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Showing papers by "German Martinez published in 2008"


Journal ArticleDOI
TL;DR: The Compact Muon Solenoid (CMS) detector at the Large Hadron Collider (LHC) at CERN as mentioned in this paper was designed to study proton-proton (and lead-lead) collisions at a centre-of-mass energy of 14 TeV (5.5 TeV nucleon-nucleon) and at luminosities up to 10(34)cm(-2)s(-1)
Abstract: The Compact Muon Solenoid (CMS) detector is described. The detector operates at the Large Hadron Collider (LHC) at CERN. It was conceived to study proton-proton (and lead-lead) collisions at a centre-of-mass energy of 14 TeV (5.5 TeV nucleon-nucleon) and at luminosities up to 10(34)cm(-2)s(-1) (10(27)cm(-2)s(-1)). At the core of the CMS detector sits a high-magnetic-field and large-bore superconducting solenoid surrounding an all-silicon pixel and strip tracker, a lead-tungstate scintillating-crystals electromagnetic calorimeter, and a brass-scintillator sampling hadron calorimeter. The iron yoke of the flux-return is instrumented with four stations of muon detectors covering most of the 4 pi solid angle. Forward sampling calorimeters extend the pseudo-rapidity coverage to high values (vertical bar eta vertical bar <= 5) assuring very good hermeticity. The overall dimensions of the CMS detector are a length of 21.6 m, a diameter of 14.6 m and a total weight of 12500 t.

5,193 citations


Journal ArticleDOI
Georges Aad1, M. Ackers2, F. Alberti, M. Aleppo3  +264 moreInstitutions (18)
TL;DR: In this article, the silicon pixel tracking system for the ATLAS experiment at the Large Hadron Collider is described and the performance requirements are summarized and detailed descriptions of the pixel detector electronics and the silicon sensors are given.
Abstract: The silicon pixel tracking system for the ATLAS experiment at the Large Hadron Collider is described and the performance requirements are summarized. Detailed descriptions of the pixel detector electronics and the silicon sensors are given. The design, fabrication, assembly and performance of the pixel detector modules are presented. Data obtained from test beams as well as studies using cosmic rays are also discussed.

709 citations


Journal ArticleDOI
Néstor Armesto1, Nicolas Borghini2, Sangyong Jeon3, Urs Achim Wiedemann4  +191 moreInstitutions (63)
TL;DR: A compilation of predictions for the forthcoming Heavy Ion Program at the Large Hadron Collider, as presented at the CERN Theory Institute 'Heavy Ion Collisions at the LHC - Last Call for Predictions', held from 14th May to 10th June 2007, can be found in this article.
Abstract: This writeup is a compilation of the predictions for the forthcoming Heavy Ion Program at the Large Hadron Collider, as presented at the CERN Theory Institute 'Heavy Ion Collisions at the LHC - Last Call for Predictions', held from 14th May to 10th June 2007.

234 citations


Journal ArticleDOI
A. Adare1, S. S. Adler2, S. Afanasiev3, Christine Angela Aidala4  +487 moreInstitutions (51)
TL;DR: In this paper, a new analysis of J/psi production yields in deuteron-gold collisions at root s(NN) =200 GeV using data taken from the PHENIX experiment in 2003 and previously published in S. S. Adler [Phys. Rev.
Abstract: We present a new analysis of J/psi production yields in deuteron-gold collisions at root s(NN) =200 GeV using data taken from the PHENIX experiment in 2003 and previously published in S. S. Adler [Phys. Rev. Lett 96, 012304 (2006)]. The high statistics proton-proton J/psi data taken in 2005 are used to improve the baseline measurement and thus construct updated cold nuclear matter modification factors (R-dAu). A suppression of J/psi in cold nuclear matter is observed as one goes forward in rapidity (in the deuteron-going direction), corresponding to a region more sensitive to initial-state low-x gluons in the gold nucleus. The measured nuclear modification factors are compared to theoretical calculations of nuclear shadowing to which a J/psi (or precursor) breakup cross section is added. Breakup cross sections of sigma(breakup)=2.8(-1.4)(+1.7) (2.2(-1.5)(+1.6)) mb are obtained by fitting these calculations to the data using two different models of nuclear shadowing. These breakup cross-section values are consistent within large uncertainties with the 4.2 +/- 0.5 mb determined at lower collision energies. Projecting this range of cold nuclear matter effects to copper-copper and gold-gold collisions reveals that the current constraints are not sufficient to firmly quantify the additional hot nuclear matter effect.

92 citations


Journal ArticleDOI
Salavat Abdullin1, Salavat Abdullin2, V. Abramov, B. S. Acharya3  +221 moreInstitutions (34)
TL;DR: In this article, the authors report on the test beam results and calibration methods using high energy electrons, pions and muons with the CMS forward calorimeter (HF), which is essential for a large number of physics channels with missing transverse energy.
Abstract: We report on the test beam results and calibration methods using high energy electrons, pions and muons with the CMS forward calorimeter (HF). The HF calorimeter covers a large pseudorapidity region (\(3\leq|\eta|\leq5\)), and is essential for a large number of physics channels with missing transverse energy. It is also expected to play a prominent role in the measurement of forward tagging jets in weak boson fusion channels in Higgs production. The HF calorimeter is based on steel absorber with embedded fused-silica-core optical fibers where Cherenkov radiation forms the basis of signal generation. Thus, the detector is essentially sensitive only to the electromagnetic shower core and is highly non-compensating (e/h≈5). This feature is also manifest in narrow and relatively short showers compared to similar calorimeters based on ionization. The choice of fused-silica optical fibers as active material is dictated by its exceptional radiation hardness. The electromagnetic energy resolution is dominated by photoelectron statistics and can be expressed in the customary form as \(\frac{a}{\sqrt{E}}\oplus{b}\). The stochastic term a is 198% and the constant term b is 9%. The hadronic energy resolution is largely determined by the fluctuations in the neutral pion production in showers, and when it is expressed as in the electromagnetic case, a = 280% and b = 11%.

88 citations


Journal ArticleDOI
A. Adare1, S. S. Adler2, S. Afanasiev3, Christine Angela Aidala4  +501 moreInstitutions (51)
TL;DR: A comprehensive survey of event-by-event fluctuations of charged hadron multiplicity in relativistic heavy ions is presented in this paper, which covers Au+Au collisions at s(NN) = 62.4 and 200 GeV, and Cu+Cu collisions at 22.5,62.4, and 200 geV.
Abstract: A comprehensive survey of event-by-event fluctuations of charged hadron multiplicity in relativistic heavy ions is presented. The survey covers Au+Au collisions at s(NN) =62.4 and 200 GeV, and Cu+Cu collisions at s(NN) =22.5,62.4, and 200 GeV. Fluctuations are measured as a function of collision centrality, transverse momentum range, and charge sign. After correcting for nondynamical fluctuations due to fluctuations in the collision geometry within a centrality bin, the remaining dynamical fluctuations expressed as the variance normalized by the mean tend to decrease with increasing centrality. The dynamical fluctuations are consistent with or below the expectation from a superposition of participant nucleon-nucleon collisions based upon p+p data, indicating that this dataset does not exhibit evidence of critical behavior in terms of the compressibility of the system. A comparison of the data with a model where hadrons are independently emitted from a number of hadron clusters suggests that the mean number of hadrons per cluster is small in heavy ion collisions.

66 citations


Proceedings ArticleDOI
TL;DR: DECam as mentioned in this paper is a 3 sq. deg. mosaic camera mounted at the prime focus of the Blanco 4m telescope at the Cerro-Tololo Observatory at the International Observatory (CTIO).
Abstract: We describe the Dark Energy Camera (DECam), which will be the primary instrument used in the Dark Energy Survey. DECam will be a 3 sq. deg. mosaic camera mounted at the prime focus of the Blanco 4m telescope at the Cerro-Tololo International Observatory (CTIO). DECam includes a large mosaic CCD focal plane, a five element optical corrector, five filters (g,r,i,z,Y), and the associated infrastructure for operation in the prime focus cage. The focal plane consists of 62 2K x 4K CCD modules (0.27"/pixel) arranged in a hexagon inscribed within the roughly 2.2 degree diameter field of view. The CCDs will be 250 micron thick fully-depleted CCDs that have been developed at the Lawrence Berkeley National Laboratory (LBNL). Production of the CCDs and fabrication of the optics, mechanical structure, mechanisms, and control system for DECam are underway; delivery of the instrument to CTIO is scheduled for 2010.

45 citations


Journal ArticleDOI
Madan M. Aggarwal, Zubayer Ahammed, A.L.S. Angelis, V.G. Antonenko, V. Arefiev, V. Astakhov, V. Avdeitchikov, T. C. Awes, P.V.K.S. Baba, S. K. Badyal, S. Bathe, B. Batiounia, C. Baumann, T. Bernier, K. B. Bhalla, V. S. Bhatia, Christoph Blume, D. Bucher, H. Büsching, Lars Carlén, Sukalyan Chattopadhyay, M. P. Decowski, H. Delagrange, P. Donni, M. R. Dutta Majumdar, K. El Chenawi, Anand Kumar Dubey, K. Enosawa, Sergey Fokin, Vladimir Frolov, M. S. Ganti, S. Garpman, O. P. Gavrishchuk, Frank Jm Geurts, T. K. Ghosh, R. Glasow, B.N. Gus'kov, H. A. Gustafsson, H.H. Gutbrod, Ivana Hrivnacova, Mikhail Ippolitov, H. Kalechofsky, R. Kamermans, K. Karadjev, Krzysztof Karpio, B. W. Kolb, I. Kosarev, I. Koutcheryaev, A. Kugler, P. Kulinich, M. Kurata, A. Lebedev, Herbert Löhner, L. Luquin, D. P. Mahapatra, Vladislav Manko, MV Manzano Martin, German Martinez, A. Maximov, Yasuo Miake, G. C. Mishra, Bedangadas Mohanty, M. J. Mora, D. P. Morrison, T. Mukhanova, D. Mukhopadhyay, H. Naef, Basanta Kumar Nandi, S. K. Nayak, T. K. Nayak, A. Nianine, V. Nikitine, Sergey Nikolaev, Peter M. Nilsson, Shunji Nishimura, Petr Nomokonov, Joakim Nystrand, Agneta Oskarsson, I. Otterlund, S. Pavliouk, T. Peitzmann, D. Y.-U. Peressounko, V. Petráček, S. C. Phatak, W. Pinganaud, F. Plasil, Martin Purschke, J. Rak, M. Rammler, Rashmi Raniwala, Sudhir Raniwala, N. K. Rao, F. Retiere, Klaus Johannes Reygers, Gunther Roland, L. Rosselet, I. Roufanov, C. Roy, J. M. Rubio, Sanjeev Singh Sambyal, R. Santo, Susumu Sato, H. Schlagheck, Hr Schmidt, Yves Roland Schutz, G.S. Shabratova, T. H. Shah, I. Sibiriak, Teodor Siemiarczuk, D. Silvermyr, Bikash Sinha, Nikolai V Slavine, K. Söderström, G. Sood, S. P. Sorensen, P. W. Stankus, G. Stefanek, P. Steinberg, E. Stenlund, Michal Sumbera, T. Svensson, A. A. Tsvetkov, L. Tykarski, E. C. v. d. Pijll, N. v. Eijndhoven, Gerrit Jan van Nieuwenhuizen, A. A. Vinogradov, Y. P. Viyogi, A.S. Vodopianov, S. Vörös, Bolek Wyslouch, G. R. Young 
TL;DR: For a wide range of Pb+Pb centralities (N{part} less than or approximately equal 300), the yield of pi{0}'s with p{T} greater than or about equal 2 GeV/c is larger than or consistent with the p+C or p-Pb yields scaled with the number of nucleon-nucleon collisions.
Abstract: Neutral pion transverse momentum spectra were measured in $p+\mathrm{C}$ and $p+\mathrm{Pb}$ collisions at $\sqrt{{s}_{NN}}=174\text{ }\text{ }\mathrm{GeV}$ at midrapidity ($23\ensuremath{\lesssim}{\ensuremath{\eta}}_{\mathrm{lab}}\ensuremath{\lesssim}30$) over the range $07\ensuremath{\lesssim}{p}_{T}\ensuremath{\lesssim}35\text{ }\text{ }\mathrm{GeV}/c$ The spectra are compared to ${\ensuremath{\pi}}^{0}$ spectra measured in $\mathrm{Pb}+\mathrm{Pb}$ collisions at $\sqrt{{s}_{NN}}=173\text{ }\text{ }\mathrm{GeV}$ in the same experiment For a wide range of $\mathrm{Pb}+\mathrm{Pb}$ centralities (${N}_{\mathrm{part}}\ensuremath{\lesssim}300$), the yield of ${\ensuremath{\pi}}^{0}$'s with ${p}_{T}\ensuremath{\gtrsim}2\text{ }\text{ }\mathrm{GeV}/c$ is larger than or consistent with the $p+\mathrm{C}$ or $p+\mathrm{Pb}$ yields scaled with the number of nucleon-nucleon collisions (${N}_{\mathrm{coll}}$), while for central $\mathrm{Pb}+\mathrm{Pb}$ collisions with ${N}_{\mathrm{part}}\ensuremath{\gtrsim}350$, the ${\ensuremath{\pi}}^{0}$ yield is suppressed

26 citations


Journal ArticleDOI
S. S. Adler1, S. Afanasiev2, Christine Angela Aidala3, N. N. Ajitanand4  +339 moreInstitutions (45)
TL;DR: In this article, the transverse momentum (p(T)) spectra of charged hadrons measured in deuteron-gold and nucleon gold collisions at root s(NN)=200 GeV were presented.
Abstract: We present transverse momentum (p(T)) spectra of charged hadrons measured in deuteron-gold and nucleon-gold collisions at root s(NN)=200 GeV for four centrality classes. Nucleon-gold collisions were selected by tagging events in which a spectator nucleon was observed in one of two forward rapidity detectors. The spectra and yields were investigated as a function of the number of binary nucleon-nucleon collisions, nu, suffered by deuteron nucleons. A comparison of charged particle yields to those in p+p collisions show that yield per nucleon-nucleon collision saturates with nu for high momentum particles. We also present the charged hadron to neutral pion ratios as a function of p(T).

22 citations


Journal ArticleDOI
Salavat Abdullin, V. Abramov, B. S. Acharya1, N. E. Adam2  +259 moreInstitutions (34)
TL;DR: The outer hadron calorimeter (HCAL HO) as mentioned in this paper was designed to measure the energy that is not contained by the barrel and electromagnetic (ECAL EB) calorimeters.
Abstract: The Outer Hadron Calorimeter (HCAL HO) of the CMS detector is designed to measure the energy that is not contained by the barrel (HCAL HB) and electromagnetic (ECAL EB) calorimeters. Due to space limitation the barrel calorimeters do not contain completely the hadronic shower and an outer calorimeter (HO) was designed, constructed and inserted in the muon system of CMS to measure the energy leakage. Testing and calibration of the HO was carried out in a 300 GeV/c test beam that improved the linearity and resolution. HO will provide a net improvement in missing E T measurements at LHC energies. Information from HO will also be used for the muon trigger in CMS.

19 citations


Proceedings ArticleDOI
TL;DR: The Dark Energy Survey Camera (DECam) as discussed by the authors was the first camera with a large number of CCDs and was used for image acquisition at the National Optical Astronomy Observatory (NOAO).
Abstract: The Dark Energy Survey Camera (DECam), when completed, is going to have one of the largest existing focal planes, equipped with more than 70 CCDs. Due to the large number of CCDs and the tight space on the camera, the DECam electronics group has developed new compact front-end electronics capable of flexibly and rapidly reading out all the focal plane CCDs. The system is based on the existing MONSOON Image Acquisition System designed by the National Optical Astronomy Observatory (NOAO), and it is currently being used for testing and characterization of CCDs. Boards for the new readout are being developed in USA and Spain, with the first prototypes already produced and tested. The next version with some improvements will be tested during 2008 and the system will be ready for production at the beginning of 2009. Custom MONSOON boards and the electronics path will be described.

Proceedings ArticleDOI
TL;DR: In this article, the clock board has been redesigned to meet the stringent requirements of the Dark Energy Survey, and the first test results with the new clock board showed a clear improvement in the charge transfer efficiency (CTE) response when reading out at the higher frequencies required for the guide CCDs.
Abstract: The Dark Energy Camera will be comprised of 74 CCDs with high efficiency out to a wavelength of 1 micron. The CCDs will be read out by a Monsoon-based system consisting of three boards: Master Control, CCD Acquisition, and Clock boards. The charge transfer efficiency (CTE) is closely related to the clock waveforms provided by the Clock Board (CB). The CB has been redesigned to meet the stringent requirements of the Dark Energy Survey. The number of signals provided by the clock board has been extended from 32 (the number required for 2 CCDs) up to 135 signals (the number required for 9 CCDs). This modification is required to fit the electronics into the limited space available on the imager vessel. In addition, the drivers have been changed to provide more current. The first test result with the new clock board shows a clear improvement in the CTE response when reading out at the higher frequencies required for the guide CCDs.