278 results on '"P. Salabura"'
Search Results
252. Plastic scintillators for positron emission tomography obtained by the bulk polymerization method
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Kapłon, Łukasz, Kochanowski, Andrzej, Molenda, Marcin, Moskal, Paweł, Wieczorek, Anna, Bednarski, Tomasz, Białas, Piotr, Czerwiński, Eryk, Korcyl, Grzegorz, Kowal, Jakub, Kowalski, Paweł, Kozik, Tomasz, Krzemień, Wojciech, Niedźwiecki, Szymon, Pałka, Marek, Pawlik, Monika, Raczyński, Lech, Rudy, Zbigniew, Salabura, Piotr, Gupta-Sharma, Neha, Silarski, Michał, Słomski, Artur, Smyrski, Jerzy, Strzelecki, Adam, Wiślicki, Wojciech, Zieliński, Marcin, and Zoń, Natalia
- Abstract
AbstractThis paper describes three methods regarding the production of plastic scintillators. One method appears to be suitable for the manufacturing of plastic scintillators, revealing properties which fulfill the requirements of novel positron emission tomography scanners based on plastic scintillators. The key parameters of the manufacturing process are determined and discussed.
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- 2014
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253. Trigger-less and reconfigurable data acquisition system for positron emission tomography
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Korcyl, Grzegorz, Moskal, Paweł, Bednarski, Tomasz, Białas, Piotr, Czerwiński, Eryk, Kapłon, Łukasz, Kochanowski, Andrzej, Kowal, Jakub, Kowalski, Paweł, Kozik, Tomasz, Krzemień, Wojciech, Molenda, Marcin, Niedźwiecki, Szymon, Pałka, Marek, Pawlik, Monika, Raczyński, Lech, Rudy, Zbigniew, Salabura, Piotr, Gupta-Sharma, Neha, Silarski, Michał, Słomski, Artur, Smyrski, Jerzy, Strzelecki, Adam, Wiślicki, Wojciech, Zieliński, Marcin, and Zoń, Natalia
- Abstract
AbstractThis article is focused on data acquisition system (DAQ) designed especially to be used in positron emission tomography (PET) or single-photon emission computed tomography. The system allows for continuous registration of analog signals during measurement. It has been designed to optimize registration and processing of the information carried by signals from the detector system in PET scanner. The processing does not require any rejection of data with a trigger system. The proposed system possesses also an ability to implement various data analysis algorithms that can be performed in real time during data collection.
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- 2014
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254. Calibration of photomultipliers gain used in the J-PET detector
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Bednarski, Tomasz, Czerwiński, Eryk, Moskal, Paweł, Białas, Piotr, Giergiel, Krzysztof, Kapłon, Łukasz, Kochanowski, Andrzej, Korcyl, Grzegorz, Kowal, Jakub, Kowalski, Paweł, Kozik, Tomasz, Krzemień, Wojciech, Molenda, Marcin, Moskal, Ines, Niedźwiecki, Szymon, Pałka, Marek, Pawlik, Monika, Raczyński, Lech, Rudy, Zbigniew, Salabura, Piotr, Sharma, Neha Gupta, Silarski, Michał, Słomski, Artur, Smyrski, Jerzy, Strzelecki, Adam, Szymański, Konrad Jan, Wiślicki, Wojciech, Witkowski, Piotr, Zieliński, Marcin, and Zoń, Natalia
- Abstract
AbstractPhotomultipliers are commonly used in commercial PET scanner as devices that convert light produced in scintillator by gamma quanta from positron-electron annihilation into electrical signal. For proper analysis of obtained electrical signal, a photomultiplier gain curve must be known, since gain can be significantly different even between photomultipliers of the same model. In this article, we describe single photoelectron method used for photomultiplier calibration applied for J-PET scanner, a novel PET detector being developed at Jagiellonian University. A description of calibration method, an example of calibration curve, and a gain of few Hamamatsu R4998 photomultipliers are presented.
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- 2014
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255. List-mode reconstruction in 2D strip PET
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Białas, Piotr, Kowal, Jakub, Strzelecki, Adam, Bednarski, Tomasz, Czerwiński, Eryk, Giergiel, Krzysztof, Kapłon, Łukasz, Kochanowski, Andrzej, Korcyl, Grzegorz, Kowalski, Paweł, Kozik, Tomasz, Krzemień, Wojciech, Molenda, Marcin, Moskal, Ines, Moskal, Paweł, Niedźwiecki, Szymon, Pałka, Marek, Pawlik, Monika, Raczyński, Lech, Rudy, Zbigniew, Salabura, Piotr, Sharma, Neha G., Silarski, Michał, Słomski, Artur, Smyrski, Jerzy, Szymański, Konrad, Wiślicki, Wojciech, Witkowski, Piotr, Zieliński, Marcin, and Zoń, Natalia
- Abstract
AbstractUsing a theory of list-mode maximum likelihood expectation-maximization (MLEM) algorithm, in this contribution, we present a derivation of the system response kernel for a novel positron emission tomography (PET) detector based on plastic scintillators.
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- 2014
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256. J-PET analysis framework for the prototype TOF-PET detector
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Krzemień, Wojciech, Silarski, Michał, Stoła, Karol, Trybek, Damian, Bednarski, Tomasz, Białas, Piotr, Czerwiński, Eryk, Kapłon, Łukasz, Kochanowski, Andrzej, Korcyl, Grzegorz, Kowal, Jakub, Kowalski, Paweł, Kozik, Tomasz, Molenda, Marcin, Moskal, Paweł, Niedźwiecki, Szymon, Pałka, Marek, Pawlik, Monika, Raczyński, Lech, Rudy, Zbigniew, Salabura, Piotr, Sharma, Neha Gupta, Słomski, Artur, Smyrski, Jerzy, Strzelecki, Adam, Wiślicki, Wojciech, Zieliński, Marcin, and Zoń, Natalia
- Abstract
AbstractNovel time-of-flight positron emission tomography (TOF-PET) scanner solutions demand, apart from the state-of-the-art detectors, software for fast processing of the gathered data, monitoring of the whole scanner, and reconstruction of the PET image. In this article, we present an analysis framework for the novel STRIP-PET scanner developed by the J-PET collaboration in the Institute of Physics of the Jagiellonian University. This software is based on the ROOT package used in many particle physics experiments.
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- 2014
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257. 3D PET image reconstruction based on the maximum likelihood estimation method (MLEM) algorithm
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Słomski, Artur, Rudy, Zbigniew, Bednarski, Tomasz, Białas, Piotr, Czerwiński, Eryk, Kapłon, Łukasz, Kochanowski, Andrzej, Korcyl, Grzegorz, Kowal, Jakub, Kowalski, Paweł, Kozik, Tomasz, Krzemień, Wojciech, Molenda, Marcin, Moskal, Paweł, Niedźwiecki, Szymon, Pałka, Marek, Pawlik, Monika, Raczyński, Lech, Salabura, Piotr, Gupta-Sharma, Neha, Silarski, Michał, Smyrski, Jerzy, Strzelecki, Adam, Wiślicki, Wojciech, Zieliński, Marcin, and Zoń, Natalia
- Abstract
AbstractA positron emission tomography (PET) scan does not measure an image directly. Instead, a PET scan measures a sinogram at the boundary of the field-of-view that consists of measurements of the sums of all the counts along the lines connecting the two detectors. Because there is a multitude of detectors built in a typical PET structure, there are many possible detector pairs that pertain to the measurement. The problem is how to turn this measurement into an image (this is called imaging). Significant improvement in PET image quality was achieved with the introduction of iterative reconstruction techniques. This was realized approximately 20 years ago (with the advent of new powerful computing processors). However, three-dimensional imaging still remains a challenge. The purpose of the image reconstruction algorithm is to process this imperfect count data for a large number (many millions) of lines of response and millions of detected photons to produce an image showing the distribution of the labeled molecules in space.
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- 2014
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258. A novel method for calibration and monitoring of time synchronization of TOF-PET scanners by means of cosmic rays
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Silarski, Michał, Czerwiński, Eryk, Bednarski, Tomasz, Moskal, Paweł, Białas, Piotr, Kapłon, Łukasz, Kochanowski, Andrzej, Korcyl, Grzegorz, Kowal, Jakub, Kowalski, Paweł, Kozik, Tomasz, Krzemień, Wojciech, Molenda, Marcin, Niedźwiecki, Szymon, Pałka, Marek, Pawlik, Monika, Raczyński, Lech, Rudy, Zbigniew, Salabura, Piotr, Sharma, Neha Gupta, Słomski, Artur, Smyrski, Jerzy, Strzelecki, Adam, Wiślicki, Wojciech, Zieliński, Marcin, and Zoń, Natalia
- Abstract
AbstractAll of the present methods for calibration and monitoring of time-of-flight positron emission tomography (TOF-PET) scanner detectors utilize radioactive isotopes, such as 22Na or 68Ge, which are placed or rotate inside the scanner. In this article, we describe a novel method based on the cosmic rays application to the PET calibration and monitoring methods. The concept allows to overcome many of the drawbacks of the present methods and it is well suited for newly developed TOF-PET scanners with a large longitudinal field of view. The method enables also the monitoring of the quality of the scintillator materials and in general allows for the continuous quality assurance of the PET detector performance.
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- 2014
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259. A novel method based solely on field programmable gate array (FPGA) units enabling measurement of time and charge of analog signals in positron emission tomography (PET)
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Pałka, Marek, Moskal, Paweł, Bednarski, Tomasz, Białas, Piotr, Czerwiński, Eryk, Kapłon, Łukasz, Kochanowski, Andrzej, Korcyl, Grzegorz, Kowal, Jakub, Kowalski, Paweł, Kozik, Tomasz, Krzemień, Wojciech, Molenda, Marcin, Niedźwiecki, Szymon, Pawlik, Monika, Razyński, Lech, Rudy, Zbigniew, Salabura, Piotr, Gupta-Sharma, Neha, Silarski, Michał, Słomski, Artur, Smyrski, Jerzy, Strzelecki, Adam, Wiślicki, Wojciech, Zieliński, Marcin, and Zoń, Natalia
- Abstract
AbstractThis article presents an application of a novel technique for precise measurements of time and charge based solely on a field programmable gate array (FPGA) device for positron emission tomography (PET). The described approach simplifies electronic circuits, reduces the power consumption, lowers costs, merges front-end electronics with digital electronics, and also makes more compact final design. Furthermore, it allows to measure time when analog signals cross a reference voltage at different threshold levels with a very high precision of ~15 ps (rms) and thus enables sampling of signals in a voltage domain.
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- 2014
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260. Conception d'un tribom?tre environnemental pour l'?tude de la r?activit? des surfaces frottantes
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Salabura, J.-C., Adamou, A., Denape, J., Paris, J.-Y., and Andrieu, E.
- Abstract
In tribology, a way of improving efficiently the understanding of the mechanical/thermal/environmental interactions on the chemical reactivity at the surface and interface level is to perform experiments where contact conditions are perfectly controlled (in terms of partial oxygen pressure, moisture or vacuum, and temperature). For this reason, an environmental tribometer was developed. The aim of this article is to set out the chosen technological solutions, to present the instrumentation (force, displacement, pressure temperature and contact resistance sensors, in situ gas analyser), and to describe the performances of this protoype. En tribologie, un moyen de progresser efficacement dans la compr?hension des ph?nom?nes de couplage m?canique/thermique/environnemental sur la r?activit? au niveau des surfaces et des interfaces est l'exp?rimentation o? les conditions de contact sont parfaitement contr?l?es (en termes de pression partielle d'oxyg?ne, d'humidit? ou sous vide, et de temp?rature). Pour cela, un tribom?tre environnemental a ?t? d?velopp?. L'objet de cet article est d'exposer les solutions technologiques adopt?es, de pr?senter l'instrumentation (capteurs de force, de d?placement, de pression, de temp?rature, de r?sistance de contact, analyseur de gaz in?situ), et de d?crire les performances de ce prototype.
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- 2006
261. Multi-Sample Thermobalance for Rapid Cyclic Oxidation under Controlled Atmosphere
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Salabura, Jean-Claude and Monceau, Daniel
- Abstract
Not Available
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- 2004
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262. Influence of heavy-ion bombardment on the structure of targets for atomic and nuclear interaction studies
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H. Folger, K. Bethge, K. E. Stiebing, P. Salabura, H. Bokemeyer, and D. Kraft
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Physics ,Nuclear and High Energy Physics ,Positron ,Ion implantation ,Proton ,Projectile ,Irradiation ,Atomic physics ,Nuclear Experiment ,Spectroscopy ,Instrumentation ,Beam (structure) ,Ion - Abstract
An accurate knowledge of the absolute magnitude of the energy loss of heavy ions inside targets is necessary in many experiments. The energy loss and target properties are directly correlated. Even if the initial status of a target is known, the heavy-ion bombardment may lead to a drastic change of its properties or even to its total deterioration. The degree and timescale of a possible variation depends on the type of the projectile beam and on the target properties itself, the latter being influenced by the chemical composition, the physical characteristics, and the mechanical arrangement of the target system. Structural changes of a target system limit its useful lifetime; it can be prolonged by special techniques like the application of target wobblers or target wheels. 1.6 MeV proton backscattering has been employed to investigate series of targets prior to and after their irradiation in heavy-ion beams in order to gain information on structural changes for the interpretation of experimental results obtained in heavy-ion positron spectroscopy.
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- 1989
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263. Production of η′and K−mesons in pp reactions at 2.85 GeV
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Kühn, W., Balestra, F., Bedfer, Y., Bertini, R., Bland, L.C., Brochard, F., Bussa, M.P., Chalyshev, V., Choi, Seonho, Debowski, M., Dzemidzic, M., Faivre, J.-Cl., Falomkin, I.V., Fava, L., Ferrero, L., Foryciarz, J., Frolov, V., Fröhlich, T., Garfagnini, R., Gill, D., Grasso, A., Heinz, S., Tvanov, V.V., Jacobs, W.W., Maggiora, A., Maggiora, M., Manara, A., Panzieri, D., Pfaff, H.-W., Piragino, G., Pontecorvo, G.B., Popov, A., Ritman, J., Salabura, P., Tosello, F., Vigdor, S.E., and Zosi, G.
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- 2000
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264. Spin observables in hyperon production
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Maggiora, M., Balestra, F., Bedfer, Y., Bertini, R., Bland, L.C., Brochard, F., Bussa, M.P., Chalyshev, V., Choi, Seonho, Debowski, M., Dzemidzic, M., Faivre, J.-Cl., Falomkin, I.V., Fava, L., Ferrero, L., Foryciarz, J., Frolov, V., Fröhlich, I., Garfagnini, R., Gill, D., Grasso, A., Heinz, S., Ivanov, V.V., Jacobs, W.W., Kühn, W., Maggiora, A., Manara, A., Panzieri, D., Pfaff, H.-W., Piragino, G., Pontecorvo, G.B., Popov, A., Ritman, J., Salabura, P., Tosello, F., Vigdor, S.E., and Zosi, G.
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- 2000
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265. A versatile method for simulating pp $ \rightarrow$ ppe+e- and dp $ \rightarrow$ pne+e-pspec reactions
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B. Ramstein, F. Dohrmann, P.K. Kaehlitz, Y. C. Pachmayer, J. Van de Wiele, R. Holzmann, Joachim Stroth, J. Wuestenfeld, Tetyana Galatyuk, R. Trebacz, P. Salabura, I. Froehlich, E. Morinière, and B. Kaempfer
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Physics ,Particle physics ,Nuclear and High Energy Physics ,Spectrometer ,010308 nuclear & particles physics ,Interface (Java) ,Bremsstrahlung ,Software package ,01 natural sciences ,7. Clean energy ,Interpretation (model theory) ,0103 physical sciences ,Production (computer science) ,010306 general physics ,Nuclear Experiment - Abstract
We have developed a versatile software package for the simulation of di-electron production in $pp$ and $dp$ collisions at SIS energies. Particular attention has been paid to incorporate different descriptions of the Dalitz decay $\Delta \to N e^+e^-$ via a common interface. In addition, suitable parameterizations for the virtual bremsstrahlung process $NN \to NN e^+e^-$ based on one-boson exchange models have been implemented. Such simulation tools with high flexibility of the framework are important for the interpretation of the di-electron data taken with the HADES spectrometer and the design of forthcoming experiments.
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266. Track finding algorithm using the track road method for the PANDA Forward Tracker.
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Płażek, J., Smyrski, J., Salabura, P., Przygoda, W., and Korcyl, K.
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TRACKING algorithms ,MAGNETIC particles ,PANDAS ,PATTERN recognition systems ,ALGORITHMS ,MUONS - Abstract
• A semi-analytical method is proposed to the 3D pattern recognition of particle traces. • Particles move on straight line in absence of magnetic field and on helix inside. • The efficiency for events with 5 tracks is above 91% for higher energy, 79% for 0.55 GeV/c. In this study, we present an algorithm for 3D track finding in the Forward Tracker of the PANDA experiment. This tracker is based on straw tube detectors and is designed to measure the deflection of particles in the magnetic field of the PANDA dipole magnet in order to determine their momenta. The algorithm uses the track road method for selecting track candidates. The applied track model in the projection onto the bending plane in the region before, inside and after the dipole magnet gap consists of line, circle and line, respectively. In the non-bending plane, a track projection is represented by a straight line. The algorithm was tested using simulated tracks of muons and obtained results for the track finding efficiency and for the momentum resolution are presented. [ABSTRACT FROM AUTHOR]
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- 2021
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267. An angle-sensitive detection system for scattered heavy ions
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Ganz, R, Thee, P, Bär, R, Bethge, K, Bokemeyer, H, Folger, H, Samek, M, Salabura, P, Schwalm, D, and Stiebing, K.E
- Abstract
A compact detection system for heavy ions scattered in collisions at the Coulomb barrier is presented. This system, consisting of four identical, low-pressure Parallel Plate Avalanche Counter (PPAC) modules with two sensitive layers each, was built to operate in an ultra-high-vacuum environment inside the EPoS II solenoid spectrometer at GSI Darmstadt. The detector covers polar angles between 20° and 70° with respect to the beam axis, and about 80% of 2π in azimuthal angle. Segmented cathodes and a delay-line read-out allow for a determination of both angles with a precision of δΘ≈0.7° in polar and δΦ≈1.5° in azimuthal angle, respectively. The system has been proven to be capable of handling instantaneous rates of up to 5×105detected ions per second per module. It neither exhibits the degradation of detection efficiency nor loss in resolution over a 500 h period of a 6 MeV/u238U+181Tameasurement at average luminosities of 8×1027cm−2s−1.
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- 1999
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268. On the two first excited K= 0 bands in 238U and 240Pu
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Hoogduin, J.M., Ditzel, E., Balanda, A., de Boer, F.W.N., Bokemeyer, H., Gerl, J., Heyde, K., van Klinken, J., Krasznahorkay, A., Salabura, P., and Wollersheim, H.J.
- Abstract
E0-enhanced spectra of conversion electrons taken after (α,α′) and (α,2n) reactions and after projectile Coulomb excitation improve our knowledge about first and second excited bands in 238U and 240Pu built on 02+and 03+states which lie anomalously close together. The two bands are of different structure.
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- 1996
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269. Doppler-corrected spectroscopy of conversion electrons with Mini-Oranges after heavy-ion collisions
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Ditzel, E., Hoogduin, J. M., Backe, H., Boer, F. W. N. De, Bokemeyer, H., Debowski, M., Klinken, J. Van, Salabura, P., Wollersheim, H. J., and Xie, H.
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- 1996
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270. Dilepton production in pp and CC collisions with HADES
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I. Fröhlich, G. Agakishiev, C. Agodi, A. Balanda, G. Bellia, D. Belver, A. Belyaev, A. Blanco, M. Böhmer, J. L. Boyard, P. Braun-Munzinger, P. Cabanelas, E. Castro, S. Chernenko, T. Christ, M. Destefanis, J. Díaz, F. Dohrmann, T. Eberl, L. Fabbietti, O. Fateev, P. Finocchiaro, P. J. R. Fonte, J. Friese, T. Galatyuk, J. A. Garzón, R. Gernhäuser, C. Gilardi, M. Golubeva, D. González-Díaz, E. Grosse, F. Guber, Ch. Hadjivasiliou, M. Heilmann, T. Hennino, R. Holzmann, A. Ierusalimov, I. Iori, A. Ivashkin, M. Jurkovic, B. Kämpfer, K. Kanaki, T. Karavicheva, D. Kirschner, I. Koenig, W. Koenig, B. W. Kolb, R. Kotte, A. Kozuch, F. Krizek, R. Krücken, A. Kugler, W. Kühn, A. Kurepin, J. Lamas-Valverde, S. Lang, S. Lange, L. Lopes, A. Mangiarotti, J. Marín, J. Markert, V. Metag, B. Michalska, D. Mishra, E. Moriniere, J. Mousa, C. Müntz, L. Naumann, R. Novotny, J. Otwinowski, Y. C. Pachmayer, M. Palka, V. Pechenov, O. Pechenova, T. Pérez Cavalcanti, J. Pietraszko, W. Przygoda, B. Ramstein, A. Reshetin, M. Roy-Stephan, A. Rustamov, A. Sadovsky, B. Sailer, P. Salabura, A. Schmah, R. Simon, S. Spataro, B. Spruck, H. Ströbele, J. Stroth, C. Sturm, M. Sudol, K. Teilab, P. Tlusty, M. Traxler, R. Trebacz, H. Tsertos, I. Veretenkin, V. Wagner, H. Wen, M. Wisniowski, T. Wojcik, J. Wüstenfeld, Y. Zanevsky, and P. Zumbruch
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010308 nuclear & particles physics ,0103 physical sciences ,010306 general physics ,01 natural sciences
271. Spin observables in hyperon production
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S. Heinz, L. Fava, Y. Bedfer, G.B. Pontecorvo, H.-W. Pfaff, F. Balestra, F. Brochard, L. Ferrero, J. Foryciarz, I.V. Falomkin, W. Kühn, A. Grasso, W. W. Jacobs, V. Frolov, Seonho Choi, D. Panzieri, M.P. Bussa, V.V. Ivanov, Gianfranco Zosi, G. Piragino, A. Maggiora, J.-Cl. Faivre, V. Chalyshev, S. E. Vigdor, P. Salabura, D. R. Gill, M. Maggiora, M. Debowski, J. Ritman, R. Garfagnini, R. Bertini, F. Tosello, I. Fröhlich, Mario Dzemidzic, A. Popov, L. C. Bland, and A. Manara
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Nuclear physics ,Physics ,Nuclear reaction ,Nuclear and High Energy Physics ,Electron transfer ,Particle physics ,Spectrometer ,Hyperon ,Observable ,Production (computer science) ,Beam (structure) ,Spin-½ - Abstract
4(DISTO Collaboration) * The first exclusive measurements of the spin transfer parameter DN N in the reaction fJp -t p[{+Ahas been performed at Saturne with the polarized beam and with the DISTO spectrometer. The results suggest an OBE mechanism dominated by kaon exchange.
272. Production of η′ and K- mesons in pp reactions at 2.85 GeV
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L. Fava, G. Piragino, V. V. Tvanov, T. Fröhlich, M. Maggiora, F. Brochard, L. Ferrero, Gianfranco Zosi, V. V. Frolov, P. Salabura, W. Kühn, A. Grasso, F. Tosello, A. Popov, J.-Cl. Faivre, A. Maggiora, J. Foryciarz, G.B. Pontecorvo, H.-W. Pfaff, M. Debowski, D. Panzieri, R. Garfagnini, D. R. Gill, F. Balestra, R. Bertini, S. Heinz, S. E. Vigdor, Seonho Choi, J. Ritman, V. Chalyshev, Mario Dzemidzic, L. C. Bland, A. Manara, I.V. Falomkin, W. W. Jacobs, Y. Bedfer, and M.P. Bussa
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Nuclear reaction ,Physics ,Nuclear physics ,Nuclear and High Energy Physics ,Particle physics ,Meson ,Hadron ,Elementary particle ,Boson
273. Measurement of gamma quantum interaction point in plastic scintillator with WLS strips
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Daria Kamińska, Bartosz Głowacz, N. Gupta-Sharma, N. Krawczyk, Paweł Moskal, Aleksander Gajos, Kamil Dulski, Zbigniew Rudy, Wojciech Krzemien, Lech Raczyński, Muhsin Mohammed, Grzegorz Korcyl, J. Wojnarska, Bożena Zgardzińska, Ewelina Kubicz, Eryk Czerwiński, Adam Strzelecki, Szymon Niedźwiecki, Paweł Kowalski, M. Kajetanowicz, Wojciech Wiślicki, Monika Pawlik-Niedźwiecka, Bożena Jasińska, Jerzy Smyrski, Marcin Zieliński, Marek Gorgol, Michał Silarski, Piotr Białas, P. Salabura, Anna Wieczorek, D. Alfs, and Tomasz Bednarski
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Nuclear and High Energy Physics ,Photomultiplier ,Photon ,positron emission tomography ,Physics - Instrumentation and Detectors ,Physics::Instrumentation and Detectors ,Physics::Medical Physics ,FOS: Physical sciences ,STRIPS ,Scintillator ,Wavelength shifter ,01 natural sciences ,plastic scintillator ,030218 nuclear medicine & medical imaging ,law.invention ,wavelength shifter ,03 medical and health sciences ,0302 clinical medicine ,Optics ,Silicon photomultiplier ,law ,0103 physical sciences ,Instrumentation ,Physics ,Scintillation ,Interaction point ,010308 nuclear & particles physics ,business.industry ,Instrumentation and Detectors (physics.ins-det) ,business ,silicon photomultipliers - Abstract
We demonstrated the feasibility of measuring the axial coordinate of a gamma quantum interaction point in a plastic scintillator bar via the detection of scintillation photons escaping from the scintillator with an array of wavelength-shifting (WLS) strips. Using a test set-up comprising a BC-420 scintillator bar and an~array of sixteen BC-482A WLS strips we achieved a spatial resolution of~5\,mm~($\sigma$) for annihilation photons from a $^{22}$Na isotope. The studied method can be used to improve the spatial resolution of a plastic-scintillator-based PET scanner which is being developed by the J-PET collaboration., Comment: 13 pages, 8 figures; Submitted to Nuclear Instruments and Methods in Physics Research Section A
274. Physics Performance Report for PANDA: Strong Interaction Studies with Antiprotons
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PANDA Collaboration, W. Erni, I. Keshelashvili, B. Krusche, M. Steinacher, Y. Heng, Z. Liu, H. Liu, X. Shen, O. Wang, H. Xu, J. Becker, F. Feldbauer, F. -H. Heinsius, T. Held, H. Koch, B. Kopf, M. Pelizaeus, T. Schroeder, M. Steinke, U. Wiedner, J. Zhong, A. Bianconi, M. Bragadireanu, D. Pantea, A. Tudorache, V. Tudorache, M. De Napoli, F. Giacoppo, G. Raciti, E. Rapisarda, C. Sfienti, E. Bialkowski, A. Budzanowski, B. Czech, M. Kistryn, S. Kliczewski, A. Kozela, P. Kulessa, K. Pysz, W. Schaefer, R. Siudak, A. Szczurek, W. Czy. Zycki, M. Domagala, M. Hawryluk, E. Lisowski, F. Lisowski, L. Wojnar, D. Gil, P. Hawranek, B. Kamys, St. Kistryn, K. Korcyl, W. Krzemien, A. Magiera, P. Moskal, Z. Rudy, P. Salabura, J. Smyrski, A. Wronska, M. Al-Turany, I. Augustin, H. Deppe, H. Flemming, J. Gerl, K. Goetzen, R. Hohler, D. Lehmann, B. Lewandowski, J. Luehning, F. Maas, D. Mishra, H. Orth, K. Peters, T. Saito, G. Schepers, C. J. Schmidt, L. Schmitt, C. Schwarz, B. Voss, P. Wieczorek, A. Wilms, K. -T. Brinkmann, H. Freiesleben, R. Jaekel, R. Kliemt, T. Wuerschig, H. -G. Zaunick, V. M. Abazov, G. Alexeev, A. Arefiev, V. I. Astakhov, M. Yu. Barabanov, B. V. Batyunya, Yu. I. Davydov, V. Kh. Dodokhov, A. A. Efremov, A. G. Fedunov, A. A. Feshchenko, A. S. Galoyan, S. Grigoryan, A. Karmokov, E. K. Koshurnikov, V. Ch. Kudaev, V. I. Lobanov, Yu. Yu. Lobanov, A. F. Makarov, L. V. Malinina, V. L. Malyshev, G. A. Mustafaev, A. Olshevski, M. A. . Pasyuk, E. A. Perevalova, A. A. Piskun, T. A. Pocheptsov, G. Pontecorvo, V. K. Rodionov, Yu. N. Rogov, R. A. Salmin, A. G. Samartsev, M. G. Sapozhnikov, A. Shabratova, G. S. Shabratova, A. N. Skachkova, N. B. Skachkov, E. A. Strokovsky, M. K. Suleimanov, R. Sh. Teshev, V. V. Tokmenin, V. V. Uzhinsky, A. S. Vodopianov, S. A. Zaporozhets, N. I. Zhuravlev, A. G. Zorin, D. Branford, K. Foehl, D. Glazier, D. Watts, P. Woods, W. Eyrich, A. Lehmann, A. Teufel, S. Dobbs, Z. Metreveli, K. Seth, B. Tann, A. Tomaradze, D. Bettoni, V. Carassiti, A. Cecchi, P. Dalpiaz, E. Fioravanti, I. Garzia, M. Negrini, M. Savri`E, G. Stancari, B. Dulach, P. Gianotti, C. Guaraldo, V. Lucherini, E. Pace, A. Bersani, M. Macri, M. Marinelli, R. F. Parodi, I. Brodski, W. Doering, P. Drexler, M. Dueren, Z. Gagyi-Palffy, A. Hayrapetyan, M. Kotulla, W. Kuehn, S. Lange, M. Liu, V. Metag, M. Nanova, R. Novotny, C. Salz, J. Schneider, P. Schoenmeier, R. Schubert, S. Spataro, H. Stenzel, C. Strackbein, M. Thiel, U. Thoering, S. Yang, T. Clarkson, E. Cowie, E. Downie, G. Hill, M. Hoek, D. Ireland, R. Kaiser, T. Keri, I. Lehmann, K. Livingston, S. Lumsden, D. MacGregor, B. McKinnon, M. Murray, D. Protopopescu, G. Rosner, B. Seitz, G. Yang, M. Babai, A. K. Biegun, A. Bubak, E. Guliyev, V. S. Jothi, M. Kavatsyuk, H. Loehner, J. Messchendorp, H. Smit, J. C. Van Der Weele, F. Garcia, D. -O. Riska, M. Buescher, R. Dosdall, R. Dzhygadlo, A. Gillitzer, D. Grunwald, V. Jha, G. Kemmerling, H. Kleines, A. Lehrach, R. Maier, M. Mertens, H. Ohm, D. Prasuhn, T. Randriamalala, J. Ritman, M. Roeder, T. Stockmanns, P. Wintz, P. Wuestner, J. Kisiel, S. Li, Z. Li, Z. Sun, S. Fissum, K. Hansen, L. Isaksson, M. Lundin, B. Schroeder, P. Achenbach, M. C. Mora Espi, J. Pochodzalla, S. Sanchez, A. Sanchez-Lorente, V. I. Dormenev, A. A. Fedorov, M. V. Korzhik, O. V. Missevitch, V. Balanutsa, V. Chernetsky, A. Demekhin, A. Dolgolenko, P. Fedorets, A. Gerasimov, V. Goryachev, A. Boukharov, O. Malyshev, I. Marishev, A. Semenov, C. Hoeppner, B. Ketzer, I. Konorov, A. Mann, S. Neubert, S. Paul, Q. Weitzel, A. Khoukaz, T. Rausmann, A. Taeschner, J. Wessels, R. Varma, E. Baldin, K. Kotov, S. Peleganchuk, Yu. Tikhonov, J. Boucher, T. Hennino, R. Kunne, S. Ong, J. Pouthas, B. Ramstein, P. Rosier, M. Sudol, J. Van De Wiele, T. Zerguerras, K. Dmowski, R. Korzeniewski, D. Przemyslaw, B. Slowinski, G. Boca, A. Braghieri, S. Costanza, A. Fontana, P. Genova, L. Lavezzi, P. Montagna, A. Rotondi, N. I. Belikov, A. M. Davidenko, A. A. Derevschikov, Y. M. Goncharenko, V. N. Grishin, V. A. Kachanov, D. A. Konstantinov, V. A. Kormilitsin, V. I. Kravtsov, Y. A. Matulenko, Y. M. Melnik, A. P. Meschanin, N. G. Minaev, V. V. Mochalov, D. A. Morozov, L. V. Nogach, S. B. Nurushev, A. V. Ryazantsev, P. A. Semenov, L. F. Soloviev, A. V. Uzunian, A. N. Vasiliev, A. E. Yakutin, T. Baeck, B. Cederwall, C. Bargholtz, L. Geren, P. E. Tegner, S. Belostotski, G. Gavrilov, A. Itzotov, A. Kisselev, P. Kravchenko, S. Manaenkov, O. Miklukho, Y. Naryshkin, D. Veretennikov, V. Vikhrov, A. Zhadanov, L. Fava, D. Panzieri, D. Alberto, A. Amoroso, E. Botta, T. Bressani, S. Bufalino, M. P. Bussa, L. Busso, F. De Mori, M. Destefanis, L. Ferrero, A. Grasso, M. Greco, T. Kugathasan, M. Maggiora, S. Marcello, G. Serbanut, S. Sosio, R. Bertini, D. Calvo, S. Coli, P. De Remigis, A. Feliciello, A. Filippi, G. Giraudo, G. Mazza, A. Rivetti, K. Szymanska, F. Tosello, R. Wheadon, O. Morra, M. Agnello, F. Iazzi, R. Birsa, F. Bradamante, A. Bressan, A. Martin, H. Clement, C. Ekstroem, H. Calen, S. Grape, B. Hoeistad, T. Johansson, A. Kupsc, P. Marciniewski, E. Thome, J. Zlomanczuk, J. Diaz, A. Ortiz, S. Borsuk, A. Chlopik, Z. Guzik, J. Kopec, T. Kozlowski, D. Melnychuk, M. Plominski, J. Szewinski, K. Traczyk, B. Zwieglinski, P. Buehler, A. Gruber, P. Kienle, J. Marton, E. Widmann, J. Zmeskal, M. F. M. Lutz, B. Pire, O. Scholten, and R. Timmermans
- Subjects
Physics::Instrumentation and Detectors ,Nuclear Theory ,High Energy Physics::Experiment ,Nuclear Experiment ,7. Clean energy - Abstract
To study fundamental questions of hadron and nuclear physics in interactions of antiprotons with nucleons and nuclei, the universal PANDA detector will be built. Gluonic excitations, the physics of strange and charm quarks and nucleon structure studies will be performed with unprecedented accuracy thereby allowing high-precision tests of the strong interaction. The proposed PANDA detector is a state-of-the art internal target detector at the HESR at FAIR allowing the detection and identification of neutral and charged particles generated within the relevant angular and energy range. This report presents a summary of the physics accessible at PANDA and what performance can be expected.
275. HADES — A High Acceptance DiElectron Spectrometer
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SALABURA, P
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- 1995
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276. Directed, Elliptic, and Higher Order Flow Harmonics of Protons, Deuterons, and Tritons in Au+Au Collisions at sqrt[s_{NN}]=2.4 GeV.
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Adamczewski-Musch J, Arnold O, Behnke C, Belounnas A, Belyaev A, Berger-Chen JC, Blanco A, Blume C, Böhmer M, Bordalo P, Chernenko S, Chlad L, Ciepal I, Deveaux C, Dreyer J, Epple E, Fabbietti L, Fateev O, Filip P, Fonte P, Franco C, Friese J, Fröhlich I, Galatyuk T, Garzón JA, Gernhäuser R, Golosov O, Golubeva M, Greifenhagen R, Guber F, Gumberidze M, Harabasz S, Heinz T, Hennino T, Hlavac S, Höhne C, Holzmann R, Ierusalimov A, Ivashkin A, Kämpfer B, Karavicheva T, Kardan B, Koenig I, Koenig W, Kohls M, Kolb BW, Korcyl G, Kornakov G, Kornas F, Kotte R, Kugler A, Kunz T, Kurepin A, Kurilkin A, Kurilkin P, Ladygin V, Lalik R, Lapidus K, Lebedev A, Lopes L, Lorenz M, Mahmoud T, Maier L, Malige A, Mamaev M, Mangiarotti A, Markert J, Matulewicz T, Maurus S, Metag V, Michel J, Mihaylov DM, Morozov S, Müntz C, Münzer R, Naumann L, Nowakowski K, Parpottas Y, Pechenov V, Pechenova O, Petukhov O, Piasecki K, Pietraszko J, Przygoda W, Pysz K, Ramos S, Ramstein B, Rathod N, Reshetin A, Rodriguez-Ramos P, Rosier P, Rost A, Rustamov A, Sadovsky A, Salabura P, Scheib T, Schuldes H, Schwab E, Scozzi F, Seck F, Sellheim P, Selyuzhenkov I, Siebenson J, Silva L, Singh U, Smyrski J, Sobolev YG, Spataro S, Spies S, Ströbele H, Stroth J, Sturm C, Svoboda O, Szala M, Tlusty P, Traxler M, Tsertos H, Usenko E, Wagner V, Wendisch C, Wiebusch MG, Wirth J, Wójcik D, Zanevsky Y, and Zumbruch P
- Abstract
Flow coefficients v_{n} of the orders n=1-6 are measured with the High-Acceptance DiElectron Spectrometer (HADES) at GSI for protons, deuterons, and tritons as a function of centrality, transverse momentum, and rapidity in Au+Au collisions at sqrt[s_{NN}]=2.4 GeV. Combining the information from the flow coefficients of all orders allows us to construct for the first time, at collision energies of a few GeV, a multidifferential picture of the angular emission pattern of these particles. It reflects the complicated interplay between the effect of the central fireball pressure on the emission of particles and their subsequent interaction with spectator matter. The high precision information on higher order flow coefficients is a major step forward in constraining the equation of state of dense baryonic matter.
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- 2020
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277. Strong Absorption of Hadrons with Hidden and Open Strangeness in Nuclear Matter.
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Adamczewski-Musch J, Arnold O, Atomssa ET, Behnke C, Belounnas A, Belyaev A, Berger-Chen JC, Biernat J, Blanco A, Blume C, Böhmer M, Chernenko S, Chlad L, Chudoba P, Ciepał I, Deveaux C, Dittert D, Dreyer J, Epple E, Fabbietti L, Fateev O, Fonte P, Franco C, Friese J, Fröhlich I, Galatyuk T, Garzón JA, Gernhäuser R, Golubeva M, Greifenhagen R, Guber F, Gumberidze M, Harabasz S, Heinz T, Hennino T, Höhne C, Holzmann R, Ierusalimov A, Ivashkin A, Kämpfer B, Kardan B, Koenig I, Koenig W, Kolb BW, Korcyl G, Kornakov G, Kornas F, Kotte R, Kuboś J, Kugler A, Kunz T, Kurepin A, Kurilkin A, Kurilkin P, Ladygin V, Lalik R, Lapidus K, Lebedev A, Linev S, Lopes L, Lorenz M, Mahmoud T, Maier L, Malige A, Markert J, Maurus S, Metag V, Michel J, Mihaylov DM, Mikhaylov V, Morozov S, Müntz C, Münzer R, Naumann L, Nowakowski K, Parpottas Y, Pechenov V, Pechenova O, Petukhov O, Pietraszko J, Prozorov AP, Przygoda W, Ramstein B, Rathod N, Reshetin A, Rodriguez-Ramos P, Rost A, Sadovsky A, Salabura P, Scheib T, Schmidt-Sommerfeld K, Schuldes H, Schwab E, Scozzi F, Seck F, Sellheim P, Siebenson J, Silva L, Smyrski J, Spataro S, Spies S, Ströbele H, Stroth J, Strzempek P, Sturm C, Svoboda O, Szala M, Tlusty P, Traxler M, Tsertos H, Ungethüm C, Vázquez Doce O, Wagner V, Wendisch C, Wiebusch MG, Wirth J, Wójcik D, Zanevsky Y, Zumbruch P, Curceanu C, Piscicchia K, and Scordo A
- Abstract
We present the first observation of K^{-} and ϕ absorption within nuclear matter by means of π^{-}-induced reactions on C and W targets at an incident beam momentum of 1.7 GeV/c studied with HADES at SIS18/GSI. The double ratio (K^{-}/K^{+})_{W}/(K^{-}/K^{+})_{C} is found to be 0.319±0.009(stat)_{-0.012}^{+0.014}(syst) indicating a larger absorption of K^{-} in heavier targets as compared to lighter ones. The measured ϕ/K^{-} ratios in π^{-}+C and π^{-}+W reactions within the HADES acceptance are found to be equal to 0.55±0.04(stat)_{-0.07}^{+0.06}(syst) and to 0.63±0.06(stat)_{-0.11}^{+0.11}(syst), respectively. The similar ratios measured in the two different reactions demonstrate for the first time experimentally that the dynamics of the ϕ meson in nuclear medium is strongly coupled to the K^{-} dynamics. The large difference in the ϕ production off C and W nuclei is discussed in terms of a strong ϕN in-medium coupling. These results are relevant for the description of heavy-ion collisions and the structure of neutron stars.
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- 2019
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278. Dielectron production in 12C+12C collisions at 2A GeV with the HADES spectrometer.
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Agakichiev G, Agodi C, Alvarez-Pol H, Bałanda A, Bertini D, Bielcik J, Bellia G, Böhmer M, Bokemeyer H, Boyard JL, Braun-Munzinger P, Cabanelas P, Chernenko S, Christ T, Coniglione R, Cosentino L, Díaz J, Dohrmann F, Durán I, Eberl T, Enghardt W, Fabbietti L, Fateev O, Fernandez C, Finocchiaro P, Friese J, Fröhlich I, Fuentes B, Garabatos C, Garzón JA, Gernhäuser R, Gilardi C, Golubeva M, González-Díaz D, Grosse E, Guber F, Hennino T, Hlavac S, Holzmann R, Homolka J, Ierusalimov A, Iori I, Ivashkin A, Jaskuła M, Jurkovic M, Kagarlis M, Kajetanowicz M, Kämpfer B, Kanaki K, Karavicheva T, Kastenmüller A, Kidoń L, Kienle P, Koenig I, Koenig W, Körner HJ, Kolb BW, Kotte R, Krücken R, Kugler A, Kühn W, Kulessa R, Kurepin A, Lang S, Lange S, Lehnert J, Lins E, Magestro D, Maiolino C, Malarz A, Markert J, Metag V, Mousa J, Münch M, Müntz C, Naumann L, Nekhaev A, Novotny J, Otwinowski J, Pachmayer YC, Pechenov V, Pérez T, Piattelli P, Pietraszko J, Pleskac R, Płoskoń M, Pospísil V, Prokopowicz W, Przygoda W, Ramstein B, Reshetin A, Ritman J, Roy-Stephan M, Rustamov A, Sadovsky A, Sailer B, Salabura P, Sánchez M, Sapienza P, Schmah A, Schön H, Schön W, Schröder C, Schwab E, Simon RS, Smolyankin V, Smykov L, Spataro S, Spruck B, Ströbele H, Stroth J, Sturm C, Sudoł M, Suk M, Taranenko A, Tlusty P, Toia A, Traxler M, Tsertos H, Vassiliev D, Vázquez A, Wagner V, Waluś W, Wiśniowski M, Wójcik T, Wüstenfeld J, Zanevsky Y, Zeitelhack K, Zovinec D, and Zumbruch P
- Abstract
The invariant-mass spectrum of e+e- pairs produced in 12C+12C collisions at an incident energy of 2 GeV per nucleon has been measured for the first time. The measured pair production probabilities span over 5 orders of magnitude from the pi(0)-Dalitz to the rho/omega invariant-mass region. Dalitz decays of pi(0) and eta account for all the yield up to 0.15 GeV/c(2), but for only about 50% above this mass. A comparison with model calculations shows that the excess pair yield is likely due to baryon-resonance and vector-meson decays. Transport calculations based on vacuum spectral functions fail, however, to describe the entire mass region.
- Published
- 2007
- Full Text
- View/download PDF
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