scispace - formally typeset
Search or ask a question

Showing papers by "Université Paris-Saclay published in 2007"


Journal ArticleDOI
G. L. Bayatian, S. Chatrchyan, G. Hmayakyan, Albert M. Sirunyan  +2060 moreInstitutions (143)
TL;DR: In this article, the authors present a detailed analysis of the performance of the Large Hadron Collider (CMS) at 14 TeV and compare it with the state-of-the-art analytical tools.
Abstract: CMS is a general purpose experiment, designed to study the physics of pp collisions at 14 TeV at the Large Hadron Collider (LHC). It currently involves more than 2000 physicists from more than 150 institutes and 37 countries. The LHC will provide extraordinary opportunities for particle physics based on its unprecedented collision energy and luminosity when it begins operation in 2007. The principal aim of this report is to present the strategy of CMS to explore the rich physics programme offered by the LHC. This volume demonstrates the physics capability of the CMS experiment. The prime goals of CMS are to explore physics at the TeV scale and to study the mechanism of electroweak symmetry breaking--through the discovery of the Higgs particle or otherwise. To carry out this task, CMS must be prepared to search for new particles, such as the Higgs boson or supersymmetric partners of the Standard Model particles, from the start-up of the LHC since new physics at the TeV scale may manifest itself with modest data samples of the order of a few fb−1 or less. The analysis tools that have been developed are applied to study in great detail and with all the methodology of performing an analysis on CMS data specific benchmark processes upon which to gauge the performance of CMS. These processes cover several Higgs boson decay channels, the production and decay of new particles such as Z' and supersymmetric particles, Bs production and processes in heavy ion collisions. The simulation of these benchmark processes includes subtle effects such as possible detector miscalibration and misalignment. Besides these benchmark processes, the physics reach of CMS is studied for a large number of signatures arising in the Standard Model and also in theories beyond the Standard Model for integrated luminosities ranging from 1 fb−1 to 30 fb−1. The Standard Model processes include QCD, B-physics, diffraction, detailed studies of the top quark properties, and electroweak physics topics such as the W and Z0 boson properties. The production and decay of the Higgs particle is studied for many observable decays, and the precision with which the Higgs boson properties can be derived is determined. About ten different supersymmetry benchmark points are analysed using full simulation. The CMS discovery reach is evaluated in the SUSY parameter space covering a large variety of decay signatures. Furthermore, the discovery reach for a plethora of alternative models for new physics is explored, notably extra dimensions, new vector boson high mass states, little Higgs models, technicolour and others. Methods to discriminate between models have been investigated. This report is organized as follows. Chapter 1, the Introduction, describes the context of this document. Chapters 2-6 describe examples of full analyses, with photons, electrons, muons, jets, missing ET, B-mesons and τ's, and for quarkonia in heavy ion collisions. Chapters 7-15 describe the physics reach for Standard Model processes, Higgs discovery and searches for new physics beyond the Standard Model

973 citations


Journal ArticleDOI
J. Abraham1, P. Abreu2, Marco Aglietta3, C. Aguirre  +449 moreInstitutions (69)
09 Nov 2007-Science
TL;DR: In this article, the authors demonstrate that there is a correlation between the arrival directions of cosmic rays with energy above 6 x 10{sup 19} eV and the positions of active galactic nuclei lying within 75 Mpc.
Abstract: Using data collected at the Pierre Auger Observatory during the past 3.7 years, we demonstrate that there is a correlation between the arrival directions of cosmic rays with energy above {approx} 6 x 10{sup 19} eV and the positions of active galactic nuclei (AGN) lying within {approx} 75 Mpc. We reject the hypothesis of an isotropic distribution of these cosmic rays at over 99% confidence level from a prescribed a priori test. The correlation we observe is compatible with the hypothesis that the highest energy particles originate from nearby extragalactic sources whose flux has not been significantly reduced by interaction with the cosmic background radiation. AGN or objects having a similar spatial distribution are possible sources.

798 citations


Journal ArticleDOI
01 Jun 2007-Science
TL;DR: It is shown by complete genome sequencing of two symbiotic, photosynthetic, Bradyrhizobium strains, BTAi1 and ORS278, that canonical nodABC genes and typical lipochito-oligosaccharidic Nod factors are not required for symbiosis in some legumes.
Abstract: Leguminous plants (such as peas and soybeans) and rhizobial soil bacteria are symbiotic partners that communicate through molecular signaling pathways, resulting in the formation of nodules on legume roots and occasionally stems that house nitrogen-fixing bacteria. Nodule formation has been assumed to be exclusively initiated by the binding of bacterial, host-specific lipochito-oligosaccharidic Nod factors, encoded by the nodABC genes, to kinase-like receptors of the plant. Here we show by complete genome sequencing of two symbiotic, photosynthetic, Bradyrhizobium strains, BTAi1 and ORS278, that canonical nodABC genes and typical lipochito-oligosaccharidic Nod factors are not required for symbiosis in some legumes. Mutational analyses indicated that these unique rhizobia use an alternative pathway to initiate symbioses, where a purine derivative may play a key role in triggering nodule formation.

574 citations


Journal ArticleDOI
David D'Enterria1, David D'Enterria2, M. Ballintijn3, M. Bedjidian4  +2185 moreInstitutions (141)
TL;DR: In this paper, the capabilities of the CERN Large Hadron Collider (LHC) experiment to explore the rich heavy-ion physics program offered by the LHC are presented, and the potential of the CMS experiment to carry out a series of representative Pb-Pb measurements.
Abstract: This report presents the capabilities of the CMS experiment to explore the rich heavy-ion physics programme offered by the CERN Large Hadron Collider (LHC). The collisions of lead nuclei at energies , will probe quark and gluon matter at unprecedented values of energy density. The prime goal of this research is to study the fundamental theory of the strong interaction ? Quantum Chromodynamics (QCD) ? in extreme conditions of temperature, density and parton momentum fraction (low-x).This report covers in detail the potential of CMS to carry out a series of representative Pb-Pb measurements. These include bulk observables, (charged hadron multiplicity, low pT inclusive hadron identified spectra and elliptic flow) which provide information on the collective properties of the system, as well as perturbative probes such as quarkonia, heavy-quarks, jets and high pT hadrons which yield tomographic information of the hottest and densest phases of the reaction.

361 citations


Journal ArticleDOI
A. Adare1, S. Afanasiev2, Christine Angela Aidala3, N. N. Ajitanand4  +459 moreInstitutions (49)
TL;DR: In this paper, the scaling of elliptic flow (v(2) with eccentricity, system size, and transverse kinetic energy (KET) was shown to be compatible with hydrodynamic expansion of thermalized fluid.
Abstract: Differential measurements of elliptic flow (v(2)) for Au+Au and Cu+Cu collisions at root s(NN)=200 GeV are used to test and validate predictions from perfect fluid hydrodynamics for scaling of v(2) with eccentricity, system size, and transverse kinetic energy (KET). For KET equivalent to m(T)-m up to similar to 1 GeV the scaling is compatible with hydrodynamic expansion of a thermalized fluid. For large values of KET mesons and baryons scale separately. Quark number scaling reveals a universal scaling of v(2) for both mesons and baryons over the full KET range for Au+Au. For Au+Au and Cu+Cu the scaling is more pronounced in terms of KET, rather than transverse momentum.

333 citations


Journal ArticleDOI
Takeshi Itoh1, Takeshi Itoh2, Tsuyoshi Tanaka1, Roberto A. Barrero, Chisato Yamasaki2, Yasuyuki Fujii2, Phillip Hilton2, Baltazar A. Antonio1, Hideo Aono, Rolf Apweiler, Richard Bruskiewich3, Thomas E. Bureau4, Frances A. Burr5, Antonio Costa de Oliveira6, Galina Fuks7, Takuya Habara2, Georg Haberer, Bin Han, Erimi Harada2, Aiko T. Hiraki2, Hirohiko Hirochika1, Douglas R. Hoen4, Hiroki Hokari2, Satomi Hosokawa, Yue-Ie C. Hsing8, Hiroshi Ikawa9, Kazuho Ikeo, Tadashi Imanishi10, Tadashi Imanishi2, Yukiyo Ito, Pankaj Jaiswal11, Masako Kanno2, Yoshihiro Kawahara12, Yoshihiro Kawahara2, Toshiyuki Kawamura2, Hiroaki Kawashima2, Jitendra P. Khurana13, Shoshi Kikuchi1, Setsuko Komatsu1, Kanako O. Koyanagi10, Hiromi Kubooka2, Damien Lieberherr14, Yao-Cheng Lin8, David M. Lonsdale, Takashi Matsumoto1, Akihiro Matsuya2, W. Richard McCombie15, Joachim Messing7, Akio Miyao1, Nicola Mulder, Yoshiaki Nagamura1, Jongmin Nam16, Jongmin Nam17, Nobukazu Namiki, Hisataka Numa1, Shin Nurimoto2, Claire O'Donovan, Hajime Ohyanagi9, Toshihisa Okido, Satoshi Oota, Naoki Osato, Lance E. Palmer15, Lance E. Palmer18, Francis Quetier19, Saurabh Raghuvanshi13, Naomi Saichi2, Hiroaki Sakai1, Hiroaki Sakai2, Yasumichi Sakai9, Katsumi Sakata9, Tetsuya Sakurai, Fumihiko Sato2, Yoshiharu Sato2, Heiko Schoof20, Heiko Schoof21, Motoaki Seki, Michie Shibata, Yuji Shimizu9, Kazuo Shinozaki, Yuji Shinso2, Nagendra K. Singh22, Brian Smith-White23, Jun-ichi Takeda2, Motohiko Tanino2, Tatiana Tatusova23, Supat Thongjuea24, Fusano Todokoro2, Mika Tsugane, Akhilesh K. Tyagi13, Apichart Vanavichit24, Aihui Wang25, Rod A. Wing, Kaori Yamaguchi2, Mayu Yamamoto, Naoyuki Yamamoto2, Yeisoo Yu26, Hao Zhang2, Qiang Zhao, Kenichi Higo1, Benjamin Burr5, Takashi Gojobori2, Takuji Sasaki1 
TL;DR: The results suggest that natural selection may have played a role for duplicated genes in both species, so that duplication was suppressed or favored in a manner that depended on the function of a gene.
Abstract: We present here the annotation of the complete genome of rice Oryza sativa L. ssp. japonica cultivar Nipponbare. All functional annotations for proteins and non-protein-coding RNA (npRNA) candidates were manually curated. Functions were identified or inferred in 19,969 (70%) of the proteins, and 131 possible npRNAs (including 58 antisense transcripts) were found. Almost 5000 annotated protein-coding genes were found to be disrupted in insertional mutant lines, which will accelerate future experimental validation of the annotations. The rice loci were determined by using cDNA sequences obtained from rice and other representative cereals. Our conservative estimate based on these loci and an extrapolation suggested that the gene number of rice is ∼32,000, which is smaller than previous estimates. We conducted comparative analyses between rice and Arabidopsis thaliana and found that both genomes possessed several lineage-specific genes, which might account for the observed differences between these species, while they had similar sets of predicted functional domains among the protein sequences. A system to control translational efficiency seems to be conserved across large evolutionary distances. Moreover, the evolutionary process of protein-coding genes was examined. Our results suggest that natural selection may have played a role for duplicated genes in both species, so that duplication was suppressed or favored in a manner that depended on the function of a gene.

254 citations


Journal ArticleDOI
TL;DR: In this paper, the absolute calibration and characterization of the MIPS 70 μm coarse and fine-scale imaging modes are presented based on over 2.5 years of observations, and the point-spread function (PSF) fitting photometry is found to give more accurate flux densities than aperture photometry.
Abstract: The absolute calibration and characterization of the Multiband Imaging Photometer for Spitzer (MIPS) 70 μm coarse‐and fine‐scale imaging modes are presented based on over 2.5 yr of observations. Accurate photometry (especially for faint sources) requires two simple processing steps beyond the standard data reduction to remove long‐term detector transients. Point‐spread function (PSF) fitting photometry is found to give more accurate flux densities than aperture photometry. Based on the PSF fitting photometry, the calibration factor shows no strong trend with flux density, background, spectral type, exposure time, or time since anneals. The coarse‐scale calibration sample includes observations of stars with flux densities from 22 mJy to 17 Jy, on backgrounds from 4 to 26 MJy sr^(−1), and with spectral types from B to M. The coarse‐scale calibration is 702 ± 35 MJy sr^(−1) MIPS70^(−1) (5% uncertainty) and is based on measurements of 66 stars. The instrumental units of the MIPS 70 μm coarse‐ and fine‐scale imaging modes are called MIPS70 and MIPS70F, respectively. The photometric repeatability is calculated to be 4.5% from two stars measured during every MIPS campaign and includes variations on all timescales probed. The preliminary fine‐scale calibration factor is 2894 ± 294 MJy sr^(−1) MIPS70F^(−1) (10% uncertainty) based on 10 stars. The uncertainties in the coarse‐ and fine‐scale calibration factors are dominated by the 4.5% photometric repeatability and the small sample size, respectively. The 5 σ, 500 s sensitivity of the coarse‐scale observations is 6–8 mJy. This work shows that the MIPS 70 μm array produces accurate, well‐calibrated photometry and validates the MIPS 70 μm operating strategy, especially the use of frequent stimulator flashes to track the changing responsivities of the Ge:Ga detectors.

225 citations


Journal ArticleDOI
A. Adare1, S. Afanasiev2, Christine Angela Aidala3, N. N. Ajitanand4  +380 moreInstitutions (49)
TL;DR: In this article, the PHENIX experiment presented results from the Relativistic Heavy Ion Collider 2005 run with polarized proton collisions at 200 GeV, for inclusive {pi}{sup 0} production at midrapidity.
Abstract: The PHENIX experiment presents results from the Relativistic Heavy Ion Collider 2005 run with polarized proton collisions at sqrt(s)=200 GeV, for inclusive {pi}{sup 0} production at midrapidity. Unpolarized cross section results are given for transverse momenta p{sub T}=0.5 to 20 GeV/c, extending the range of published data to both lower and higher p{sub T}. The cross section is described well for p{sub T} 2 GeV/c, by perturbative QCD. Double helicity asymmetries ALL are presented based on a factor of 5 improvement in uncertainties as compared to previously published results, due to both an improved beam polarization of 50%, and to higher integrated luminosity. These measurements are sensitive to the gluon polarization in the proton. Using one representative model of gluon polarization it is demonstrated that the gluon spin contribution to the proton spin is significantly constrained.

189 citations


Journal ArticleDOI
TL;DR: New shell model calculations indicate that (42)Si is best described as a well-deformed oblate rotor, which provides evidence for the disappearance of the Z=14 and N=28 spherical shell closures.
Abstract: The energies of the excited states in very neutron-rich Si-42 and P-41,P-43 have been measured using in-beam gamma-ray spectroscopy from the fragmentation of secondary beams of S-42,S-44 at 39A MeV. The low 2(+) energy of Si-42, 770(19) keV, together with the level schemes of P-41,P-43, provides evidence for the disappearance of the Z=14 and N=28 spherical shell closures, which is ascribed mainly to the action of proton-neutron tensor forces. New shell model calculations indicate that Si-42 is best described as a well-deformed oblate rotor.

189 citations


Journal ArticleDOI
Bernard Aubert1, Marcella Bona1, D. Boutigny1, Y. Karyotakis1  +562 moreInstitutions (77)
TL;DR: In this article, the invariant mass of the hadronic final state defines the effective center-of-mass energy, so that the obtained cross sections from the threshold to about 5 GeV can be compared with corresponding direct \epem measurements.
Abstract: We study the processes $e^+ e^-\to 2(\pi^+\pi^-)\pi^0\gamma$, $2(\pi^+\pi^-)\eta\gamma$, $K^+ K^-\pi^+\pi^-\pi^0\gamma$ and $K^+ K^-\pi^+\pi^-\eta\gamma$ with the hard photon radiated from the initial state. About 20000, 4300, 5500 and 375 fully reconstructed events, respectively, are selected from 232 fb$^{-1}$ of BaBar data. The invariant mass of the hadronic final state defines the effective $e^+ e^-$ center-of-mass energy, so that the obtained cross sections from the threshold to about 5 GeV can be compared with corresponding direct \epem measurements, currently available only for the $\eta\pi^+\pi^-$ and $\omega\pi^+\pi^-$ submodes of the $e^+ e^-\to 2(\pi^+\pi^-)\pi^0$ channel. Studying the structure of these events, we find contributions from a number of intermediate states, and we extract their cross sections where possible. In particular, we isolate the contribution from $e^+ e^-\to\omega(782)\pi^+\pi^-$ and study the $\omega(1420)$ and $\omega(1650)$ resonances. In the charmonium region, we observe the $J/\psi$ in all these final states and several intermediate states, as well as the $\psi(2S)$ in some modes, and we measure the corresponding branching fractions.

151 citations


Journal ArticleDOI
TL;DR: It is shown that calreticulin exposure was necessary and sufficient to increase proimmunogenic killing by other chemotherapies, and that tactics to expose cal reticulin might improve the clinical efficacy of many cancer therapies.
Abstract: In contrast to prior belief, tumor cell apoptosis is not necessarily silent but can be immunogenic. By tracing how anthracyclines and γ-irradiation trigger immunogenic cell deaths, we found that they were causally connected to the exposure of calreticulin on the tumor cell surface, before apoptosis in the tumor cell itself occurred. Furthermore, we showed that calreticulin exposure was necessary and sufficient to increase proimmunogenic killing by other chemotherapies. Our findings suggest that calreticulin could serve as a biomarker to predict therapy-associated immune responses, and that tactics to expose calreticulin might improve the clinical efficacy of many cancer therapies. [Cancer Res 2007;67(17):7941–4]

Journal ArticleDOI
S. S. Adler1, S. Afanasiev2, Christine Angela Aidala3, N. N. Ajitanand4  +340 moreInstitutions (44)
TL;DR: In this article, the authors measured the dependence of transverse momentum spectra of neutral pions and eta mesons with p(T) < 16 GeV/c and pT < 12 GeV /c, respectively, on the centrality of the collision at midrapidity by PHENIX experiment at the BNL Relativistic Heavy Ion Collider (RHIC) in d + Au collisions at root s(NN) = 200 GeV.
Abstract: The dependence of transverse momentum spectra of neutral pions and eta mesons with p(T) < 16 GeV/c and p(T) < 12 GeV/c, respectively, on the centrality of the collision has been measured at midrapidity by the PHENIX experiment at the BNL Relativistic Heavy Ion Collider (RHIC) in d + Au collisions at root s(NN) = 200 GeV. The measured yields are compared to those in p + p collisions at the same root s(NN) scaled by the number of underlying nucleon-nucleon collisions in d + Au. At all centralities, the yield ratios show no suppression, in contrast to the strong suppression seen for central An + Au collisions at RHIC. Only a weak p(T) and centrality dependence can be observed.

Journal ArticleDOI
M. Benali1, C. Desnault2, M. Mazouz, Z. Ahmed3, H. Albataineh4, Kalyan Allada5, K. A. Aniol6, V. Bellini, W. U. Boeglin7, P. Bertin1, P. Bertin8, M. Brossard1, A. Camsonne8, Mustafa Canan9, S. Chandavar10, Chunhui Chen11, J. P. Chen8, Maxime Defurne12, C. W. de Jager8, R. De Leo13, A. Deur8, L. El Fassi14, L. El Fassi15, Rolf Ent8, D. Flay16, M. Friend17, E. Fuchey1, S. Frullani, F. Garibaldi, David Gaskell8, A. Giusa, O. Glamazdin18, S. Golge19, J. Gomez8, Olfred Hansen8, Douglas Higinbotham8, T. Holmstrom20, Tanja Horn21, J. Huang5, M. Huang22, G. M. Huber23, Charles Hyde1, Charles Hyde9, S. Iqbal6, F. Itard1, Ho. Kang24, H. Kang24, A. Kelleher25, Cynthia Keppel8, S. Koirala9, I. Korover26, J. LeRose8, R. A. Lindgren27, E. Long28, M. Magne1, Juliette Mammei29, D. J. Margaziotis6, Pete Markowitz7, A. Martí Jiménez-Argüello30, A. Martí Jiménez-Argüello2, Franco Meddi, D. G. Meekins8, R. Michaels8, M. Mihovilovic31, N. Muangma5, C. Munoz Camacho2, C. Munoz Camacho1, P. Nadel-Turonski8, N. Nuruzzaman11, R. Paremuzyan2, R. I. Pomatsalyuk18, Andrew Puckett32, V. A. Punjabi33, Yujie Qiang8, Abdurahim Rakhman3, M. N. H. Rashad9, S. Riordan34, J. Roche10, G.V. Russo, F. Sabatié12, Kiadtisak Saenboonruang35, Kiadtisak Saenboonruang27, Arijit Saha8, B. Sawatzky16, B. Sawatzky8, L. Selvy28, A. Shahinyan36, Simon Širca31, P. Solvignon8, M. L. Sperduto, R. Subedi37, Vincent Sulkosky5, C. M. Sutera, William A. Tobias27, G. M. Urciuoli, D. Wang27, Bogdan Wojtsekhowski8, H. Yao16, Z. Ye27, L. Zana3, X. Zhan34, Jie Zhang8, B. Zhao25, Z. W. Zhao27, X. Zheng27, P. Zhu27 
TL;DR: The present experiment exploits the interference between the deeply virtual Compton scattering (DVCS) and the Bethe-Heitler processes to extract a linear combination of generalized parton distributions (GPDs) particularly sensitive to E_{q}, the least constrained GPD.
Abstract: The three-dimensional structure of nucleons (protons and neutrons) is embedded in so-called generalized parton distributions, which are accessible from deeply virtual Compton scattering. In this process, a high-energy electron is scattered off a nucleon by exchanging a virtual photon. Then, a highly energetic real photon is emitted from one of the quarks inside the nucleon, which carries information on the quark’s transverse position and longitudinal momentum. By measuring the cross-section of deeply virtual Compton scattering, Compton form factors related to the generalized parton distributions can be extracted. Here, we report the observation of unpolarized deeply virtual Compton scattering off a deuterium target. From the measured photon-electroproduction cross-sections, we have extracted the cross-section of a quasifree neutron and a coherent deuteron. Due to the approximate isospin symmetry of quantum chromodynamics, we can determine the contributions from the different quark flavours to the helicity-conserved Compton form factors by combining our measurements with previous ones probing the proton’s internal structure. These results advance our understanding of the description of the nucleon structure, which is important to solve the proton spin puzzle. The internal structure of the neutron has now been probed by highly energetic photons scattering off it. Combined with previous results for protons, these measurements reveal the contributions of quark flavours to the nucleon structure.

Journal ArticleDOI
Bernard Aubert1, Marcella Bona1, D. Boutigny1, Y. Karyotakis1  +557 moreInstitutions (76)
TL;DR: In this article, the e+e- --> Lambda anti-Lambda gamma, lambda anti-Sigma0 gamma, and Sigma 0 antiSigma 0 gamma processes were studied using 230 fb-1 of integrated luminosity collected by the BABAR detector at an e +e- center-of-mass energy of 10.58 GeV.
Abstract: We study the e+e- --> Lambda anti-Lambda gamma, Lambda anti-Sigma0 gamma, Sigma0 anti-Sigma0 gamma processes using 230 fb-1 of integrated luminosity collected by the BABAR detector at e+e- center-of-mass energy of 10.58 GeV. From the analysis of the baryon-antibaryon mass spectra the cross sections for e+e- --> Lambda anti-Lambda, Lambda anti-Sigma0, Sigma0 anti-Sigma0 are measured in the dibaryon mass range from threshold up to 3 GeV/c^2. The ratio of electric and magnetic form factors, |G_E/G_M|, is measured for e+e- --> Lambda anti-Lambda, and limits on the relative phase between Lambda form factors are obtained. We also measure the J/psi --> Lambda anti-Lambda, Sigma0 anti-Sigma0 and psi(2S) --> Lambda anti-Lambda branching fractions.

Journal ArticleDOI
Bernard Aubert1, Marcella Bona1, D. Boutigny1, Y. Karyotakis1  +568 moreInstitutions (77)
TL;DR: In this article, the processes e+e-→K+k-π+π-γ, K+K-π0π0γ and K+kπ-K+π+γ, where the photon is radiated from the initial state were studied.
Abstract: We study the processes e+e-→K+K-π+π-γ, K+K-π0π0γ and K+K-K+K-γ, where the photon is radiated from the initial state. About 34600, 4400 and 2300 fully reconstructed events, respectively, are selected from 232fb-1 of BABAR data. The invariant mass of the hadronic final state defines the effective e+e- center-of-mass energy, so that the K+K-π+π-γ data can be compared with direct measurements of the e+e-→K+K-π+π- reaction; no direct measurements exist for the e+e-→K+K-π0π0 or e+e-→K+K-K+K- reactions. Studying the structure of these events, we find contributions from a number of intermediate states, and we extract their cross sections where possible. In particular, we isolate the contribution from e+e-→ (1020)f0(980) and study its structure near threshold. In the charmonium region, we observe the J/ψ in all three final states and several intermediate states, as well as the ψ(2S) in some modes, and measure the corresponding branching fractions. We see no signal for the Y(4260) and obtain an upper limit of BY(4260)→ π+π- •ΓeeY<0.4eV at 90% C.L. © 2007 The American Physical Society.

Journal ArticleDOI
S. Afanasiev1, Christine Angela Aidala2, N. N. Ajitanand3, Y. Akiba  +345 moreInstitutions (43)
TL;DR: Differential elliptic flow (v(2)) for phi mesons and (anti)deuterons ((d) over bar )d is measured for Au + Au collisions at root s(NN) = 200 GeV.
Abstract: Differential elliptic flow (v(2)) for phi mesons and (anti)deuterons ((d) over bar )d is measured for Au + Au collisions at root s(NN) = 200 GeV. The v(2) for phi mesons follows the trend of lighter pi(+/-) and K-+/- mesons, suggesting that ordinary hadrons interacting with standard hadronic cross sections are not the primary driver for elliptic flow development. The v(2) values for ((d) over bar )d suggest that elliptic flow is additive for composite particles. This further validation of the universal scaling of v(2) per constituent quark for baryons and mesons suggests that partonic collectivity dominates the transverse expansion dynamics.

Journal ArticleDOI
V. M. Abazov1, Brad Abbott2, M. Abolins3, B. S. Acharya4  +595 moreInstitutions (84)
TL;DR: In this article, the first direct observation of the b baryon Xi(b)- (Xi(b)+ was reported, and the significance of the observed signal is 5.5 sigma, equivalent to a probability of 3.3 x 10−8 of it arising from a background fluctuation.
Abstract: We report the first direct observation of the strange b baryon Xi(b)- (Xi(b)+). We reconstruct the decay Xi(b)- -->J/psiXi-, with J/psi-->mu+mu-, and Xi--->Lambdapi--->ppi-pi- in pp collisions at square root of s =1.96 TeV. Using 1.3 fb(-1) of data collected by the D0 detector, we observe 15.2 +/- 4.4(stat)(-0.4)(+1.9)(syst) Xi(b)- candidates at a mass of 5.774 +/- 0.011(stat) +/- 0.015(syst) GeV. The significance of the observed signal is 5.5 sigma, equivalent to a probability of 3.3 x 10(-8) of it arising from a background fluctuation. Normalizing to the decay Lambda(b)-->J/psiLambda, we measure the relative rate sigma(Xi(b-) x B(Xi)b})- -->J/psiXi-)/sigma(Lambda(b)) x B(Lambda(b)-->J/psiLambda) = 0.28+/-0.09(stat)(-0.08)(+0.09)(syst).

Journal ArticleDOI
TL;DR: In this article, the transverse momentum spectra of eta mesons in the range p(T)approximate to 2-12 GeV/c have been measured at midrapidity (vertical bar eta vertical bar gamma gamma channel for the three colliding systems as well as through the eta decay mode in p+p and d+Au collisions.
Abstract: Inclusive transverse momentum spectra of eta mesons in the range p(T)approximate to 2-12 GeV/c have been measured at midrapidity (vertical bar eta vertical bar gamma gamma channel for the three colliding systems as well as through the eta ->pi(0)pi(+)pi(-) decay mode in p+p and d+Au collisions The nuclear modification factor in d+Au collisions, R-dAu(p(T))approximate to 10-11, suggests at most only modest p(T) broadening ("Cronin enhancement") In central Au+Au reactions, the eta yields are significantly suppressed, with R-AuAu(p(T))approximate to 02 The ratio of eta to pi(0) yields is approximately constant as a function of p(T) for the three colliding systems in agreement with the high-p(T) world average of R-eta/pi(0)approximate to 05 in hadron-hadron, hadron-nucleus, and nucleus-nucleus collisions for a wide range of center-of-mass energies (root sNN approximate to 3-1800 GeV) as well as, for high scaled momentum x(p), in e(+)e(-) annihilations at root s=912 GeV These results are consistent with a scenario where high-p(T) eta production in nuclear collisions at the Relativistic Heavy Ion Collider is largely unaffected by initial-state effects but where light-quark mesons (pi(0),eta) are equally suppressed due to final-state interactions of the parent partons in the dense medium produced in Au+Au reactions

Journal ArticleDOI
S. S. Adler1, S. Afanasiev2, Christine Angela Aidala1, N. N. Ajitanand3  +341 moreInstitutions (42)
TL;DR: In this paper, the results of the PHENIX Level-2 trigger for the first RHIC Au+Au run at the design center-of-mass energy were presented.
Abstract: Measurements of neutral pion (pi(0)) production at midrapidity in root s(NN)=200 GeV Au+Au collisions as a function of transverse momentum, p(T), collision centrality, and angle with respect to reaction plane are presented. The data represent the final pi(0) results from the PHENIX experiment for the first RHIC Au+Au run at design center-of-mass energy. They include additional data obtained using the PHENIX Level-2 trigger with more than a factor of 3 increase in statistics over previously published results for p(T)>6 GeV/c. We evaluate the suppression in the yield of high-p(T) pi(0)'s relative to pointlike scaling expectations using the nuclear modification factor R-AA. We present the p(T) dependence of R-AA for nine bins in collision centrality. We separately integrate R-AA over larger p(T) bins to show more precisely the centrality dependence of the high-p(T) suppression. We then evaluate the dependence of the high-p(T) suppression on the emission angle Delta phi of the pions with respect to event reaction plane for seven bins in collision centrality. We show that the yields of high-p(T) pi(0)'s vary strongly with Delta phi, consistent with prior measurements 1,2. We show that this variation persists in the most peripheral bin accessible in this analysis. For the peripheral bins we observe no suppression for neutral pions produced aligned with the reaction plane, whereas the yield of pi(0)'s produced perpendicular to the reaction plane is suppressed by a factor of similar to 2. We analyze the combined centrality and Delta phi dependence of the pi(0) suppression in different p(T) bins using different possible descriptions of parton energy loss dependence on jet path-length averages to determine whether a single geometric picture can explain the observed suppression pattern.


Journal ArticleDOI
TL;DR: In this paper, the authors used the reverse kinematics technique and the fragment separator at GSI (Darmstadt) to measure the spallation residues produced in the bombardment of 56)Fe at 1.5A, 1.0A, 0.75A and 0.3A GeV.
Abstract: The spallation residues produced in the bombardment of ^(56)Fe at 1.5A, 1.0A, 0.75A, 0.5A, and 0.3A GeV on a liquid-hydrogen target have been measured using the reverse kinematics technique and the fragment separator at GSI (Darmstadt). This technique has permitted the full identification in charge and mass of all isotopes produced with cross sections larger than 10^(-2) mb down to Z=8. Their individual production cross sections and recoil velocities at the five energies are presented. Production cross sections are compared with previously existing data and with empirical parametric formulas, often used in cosmic-ray astrophysics. The experimental data are also extensively compared with the results of different combinations of intranuclear cascade and deexcitation models. It is shown that the yields of the lightest isotopes cannot be accounted for by standard evaporation models. The GEMINI model, which includes an asymmetric fission decay mode, gives an overall good agreement with the data. These experimental data can be directly used for the estimation of composition modifications and damages in materials containing iron in spallation sources. They are also useful for improving high-precision cosmic-ray measurements.

Journal ArticleDOI
TL;DR: The α2/β2-Na+/K+-ATPase is identified and it is shown that this astroglial ATPase interacts directly with the immunoglobulin superfamily adhesion molecule basigin and may be functional in the metabolic cross talk between astrocytes and neurons, most likely under stress.
Abstract: Prion-related protein (PrP) is a neural cell adhesion molecule involved in neurite outgrowth, neuronal survival, and synaptic function. In search of novel binding partners for PrP, we identified the α2/β2-Na+/K+-ATPase and showed that this astroglial ATPase interacts directly with the immunoglobulin superfamily adhesion molecule basigin. In cultured astrocytes, PrP is involved in regulating lactate transport via the astroglial monocarboxylate transporter 1 (MCT1) and in conjunction with α2/β2-ATPase and basigin. Lactate transport via MCT1 is glutamate dependent and regulated by glutamate receptor 2 (GluR2)-containing AMPA receptors with which PrP interacts. The functional interplay between PrP, GluR2, α2/β2-ATPase, basigin, and MCT1 in regulating lactate transport of astrocytes may be functional in the metabolic cross talk between astrocytes and neurons, most likely under stress.

Journal ArticleDOI
TL;DR: Inelastic α scattering on 16 O is studied at 400 MeV using an ice target in this article, where a broad peak is observed at an excitation energy of 13.6 ± 0.1 ǫ with a width of 0.6 − 0.2

Journal ArticleDOI
Bernard Aubert1, Marcella Bona1, D. Boutigny1, Y. Karyotakis1  +567 moreInstitutions (78)
TL;DR: In this article, the branching fractions and CP asymmetries for B{sup 0,yields,pi,sup 0,pi,su,su 0,pi,su,Su,Su 0,Su 1,Su 2,Su 3,Su 4,Su 5,Su 6,Su 7,Su 0,Su 1 ] were measured by the BABAR detector at the PEP-II asymmetric energy B factory at SLAC.
Abstract: We present updated measurements of the branching fractions and CP asymmetries for B{sup 0}{yields}{pi}{sup 0}{pi}{sup 0}, B{sup {+-}}{yields}{pi}{sup {+-}}{pi}{sup 0}, and B{sup {+-}}{yields}K{sup {+-}}{pi}{sup 0}. Based on a sample of 383x10{sup 6} {upsilon}(4S){yields}BB decays collected by the BABAR detector at the PEP-II asymmetric-energy B factory at SLAC, we measure B(B{sup 0}{yields}{pi}{sup 0}{pi}{sup 0})=(1.47{+-}0.25{+-}0.12)x10{sup -6}, B(B{sup {+-}}{yields}{pi}{sup {+-}}{pi}{sup 0})=(5.02{+-}0.46{+-}0.29)x10{sup -6}, and B(B{sup {+-}}{yields}K{sup {+-}}{pi}{sup 0})=(13.6{+-}0.6{+-}0.7)x10{sup -6}. We also measure the CP asymmetries C{sub {pi}{sup 0}}{sub {pi}{sup 0}}=-0.49{+-}0.35{+-}0.05, A{sub {pi}{sup {+-}}}{sub {pi}{sup 0}}=0.03{+-}0.08{+-}0.01, and A{sub K{sup {+-}}}{sub {pi}{sup 0}}=0.030{+-}0.039{+-}0.010. Finally, we present bounds on the Cabibbo-Kobayashi-Maskawa angle {alpha} using isospin relations.

Journal ArticleDOI
Bernard Aubert1, Marcella Bona1, D. Boutigny1, Y. Karyotakis1  +567 moreInstitutions (78)
TL;DR: A measurement of the tau(-)-> K-pi(0)nu(tau) branching fraction has been made using 230.2 fb(-1) of data recorded by the BABAR detector at the PEP-II e(+)e(-) collider, located at the Stanford Linear Accelerator Center (SLAC), at a center-of-mass energy root s close to 10.58 GeV.
Abstract: A measurement of the tau(-)-> K-pi(0)nu(tau) branching fraction has been made using 230.2 fb(-1) of data recorded by the BABAR detector at the PEP-II e(+)e(-) collider, located at the Stanford Linear Accelerator Center (SLAC), at a center-of-mass energy root s close to 10.58 GeV. We measure B(tau(-)-> K-pi(0)nu(tau))=(0.416 +/- 0.003(stat)+/- 0.018(syst))%.

Journal ArticleDOI
Bernard Aubert1, Marcella Bona1, D. Boutigny1, Y. Karyotakis1  +569 moreInstitutions (78)
TL;DR: In this article, a preliminary measurement of the q2 dependence of the D0 --> K- e+ nu_e decay rate is presented, which is proportional to the hadronic form factor squared, specified by a single parameter.
Abstract: We present a preliminary measurement of the q2 dependence of the D0 --> K- e+ nu_e decay rate. This rate is proportional to the hadronic form factor squared, specified by a single parameter. This is either the mass in the simple pole ansatz m_pole = (1.854 +- 0.016 +- 0.020) GeV/c2 or the scale in the modified pole ansatz alpha_pole = 0.43 +- 0.03 +- 0.04. The first error refers to the statistical, the second to the systematic uncertainty.

Journal ArticleDOI
A. Adare1, S. S. Adler2, S. Afanasiev3, Christine Angela Aidala4  +501 moreInstitutions (51)
TL;DR: The broadening and peak location are found to depend upon the number of participants in the collision, but not on the collision energy or beam nuclei, and pose challenges to Cherenkov gluon radiation models.
Abstract: We present azimuthal angle correlations of intermediate transverse momentum (1-4 GeV/c) hadrons from dijets in Cu+Cu and Au+Au collisions at root s(NN)=62.4 and 200 GeV. The away-side dijet induced azimuthal correlation is broadened, non-Gaussian, and peaked away from Delta phi=pi in central and semicentral collisions in all the systems. The broadening and peak location are found to depend upon the number of participants in the collision, but not on the collision energy or beam nuclei. These results are consistent with sound or shock wave models, but pose challenges to Cherenkov gluon radiation models.

Journal ArticleDOI
Bernard Aubert1, Marcella Bona1, D. Boutigny1, Y. Karyotakis1  +578 moreInstitutions (78)
TL;DR: The analysis uses events in which the signal B decays are reconstructed with an innovative loose neutrino reconstruction technique, and finds the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element /Vub/ to be (4.4_{FF}) x 10(-3), where the last uncertainty is due to the normalization of the form factor.
Abstract: We report the results of a study of the exclusive charmless semileptonic decay, B-0 ->pi(-)center dot(+)nu, undertaken with approximately 227x10(6) BB pairs collected at the Upsilon(4S) resonance with the BABAR detector. The analysis uses events in which the signal B decays are reconstructed with an innovative loose neutrino reconstruction technique. We obtain partial branching fractions in 12 bins of q(2), the momentum transfer squared, from which we extract the f(+)(q(2)) form-factor shape and the total branching fraction B(B-0 ->pi(-)l(+)nu)=(1.46 +/- 0.07(stat)+/- 0.08(syst))x10(-4). Based on a recent unquenched lattice QCD calculation of the form factor in the range q(2)> 16 GeV2, we find the magnitude of the Cabibbo-Kobayashi-Maskawa matrix element vertical bar V-ub vertical bar to be (4.1 +/- 0.2(stat)+/- 0.2(syst)+0.6-0.4(FF))x10(-3), where the last uncertainty is due to the normalization of the form factor.

Journal ArticleDOI
V. M. Abazov1, Brad Abbott2, M. Abolins3, B. S. Acharya4  +591 moreInstitutions (79)
TL;DR: The first direct measurement of the CP-violating mixing phase in the B-s(0) system was reported in this paper, where the width difference between the light and heavy mass eigenstates Delta Gamma equivalent to (Gamma(L)-Gamma (H))=0.17 +/- 0.09(stat)+/- 0.02(syst) ps(-1) and the CPviolating phase phi(s)=-0.79 +/-0.56(stat)(-0.12(-0.10)(+0.08)(stat
Abstract: From an analysis of the decay B-s(0)-> J/psi phi, we obtain the width difference between the light and heavy mass eigenstates Delta Gamma equivalent to(Gamma(L)-Gamma(H))=0.17 +/- 0.09(stat)+/- 0.02(syst) ps(-1) and the CP-violating phase phi(s)=-0.79 +/- 0.56(stat)(-0.01)(+0.14)(syst). Under the hypothesis of no CP violation (phi(s)equivalent to 0), we obtain 1/Gamma=tau/(B-s(0))=1.52 +/- 0.08(stat)(-0.03)(+0.01)(syst) ps and Delta Gamma=0.12(-0.10)(+0.08)(stat)+/- 0.02(syst) ps(-1). The data sample corresponds to an integrated luminosity of about 1.1 fb(-1) accumulated with the D0 detector at the Fermilab Tevatron collider. This is the first direct measurement of the CP-violating mixing phase in the B-s(0) system.