13 research outputs found
DIII-D research advancing the physics basis for optimizing the tokamak approach to fusion energy
- Author
- Abbate J.
- Abe S.
- Abrams T.
- Adams M.
- Adamson B.
- Aiba N.
- Akiyama Tsuyoshi
- Aleynikov P B
- Allen E.
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- Anand H.
- Anderson Johan
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- Appelt D.
- Arbon R.
- Ashikawa N.
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- Austin M.
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- Cruz Zabala D.J.
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- Dal Molin A.
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- Davda K.
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- Wu Y.
- Wukitch S.
- Wurden G.
- Xiao W.
- Xie R.
- Xing Z.
- Xu C.
- Xu G.
- Xu X.
- Yan Z.
- Yang S.
- Yang X.
- Yokoyama T.
- Yoneda R.
- Yoshida Maiko
- You K.
- Younkin T.
- Yu G.
- Yu J.
- Yu M.
- Yuan Q.
- Zaidenberg L.
- Zakharov L.
- Zamengo A.
- Zamperini S.
- Zarnstorff M.
- Zeger E.
- Zeller K.
- Zeng L.
- Zerbini M.
- Zhang B.
- Zhang J.
- Zhang J.
- Zhang L.
- Zhang R.
- Zhang X.
- Zhao B.
- Zhao L.
- Zheng L.
- Zheng Y.
- Zhu B.
- Zhu J.
- Zhu Y.
- Zhu Y.
- Zsutty M.
- Zuin M.
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2022
- Field of study
Get PDFFunding Information: This material is based upon work supported by the US Department of Energy, Office of Science, Office of Fusion Energy Sciences, using the DIII-D National Fusion Facility, a DOE Office of Science user facility, under Awards DE-FC02-04ER54698 and DE-AC52-07NA27344. Publisher Copyright: © 2022 IAEA, Vienna.DIII-D physics research addresses critical challenges for the operation of ITER and the next generation of fusion energy devices. This is done through a focus on innovations to provide solutions for high performance long pulse operation, coupled with fundamental plasma physics understanding and model validation, to drive scenario development by integrating high performance core and boundary plasmas. Substantial increases in off-axis current drive efficiency from an innovative top launch system for EC power, and in pressure broadening for Alfven eigenmode control from a co-/counter-I p steerable off-axis neutral beam, all improve the prospects for optimization of future long pulse/steady state high performance tokamak operation. Fundamental studies into the modes that drive the evolution of the pedestal pressure profile and electron vs ion heat flux validate predictive models of pedestal recovery after ELMs. Understanding the physics mechanisms of ELM control and density pumpout by 3D magnetic perturbation fields leads to confident predictions for ITER and future devices. Validated modeling of high-Z shattered pellet injection for disruption mitigation, runaway electron dissipation, and techniques for disruption prediction and avoidance including machine learning, give confidence in handling disruptivity for future devices. For the non-nuclear phase of ITER, two actuators are identified to lower the L-H threshold power in hydrogen plasmas. With this physics understanding and suite of capabilities, a high poloidal beta optimized-core scenario with an internal transport barrier that projects nearly to Q = 10 in ITER at ∼8 MA was coupled to a detached divertor, and a near super H-mode optimized-pedestal scenario with co-I p beam injection was coupled to a radiative divertor. The hybrid core scenario was achieved directly, without the need for anomalous current diffusion, using off-axis current drive actuators. Also, a controller to assess proximity to stability limits and regulate β N in the ITER baseline scenario, based on plasma response to probing 3D fields, was demonstrated. Finally, innovative tokamak operation using a negative triangularity shape showed many attractive features for future pilot plant operation.Peer reviewe
Search for radiative b-hadron decays in p(p)over-bar collisions at root s=1.8 TeV RID C-1693-2008 RID A-5169-2010 RID E-4473-2011 RID C-2406-2008
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2002
- Field of study
No full textWe have performed a search for radiative b-hadron decays using events produced in p (p) over bar collisions at roots=1.8 TeV and collected by the Collider Detector at Fermilab. The decays we considered were (B) over bar (0)(d)-->(K) over bar*(0)(-->K(-)pi(+))gamma, (B) over bar (0)(s)-->phi(-->K+K-)gamma, Lambda(b)(0)-->Lambda(-->ppi(-))gamma, and their charge conjugates. Two independent methods to identify photons from such decays were employed. In the first method, the photon was detected in the electromagnetic calorimeter. In the second method, the photon was identified by an electron-positron pair produced through the external photon conversion before the tracking detector volume. By combining the two methods we obtain upper limits on the branching fractions for the (B) over bar (0)(d), (B) over bar (0)(s), and Lambda(b)(0) radiative decays which, at the 95% confidence level, are found to be B((B) over bar (0)(d)-->(K) over bar*(0)gamma)phigamma)Lambdagamma)<1.9x10(-3)
Measurement of time-dependent CP asymmetries and the CP-odd fraction in the decay B-0 -> D*+D*- RID C-2728-2008 RID C-5223-2009 RID C-5719-2008 RID D-1055-2009 RID A-2675-2009
- Author
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- Abe T
- Abrams GS
- Adam I.
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- Alam MS
- Albert J
- Albert J.
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- Altenburg D
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- Anthony P. L.
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2003
- Field of study
No full textWe present a measurement of time-dependent CP asymmetries and an updated determination of the CP-odd fraction in the decay B-0-->D*+D*- using a data sample of 88x10(6)B (B) over bar pairs collected by the BABAR detector at the PEP-II B Factory at SLAC. We determine the CP-odd fraction to be 0.063+/-0.055(stat)+/-0.009(syst). The time-dependent CP asymmetry parameters Im(lambda(+)) and \lambda(+)\ are determined to be 0.05+/-0.29(stat)+/-0.10(syst) and 0.75+/-0.19(stat)+/-0.02(syst), respectively. The standard model predicts these parameters to be -sin2beta and 1, respectively, in the absence of penguin diagram contributions
Simultaneous measurement of the B-0 meson lifetime and mixing frequency with B-0 -> D(*-)l(+)nu(l) decays RID C-2728-2008 RID C-5223-2009 RID C-5719-2008 RID D-1055-2009 RID A-2675-2009
- Author
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- Adesanya A.
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- Kral JF
- Kravchenko EA
- Krebs H. J.
- Krishnamurthy M
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- Kurup A
- Kutter PE
- Kuznetsova N
- Kyberd P
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- Lafferty GD
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- Lamsa J
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- Luitz S
- Luitz S.
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- Madani S.
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- Mandelkern M
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- McKenna JA
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- Messner R
- Messner R.
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- Metcalfe S.
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- Meyer WT
- Micout P.
- Miftakov V
- Miftakov V.
- Mihalyi A
- Milek M
- Mir LM
- Mohapatra AK
- Mohapatra AK
- Mols J. P.
- Mommsen RK
- Monge MR
- Moore TB
- Morandin M
- Morganti M
- Morganti M.
- Morganti S
- Morganti S.
- Morii M
- Morii M.
- Morsani F.
- Morton GW
- Mouly J. P.
- Mount R.
- Muheim F
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- Narsky I
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- Paar HP
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- Paick K.
- Palano A
- Palombo F
- Pan Y
- Pan Y
- Pan Y
- Panetta J
- Panvini R. S.
- Panvini RS
- Panvini RS
- Paoloni E
- PAOLONI EUGENIO
- Paolucci P
- Paolucci P.
- Passaggio S
- Pastore FC
- Patel PM
- Patrignani C
- Patteri P
- Pavel T.
- Payne DJ
- Pelizaeus M
- Penichot Y.
- Penny RC
- Perazzo A
- Perl J.
- Perl M
- Pertsova M.
- Peruzzi IM
- Peters K
- Petersen TC
- Petrak S
- Petrak S.
- Piccolo D
- Piccolo M
- Piemontese L
- Piredda G
- Piredda G.
- Pitman D.
- Pivk M
- Plano R. J.
- Plaszczynski S
- Playfer S
- Pompili A
- Pompili A
- Pompili A.
- Poropat P
- Poropat P.
- Porter FC
- Posocco M
- Potter CT
- Prell S
- Prepost R
- Prepost R
- Prepost R
- Prest M.
- Pripstein M
- Profeti A.
- Pulliam T
- Purohit M. V.
- Purohit MV
- Putallaz G.
- Qi ND
- Raffaelli F.
- Rahatlou S
- Raines P. E.
- Rama M
- Rama M.
- Rankin P
- Rashevskaia I.
- Ratcliff B. N.
- Ratcliff BN
- Raven G
- Re V
- Reidy J
- Reif R.
- RI Roe Natalie/A
- Ricciardi S
- Richman JD
- Rizzo G.
- RIZZO GIULIANA
- Roat C
- Roat C.
- Robbe P
- Roberts DA
- Robertson S. H.
- Robertson SH
- Robutti E
- Rochester L. S.
- Roe NA
- Rolquin J.
- Romosan A
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- Sapozhnikov L.
- Sarti A
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- Saxton O. H.
- Schaffner S. F.
- Schalk T
- Schietinger T
- Schietinger T.
- Schindler R. H.
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- Schmitz RE
- Schmuecker H
- Schott G
- Schubert KR
- Schumm BA
- Schune MH
- Schwanke U
- Schwiening J
- Schwiening J.
- Schwierz R
- Sciacca C
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- Scott IJ
- Seeman J. T.
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- Serednyakov SI
- Serfass B
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- Shapiro S.
- Sharma V
- Shelkov VG
- Shorthouse HW
- Simi G
- Simi G.
- Simonetto F
- Sinev NB
- Skarpass Sr K.
- Skovpen YI
- Sloane RJ
- Smith A. J. S.
- Smith AJS
- Smith JG
- Smol A
- Smol A.
- Snyder A
- Snyder A.
- Soderstrom E.
- Soffer A
- Soha A
- Soha A.
- Sokoloff MD
- Spaan B
- Spanier S. M.
- Spanier SM
- Speziali V
- Staengle H
- Stahl A.
- Stark J
- Steinke M
- Stelzer J
- Stiles P.
- Stoker DP
- Stroili R
- Strom D
- Strother P
- Stugu B
- Su D
- Su D.
- Sullivan M. K.
- Sullivan MK
- Summers DJ
- Swain JE
- T'Jampens S
- Talby M.
- Tanaka H. A.
- Tanaka HA
- Tantot L
- Taras P
- Taylor F
- Taylor GP
- Tehrani FS
- Telnov AV
- Thiebaux C
- Thiessen D
- Tinslay J
- Tiozzo G
- Tisserand V
- Toki WH
- Torrence E
- Tosi S
- Touramanis C
- Toussaint J. C.
- Trapani P. P.
- Treadwell E
- Triggiani G.
- TRIGGIANI GIUSEPPE
- Tumanov A
- Tumanov A.
- Turcotte M.
- Turnbull L
- Turnbull L.
- Turri M
- Usseglio M.
- Va'vra J
- Va'vra J.
- Vaitsas G
- Vallazza E.
- van Bibber K
- van Hoek WC
- Varnes E. W.
- Varnes EW
- Vasileiadis G
- Vasseur G
- Vasseur G.
- Verderi M
- Verkerke W
- Vidal PB
- Vitale L
- Voci C
- Voena C
- Voena C.
- von Wimmerspeig Toeller JH
- von Wimmersperg Toeller JH
- von Wimmersperg Toeller JH
- Vuagnin G
- Vuagnin G
- Vuagnin G.
- Wagner G
- Wagner S. R.
- Wagner SR
- Wagoner D. E.
- Wagoner DE
- Waldi R
- Waldi R.
- Walkowiak W
- Walsh J
- Wang P
- Wang R.
- Watson AT
- Watson NK
- Watt M.
- Weatherall JH
- Weaver M
- Weber T.
- Weidemann A. W.
- Weidemann AW
- Weinstein A. J. R.
- Weinstein AJR
- Wenzel WA
- White J. L.
- Wienands U.
- Wilden L
- Williams DC
- Williams JC
- Willocq S
- Wilson FF
- Wilson MG
- Wilson RJ
- Winter MA
- Wisniewski W. J.
- Wisniewski WJ
- Wormser G
- Wright DH
- Wright DM
- Wu J
- Wu J
- Wu J
- Wu SL
- Wu SL
- Wu SL
- Wu SL
- Xella S. M.
- Xella SM
- Yamamoto RK
- Yang S
- Yeche C
- Yeche C.
- Yi J
- Young C. C.
- Young CC
- Yu N.
- Yu Z
- Yu Z
- Yu Z
- Yu Z
- Yumiceva F. X.
- Yumiceva FX
- Yushkov AN
- Zallo A
- Zanin D
- Zanin D.
- Zghiche A
- Zhang J
- Zhang L
- Zhao H
- Zhu YS
- Zito M
- Zito M.
- Zobernig H
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2003
- Field of study
No full textWe measure the B-0 lifetime tau(B)(0) and the B-0-(B) over bar (0) oscillation frequency Deltam(d) with a sample of approximately 14000 exclusively reconstructed B-0-->D(*-)l(+)nul signal events, selected from 23 million B (B) over bar pairs recorded at the Y(4S) resonance with the BABAR detector at the Stanford Linear Accelerator Center. The decay position of the other B is determined with the remaining tracks in the event, and its b-quark flavor at the time of decay is determined with a tagging algorithm that exploits the correlation between the flavor of the b quark and the charges of its decay products. The lifetime and oscillation frequencies are measured simultaneously with an unbinned maximum-likelihood fit that uses, for each event, the measured difference in decay times of the two B mesons (Deltat), the calculated uncertainty on Deltat, the signal and background probabilities, and b-quark tagging information for the other B. The results are tau(B)(0)=(1.523(-0.023)(+0.024)+/-0.022) ps and Deltam(d)=(0.492+/-0.018+/-0.013) ps(-1). The statistical correlation coefficient between tau(B)(0) and Deltam(d) is -0.22
Recommended from our members
The BABAR detector
- Author
- Abbott B
- Abe K
- Abrams GS
- Adam I
- Adesanya A
- Adye T
- Ahsan A
- Albert J
- Albert JN
- Aleksan R
- Alford O
- Allison J
- Alsmiller JRG
- Amerman L
- Andress JC
- Angelini C
- Anjomshoaa A
- Anthony PL
- Antohin EI
- Anulli F
- Arguin JF
- Arisaka K
- Aspinwall ML
- Aston D
- Aubert B
- Azzopardi DE
- Back JJ
- Bagnasco S
- Bailly P
- Baldini-Ferroli R
- Band HR
- Bard R
- Barlow NR
- Barlow RJ
- Bartelt J
- Bartoldus R
- Batignani G
- Bauer JM
- Bazan A
- Beaulieu M
- Becla J
- Behne D
- Behr L
- Beigbeder C
- Bell R
- Benayoun M
- Benkebil M
- Benninger T
- Beringer J
- Bernard D
- Bernet R
- Berridge S
- Besson P
- Bettarini S
- Bhimji W
- Bianchi F
- Bionta RM
- Blaylock G
- Blinov VE
- Bloom E
- Bloom P
- Blouw J
- Boeheim CT
- Bona M
- Bondioli M
- Bonneaud GR
- Booke M
- Booth J
- Borgland AW
- Bosi F
- Bosisio L
- Boucham A
- Bourgeois P
- Boutigny D
- Bowerman DA
- Bowman J
- Boyarski AM
- Boyce RF
- Boyd JT
- Bozzi C
- Brandt T
- Brau B
- Breon AB
- Breton D
- Briand H
- Briggs D
- Bright-Thomas PG
- Brigljevic V
- Britton DI
- Brochard F
- Bronzini F
- Brooks A
- Broomer B
- Brose J
- Brown C
- Brown D
- Brown DN
- Buccheri A
- Buchanan C
- Bugg W
- Bukin AD
- Bukin DA
- Bula C
- Bulfon C
- Bulos F
- Burchat PR
- Burgess W
- Burke S
- Button-Shafer J
- Buzykaev AR
- Buzzo A
- Byers B
- Calcaterra A
- Calderini G
- Callahan D
- Camanzi B
- Campagnari C
- Caracciolo R
- Carpinelli M
- Carroll M
- Cartaro C
- Cason NM
- Cavallo N
- Cavoto G
- Charles E
- Chauveau J
- Chen E
- Chen GP
- Chen JC
- Cheng CH
- Chestnut R
- Chevalier N
- Chun S
- Cizeron R
- Clark AR
- Clark PJ
- Claus R
- Claxton B
- Cochran J
- Cohen-Tanugi J
- Cohn H
- Colecchia F
- Contri R
- Convert P
- Convery MR
- Cooke P
- Coombes R
- Copty N
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- Cottrell L
- Coupal DP
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- Coward DH
- Craddock WW
- Crawley HB
- Cremaldi L
- Crosetti G
- Dacosta VA
- Dahlinger G
- Dahmes B
- Dal Corso F
- Dallapiccola C
- Dardin S
- Dasu S
- Daudo F
- Dauncey PD
- David P
- Davis CL
- Day C
- De Bonis I
- De Domenico G
- de Freitas PM
- De Groot N
- De la Vaissiere C
- de Lesquen A
- de Monchenault GH
- De Nardo G
- de Sangro R
- De Silva A
- DeBarger S
- Del Buono L
- del Re D
- Della Ricca G
- Deppermann T
- DeStaebler H
- Devmal S
- DeWitt J
- Di Girolamo B
- Di Lodovico F
- Dickopp M
- Dignan T
- Dittongo S
- Dixon P
- Dorfan DE
- Dorfan J
- Doser M
- Dow SF
- Dowdell J
- Du S
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- Dubois-Felsmann GP
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- Dyce N
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- Eisner AM
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- Erdos E
- Eschrich I
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- Faccini R
- Fackler O
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- Fan Q
- Farbin A
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- Fernholz R
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- Fieguth TH
- Finocchiaro G
- Fischer PA
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- Ford WT
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- Foster B
- Fouque G
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- Frank ED
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- Freytag DR
- Fry JR
- Fujino D
- Fullwood J
- Futterschneider H
- Gabathuler E
- Gabriel TA
- Gaddi A
- Gaede F
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- Galagedera S
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- Heck J
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- Heusch CA
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- Krishnamurthy M
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- Long M
- Long O
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- Lou XC
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- Lu C
- Luft P
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- Luo L
- Lusiani A
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- Lutz AM
- Lynch G
- Lynch HL
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- Mallik U
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- Marker CE
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- Marzolla M
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- McKemey AK
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- Meyer AB
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- Michelon G
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- Miftakov V
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- Minor R
- Minutoli S
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- Paoloni E
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- Pulliam T
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- Qi ND
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- Raffaelli F
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- Rama M
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- Rashevskaia I
- Rasson JE
- Ratcliff BN
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- Roeben M
- Rolquin J
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- Roney JM
- Rong G
- Roodman A
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- Rosenberg EI
- Rotondo M
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- Russel JJ
- Ryd A
- Sadrozinski H
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Sanders P
- Sandrelli F
- Sands B
- Santi S
- Santroni A
- Sapozhnikov L
- Savvas N
- Saxton OH
- Schaffner SF
- Schalk T
- Schieck JR
- Schietinger T
- Schindler RH
- Schmitz RE
- Schmuecker H
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwierz R
- Sciacca C
- Sciolla G
- Scott I
- Scott IJ
- Seeman JT
- Seiden A
- Seitz R
- Sen S
- Serbo VV
- Serednyakov SI
- Serfass B
- Serra M
- Shapiro S
- Sharma V
- Shelkov VG
- Shi X
- Shorthouse HW
- Simi G
- Simonetto F
- Simopoulos ET
- Sinev NB
- Skarpass K
- Skovpen YI
- Sloane RJ
- Smith AJS
- Smith D
- Smith JG
- Smol A
- Snyder A
- Soderstrom E
- Soffer A
- Soha A
- Sokoloff MD
- Spaan B
- Spanier SM
- Spencer EN
- Speziali V
- Stahl A
- Stark J
- Steinke M
- Stiles P
- Stoker DP
- Stone R
- Stroili R
- Strother PD
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sutcliffe P
- Sutton CS
- Swain JE
- T\u27Jampens S
- Talby M
- Tanaka HA
- Taras P
- Taylor F
- Tehrani FS
- Telnov AV
- Telnov VI
- Thiebaux C
- Thiessen D
- Thompson RJ
- Tinslay J
- Tisserand V
- Toki WH
- Torassa E
- Touramanis C
- Toussaint JC
- Trapani PP
- Treadwell E
- Triggiani G
- Trincaz-Duvoid S
- Trischuk J
- Truong K
- Tumanov A
- Turcotte M
- Turnbull L
- Turri M
- Usseglio M
- Va\u27vra J
- Vaitsas G
- Valassi A
- Vallazza E
- van Bibber K
- van Hoek WC
- Varnes EW
- Vasileiadis G
- Vasseur G
- Verderi M
- Verkerke W
- Versille S
- Vidal PB
- Voci C
- Voena C
- von der Lippe H
- Vuagnin G
- Wagner DL
- Wagner SR
- Wagoner DE
- Waldi R
- Walkowiak W
- Wallom D
- Walsh J
- Wang P
- Wang R
- Warner DW
- Watson AT
- Watson NK
- Watt M
- Weatherall JH
- Weaver M
- Weber T
- Weber TF
- Weidemann AW
- Weinstein AJR
- Wenaus TJ
- Wenzel WA
- White JL
- Wienands U
- Wilden L
- Wilder M
- Williams DC
- Williams MI
- Willocq S
- Wilson FF
- Wilson RJ
- Wisniewski WJ
- Witherell M
- Wittlin J
- Woch A
- Wormser G
- Wright DM
- Wu SL
- Wuest CR
- Xella SM
- Xie Y
- Yamamoto B
- Yamamoto RK
- Yang S
- Yeche C
- Yellin S
- Young CC
- Yu N
- Yu Z
- Yumiceva FX
- Yushkov AN
- Zacek V
- Zachariadou K
- Zallo A
- Zanin D
- Zhang B
- Zhang J
- Zhu RY
- Zhu YS
- Zioulas G
- Zito M
- Zizka G
- Zobernig H
- Publication venue
- SelectedWorks
- Publication date
- 20/10/2010
- Field of study
No full textThe BaBar detector
- Author
- Abbott B
- Abe K
- Abrams Gs
- Adam I
- Adesanya A
- Adye T
- Ahsan A
- Albert J
- Albert Jn
- Aleksan R
- Alford O
- Allison J
- Alsmiller Jrg
- Amerman L
- Andress Jc
- Angelini C
- Anjomshoaa A
- Anthony Pl
- Antohin Ei
- Anulli F
- Arguin Jf
- Arisaka K
- Aspinwall Ml
- Aston D
- Aubert B
- Azzopardi De
- Back Jj
- Bagnasco S
- Bailly P
- BALDINI FERROLI R
- Band Hr
- Bard R
- Barlow Nr
- Barlow Rj
- Bartelt J
- Bartoldus R
- Batignani G
- Bauer Jm
- Bazan A
- Beaulieu M
- Becla J
- Behne D
- Behr L
- Beigbeder C
- Bell R
- Benayoun M
- Benkebil M
- Benninger T
- Beringer J
- Bernard D
- Bernet R
- Berridge S
- Besson P
- Bettarini S
- Bhimji W
- Bianchi F
- Bionta Rm
- Blaylock G
- Blinov Ve
- Bloom E
- Bloom P
- Blouw J
- Boeheim Ct
- Bona M
- Bondioli M
- Bonneaud Gr
- Booke M
- Booth J
- Borgland Aw
- Bosi F
- Bosisio L
- Boucham A
- Bourgeois P
- Boutigny D
- Bowerman Da
- Bowman J
- Boyarski Am
- Boyce Rf
- Boyd Jt
- Bozzi C
- Brandt T
- Brau B
- Breon Ab
- Breton D
- Briand H
- Briggs D
- BRIGHT THOMAS Pg
- Brigljevic V
- Britton Di
- Brochard F
- Bronzini F
- Brooks A
- Broomer B
- Brose J
- Brown C
- Brown D
- Brown Dn
- Buccheri A
- Buchanan C
- Bugg W
- Bukin Ad
- Bukin Da
- Bula C
- Bulfon C
- Bulos F
- Burchat Pr
- Burgess W
- Burke S
- BUTTON SHAFER J
- Buzykaev Ar
- Buzzo A
- Byers B
- CA BABAR Collaboration
- Calcaterra A
- Calderini G
- Callahan D
- Camanzi B
- Campagnari C
- Caracciolo Roberto
- Carpinelli M
- Carroll M
- Cartaro C
- Cason Nm
- Cavallo N
- Cavoto G
- Charles E
- Chauveau J
- Chen E
- Chen Gp
- Chen Jc
- Cheng Ch
- Chestnut R
- Chevalier N
- Chun S
- Cizeron R
- Clark Ar
- Clark Pj
- Claus R
- Claxton B
- Cochran J
- COHEN TANUGI J
- Cohn H
- Colecchia F
- Contri R
- Convert P
- Convery Mr
- Cooke P
- Coombes R
- Copty N
- Cottingham Wn
- Cottrell L
- Coupal Dp
- Cowan G
- Cowan R
- Coward Dh
- Craddock Ww
- Crawley Hb
- Cremaldi L
- Crosetti G
- Dacosta Va
- Dahlinger G
- Dahmes B
- DAL CORSO F
- Dallapiccola C
- Dardin S
- Dasu S
- Daudo F
- Dauncey Pd
- David P
- Davis Cl
- Day C
- DE BONIS I
- DE DOMENICO G
- DE FREITAS Pm
- DE GROOT N
- DE LA VAISSIERE C
- DE LESQUEN A
- DE MONCHENAULT Gh
- DE NARDO G
- DE SANGRO R
- DE SILVA A
- Debarger S
- DEL BUONO L
- DEL RE D
- DELLA RICCA G
- Deppermann T
- Destaebler H
- Devmal S
- Dewitt J
- DI GIROLAMO B
- DI LODOVICO F
- Dickopp M
- Dignan T
- Dittongo S
- Dixon P
- Dorfan De
- Dorfan J
- Doser M
- Dow Sf
- Dowdell J
- Du S
- Dubitzky Rs
- DUBOIS FELSMANN Gp
- Dubrovin Ms
- Dunwoodie W
- Dusatko Je
- Dvoretskii A
- Dyce N
- Ecklund S
- Eckstein P
- Egede U
- Eigen G
- Eisner Am
- Elmer P
- Emery S
- Erdos E
- Eschrich I
- Fabbricatore P
- Fabozzi F
- Faccini R
- Fackler O
- Fahey S
- Falbo M
- Falciai D
- Fan Q
- Farbin A
- Farinon S
- Favier J
- Fernholz R
- Ferrag S
- Ferrarotto F
- Ferroni F
- Fieguth Th
- Finocchiaro G
- Fischer Pa
- Flood Kt
- Folegani M
- Ford Wt
- Forti F
- Foster B
- Fouque G
- Franek B
- Frank Ed
- Fratini K
- Frey A
- Freytag Dr
- Fry Jr
- Fujino D
- Fullwood J
- Futterschneider H
- Gabathuler E
- Gabriel Ta
- Gaddi A
- Gaede F
- Gagliardi D
- Gaidot A
- Gaillard Jm
- Galagedera S
- Galeazzi F
- Gamba D
- Gamet R
- Ganzhur Sf
- Gaponenko I
- Gastaldi F
- Gatto C
- Geddes Ni
- Geld Tl
- Genat Jf
- George M
- George S
- Georgette Z
- Gill Ms
- Giorgi Ma
- Gladney L
- Glanzman T
- Godfrey Gl
- Golubev Vb
- Goozen Fr
- Gopal Gp
- Gosset L
- Gowdy Sj
- Graffin P
- Green Mg
- Grillo Aa
- Gritsan A
- Grosdidier G
- Grosso P
- Grothe M
- Groysman Y
- Gunawardane Njw
- Guo Qh
- Haire M
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- Haller G
- Hamilton R
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- Hanushevsky A
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- Hart E
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- Hawkes Cm
- Hearty C
- Heck J
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- Hertzbach Ss
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- Heusch Ca
- Himel T
- Hitlin Dg
- Hocker A
- Houde M
- Huffer Me
- Hung T
- Innes Wr
- Ivanchenko Vn
- Iwasaki M
- Izen Jm
- Jackson F
- Jacobsen Rg
- Jacques Pf
- Jared Rc
- Jawahery A
- Jayatilleke S
- Jayatilleke Sm
- Jeremie A
- Jessop Cp
- Johnson Dr
- Johnson Jr
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- Judd D
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- Karcher A
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- Kawahara H
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- Kirk A
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- Kitayama I
- Klaisner L
- Kluth S
- Knowles Dj
- Koch H
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- Kolachev Gm
- Kolomensky Yg
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- Krebs Hj
- Krishnamurthy M
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- Langenegger U
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- LE DIBERDER F
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- Leclerc C
- Lees Jp
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- Luo L
- Lusiani A
- Luth V
- Lutz Am
- Lynch G
- Lynch Hl
- Macfarlane Db
- Macri M
- Madani S
- Mallik U
- Mammini P
- Mancinelli G
- Mandelkern M
- Mandelli E
- Manfredi Pf
- Manzin G
- Marino M
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- Marsiske H
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- MARTINEZ VIDAL F
- Marzolla M
- Mass A
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- Muller Dr
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- NEWMAN COBURN D
- Nicholson H
- Nief Jy
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- Sharma V
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- Shi X
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- Simi Gabriele
- Simonetto Franco
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- Sloane Rj
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- VAN HOEK Wc
- Varnes Ew
- Vasileiadis G
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- Verderi M
- Verkerke W
- Versille S
- Vidal Pb
- Voci C
- Voena C
- VON DER LIPPE H
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- Wallom D
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- Wisniewski Wj
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- Wright Dm
- Wu Sl
- Wuest Cr
- Xella Sm
- Xie Y
- Yamamoto B
- Yamamoto Rk
- Yang S
- Yeche C
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- Yu N
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- Yumiceva Fx
- Yushkov An
- Zacek V
- Zachariadou K
- Zallo A
- Zanin D
- Zhang B
- Zhang J
- Zhu Ry
- Zhu Ys
- Zioulas G
- Zito M
- Zizka G
- Zobernig H
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2001
- Field of study
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Observation of a narrow meson state decaying to D-s(+)pi(0) at a mass of 2.32 GeV/c(2) RID C-2728-2008 RID C-5223-2009 RID C-5719-2008 RID D-1055-2009 RID A-2675-2009
- Author
- Abe K
- Abe T
- Abrams GS
- Adam I.
- Adesanya A.
- Adye T
- Adye T.
- Ahmed S
- Alam MS
- Albert J
- Albert J.
- Aleksan R
- Aleksan R.
- Allison J
- Altenburg D
- Andreotti M
- ANGELINI CARLO
- Anthony P. L.
- Anulli F
- Aspinwall ML
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- Aston D.
- Aubert B
- Baak MA
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- Band HR
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- Banerjee S
- Barate R
- Barillari T
- Barlow NR
- Barlow RJ
- Bartelt J
- Bartelt J.
- Bartoldus R
- BATIGNANI GIOVANNI
- Bauer JM
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- Bellini F
- Benayoun M
- Benninger T.
- Berger N
- Beringer J
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- Berridge S.
- Berryhill JW
- Besson P.
- Best D
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- Bettoni D
- Bevan AJ
- Bhimji W
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- Blanc F
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- Bondioli M
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- Bourgeois P.
- Boutigny D
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- Boyarski A. M.
- Boyarski AM
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- Breon AB
- Briand H
- Briggs D.
- Brigljevic V
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- Bronzini F.
- Brose J
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- Crawley HB
- Cremaldi L
- Crosetti G
- Cuhadar Donszelmann T
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- Danielson N
- Dasu S
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- Datta M
- Daudo F.
- Dauncey PD
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- Davier M
- Davis CL
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- De Groot N
- de la Vaissiere C
- de Lesquen A.
- de Monchenault G. H.
- de Monchenault GH
- De Nardo G
- de Sangro R
- De Silva A
- De Silva A.
- DeBarger S.
- Del Buono L
- del Re D
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- Della Ricca G
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- Deppermann T
- DeStaebler H.
- Di Girolamo B.
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- Dong D
- Dorfan J
- Dorfan J.
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- Dubitzky RS
- Dubois Felsmann GP
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- Dunwoodie W
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- Dusatko J. E.
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- Field RC
- Finocchiaro G
- Flack RL
- Flaecher HU
- Flood KT
- Ford K
- Ford WT
- Forti AC
- FORTI FRANCESCO
- Fortin D
- Franek B
- Franek B.
- Fratini K.
- Frey R
- Freytag D. R.
- Fry JR
- Gabathuler E
- Gabriel TA
- Gaidot A
- Gaidot A.
- Gaillard JM
- Galagedera S.
- Galeazzi F
- Gallo F
- Gamba D
- Gamba D
- Gamba D.
- Gamet R
- Ganzhur S. F.
- Ganzhur SF
- Gaspero M
- Gatto C
- Geddes N. I.
- Geddes NI
- George S
- Georgette Z.
- Gill MS
- Giorgi M. A.
- GIORGI MARCELLO
- Giraud PF
- Gladney L
- Glanzman T
- Glanzman T.
- Godang R
- Godfrey G. L.
- Goetzen K
- Golubev VB
- Gopal G. P.
- Gopal GP
- Gosset L.
- Gowdy SJ
- Graffin P.
- Grancagnolo S
- Grauges Pous E
- Green MG
- Grenier GJ
- Gritsan AV
- Grosdidier G
- Grosso P.
- Groysman Y
- Guo QH
- Hadavand HK
- Hadig T
- Haire M
- Haire M.
- Haller G.
- Halyo V
- Hamon O
- Hanushevsky A.
- Harris J.
- Harrison PF
- Harrison TJ
- Hart E.
- Hart PA
- Harton JL
- Hasan A.
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Hee C.
- Henderson R.
- Hertzbach SS
- Herve S.
- Heusch CA
- Hicheur A
- Hill EJ
- Himel T.
- Hitlin DG
- Hocker A
- Hryn'ova T
- Hu H
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- Huffer M. E.
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- Innes W. R.
- Innes WR
- Ivanchenko VN
- Izen J. M.
- Izen JM
- Jackson F
- Jackson PD
- Jacobsen RG
- Jacques P. F.
- Jawahery A
- Jayatilleke S
- Jessop C. P.
- Jessop CP
- John MJJ
- Johnson J. R.
- Johnson JR
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- Judd D
- Judd D.
- Kadel RW
- Kadyk J
- Kalelkar M.
- Karolak M.
- Karyotakis Y
- Kawahara H.
- Kay J.
- Kay M
- Keller L.
- Kelly MP
- Kelsey M. H.
- Kelsey MH
- Kerth LT
- Khan A
- Khan N.
- Kim H
- Kim P
- King M. E.
- Kirkby D
- Kirkby D.
- Kitayama I
- Kitayama I.
- Klaisner L.
- Knowles DJ
- Koch H
- Kocian ML
- Kofler R
- Kolomensky YG
- Koptchev VB
- Kordich TMB
- Kovalskyi D
- Kowalewski R
- Kowalewski R
- Kowalewski R.
- Kozanecki W
- Kozanecki W.
- Kral JF
- Kravchenko EA
- Krebs H. J.
- Krishnamurthy M
- Kroeger R
- Kukartsev G
- Kurup A
- Kutter PE
- Kuznetsova N
- Kyberd P
- Lacker HM
- Lae CK
- Lafferty GD
- Lamanna E.
- Lamsa J
- Lanceri L
- Lanceri L
- Lanceri L.
- Lange DJ
- Langenegger U
- Langenegger U.
- Langer M
- Langer M.
- Langeveld W.
- Lankford AJ
- Laplace S
- Latham TE
- Lavin D
- Lazzaro A
- Le Diberder F
- LeClerc C
- Lee SJ
- Lees JP
- Leith D. W. G. S.
- Leith DWGS
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- Lepeltier V
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- Levi ME
- Levy SL
- Lewandowski B
- Li H
- Lidbury J.
- Lillard V
- Lista L
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- London GW
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- Lou X. C.
- Lou XC
- Louie S. K.
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- Lu C.
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- Luitz S.
- Luppi E
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- Lusiani A.
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- Luth V.
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- Lynch HL
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- Mandelkern M
- Manfredi PF
- Mangeol DJJ
- Manzin G.
- Marchiori G
- Margoni M
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- Markey G.
- Marques V.
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- Martinez Vidal F
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- Mattison TS
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- Mayer B.
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- Mazzoni M. A.
- Mazzoni MA
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- McDonald J.
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- McDougald M.
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- Yumiceva FX
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- Zhao HW
- Zhu YS
- Zito M
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- Zobernig H
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2003
- Field of study
No full textWe have observed a narrow state near 2.32 GeV/c(2) in the inclusive D(s)(+)pi(0) invariant mass distribution from e(+)e(-) annihilation data at energies near 10.6 GeV. The observed width is consistent with the experimental resolution. The small intrinsic width and the quantum numbers of the final state indicate that the decay violates isospin conservation. The state has natural spin-parity and the low mass suggests a J(P)=0(+) assignment. The data sample corresponds to an integrated luminosity of 91 fb(-1) recorded by the BABAR detector at the SLAC PEP-II asymmetric-energy e(+)e(-) storage ring
Measurement of B-0 -> D-s(*)D+*(-) branching fractions and B-0 -> D-s*D+*(-) polarization with a partial reconstruction technique RID C-2728-2008 RID C-5223-2009 RID C-5719-2008 RID D-1055-2009 RID A-2675-2009
- Author
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- Palombo F
- Pan Y
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- Pan Y
- Panetta J
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- Paoloni E
- PAOLONI EUGENIO
- Paolucci P
- Paolucci P.
- Passaggio S
- Pastore FC
- Patel PM
- Patrignani C
- Patteri P
- Pavel T.
- Payne DJ
- Pelizaeus M
- Penichot Y.
- Penny RC
- Perazzo A
- Perl J.
- Perl M
- Pertsova M.
- Peruzzi IM
- Peters K
- Petersen TC
- Petrak S
- Petrak S.
- Piccolo D
- Piccolo M
- Piemontese L
- Pierini M
- Piredda G
- Piredda G.
- Pitman D.
- Pivk M
- Plano R. J.
- Plaszczynski S
- Playfer S
- Pompili A
- Pompili A
- Pompili A.
- Poropat P
- Poropat P.
- Porter FC
- Posocco M
- Potter CT
- Prell S
- Prepost R
- Prepost R
- Prepost R
- Prest M.
- Pripstein M
- Profeti A.
- Pulliam T
- Purohit M. V.
- Purohit MV
- Putallaz G.
- Qi ND
- Raffaelli F.
- Rahatlou S
- Raines P. E.
- Rama M
- Rama M.
- Rankin P
- Rashevskaia I.
- Ratcliff B. N.
- Ratcliff BN
- Raven G
- Re V
- Reidy J
- Reif R.
- RI Roe Natalie/A
- Ricciardi S
- Richman JD
- Rizzo G.
- RIZZO GIULIANA
- Roat C
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- Robertson S. H.
- Robertson SH
- Robutti E
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- Roe NA
- Roethel W
- Rolquin J.
- Romosan A
- Ronan MT
- Roney J. M.
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- Sands B.
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- Sarti A
- Saxton O. H.
- Schaffner S. F.
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- Schmitz RE
- Schmuecker H
- Schott G
- Schubert KR
- Schumm BA
- Schune MH
- Schwanke U
- Schwiening J
- Schwiening J.
- Schwierz R
- Sciacca C
- Sciolla G
- Sciolla G.
- Scott IJ
- Seeman J. T.
- Seiden A
- Sekula SJ
- Sekula SJ
- Sekula SJ
- Serbo V. V.
- Serednyakov SI
- Serfass B
- Serfass B.
- Serra M
- Serra M.
- Shapiro S.
- Sharma V
- Shelkov VG
- Shorthouse HW
- Simi G
- Simi G.
- Simonetto F
- Sinev NB
- Skarpass Sr K.
- Skovpen YI
- Sloane RJ
- Smith A. J. S.
- Smith AJS
- Smith JG
- Smol A
- Smol A.
- Snyder A
- Snyder A.
- Soderstrom E.
- Soffer A
- Soha A
- Soha A.
- Sokoloff MD
- Spaan B
- Spanier S. M.
- Spanier SM
- Speziali V
- Staengle H
- Stahl A.
- Stark J
- Steinke M
- Stelzer J
- Stiles P.
- Stoker DP
- Stroili R
- Strom D
- Strother P
- Stugu B
- Su D
- Su D.
- Sullivan M. K.
- Sullivan MK
- Summers DJ
- Swain JE
- T'Jampens S
- Talby M.
- Tanaka H. A.
- Tanaka HA
- Tantot L
- Taras P
- Taylor F
- Taylor GP
- Tehrani FS
- Telnov AV
- Thiebaux C
- Thiessen D
- Tinslay J
- Tiozzo G
- Tisserand V
- Toki WH
- Torrence E
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- Treadwell E
- Triggiani G.
- TRIGGIANI GIUSEPPE
- Tumanov A
- Tumanov A.
- Turcotte M.
- Turnbull L.
- Turri M
- Usseglio M.
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- van Hoek WC
- Varnes E. W.
- Varnes EW
- Vasileiadis G
- Vasseur G
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- Wisniewski WJ
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- Yamamoto RK
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- Yumiceva F. X.
- Yumiceva FX
- Yushkov AN
- Zallo A
- Zanin D
- Zanin D.
- Zghiche A
- Zhang J
- Zhang L
- Zhao HW
- Zhu YS
- Zito M
- Zito M.
- Zobernig H
- Publication venue
- Publication date
- 01/01/2003
- Field of study
No full textWe present a study of the decays B-0 --> D-s((*)) D*-, using 20.8 fb(-1) of e(+)e(-) annihilation data recorded with the BABAR detector. The analysis is conducted with a partial reconstruction technique, in which only the D-s((*)+) and the soft pion from the D*- decay are reconstructed. We measure the branching fractions B(B-0 --> Ds+D*-) = (1.03 +/- 0.14 +/- 0.13 +/- 0.26)% and B(B-0 --> D-s(*+) D*-) = (1.97 +/- 0.15 +/- 0.30+/- 0.49)%, where the first error is statistical, the second is systematic, and the third is the error due to the D-s(+) --> phipi(+) branching fraction uncertainty. From the B-0 --> D-s(*+) D*- angular distributions, we measure the fraction of longitudinal polarization Gamma(L)/Gamma = (51.9 +/- 5.0 +/- 2.8)%, which is consistent with theoretical predictions based on factorization
Measurement of the branching fraction for inclusive semileptonic B meson decays
- Author
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- Abrams GS
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- Adesanya A.
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- Beringer J
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- Berryhill JW
- Besson P.
- Best D
- Bettarini S
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- Bhimji W
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- Wisniewski WJ
- Wormser G
- Wright DH
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- Yumiceva F.X.
- Yumiceva FX
- Yushkov AN
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- Zanin D.
- Zghiche A
- Zhang J
- Zhang L
- Zhu YS
- Zito M
- Zito M.
- Zobernig H
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2002
- Field of study
Get PDFA largely model-independent measurement of the inclusive electron momentum
spectrum and branching fraction for semileptonic decays of B mesons is
presented based on data recorded at the Upsilon(4S) resonance with the BABAR
detector. Backgrounds from secondary charm decays are separated from prompt B
decays using charge and angular correlations between the electron from one B
meson and a high momentum electron tag from the second B meson. The resulting
branching fraction is BR(B -> X e nu) = (10.87 +-0.18(stat)+-0.30(syst))%.
Based on this measurement we determine the CKM matrix element |V_cb|
Measurement of the branching fraction for inclusive semileptonic B meson decays
- Author
- Aubert B
- Boutigny D
- Gaillard JM
- Hicheur A
- Karyotakis Y
- Lees JP
- Robbe P
- Tisserand V
- Zghiche A
- Palano A
- Pompili A
- Chen JC
- Qi ND
- Rong G
- Wang P
- Zhu YS
- Eigen G
- Ofte I
- Stugu B
- Abrams GS
- Borgland AW
- Breon AB
- Brown DN
- Button-Shafer J
- Cahn RN
- Charles E
- Gill MS
- Gritsan AV
- Groysman Y
- Jacobsen RG
- Kadel RW
- Kadyk J
- Kerth LT
- Kolomensky YG
- Kral JF
- LeClerc C
- Levi ME
- Lynch G
- Mir LM
- Oddone PJ
- Orimoto TJ
- Pripstein M
- Roe NA
- Romosan A
- Ronan MT
- Shelkov VG
- Telnov AV
- Wenzel WA
- Harrison TJ
- Hawkes CM
- Knowles DJ
- O'Neale SW
- Penny RC
- Watson AT
- Watson NK
- Deppermann T
- Goetzen K
- Koch H
- Lewandowski B
- Peters K
- Schmuecker H
- Steinke M
- Barlow NR
- Bhimji W
- Boyd JT
- Chevalier N
- Clark PJ
- Cottingham WN
- Mackay C
- Wilson FF
- Abe K
- Hearty C
- Mattison TS
- McKenna JA
- Thiessen D
- Jolly S
- McKemey AK
- Blinov VE
- Bukin AD
- Buzykaev AR
- Golubev VB
- Ivanchenko VN
- Korol AA
- Kravchenko EA
- Onuchin AP
- Serednyakov SI
- Skovpen YI
- Yushkov AN
- Best D
- Chao M
- Kirkby D
- Lankford AJ
- Mandelkern M
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- et al
- RI Roe Natalie/A-
- Publication venue
- Publication date
- 01/01/2002
- Field of study
Get PDFA largely model-independent measurement of the inclusive electron momentum
spectrum and branching fraction for semileptonic decays of B mesons is
presented based on data recorded at the Upsilon(4S) resonance with the BABAR
detector. Backgrounds from secondary charm decays are separated from prompt B
decays using charge and angular correlations between the electron from one B
meson and a high momentum electron tag from the second B meson. The resulting
branching fraction is BR(B -> X e nu) = (10.87 +-0.18(stat)+-0.30(syst))%.
Based on this measurement we determine the CKM matrix element |V_cb|
