695 research outputs found
Functional dissection of the Drosophila Kallmann's syndrome protein DmKal-1
- Author
- A Cariboni
- AH Brand
- B Franco
- B Lutz
- C Dode
- D Andrenacci
- Davide Andrenacci
- E Wieschaus
- EI Rugarli
- EI Rugarli
- EI Rugarli
- Elena I Rugarli
- Elena Riano
- F Garoia
- F Kallmann
- Franco Graziani
- G Maccoll
- GM Rubin
- HE Bülow
- J Albuisson
- J Capdevila
- J Mohler
- JD Wegenke
- JP Hardelin
- JP Hardelin
- JS Colquhoun-Kerr
- L Garcia-Alonso
- L Loidi
- L Manseau
- M Capovilla
- M Hermanussen
- M Schwanzel-Fukuda
- Maria R Grimaldi
- N Sato
- N Soussi-Yanicostas
- N Soussi-Yanicostas
- R Legouis
- R Legouis
- RE Hileman
- S Wray
- TJ DeFalco
- Vittorio Panetta
- Y Hu
- Publication venue
- BioMed Central
- Publication date
- 01/01/2006
- Field of study
BACKGROUND: Anosmin-1, the protein implicated in the X-linked Kallmann's syndrome, plays a role in axon outgrowth and branching but also in epithelial morphogenesis. The molecular mechanism of its action is, however, widely unknown. Anosmin-1 is an extracellular protein which contains a cysteine-rich region, a whey acidic protein (WAP) domain homologous to some serine protease inhibitors, and four fibronectin-like type III (FnIII) repeats. Drosophila melanogaster Kal-1 (DmKal-1) has the same protein structure with minor differences, the most important of which is the presence of only two FnIII repeats and a C-terminal region showing a low similarity with the third and the fourth human FnIII repeats. We present a structure-function analysis of the different DmKal-1 domains, including a predicted heparan-sulfate binding site. RESULTS: This study was performed overexpressing wild type DmKal-1 and a series of deletion and point mutation proteins in two different tissues: the cephalopharyngeal skeleton of the embryo and the wing disc. The overexpression of DmKal-1 in the cephalopharyngeal skeleton induced dosage-sensitive structural defects, and we used these phenotypes to perform a structure-function dissection of the protein domains. The reproduction of two deletions found in Kallmann's Syndrome patients determined a complete loss of function, whereas point mutations induced only minor alterations in the activity of the protein. Overexpression of the mutant proteins in the wing disc reveals that the functional relevance of the different DmKal-1 domains is dependent on the extracellular context. CONCLUSION: We suggest that the role played by the various protein domains differs in different extracellular contexts. This might explain why the same mutation analyzed in different tissues or in different cell culture lines often gives opposite phenotypes. These analyses also suggest that the FnIII repeats have a main and specific role, while the WAP domain might have only a modulator role, strictly connected to that of the fibronectins
Search for supersymmetric particles in scenarios with a gravitino LSP and stau NLSP
- Author
- Abreu P
- Adam W
- Adye T
- Adzic P
- Albrecht Z
- Alderweireld T
- Alekseev GD
- Alemany R
- Allmendinger T
- Allport PP
- Almehed S
- Amaldi U
- Amapane N
- Amato S
- Anassontzis EG
- Andersson P
- Andreazza A
- Andringa S
- Antilogus P
- Apel WD
- Arnoud Y
- Asman B
- Augustin JE
- Augustinus A
- Baillon P
- Ballestrero A
- Bambade P
- Barao F
- Barbiellini G
- Barbier R
- Bardin DY
- Barker G
- Baroncelli A
- Battaglia M
- Baubillier M
- Becks KH
- Begalli M
- Behrmann A
- Beilliere P
- Belokopytov Y
- Belous K
- Benekos NC
- Benvenuti AC
- Berat C
- Berggren M
- Bertrand D
- Besancon M
- Bilenky MS
- Bizouard MA
- Bloch D
- Blom HM
- Bonesini M
- Boonekamp M
- Booth PSL
- Borisov G
- Bosio C
- Botner O
- Boudinov E
- Bouquet B
- Bourdarios C
- Bowcock TJV
- Boyko I
- Bozovic I
- Bozzo M
- Bracko M
- Branchini P
- Brenner RA
- Bruckman P
- Brunet JM
- Bugge L
- Buran T
- Buschbeck B
- Buschmann P
- Caballero IG
- Cabrera S
- Caccia M
- Calvi M
- Camporesi T
- Canale V
- Carena F
- Carroll L
- Caso C
- Cattai A
- Cavallo FR
- Chabaud V
- Chapkin M
- Charpentier P
- Checchia P
- Chelkov GA
- Chierici R
- Chliapnikov P
- Chochula P
- Chorowicz V
- Chudoba J
- Cieslik K
- Collaboration DELPHI
- Collins P
- Contri R
- Cortina E
- Cosme G
- Cossutti F
- Costa M
- Crawley HB
- Crennell D
- Crepe S
- Crosetti G
- Czellar S
- Da Silva W
- Davenport M
- De Angelis A
- De Boer W
- De Clercq C
- De Lotto B
- De Min A
- De Paula L
- Della Ricca G
- Delpierre P
- Demaria N
- Di Ciaccio L
- Dijkstra H
- Dolbeau J
- Doroba K
- Dracos M
- Drees J
- Dris M
- Duperrin A
- Durand JD
- Eigen G
- Ekelof T
- Ekspong G
- Ellert M
- Elsing M
- Engel JP
- Fanourakis G
- Fassouliotis D
- Fayot J
- Feindt M
- Ferrer A
- Ferrer-Ribas E
- Ferro F
- Fichet S
- Firestone A
- Flagmeyer U
- Foeth H
- Fokitis E
- Fontanelli F
- Franek B
- Frodesen AG
- Fruhwirth R
- Fulda-Quenzer F
- Fuster J
- Galloni A
- Gamba D
- Gamblin S
- Gandelman M
- Garcia C
- Garcia SMI
- Gaspar C
- Gaspar M
- Gasparini U
- Gavillet P
- Gazis EN
- Gele D
- Geralis T
- Ghodbane N
- Gil I
- Gimenez MVC
- Glege F
- Gokieli R
- Golob B
- Gomez-Ceballos G
- Goncalves P
- Gopal G
- Gorn L
- Gouz Y
- Gracco V
- Grahl J
- Graziani E
- Gris P
- Grosdidier G
- Grzelak K
- Guy J
- Haag C
- Hahn F
- Hahn S
- Haider S
- Hallgren A
- Hamacher K
- Hansen J
- Harris FJ
- Hauler F
- Hedberg V
- Heising S
- Hernandez JJ
- Herquet P
- Herr H
- Hessing TL
- Heuser JM
- Higon E
- Holmgren SO
- Holt PJ
- Hoorelbeke S
- Houlden M
- Hrubec J
- Huber M
- Huet K
- Hughes GJ
- Hultqvist K
- Jackson JN
- Jacobsson R
- Jalocha P
- Janik R
- Jarlskog C
- Jarlskog G
- Jarry P
- Jean-Marie B
- Jeans D
- Johansson EK
- Jonsson P
- Joram C
- Juillot P
- Jungermann L
- Kapusta F
- Karafasoulis K
- Katsanevas S
- Katsoufis EC
- Keranen R
- Kernel G
- Kersevan BP
- Khokhlov Y
- Khomenko BA
- Khovanski NN
- Kiiskinen A
- King B
- Kinvig A
- Kjaer NJ
- Klapp O
- Klein H
- Kluit P
- Kokkinias P
- Kostioukhine V
- Kourkoumelis C
- Kouznetsov O
- Krammer M
- Kriznic E
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- Kubinec P
- Kurowska J
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- Lamsa JW
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- Maestro JC
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- Maio A
- Malek A
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- Matthiae G
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- McKay R
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- Murray WJ
- Muryn B
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- Niezurawski P
- Nikolenko M
- Nomokonov V
- Nygren A
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- Olshevski AG
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- Palka H
- Papadopoulou TD
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- Parkes C
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- Rohne O
- Romero A
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- Rosenberg EI
- Rosinsky P
- Roudeau P
- Rovelli T
- Royon C
- Ruhlmann-Kleider V
- Ruiz A
- Saarikko H
- Sacquin Y
- Sadovsky A
- Sajot G
- Salt J
- Sampsonidis D
- Sannino M
- Santo ME
- Schwemling P
- Schwering B
- Schwickerath U
- Scuri F
- Seager P
- Sedykh Y
- Segar AM
- Seibert N
- Sekulin R
- Shellard RC
- Siebel M
- Simard L
- Simonetto F
- Sisakian AN
- Smadja G
- Smirnova O
- Smith GR
- Solovianov O
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- Sosnowski R
- Spassov T
- Spiriti E
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- Strauss J
- Strub R
- Stugu B
- Szczekowski M
- Szeptycka M
- Tabarelli T
- Taffard A
- Tegenfeldt F
- Terranova F
- Thomas J
- Timmermans J
- Tinti N
- Tkatchev LG
- Tobin M
- Todorova S
- Tomaradze A
- Tome B
- Tonazzo A
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- Tortosa P
- Transtromer G
- Treille D
- Tristram G
- Trochimczuk M
- Troncon C
- Turluer ML
- Tyapkin IA
- Tyapkin P
- Tzamarias S
- Ullaland O
- Uvarov V
- Valenti G
- Vallazza E
- Van Dam P
- Van den Boeck W
- Van Eldik J
- Van Lysebetten A
- van Remortel N
- Van Vulpen I
- Vegni G
- Ventura L
- Venus W
- Verbeure F
- Verdier P
- Verlato M
- Vertogradov LS
- Verzi V
- Vilanova D
- Vitale L
- Vlasov E
- Vodopyanov AS
- Voulgaris G
- Vrba V
- Wahlen H
- Walck C
- Washbrook AJ
- Weiser C
- Wicke D
- Wickens JH
- Wilkinson GR
- Winter M
- Witek M
- Wolf G
- Yi J
- Yushchenko O
- Zalewska A
- Zalewski P
- Zavrtanik D
- Zevgolatakos E
- Zimin NI
- Zintchenko A
- Zoller P
- Zucchelli GC
- Zumerle G
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2000
- Field of study
Sleptons, neutralinos and charginos were searched for in the context of
scenarios where the lightest supersymmetric particle is the gravitino. It was
assumed that the stau is the next-to-lightest supersymmetric particle. Data
collected with the DELPHI detector at a centre-of-mass energy near 189 GeV were
analysed combining the methods developed in previous searches at lower
energies. No evidence for the production of these supersymmetric particles was
found. Hence, limits were derived at 95% confidence level.Comment: 31 pages, 14 figure
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
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- Clark PJ
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- Cochran J
- Coleman JP
- Collaboration BABAR
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- Convery MR
- Cossutti F
- Cote D
- Cottingham WN
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- Cowan G
- Cowan R
- Crawley HB
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- Plaszczynski S
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- Poireau V
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- Porter FC
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- Potter CT
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- Pulliam T
- Purohit MV
- Qi ND
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- Salnikov AA
- Salvatore F
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- Schumm BA
- Schune MH
- Schwiening J
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- Sekula SJ
- Serednyakov SI
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- Shen BC
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- Smith AJS
- Smith JG
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- Summers DJ
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- Torrence E
- Tosi S
- Touramanis C
- Ulmer KA
- Uwer U
- Va'vra J
- van Bakel N
- Vasileiadis G
- Vasseur G
- Vazquez WP
- Verderi M
- Verkerke W
- Vetere ML
- Viaud FB
- Vitale L
- Voci C
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- Wagoner DE
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- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
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- Willocq SY
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- Winklmeier F
- Wisniewski WJ
- Wittgen M
- Wong QK
- Wormser G
- Wright DH
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- Wu J
- Wu SL
- Xie Y
- Yamamoto RK
- Yarritu AK
- Ye S
- Yeche C
- 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
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
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- Zhemchugov A
- Zheng S
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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
- Author
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- Zhemchugov A
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- Zieminska D
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- Zmouchko VV
- Zobernig G
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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
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
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- Akesson TPA
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- 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
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- Yao L
- Yao 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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- Yurkewicz A
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- Zaidan R
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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
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- Acharya BS
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- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
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- Alexandre G
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- Aliev M
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- Allbrooke BMM
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- Allwood-Spiers SE
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- 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
- 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
Measurement of Trilinear Gauge Couplings in e+e− Collisions at 161 GeV and 172 GeV
- Author
- Abreu P
- Adam W
- Adye T
- Adzic P
- Alekseev GD
- Alemany R
- Allport PP
- Almehed S
- Amaldi U
- Amato S
- Andersson P
- Andreazza A
- Antilogus P
- Apel WD
- Arnoud Y
- Asman B
- Augustin JE
- Augustinus A
- Baillon P
- Bambade P
- Barao F
- Barbier R
- Bardin DY
- Barker G
- Baroncelli A
- Barring O
- Bates MJ
- Battaglia M
- Baubillier M
- Becks KH
- Begalli M
- Beilliere P
- Belokopytov Y
- Benvenuti AC
- Berat C
- Berggren M
- Bertini D
- Bertrand D
- Besancon M
- Bianchi F
- Bigi M
- Bilenky MS
- Billoir P
- Bizouard MA
- Bloch D
- Bonesini M
- Bonivento W
- Boonekamp M
- Booth PSL
- Borgland AW
- Borisov G
- Bosio C
- Botner O
- Boudinov E
- Bouquet B
- Bourdarios C
- Bowcock TJV
- Bozovic I
- Bozzo M
- Branchini P
- Brand KD
- Brenke T
- Brenner RA
- Brown R
- Bruckman P
- Brunet JM
- Bugge L
- Buran T
- Burgsmueller T
- Buschmann P
- Caballero IG
- Cabrera S
- Caccia M
- Calvi M
- Camporesi T
- Canale V
- Canepa M
- Carena F
- Carroll L
- Caso C
- Cattai A
- Cavallo FR
- Cerruti C
- Chabaud V
- Chapkin M
- Charpentier P
- Chaussard L
- Checchia P
- Chelkov GA
- Chen M
- Chierici R
- Chliapnikov P
- Chochula P
- Chorowicz V
- Chudoba J
- Collaboration D
- Collins P
- Colomer M
- Contri R
- Cortina E
- Cosme G
- Cossutti F
- Cowell JH
- Crawley HB
- Crennell D
- Crosetti G
- Czellar S
- Da Silva W
- Dalmagne B
- Damgaard G
- Dauncey PD
- Davenport M
- De Angelis A
- De Boer W
- De Brabandere S
- De Clercq C
- De la Vaissiere C
- De Lotto B
- De Min A
- De Paula L
- Deghorain A
- Della Ricca G
- Delpierre P
- Demaria N
- Di Ciaccio L
- Di Diodato A
- Dijkstra H
- Djannati A
- Dolbeau J
- Doroba K
- Dracos M
- Drees J
- Drees KA
- Dris M
- Duperrin A
- Durand JD
- Edsall D
- Ehret R
- Eigen G
- Ekelof T
- Ekspong G
- Ellert M
- Elsing M
- Engel JP
- Erzen B
- Falk E
- Fanourakis G
- Fassouliotis D
- Fayot J
- Feindt M
- Ferrari P
- Ferrer A
- Fichet S
- Firestone A
- Fischer PA
- Flagmeyer U
- Foeth H
- Fokitis E
- Fontanelli F
- Formenti F
- Franek B
- Frodesen AG
- Fruhwirth R
- Fulda-Quenzer F
- Fuster J
- Galloni A
- Gamba D
- Gandelman M
- Garcia C
- Garcia J
- Garcia SM
- Gaspar C
- Gaspar M
- Gasparini U
- Gavillet P
- Gazis EN
- Gele D
- Gerber JP
- Gerdyukov L
- Ghodbane N
- Gimenez MVC
- Glege F
- Gokieli R
- Golob B
- Goncalves P
- Gopal G
- Gorn L
- Gorski M
- Gouz Y
- Gracco V
- Grahl J
- Graziani E
- Green C
- Grefrath A
- Gris P
- Grosdidier G
- Grzelak K
- Gunther M
- Guy J
- Hahn F
- Hahn S
- Haider S
- Hajduk Z
- Hallgren A
- Hamacher K
- Harris FJ
- Hedberg V
- Heising S
- Henriques R
- Hernandez JJ
- Herquet P
- Herr H
- Hessing TL
- Heuser JM
- Higon E
- Holmgren SO
- Holt PJ
- Holthuizen D
- Hoorelbeke S
- Houlden M
- Hrubec J
- Huet K
- Hultqvist K
- Jackson JN
- Jacobsson R
- Jalocha P
- Janik R
- Jarlskog C
- Jarlskog G
- Jarry P
- Jean-Marie B
- Johansson EK
- Jonsson L
- Jonsson P
- Joram C
- Juillot P
- Kapusta F
- Karafasoulis K
- Katsanevas S
- Katsoufis EC
- Keranen R
- Khomenko BA
- Khovanski NN
- King B
- Kjaer NJ
- Klapp O
- Klein H
- Kluit P
- Knoblauch D
- Kokkinias P
- Koratzinos M
- Korcyl K
- Kostioukhine V
- Kourkoumelis C
- Kouznetsov O
- Krammer M
- Kreuter C
- Kronkvist I
- Krumstein Z
- Kubinec P
- Kucewicz W
- Kurvinen K
- Lacasta C
- Lamsa JW
- Lanceri L
- Lane DW
- Langefeld P
- Lapin V
- Laugier JP
- Lauhakangas R
- Leder G
- Ledroit F
- Lefebure V
- Legan CK
- Leisos A
- Leitner R
- Lemonne J
- Lenzen G
- Lepeltier V
- Lesiak T
- Lethuillier M
- Libby J
- Liko D
- Lipniacka A
- Lippi I
- Loerstad B
- Loken JG
- Lopes JH
- Lopez JM
- Loukas D
- Lutz P
- Lyons L
- MacNaughton J
- Maestro JC
- Mahon JR
- Maio A
- Malek A
- Malmgren TGM
- Malychev V
- Mandl F
- Marco J
- Marco R
- Marechal B
- Margoni M
- Marin JC
- Mariotti C
- Markou A
- Martinez-Rivero C
- Martinez-Vidal F
- Matorras F
- Matteuzzi C
- Matthiae G
- Mazzucato F
- Mazzucato M
- Mc Cubbin M
- Mc Kay R
- Mc Nulty R
- Mc Pherson G
- Medbo J
- Meroni C
- Meyer WT
- Michelotto M
- Migliore E
- Mirabito L
- Mitaroff WA
- Mjoernmark U
- Moa T
- Moeller R
- Moenig K
- Monge MR
- Moreau X
- Morettini P
- Muenich K
- Mulders M
- Mundim LM
- Murray WJ
- Muryn B
- Myatt G
- Myklebust T
- Naraghi F
- Navarria FL
- Navas S
- Nawrocki K
- Negri P
- Nemecek S
- Neufeld N
- Neumann W
- Neumeister N
- Nicolaidou R
- Nielsen BS
- Nieuwenhuizen M
- Nikolaenko V
- Nikolenko M
- Niss P
- Nomerotski A
- Normand A
- Nygren A
- Oberschulte-Beckmann W
- Obraztsov V
- Olshevski AG
- Onofre A
- Orava R
- Orazi G
- Osterberg K
- Ouraou A
- Paganini P
- Paganoni M
- Paiano S
- Pain R
- Paiva R
- Palka H
- Papadopoulou TD
- Papageorgiou K
- Pape L
- Parkes C
- Parodi F
- Parzefall U
- Passeri A
- Pegoraro M
- Pernegger H
- Pernicka M
- Perrotta A
- Petridou C
- Petrolini A
- Phillips HT
- Piana G
- Pierre F
- Pimenta M
- Piotto E
- Podobnik T
- Podobrin O
- Pol ME
- Polok G
- Poropat P
- Pozdniakov V
- Privitera P
- Pukhaeva N
- Pullia A
- Radojicic D
- Ragazzi S
- Rahmani H
- Rames J
- Ratoff PN
- Read AL
- Rebecchi P
- Redaelli NG
- Regler M
- Reid D
- Reinhardt R
- Renton PB
- Resvanis LK
- Richard F
- Ridky J
- Rinaudo G
- Rohne O
- Romero A
- Ronchese P
- Rosenberg EI
- Rosinsky P
- Roudeau P
- Rovelli T
- Rozas AJC
- Ruhlmann-Kleiner V
- Ruiz A
- Saarikko H
- Sacquin Y
- Sadovsky A
- Sajot G
- Salt J
- Sampsonidis D
- Sannino M
- Santo ME
- Schneider H
- Schwickerath U
- Schyns MAE
- Scuri F
- Seager P
- Sedykh Y
- Segar AM
- Sekulin R
- Senko V
- Shellard RC
- Sheridan A
- Silvestre R
- Simonetto F
- Sisakian AN
- Skaali TB
- Smadja G
- Smirnov N
- Smirnova O
- Smith GR
- Solovianov O
- Sopczak A
- Sosnowski R
- Souza-Santos D
- Spassov T
- Spiriti E
- Sponholz P
- Squarcia S
- Stampfer D
- Stanescu C
- Stanic S
- Stapnes S
- Stavitski I
- Stevenson K
- Stocchi A
- Strauss J
- Strub R
- Stugu B
- Szczekowski M
- Szeptycka M
- Tabarelli T
- Tchikilev O
- Tegenfeldt F
- Terranova F
- Thomas J
- Tilquin A
- Timmermans J
- Tkatchev LG
- Todorov T
- Todorova S
- Toet DZ
- Tomaradze A
- Tome B
- Tonazzo A
- Tortora L
- Transtromer G
- Treille D
- Tristram G
- Trombini A
- Troncon C
- Tsirou A
- Turluer ML
- Tyapkin IA
- Tyndel M
- Tzamarias S
- Ueberschaer B
- Ullaland O
- Uvarov V
- Valenti G
- Vallazza E
- Van Apeldoorn GW
- Van Dam P
- Van Doninck WK
- Van Eldik J
- Van Lysebetten A
- Van Vulpen I
- Vassilopoulos N
- Vegni G
- Ventura L
- Venus W
- Verbeure F
- Verlato M
- Vertogradov LS
- Verzi V
- Vilanova D
- Vincent P
- Vishnevsky N
- Vitale L
- Vlasov E
- Vodopyanov AS
- Vrba V
- Wahlen H
- Walck C
- Waldner F
- Weiser C
- Wetherell AM
- Wicke D
- Wickens JH
- Wilkinson GR
- Williams WSC
- Winter M
- Witek M
- Wlodek T
- Wolf G
- Yi J
- Yushchenko O
- Zalewska A
- Zalewski P
- Zavrtanik D
- Zevgolatakos E
- Zimin NI
- Zucchelli GC
- Zumerle G
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/1997
- Field of study
Trilinear gauge boson couplings are measured using data taken by DELPHI at 161~GeV and 172~GeV. Values for WWV couplings (V=Z,γ) are determined from a study of the reactions \eeWW\ and \eeWev, using differential distributions from the WW final state in which one W decays hadronically and the other leptonically, and total cross-section data from other channels. Limits are also derived on neutral ZVγ couplings from an analysis of the reaction \eegi
Search for neutral heavy leptons produced in Z decays
- Author
- Abreu P
- Adam W
- Adye T
- Alekseev GD
- Alemany R
- Allport P P
- Almehed S
- Amaldi U
- Amato S
- Andreazza A
- Andrieux ML
- Antilogus P
- Apel WD
- Asman BAA
- Augustin JE
- Augustinus A
- Azhinenko I
- Baillon P
- Bambade P
- Barao F
- Barbi M
- Barbiellini G
- Bardin D Yu
- Barker G
- Baroncelli A
- Barring O
- Barrio JA
- Bartl W
- Bates MJ
- Battaglia M
- Baubillier M
- Baudot J
- Becks KH
- Begalli M
- Beilliere P
- Belokopytov Yu
- Benvenuti AC
- Berggren M
- Bertini D
- Bertrand D
- Besancon M
- Bianchi F
- Bigi M
- Bilenky MS
- Billoir P
- Bizouard MA
- Bloch D
- Blume M
- Bolognese T
- Bonesini M
- Bonivento W
- Booth PSL
- Bosio C
- Botner O
- Boudinov E
- Bouquet B
- Bourdarios C
- Bowcock TJV
- Bozzo M
- Branchini P
- Brand KD
- Brenke T
- Brenner RA
- Bricman C
- Brown RCA
- Bruckman P
- Brunet JM
- Bugge L
- Buran T
- Burgsmueller T
- Buschmann P
- Cabrera S
- Caccia M
- Calvi M
- Camacho Rozas AJ
- Camporesi T
- Canale V
- Canepa M
- Cankocak K
- Cao F
- Carena F
- Carroll L
- Caso C
- Castillo Gimenez MV
- Cattai A
- Cavallo FR
- Chabaud V
- Chapkin M
- Charpentier P
- Chaussard L
- Checchia P
- Chelkov GA
- Chen M
- Chierici R
- Chikilev O
- Chliapnikov P
- Chochula P
- Chorowicz V
- Chudoba J
- Cindro V
- Collins P
- Contri R
- Cortina E
- Cosme G
- Cossutti F
- Cowell JH
- Crawley HB
- Crennell D
- Crosetti G
- Cuevas Maestro J
- Czellar S
- D'Almagne B
- Da Silva W
- Dahl-Jensen E
- Dahm J
- Dam M
- Damgaard G
- Dauncey PD
- Davenport M
- De Angelis A
- de Boer W
- De Brabandere S
- De Clercq C
- de la Vaissiere C
- De Lotto B
- De Min A
- De Paula L
- De Saint-Jean C
- Defoix C
- Deghorain A
- Della Ricca G
- Delpierre P
- Demaria N
- Di Ciaccio L
- Di Diodato A
- Dijkstra H
- Djama F
- Djannati A
- Dolbeau J
- Doroba K
- Dracos M
- Drees J
- Drees KA
- Dris M
- Durand JD
- Edsall D
- Ehret R
- Eigen G
- Ekelof T
- Ekspong G
- Elsing M
- Engel JP
- Erzen B
- Espirito Santo M
- Falk E
- Fassouliotis D
- Feindt M
- Fenyuk A
- Ferrer A
- Fichet S
- Filippas TA
- Firestone A
- Fischer PA
- Foeth H
- Fokitis E
- Fontanelli F
- Formenti F
- Franek B
- Frenkiel P
- Fries DC
- Frodesen AG
- Fruhwirth R
- Fulda-Quenzer F
- Fuster J
- Galloni A
- Gamba D
- Gandelman M
- Garcia C
- Garcia J
- Gaspar C
- Gasparini U
- Gavillet P
- Gazis EN
- Gele D
- Gerber JP
- Gerdyukov L
- Gokieli R
- Golob B
- Gopal G
- Gorn L
- Gorski M
- Gouz Yu
- Gracco V
- Graziani E
- Green C
- Grefrath A
- Gris P
- Grosdidier G
- Grzelak K
- Gumenyuk S
- Gunnarsson P
- Gunther M
- Guy J
- Hahn F
- Hahn S
- Hajduk Z
- Hallgren A
- Hamacher K
- Harris FJ
- Hedberg V
- Henriques R
- Hernandez JJ
- Herquet P
- Herr H
- Hessing TL
- Heuser JM
- Higon E
- Hilke HJ
- Hill TS
- Holmgren SO
- Holt PJ
- Holthuizen D
- Hoorelbeke S
- Houlden M
- Hrubec J
- Huet K
- Hultqvist K
- Jackson JN
- Jacobsson R
- Jalocha P
- Janik R
- Jarlskog C
- Jarlskog G
- Jarry P
- Jean-Marie B
- Johansson EK
- Jonsson L
- Jonsson P
- Joram C
- Juillot P
- Kaiser M
- Kapusta F
- Karafasoulis K
- Karlsson M
- Karvelas E
- Katsanevas S
- Katsoufis EC
- Keranen R
- Khokhlov Yu
- Khomenko BA
- Khovansky NN
- King B
- Kjaer NJ
- Klapp O
- Klein H
- Klovning A
- Kluit P
- Koene B
- Kokkinias P
- Koratzinos M
- Korcyl K
- Kostioukhine V
- Kourkoumelis C
- Kouznetsov O
- Krammer M
- Kreuter C
- Kronkvist I
- Krumshtein Z
- Krupinski W
- Kubinec P
- Kucewicz W
- Kurvinen K
- Lacasta C
- Laktineh I
- Lamsa JW
- Lanceri L
- Lane DW
- Langefeld P
- Lapin V
- Laugier JP
- Lauhakangas R
- Leder G
- Ledroit F
- Lefebure V
- Legan CK
- Leitner R
- Lemonne J
- Lenzen G
- Lepeltier V
- Lesiak T
- Libby J
- Liko D
- Lindner R
- Lipniacka A
- Lippi I
- Loken JG
- Lopez JM
- Lorstad B
- Loukas D
- Lutz P
- Lyons L
- MacNaughton J
- Maehlum G
- Mahon JR
- Maio A
- Malmgren TGM
- Malychev V
- Mandl F
- Marco J
- Marco R
- Marechal B
- Margoni M
- Marin JC
- Mariotti C
- Markou A
- Marti i Garcia S
- Martinez-Rivero C
- Martinez-Vidal F
- Masik J
- Matorras F
- Matteuzzi C
- Matthiae G
- Mazzucato M
- McCubbin M
- McKay R
- McNulty R
- Medbo J
- Merk M
- Meroni C
- Meyer S
- Meyer WT
- Michelotto M
- Migliore E
- Mirabito L
- Mitaroff WA
- Mjornmark U
- Moa T
- Moller R
- Monge MR
- Monig K
- Morettini P
- Mulders M
- Muller H
- Mundim LM
- Munich K
- Murray W J
- Muryn B
- Myatt G
- Naraghi F
- Navarria FL
- Navas S
- Nawrocki K
- Negri P
- Nemecek S
- Neumann W
- Nicolaidou R
- Nielsen BS
- Nieuwenhuizen M
- Nikolaenko V
- Niss P
- Nomerotski A
- Normand A
- Oberschulte-Beckmann W
- Obraztsov V
- Olshevsky AG
- Onofre A
- Orava R
- Osterberg K
- Ouraou A
- Paganini P
- Paganoni M
- Pages P
- Pain R
- Palka H
- Papadopoulou TD
- Papageorgiou K
- Pape L
- Parkes C
- Parodi F
- Passeri A
- Pegoraro M
- Peralta L
- Pernegger H
- Pernicka M
- Perrotta A
- Petridou C
- Petrolini A
- Petrovyck M
- Phillips HT
- Piana G
- Pierre F
- Pimenta M
- Podobnik T
- Podobrin O
- Pol ME
- Polok G
- Poropat P
- Pozdniakov V
- Privitera P
- Pukhaeva N
- Pullia A
- Radojicic D
- Ragazzi S
- Rahmani H
- Ratoff PN
- Read AL
- Reale M
- Rebecchi P
- Redaelli NG
- Regler M
- Reid D
- Reinhardt R
- Renton PB
- Resvanis LK
- Richard F
- Richardson J
- Ridky J
- Rinaudo G
- Ripp I
- Romero A
- Roncagliolo I
- Ronchese P
- Roos L
- Rosenberg EI
- Roudeau P
- Rovelli T
- Ruckstuhl W
- Ruhlmann-Kleider V
- Ruiz A
- Rybicki K
- Saarikko H
- Sacquin Y
- Sadovsky A
- Sahr O
- Sajot G
- Salt J
- Sanchez J
- Sannino M
- Schimmelpfennig M
- Schneider H
- Schwickerath U
- Schyns MAE
- Sciolla G
- Scuri F
- Seager P
- Sedykh Y
- Segar AM
- Seitz A
- Sekulin R
- Serbelloni L
- Shellard RC
- Siegrist P
- Silvestre R
- Simonetti S
- Simonetto F
- Sisakian AN
- Sitar B
- Skaali TB
- Smadja G
- Smirnov N
- Smirnova O
- Smith G R
- Sosnowski R
- Souza-Santos D
- Spassov T
- Spiriti E
- Sponholz P
- Squarcia S
- Stampfer D
- Stanescu C
- Stanic S
- Stapnes S
- Stavitski I
- Stevenson K
- Stocchi A
- Strauss J
- Strub R
- Stugu B
- Szczekowski M
- Szeptycka M
- Tabarelli T
- Tavernet JP
- Thomas J
- Tilquin A
- Timmermans J
- Tkachev LG
- Todorov T
- Todorova S
- Toet DZ
- Tomaradze A
- Tonazzo A
- Tortora L
- Transtromer G
- Treille D
- Tristram G
- Trombini A
- Troncon C
- Tsirou A
- Turluer ML
- Tyapkin IA
- Tyndel M
- Tzamarias S
- Uberschar B
- Ullaland O
- Uvarov V
- Valenti G
- Vallazza E
- van Apeldoorn GW
- van Dam P
- Van Doninck WK
- Van Eldik J
- Van Lysebetten A
- Vander Velde C
- Vassilopoulos N
- Vegni G
- Ventura L
- Venus W
- Verbeure F
- Verlato M
- Vertogradov LS
- Vilanova D
- Vincent P
- Vitale L
- Vlasov E
- Vodopyanov AS
- Vrba V
- Wahlen H
- Walck C
- Weierstall M
- Weilhammer P
- Weiser C
- Wetherell AM
- Wicke D
- Wickens JH
- Wielers M
- Wilkinson G R
- Williams WSC
- Winter M
- Witek M
- Wlodek T
- Woschnagg K
- Yip K
- Yushchenko O
- Zach F
- Zaitsev A
- Zalewska A
- Zalewski P
- Zavrtanik D
- Zevgolatakos E
- Zimin NI
- Zito M
- Zontar D
- Zucchelli GC
- Zumerle G
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1996
- Field of study
Weak isosinglet Neutral Heavy Leptons (νm) have been searched for using data collected by the DELPHI detector corresponding to 3.3 × 106 hadronic Z0 decays at LEP1. Four separate searches have been performed, for short-lived νm production giving monojet or acollinear jet topologies, and for long-lived νm giving detectable secondary vertices or calorimeter clusters. No indication of the existence of these particles has been found, leading to an upper limit for the branching ratio BR(Z0 → νmν̄) of about 1.3 × 10-6 at 95% confidence level for νm masses between 3.5 and 50 GeV/c2. Outside this range the limit weakens rapidly with the νm mass. The results are also interpreted in terms of limits for the single production of excited neutrinos. © Springer-Verlag 1997
Study of B0_s anti-B0_s oscillations and B0_s lifetimes using hadronic decays of B0_s mesons
- Author
- Abreu P
- Adam W
- Adye T
- Adzic P
- Ajinenko I
- Albrecht Z
- Alderweireld T
- Alekseev GD
- Alemany R
- Allmendinger T
- Allport PP
- Almehed S
- Amaldi U
- Amapane N
- Amato S
- Anassontzis EG
- Andersson P
- Andreazza A
- Andringa S
- Antilogus P
- Apel WD
- Arnoud Y
- Asman B
- Augustin JE
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- Baillon P
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- Barker G
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- Collaboration DELPHI
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2000
- Field of study
Oscillations of B0s mesons have been studied in samples selected from about
3.5 million hadronic Z decays detected by DELPHI between 1992 and 1995. One
analysis uses events in the exclusive decay channels: B0s -> Ds- pi+ or Ds- a1+
and B0s -> anti-D0 K- pi+ or anti-D0 K- a1+, where the D decays are completely
reconstructed. In addition, B0s anti-B0s oscillations have been studied in
events with an exclusively reconstructed Ds accompanied in the same hemisphere
by a high momentum hadron of opposite charge. Combining the two analyses, a
limit on the mass difference between the physical B0s states has been obtained:
Delta(m_B0s) > 4.0 ps^{-1} at the 95% C.L. with a sensitivity of Delta(m_B0s)
= 3.2 ps^{-1}. Using the latter sample of events, the B0s lifetime has been
measured and an upper limit on the decay width difference between the two
physical B0s states has been obtained:
tau(B0s) = 1.53^{+0.16}_{-0.15}(stat.) +/- {0.07}(syst.) ps
\Delta\Gamma(B0s)/\Gamma(B0s) < 0.69 at the 95% C.L.
The combination of these results with those obtained using Ds+- lepton-+
sample gives:
Delta(m_B0s) > 4.9 ps^{-1} at the 95% C.L.
with a sensitivity of Delta(m_B0s) = 8.7 ps^{-1}.
tau(B0s) = 1.46 +/- 0.11 ps and \Delta\Gamma(B0s)/\Gamma(B0s) < 0.45 at the
95% C.L.Comment: 42 pages, 13 figure
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