW
- Banerjee S
- Barberis E
- Baringer P
- Barreto J
- Bartlett JF
- Bassler U
- Bauer D
- Bean A
- Beaudette F
- Begel M
- Belyaev A
- Beri SB
- Bernardi G
- Bertram I
- Besson A
- Beuselinck R
- Bezzubov VA
- Bhat PC
- Bhatnagar V
- Bhattacharjee M
- Blazey G
- Blekman F
- Blessing S
- Boehnlein A
- Bojko NI
- Borcherding F
- Bos K
- Bose T
- Brandt A
- Breedon R
- Briskin G
- Brock R
- Brooijmans G
- Bross A
- Buchholz D
- Buehler M
- Buescher V
- Burtovoi VS
- Butler JM
- Canelli F
- Carvalho W
- Casey D
- Casilum Z
- Castilla-Valdez H
- Chakraborty D
- Chan KM
- Chekulaev SV
- Cho DK
- Choi S
- Chopra S
- Christenson JH
- Chung M
- Claes D
- Clark AR
- Cochran J
- Collaboration D
- Coney L
- Connolly B
- Cooper WE
- Coppage D
- Crepe-Renaudin S
- Cummings MAC
- Cutts D
- da Motta H
- Davis GA
- Davis K
- de Jong SJ
- De K
- Del Signore K
- Demarteau M
- Demina R
- Demine P
- Denisov D
- Denisov SP
- Desai S
- Diehl HT
- Diesburg M
- Doulas S
- Ducros Y
- Dudko LV
- Duensing S
- Duflot L
- Dugad SR
- Duperrin A
- Dyshkant A
- Edmunds D
- Ellison J
- Elvira VD
- Engelmann R
- Eno S
- Eppley G
- Ermolov P
- Eroshin OV
- Estrada J
- Evans H
- Evdokimov VN
- Fahland T
- Feher S
- Fein D
- Ferbel T
- Filthaut F
- Fisk HE
- Fisyak Y
- Flattum E
- Fleuret F
- Fortner M
- Fox H
- Frame KC
- Fu S
- Fuess S
- Gallas E
- Galyaev AN
- Gao M
- Gavrilov V
- Genik RJ
- Genser K
- Gerber CE
- Gershtein Y
- Gilmartin R
- Ginther G
- Gomez B
- Gomez G
- Goncharov PI
- Gordon H
- Goss LT
- Gounder K
- Goussiou A
- Graf N
- Graham G
- Grannis PD
- Green JA
- Greenlee H
- Greenwood ZD
- Grinstein S
- Groer L
- Grunendahl S
- Gupta A
- Gurzhiev SN
- Gutierrez G
- Gutierrez P
- Hadley NJ
- Haggerty H
- Hagopian S
- Hagopian V
- Hall RE
- Hanlet P
- Hansen S
- Hauptman JM
- Hays C
- Hebert C
- Hedin D
- Heinmiller JM
- Heinson AP
- Heintz U
- Heuring T
- Hildreth MD
- Hirosky R
- Hobbs JD
- Hoeneisen B
- Huang Y
- Illingworth R
- Ito AS
- Jaffre M
- Jain S
- Jesik R
- Johns K
- Johnson M
- Jonckheere A
- Jostlein H
- Juste A
- Kahl W
- Kahn S
- Kajfasz E
- Kalinin AM
- Karmanov D
- Karmgard D
- Kehoe R
- Khanov A
- Kharchilava A
- Kim SK
- Klima B
- Knuteson B
- Ko W
- Kohli JM
- Kostritskiy AV
- Kotcher J
- Kothari B
- Kotwal AV
- Kozelov AV
- Kozlovsky EA
- Krane J
- Krishnaswamy MR
- Krivkova P
- Krzywdzinski S
- Kubantsev M
- Kuleshov S
- Kulik Y
- Kunori S
- Kupco A
- Kuznetsov VE
- Landsberg G
- Lee SM
- Leflat A
- Leggett C
- Lehner F
- Li J
- Li QZ
- Li X
- Lima JGR
- Lincoln D
- Linn SL
- Linnemann J
- Lipton R
- Lucotte A
- Lueking L
- Lundstedt C
- Luo C
- Maciel AKA
- Madaras RJ
- Malyshev VL
- Manankov V
- Mao HS
- Marshall T
- Martin MI
- Mauritz KM
- May B
- Mayorov AA
- McCarthy R
- McMahon T
- Melanson HL
- Merkin M
- Merritt KW
- Miao C
- Miettinen H
- Mihalcea D
- Mishra CS
- Mokhov N
- Mondal NK
- Montgomery HE
- Moore RW
- Mostafa M
- Nagy E
- Nang F
- Narain M
- Narasimham VS
- Naumann NA
- Neal HA
- Negret JR
- Negroni S
- Nunnemann T
- O'Neil D
- Oguri V
- Olivier B
- Oshima N
- Padley P
- Pan LJ
- Papageorgiou K
- Para A
- Parashar N
- Partridge R
- Parua N
- Paterno M
- Patwa A
- Pawlik B
- Perkins J
- Peters O
- Petroff P
- Piegaia R
- Pope BG
- Popkov E
- Prosper HB
- Protopopescu S
- Przybycien MB
- Qian J
- Raja R
- Rajagopalan S
- Ramberg E
- Rapidis PA
- Reay NW
- Reucroft S
- Ridel M
- Rijssenbeek M
- Rizatdinova F
- Rockwell T
- Roco M
- Royon C
- Rubinov R
- Ruchti R
- Rutherfoord J
- Sabirov BM
- Sajot G
- Santoro A
- Sawyer L
- Schamberger RD
- Schellman H
- Schwartzman A
- Sen N
- Shabalina E
- Shivpuri RK
- Shpakov D
- Shupe M
- Sidwell RA
- Simak V
- Singh H
- Singh JB
- Sirotenko V
- Slattery P
- Smith E
- Smith RP
- Snihur R
- Snow GR
- Snow J
- Snyder S
- Solis JLG
- Solomon J
- Song Y
- Sorin V
- Sosebee M
- Sotnikova N
- Soustruznik K
- Souza M
- Stanton NR
- Steinbruck G
- Stephens RW
- Stichelbaut F
- Stoker D
- Stolin V
- Stone A
- Stoyanova DA
- Strang MA
- Strauss M
- Strovink M
- Stutte L
- Sznajder A
- Talby M
- Taylor W
- Tentindo-Repond S
- Tripathi SM
- Trippe TG
- Turcot AS
- Tuts PM
- Van Kooten R
- Vaniev V
- Varelas N
- Vertogradov LS
- Villeneuve-Seguier F
- Volkov AA
- Vorobiev AP
- Wahl HD
- Wang H
- Wang ZM
- Warchol J
- Watts G
- Wayne M
- Weerts H
- White A
- White JT
- Whiteson D
- Wightman JA
- Wijngaarden DA
- Willis S
- Wimpenny SJ
- Womersley J
- Wood DR
- Xu Q
- Yamada R
- Yamin R
- Yasuda T
- Yatsunenko YA
- Yip K
- Youssef S
- Yu J
- Yu Z
- Zanabria M
- Zhang X
- Zheng H
- Zhou B
- Zhou Z
- Zielinski M
- Zieminska D
- Zieminski A
- Zutshi V
- Zverev EG
- Zylberstejn A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2001
- Field of study
The inclusive cross section for production of isolated photons has been
measured in \pbarp collisions at s=630 GeV with the \D0 detector at
the Fermilab Tevatron Collider. The photons span a transverse energy (ET)
range from 7-49 GeV and have pseudorapidity ∣η∣<2.5. This measurement is
combined with to previous \D0 result at s=1800 GeV to form a ratio
of the cross sections. Comparison of next-to-leading order QCD with the
measured cross section at 630 GeV and ratio of cross sections show satisfactory
agreement in most of the ET range.Comment: 7 pages. Published in Phys. Rev. Lett. 87, 251805, (2001
Search for rare quark-annihilation decays, B --> Ds(*) Phi
- Author
- Abe T
- Abrams GS
- Adye T
- Ahmed M
- Ahmed S
- Alam MS
- Albert J
- Aleksan R
- Allen MT
- Allison J
- Allmendinger T
- Altenburg D
- Andreassen R
- Andreotti M
- Angelini C
- Anulli F
- Arnaud N
- Aston D
- Aubert B
- Azzolini V
- Baak M
- Back JJ
- Baldini-Ferroli R
- Band HR
- Banerjee S
- Barate R
- Bard DJ
- Barlow NR
- Barlow RJ
- Barrett M
- Bartoldus R
- Batignani G
- Battaglia M
- Bauer JM
- Beck TW
- Behera PK
- Bellini F
- Benayoun M
- Benelli G
- Berger N
- Bernard D
- Berryhill JW
- Best D
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhimji W
- Bhuyan B
- Bianchi F
- Biasini M
- Biesiada J
- Blanc F
- Blaylock G
- Blinov AE
- Blinov VE
- Bloom PC
- Blount NL
- Bomben M
- Bona M
- Bondioli M
- Bonneaud GR
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandenburg G
- Brandt T
- Brau J
- Breon AB
- Brose J
- Brown CL
- Brown CM
- Brown DN
- Brown DN
- Bruinsma M
- Brunet S
- Bucci F
- Buchanan C
- Buchmueller OL
- Bugg W
- Bukin AD
- Bula R
- Bulten H
- Buono LD
- Burchat PR
- Burke JP
- Button-Shafer J
- Buzzo A
- Cahn RN
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Capra R
- Carpinelli M
- Cartaro C
- Cavallo N
- Cavoto G
- Cenci R
- Chai X
- Chaisanguanthum KS
- Chao M
- Charles E
- Charles MJ
- Chauveau J
- Chavez CA
- Chen A
- Chen C
- Chen E
- Chen JC
- Chen S
- Chen X
- Cheng B
- Cheng CH
- Chia YM
- Cibinetto G
- Clark PJ
- Claus R
- Cochran J
- Coleman JP
- Collaboration BABAR
- Contri R
- Convery MR
- Cossutti F
- Cote D
- Cottingham WN
- Couderc F
- Covarelli R
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Cristinziani M
- Cuhadar-Donszelmann T
- Cunha A
- Curry S
- D'Orazio A
- Dahmes B
- Dallapiccola C
- Danielson N
- Dasu S
- Datta M
- Dauncey PD
- David P
- Davier M
- Davis CL
- Day CT
- de la Vaissiere C
- de Monchenault GH
- de Sangro R
- del Re D
- Diberder FL
- Dickopp M
- Dingfelder JC
- Dittongo S
- Dong D
- Dong L
- Dorfan J
- Druzhinin VP
- Dubitzky RS
- Dubois-Felsmann GP
- Dujmic D
- Dunwoodie W
- Dvoretskii A
- Eckhart EA
- Eckmann R
- Edgar CL
- Edwards AJ
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Elmer P
- Emery S
- Ernst JA
- Eschenburg V
- Eschrich I
- Eyges V
- Fabozzi F
- Faccini R
- Fan S
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Flacco CJ
- Flack RL
- Flaecher HU
- Flood KT
- Ford KE
- Ford WT
- Forster IJ
- Forti F
- Fortin D
- Foulkes SD
- Franek B
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Gabathuler E
- Gaidot A
- Gaillard JR
- Galeazzi F
- Gallo F
- Gamba D
- Gamet R
- Gan KK
- Ganzhur SF
- Gary JW
- Gaspero M
- Gatto C
- George KA
- Gill MS
- Gioi LL
- Giorgi MA
- Giroux X
- Gladney L
- Glanzman T
- Godang R
- Goetzen K
- Golubev VB
- Gopal GP
- Gowdy SJ
- Gradl W
- Graham MT
- Grancagnolo S
- Grauges E
- Graziani G
- Green MG
- Grenier P
- Gritsan AV
- Groot ND
- Grosdidier G
- Groysman Y
- Guo QH
- Hadavand HK
- Hadig T
- Haire M
- Halyo V
- Hamano K
- Hamon O
- Harrison PF
- Harrison TJ
- Hart AJ
- Hartfiel BL
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Held T
- Hertzbach SS
- Heusch CA
- Hill EJ
- Hirschauer JF
- Hitlin DG
- Hocker A
- Hodgkinson MC
- Hollar JJ
- Hong TM
- Honscheid K
- Hopkins DA
- Hryn'ova T
- Hufnagel D
- Hulsbergen WD
- Hutchcroft DE
- Igonkina O
- Innes WR
- Izen JM
- Jackson PD
- Jackson PS
- Jacobsen RG
- Jawahery A
- Jessop CP
- John MJJ
- Johnson JR
- Judd D
- Kadel RW
- Kadyk J
- Kagan H
- Karyotakis Y
- Kass R
- Kelly MP
- Kelsey MH
- Kerth LT
- Khan A
- Kim H
- Kim P
- Kirkby D
- Kitayama I
- Klose V
- Knecht NS
- Koch H
- Kocian ML
- Koeneke K
- Kofler R
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kozanecki W
- Kravchenko EA
- Kreisel A
- Krishnamurthy M
- Kroeger R
- Kroseberg J
- Kukartsev G
- Kutter PE
- Kyberd P
- Lacker HM
- Lae CK
- Lafferty GD
- Lanceri L
- Lange DJ
- Langenegger U
- Lankford AJ
- Latham TE
- Latour E
- Lau YP
- Lazzaro A
- Lees JP
- Legendre M
- Leith DWGS
- Lepeltier V
- Leruste P
- Lewandowski B
- Li H
- Li X
- Libby J
- Lista L
- Liu R
- Lockman WS
- Lodovico FD
- Lombardo V
- London GW
- Long O
- LoSecco JM
- Lou XC
- Lu C
- Lu M
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Macri MM
- Mader WF
- Majewski SA
- Malcles J
- Mallik U
- Mancinelli G
- Mandelkern M
- Marchiori G
- Marco ED
- Margoni M
- Marks J
- Marsiske H
- Martinez-Vidal F
- Mattison TS
- Mayer B
- Mazur MA
- Mazzoni MA
- McKenna JA
- McMahon TR
- Meadows BT
- Mellado B
- Menges W
- Messner R
- Meyer WT
- Mihalyi A
- Minamora JS
- Mir LM
- Mohanty GB
- Mohapatra AK
- Mommsen RK
- Monge MR
- Monorchio D
- Moore TB
- Morandin M
- Morgan SE
- Morganti M
- Morganti S
- Morii M
- Muheim F
- Muller DR
- Naisbit MT
- Nardo GD
- Narsky I
- Nash JA
- Nauenberg U
- Neal H
- Negrini M
- Neri N
- Nesom G
- Nicholson H
- Nikolich MB
- Nogowski R
- Nugent IM
- O'Grady CP
- Ocariz J
- Oddone PJ
- Ofte I
- Olaiya EO
- Olivas A
- Olsen J
- Onuchin AP
- Orimoto TJ
- Otto S
- Oyanguren A
- Ozcan VE
- Paar HP
- Pacetti S
- Palano A
- Palombo F
- Pan Y
- Panetta J
- Panvini RS
- Paoloni E
- Paolucci P
- Pappagallo M
- Parry RJ
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pelizaeus M
- Perazzo A
- Perl M
- Peruzzi IM
- Peters K
- Petersen BA
- Petersen TC
- Petzold A
- Piatenko T
- Piccolo D
- Piccolo M
- Piemontese L
- Pierini M
- Pioppi M
- Piredda G
- Plaszczynski S
- Playfer S
- Poireau V
- Polci F
- Pompili A
- Porter FC
- Posocco M
- Potter CT
- Prell S
- Prepost R
- Pripstein M
- Pulliam T
- Purohit MV
- Qi ND
- Rahatlou S
- Rahimi AM
- Rahmat R
- Rama M
- Ratcliff BN
- Raven G
- Reidy J
- Ricca GD
- Ricciardi S
- Richman JD
- Ritchie JL
- Rizzo G
- Roat C
- Roberts DA
- Robertson SH
- Robutti E
- Rodier S
- Roe NA
- Roethel W
- Ronan MT
- Roney JM
- Rong G
- Roodman A
- Roos L
- Rosenberg EI
- Rotondo M
- Roudeau P
- Rubin AE
- Ruddick WO
- Ryd A
- Sacco R
- Saeed MA
- Saleem M
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Santroni A
- Saremi S
- Satpathy A
- Schalk T
- Schenk S
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- Wilden L
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- Winklmeier F
- Wisniewski WJ
- Wittgen M
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- Wormser G
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- Wu SL
- Xie Y
- Yamamoto RK
- Yarritu AK
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- Yi JI
- Yi K
- Young CC
- Yu Z
- Yushkov AN
- Zain SB
- Zallo A
- Zeng Q
- Zghiche A
- Zhang J
- Zhang L
- Zhao HW
- Zhu YS
- Ziegler V
- Zito M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 12/12/2005
- Field of study
We report on searches for B- --> Ds- Phi and B- --> Ds*- Phi. In the context
of the Standard Model, these decays are expected to be highly suppressed since
they proceed through annihilation of the b and u-bar quarks in the B- meson.
Our results are based on 234 million Upsilon(4S) --> B Bbar decays collected
with the BABAR detector at SLAC. We find no evidence for these decays, and we
set Bayesian 90% confidence level upper limits on the branching fractions BF(B-
--> Ds- Phi) Ds*- Phi)<1.2x10^(-5). These results
are consistent with Standard Model expectations.Comment: 8 pages, 3 postscript figues, submitted to Phys. Rev. D (Rapid
Communications
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- 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
- Ackers M
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- Aderholz M
- Adomeit S
- Adragna P
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- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
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- Aielli G
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- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- Alessandria F
- Alexa C
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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
- Zilka B
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- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
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- 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
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
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- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
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- Archambault JP
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- Arik E
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- Armbruster AJ
- Arnaez O
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- Bai Y
- Bailey DC
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- Baker MD
- Baker OK
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- Boeriu OEV
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- Bogdanchikov A
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- Bondarenko VG
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- Boonekamp M
- Boorman G
- Booth CN
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- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borroni S
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcic I
- Bracinik J
- Braem A
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- Brandenburg GW
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- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- Bueso XP
- Bugge L
- Buira-Clark D
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- Yilmaz M
- Yoosootiniya R
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- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
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- Zeller M
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- Zemla A
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- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
- Zimmermann R
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- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
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- Zsenei A
- Zutshi V
- Zwalinski L
- 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
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
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- Yanush S
- Yao L
- Yao Y
- Yasu Y
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- Ye J
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
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- Youssef S
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
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- 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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- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhuravlov V
- 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
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- 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
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- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Aharrouche M
- Ahlen SP
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- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
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- Aliev M
- Alimonti G
- Alison J
- Allbrooke BMM
- Allport PP
- Allwood-Spiers SE
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- Amako K
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- Antonaki A
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- Wynne BM
- Xella S
- Xiao M
- Xie S
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- Xu L
- Yabsley B
- Yacoob S
- Yagci KD
- Yamada M
- Yamaguchi H
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- Yamanaka T
- Yamazaki T
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- 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
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- Yu J
- Yu J
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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
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- Zenin O
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- Zerwas D
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- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
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- 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 new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
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- Abbott DC
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- Abhayasinghe DK
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
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
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