26 research outputs found
Evidence for the h_b(1P) meson in the decay Upsilon(3S) --> pi0 h_b(1P)
- Author
- Adametz A.
- Adye T.
- Ahmed H.
- Alam M. S.
- Albert J.
- Allen M. T.
- Alwyn K. E.
- Andreassen R.
- Angelini C.
- Anh TV
- Anulli F.
- Arnaud N.
- Asgeirsson D. J.
- Aston D.
- Atmacan H.
- Ayad R.
- Bailey D.
- Baldini-Ferroli R.
- Band H. R.
- Banerjee Sw.
- Bard D. J.
- Barlow R. J.
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- Batignani G.
- Behera P. K.
- Bellis M.
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- Bernlochner F. U.
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- de Monchenault G. Hamel
- De Nardo G.
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- Zucchelli SVazquez F.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Get PDFUsing a sample of 122 million Upsilon(3S) events recorded with the BaBar
detector at the PEP-II asymmetric-energy e+e- collider at SLAC, we search for
the hb(1P) spin-singlet partner of the P-wave chi_{bJ}(1P) states in the
sequential decay Upsilon(3S) --> pi0 h_b(1P), h_b(1P) --> gamma eta_b(1S). We
observe an excess of events above background in the distribution of the recoil
mass against the pi0 at mass 9902 +/- 4(stat.) +/- 2(syst.) MeV/c^2. The width
of the observed signal is consistent with experimental resolution, and its
significance is 3.1sigma, including systematic uncertainties. We obtain the
value (4.3 +/- 1.1(stat.) +/- 0.9(syst.)) x 10^{-4} for the product branching
fraction BF(Upsilon(3S)-->pi0 h_b) x BF(h_b-->gamma eta_b).Comment: 8 pages, 4 postscript figures, submitted to Phys. Rev. D (Rapid
Communications
Measurement of the Top Pair Production Cross Section in the Dilepton Decay Channel in ppbar Collisions at sqrt s = 1.96 TeV
- Author
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- 01/01/2010
- Field of study
Get PDFSubmitted to Phys. Rev. DA measurement of the \ttbar production cross section in \ppbar collisions at s = 1.96 TeV using events with two leptons, missing transverse energy, and jets is reported. The data were collected with the CDF II Detector. The result in a data sample corresponding to an integrated luminosity 2.8 fb−1 is: \sigma_{\ttbar} = 6.27 ± 0.73(stat) ± 0.63(syst) ± 0.39(lum) pb. for an assumed top mass of 175 GeV/c2.A measurement of the tt̅ production cross section in pp̅ collisions at √s=1.96 TeV using events with two leptons, missing transverse energy, and jets is reported. The data were collected with the CDF II detector. The result in a data sample corresponding to an integrated luminosity 2.8 fb-1 is σtt̅ =6.27±0.73(stat)±0.63(syst)±0.39(lum) pb. for an assumed top mass of 175 GeV/c2.Peer reviewe
Farmers’ perception of termites in agriculture production and their indigenous utilization in Northwest Benin
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- A Dansi
- A Diop
- A Faye
- A Togola
- A van Huis
- A Vorsters
- AA Akpesse
- AD Banjo
- AD Banjo
- Alexandre Dansi
- Azize Orobiyi
- BP Freymann
- C Houndénou
- C Tenon
- D Maayiem
- D Munthali
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- DG Debelo
- EAP Vasanthi
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- J Ramos-Elorduy
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Full text linkHeavy Ion Results from ATLAS
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- Zalieckas J
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- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2017
- Field of study
Get PDFThese proceedings provide an overview of the new results obtained with the ATLAS detector at the LHC, which were
presented in the Quark Matter 2017 conference. These results were covered by twelve parallel talks, one flash talk and
eleven posters. These proceedings group these results into five areas: initial state, jet quenching, quarkonium production,
longitudinal flow dynamics, and collectivity in small systems
Measurements of photo-nuclear jet production in Pb plus Pb collisions with ATLAS
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam ER
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Albicocco P
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty M
- Alviggi MG
- Amadio BT
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
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- Kobayashi A
- Kobayashi D
- Kobayashi T
- Kobel M
- Kocian M
- Kodys P
- Koffas T
- Koffeman E
- Kohler MK
- Kohler NM
- Koi T
- Kolb M
- Koletsou I
- Komar AA
- Komori Y
- Kondo T
- Kondrashova N
- Koneke K
- Konig AC
- Kono T
- Konoplich R
- Konstantinidis N
- Kopeliansky R
- Koperny S
- Kopp AK
- Korcyl K
- Kordas K
- Korn A
- Korol AA
- Korolkov I
- Korolkova EV
- Kortner O
- Kortner S
- Kosek T
- Kostyukhin VV
- Kotwal A
- Koulouris A
- Kourkoumeli-Charalampidi A
- Kourkoumelis C
- Kourlitis E
- Kouskoura V
- Kowalewska AB
- Kowalewski R
- Kowalski TZ
- Kozakai C
- Kozanecki W
- Kozhin AS
- Kramarenko VA
- Kramberger G
- Krasnopevtsev D
- Krasny MW
- Krasznahorkay A
- Krauss D
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- Kuday S
- Kuechler JT
- Kuehn S
- Kugel A
- Kuger F
- Kuhl T
- Kukhtin V
- Kukla R
- Kulchitsky Y
- Kuleshov S
- Kulinich YP
- Kuna M
- Kunigo T
- Kupco A
- Kuprash O
- Kurashige H
- Kurchaninov LL
- Kurochkin YA
- Kurth MG
- Kus V
- Kuutmann EB
- Kuwertz ES
- Kuze M
- Kvita J
- Kwan T
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- La Rotonda L
- Lacasta C
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- Laforge B
- Lagouri T
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- Lampl W
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- Landgraf U
- Landon MPJ
- Lanfermann MC
- Lang VS
- Lange JC
- Langenberg RJ
- Lankford AJ
- Lanni F
- Lantzsch K
- Lanza A
- Lapertosa A
- Laplace S
- Laporte JF
- Lari T
- Lassnig M
- Latour BMD
- Laurelli P
- Lavrijsen W
- Law AT
- Laycock P
- Lazovich T
- Lazzaroni M
- Le Dortz O
- Le Guirriec E
- Le Quilleuc EP
- Le B
- LeBlanc M
- LeCompte T
- Ledroit-Guillon F
- Lee CA
- Lee GR
- Lee L
- Lee SC
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- Lefebvre G
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- Leggett C
- Lehan A
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- Leight WA
- Leite MAL
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- Lellouch D
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- Leney KJC
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- Lester CG
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- Levy M
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- Li S
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- Li Y
- Liang Z
- Liberti B
- Liblong A
- Lie K
- Liebal J
- Liebig W
- Limosani A
- Lin SC
- Lin TH
- Lindquist BE
- Lionti AE
- Lipeles E
- Lipniacka A
- Lisovyi M
- Liss TM
- Lister A
- Litke AM
- Liu B
- Liu H
- Liu H
- Liu J
- Liu JB
- Liu JKK
- Liu K
- Liu L
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- Liu Y
- Liu YL
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- Llacer MM
- Lleres A
- Lloyd SL
- Lo Sterzo F
- Lo CY
- Lobodzinska EM
- Loch P
- Loebinger FK
- Loew KM
- Loginov A
- Lohse T
- Lohwasser K
- Lokajicek M
- Long BA
- Long JD
- Long RE
- Longo L
- Looper KA
- Lopez JA
- Lopez SC
- Lopez SP
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- Losel PJ
- Lou X
- Lounis A
- Love J
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- Loyola JES
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- Lucotte A
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- Lukas W
- Luminari L
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- Lundberg O
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- Lynn D
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- Ma H
- Ma LL
- Ma Y
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- Macchiolo A
- Macdonald CM
- Macek B
- Madaffari D
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- Martyniuk AC
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- Mashinistov R
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- Mazza SM
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- Zimmermann C
- Zimmermann S
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- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2017
- Field of study
Get PDFUltra-peripheral heavy ion collisions provide a unique opportunity to study the parton distributions in the colliding
nuclei via the measurement of photo-nuclear jet production. An analysis of jet production in ultra-peripheral Pb+Pb
collisions at √sNN = 5.02 TeV performed using data collected with the ATLAS detector in 2015 is described. The data
set corresponds to a total Pb+Pb integrated luminosity of 0.38 nb−1. The ultra-peripheral collisions are selected using a
combination of forward neutron and rapidity gap requirements. The cross-sections, not unfolded for detector response,
are compared to results from Pythia Monte Carlo simulations re-weighted to match a photon spectrum obtained from
the STARlight model. Qualitative agreement between data and these simulations is observed over a broad kinematic
range suggesting that using these collisions to measure nuclear parton distributions is experimentally realisable
Measurements of photo-nuclear jet production in Pb + Pb collisions with ATLAS
- Author
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- Aad G
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- Abdallah J
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- Publication venue
- 26th International Conference on Ultrarelativistic Nucleus-Nucleus Collissions (Quark Matter)
- Publication date
- 01/11/2017
- Field of study
Get PDFUltra-peripheral heavy ion collisions provide a unique opportunity to study the parton distributions in the colliding nuclei via the measurement of photo-nuclear jet production. An analysis of jet production in ultra-peripheral Pb+Pb collisions at √sNN = 5.02 TeV performed using data collected with the ATLAS detector in 2015 is described. The data set corresponds to a total Pb+Pb integrated luminosity of 0.38 nb⁻¹. The ultra-peripheral collisions are selected using a combination of forward neutron and rapidity gap requirements. The cross-sections, not unfolded for detector response, are compared to results from Pythia Monte Carlo simulations re-weighted to match a photon spectrum obtained from the STARlight model. Qualitative agreement between data and these simulations is observed over a broad kinematic range suggesting that using these collisions to measure nuclear parton distributions is experimentally realisable
ReviewsRISA Encephalography and Conventional Neuroradiologic Methods: A Comparative Study. By di ChiroGiovanni, pp. 102, 1961. Acta Radiologica
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- Publication venue
- 'British Institute of Radiology'
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- Field of study
No full textReviewsPediatric X-ray Diagnosis. By CaffeyJohn, 4th ed., pp. xxvi+1,236, 1,536 illus., 1961 (Year Book Publishers), $32.
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- Publication venue
- 'British Institute of Radiology'
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- Field of study
No full textIncomplete Lower Oesophageal Diaphragm
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- 'British Institute of Radiology'
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No full textThe great venereologist Philippe Ricord (1800–1889) and the final distinction between gonorrhoea and syphilis
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- 'Springer Science and Business Media LLC'
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