Academic literature on the topic 'Antilambda'

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Journal articles on the topic "Antilambda"

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Ko, C. M., M. Asakawa, and P. Lévai. "Antilambda enhancement in ultrarelativistic heavy ion collisions." Physical Review C 46, no. 3 (1992): 1072–76. http://dx.doi.org/10.1103/physrevc.46.1072.

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Cugnon, J., and J. Vandermeulen. "Antiproton and antilambda annihilations on several nucleons." Physical Review C 39, no. 1 (1989): 181–91. http://dx.doi.org/10.1103/physrevc.39.181.

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Alberg, M. A., E. M. Henley, L. Wilets, and P. D. Kunz. "A quark model of antilambda-lambda production in p̄p interactions." Nuclear Physics A 560, no. 1 (1993): 365–88. http://dx.doi.org/10.1016/0375-9474(93)90102-4.

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GREINER, WALTER, and THOMAS J. BÜRVENICH. "VACUUM: MATTER AND ANTIMATTER." International Journal of Modern Physics D 13, no. 07 (2004): 1531–38. http://dx.doi.org/10.1142/s0218271804005778.

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In this manuscript we first present the vacuum for the e+-e- field of QED and show how it is modified for baryons in nuclear environment. Then we discuss the possibility of producing new types of nuclear systems by implanting an antibaryon into ordinary nuclei. The structure of nuclei containing one antiproton or antilambda is investigated within the framework of a relativistic mean-field model. Self-consistent calculations predict an enhanced binding and considerable compression in such systems as compared with normal nuclei. We present arguments that the life time of such nuclei with respect to the antibaryon annihilation might be long enough for their observation.
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KILIAN, K., D. GRZONKA, D. MÖHL, and W. OELERT. "WAYS TO MAKE POLARIZED ANTIPROTON BEAMS." International Journal of Modern Physics A 26, no. 03n04 (2011): 757–59. http://dx.doi.org/10.1142/s0217751x1105275x.

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For making polarized antiproton beams the so called filter method is normally discussed. It is based on the depletion of one spin component due to the spin dependent interaction if a stored beam passes a polarized target. The method has been proven by the FILTEX collaboration and detailed studies are presently performed by the PAX collaboration. Another source for polarized antiprotons is the antilambda decay as it was used in the only experiment with polarized antiprotons so far at FERMILAB. Furthermore the antiproton production process itself if showing polarisation, would be by far the best way to get polarized [Formula: see text]. It can be assumed to result from a quasi-free proton-nucleon collison. Up to now it has never been investigated in detail. In such a hadronic interaction the antiprotons may have substantial polarisation which would simplify the preparation of a polarized antiproton beam drastically. It is proposed to measure the polarisation of antiprotons produced in a fixed target experiment.
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Samanta, Chhanda. "Superheavy Nuclei to Hypernuclei: A Tribute to Walter Greiner." EPJ Web of Conferences 182 (2018): 02107. http://dx.doi.org/10.1051/epjconf/201818202107.

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In nuclear physics, superheavy and hypernuclei are two of the most important fields of research. The prediction of islands of superheavy elements (Z = 114, N = 184, 196 and Z = 164, N = 318) in late sixties by the Frankfurt school played a key role in extending the periodic table of elements up to atomic number 118. Similarly, the demonstration that nuclear matter can be compressed 510 times of its original volume by nuclear shock waves, produced during heavy ion collision, led to the production of singleand double-lambda hypernuclei, as well as anti-matter nuclei. Recent observation of antihypertriton—comprising an antiproton, an antineutron, and an antilambda hyperon, by the STAR collaboration has now made it possible to envision a 3-dimensional nuclear chart of hypernuclei. My own interest in superheavy and hypernuclei was shaped from my first meeting with Walter Greiner at the International Conference on Atomic and Nuclear clusters held at Santorini, Greece in 1993. I will present a brief summary of these exciting developments, including some of our own work. Professor Greiner’s vision, enthusiasm, and encouragement touched many lives and I was one of those privileged ones.
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Tawfik, Abdel Nasser, Hayam Yassin, and Eman R. Abo Elyazeed. "Strangeness production in high-energy collisions and Hawking–Unruh radiation." International Journal of Modern Physics E 26, no. 03 (2017): 1750001. http://dx.doi.org/10.1142/s021830131750001x.

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The assumption that the production of quark–antiquark pairs and their sequential string-breaking takes place, likely as a tunneling process, through the event horizon of the color confinement determines the freezeout temperature and gives a plausible interpretation for the thermal pattern of elementary and nucleus–nucleus collisions. When relating the black-hole electric charges to the baryon-chemical potentials, it was found that the phenomenologically deduced parameters from the ratios of various particle species and the higher-order moments of net-proton multiplicity in the statistical thermal models and Polyakov linear-sigma model agree well with the ones determined from the thermal radiation from charged black hole. Accordingly, the resulting freezeout conditions, such as normalized entropy density [Formula: see text] and average energy per particle [Formula: see text][Formula: see text]GeV, are confirmed at finite chemical potentials as well. Furthermore, the problem of strangeness production in elementary collisions can be interpreted by thermal particle production from the Hawking–Unruh radiation. Consequently, the freezeout temperature depends on the quark masses. This leads to a deviation from full equilibrium and thus a suppression of the strangeness production in the elementary collisions. But in nucleus–nucleus collisions, an average temperature should be introduced in order to dilute the quark masses. This nearly removes the strangeness suppression. An extension to finite chemical potentials is introduced. The particle ratios of kaon-to-pion ([Formula: see text]), phi-to-kaon ([Formula: see text]) and antilambda-to-pion ([Formula: see text]) are determined from Hawking–Unruh radiation and compared with the thermal calculations and the measurements in different experiments. We conclude that these particle ratios can be reproduced, at least qualitatively, as Hawking–Unruh radiation at finite chemical potential. With increasing energy, both [Formula: see text] and [Formula: see text] keep their maximum values at low SPS energies. But the further energy decrease rapidly reduces both ratios. For [Formula: see text], there is an increase with increasing [Formula: see text], i.e., no saturation is to be observed.
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Pochodzalla, Josef, and Stephan Pomp. "EXPLORING THE POTENTIAL OF ANTILAMBDAS IN NUCLEI WITH ANTIPROTONS." International Journal of Modern Physics E 19, no. 12 (2010): 2650–55. http://dx.doi.org/10.1142/s0218301310017228.

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A schematic Monte Carlo simulation is used to examine the potential of exclusive hyperon-antihyperon pair production close to threshold in antiproton nucleus interactions to extract information on the interaction of antihyperons in nuclei. It is demonstrated that for [Formula: see text] pairs produced at antiproton momenta of 1.66 GeV/c the asymmetry is sufficiently sensitive even if the density as well as the momentum dependencies of the potentials are considered. Data taken earlier by the PS185 Collaboration prove that these measurements are feasible.
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Back, B. B., R. R. Betts, J. Chang, et al. "Antilambda Production inAu+AuCollisions at11.7AGeV/c." Physical Review Letters 87, no. 24 (2001). http://dx.doi.org/10.1103/physrevlett.87.242301.

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Dissertations / Theses on the topic "Antilambda"

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Pleier, Marc-André. "Measurement of inclusive lambda, antilambda hyperon polarisation in proton nucleus collisions at 920 GeV proton beam energy." [S.l. : s.n.], 2002. http://www.bsz-bw.de/cgi-bin/xvms.cgi?SWB10047837.

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Salzwedel, Jai. "Lambda femtoscopy in √sNN = 2.76 TeV Pb-Pb collisions at ALICE." The Ohio State University, 2017. http://rave.ohiolink.edu/etdc/view?acc_num=osu1483568167792529.

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Hombach, Christoph. "Search for the rare baryonic B+ to proton anti-Lambda decay with the LHCb detector and alignment of pixel detectors." Thesis, University of Manchester, 2016. https://www.research.manchester.ac.uk/portal/en/theses/search-for-the-rare-baryonic-b-to-proton-antilambda-decay-with-the-lhcb-detector-and-alignment-of-pixel-detectors(c639221e-5c61-48ba-afd0-54b50455cf44).html.

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Mischke, André [Verfasser]. "Λ- [Lambda-] und Λ ̄-Produktion [Antilambda-Produktion] in zentralen Blei-Blei-Kollisionen bei 40, 80 und 158 GeV pro Nukleon / von André Mischke". 2005. http://d-nb.info/976007517/34.

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Pleier, Marc-André [Verfasser]. "Measurement of inclusive Λ/Λ ̄ [Lambda-Antilambda] hyperon polarisation in proton nucleus collisions at 920 GeV proton beam energy / presented by Marc-André Pleier". 2002. http://d-nb.info/96483927X/34.

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Books on the topic "Antilambda"

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Schuchmann, Simone. Modification of K0s and Lambda(AntiLambda) Transverse Momentum Spectra in Pb-Pb Collisions at √sNN = 2.76 TeV with ALICE. Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-43458-2.

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Book chapters on the topic "Antilambda"

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Schuchmann, Simone. "Introduction." In Modification of K0s and Lambda(AntiLambda) Transverse Momentum Spectra in Pb-Pb Collisions at √sNN = 2.76 TeV with ALICE. Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-43458-2_1.

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Schuchmann, Simone. "Problem Statement: Modification of $${p}_\mathrm{T}$$ p T Spectra in AA Collisions." In Modification of K0s and Lambda(AntiLambda) Transverse Momentum Spectra in Pb-Pb Collisions at √sNN = 2.76 TeV with ALICE. Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-43458-2_2.

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Schuchmann, Simone. "The ALICExperiment." In Modification of K0s and Lambda(AntiLambda) Transverse Momentum Spectra in Pb-Pb Collisions at √sNN = 2.76 TeV with ALICE. Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-43458-2_3.

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Schuchmann, Simone. "Analysis: Reconstruction of $$\mathrm{K}^\mathrm{0}_\mathrm{s}$$ and $$\Lambda (\overline{\Lambda })$$ Transverse Momentum Spectra." In Modification of K0s and Lambda(AntiLambda) Transverse Momentum Spectra in Pb-Pb Collisions at √sNN = 2.76 TeV with ALICE. Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-43458-2_4.

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Schuchmann, Simone. "Results." In Modification of K0s and Lambda(AntiLambda) Transverse Momentum Spectra in Pb-Pb Collisions at √sNN = 2.76 TeV with ALICE. Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-43458-2_5.

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Schuchmann, Simone. "Discussion." In Modification of K0s and Lambda(AntiLambda) Transverse Momentum Spectra in Pb-Pb Collisions at √sNN = 2.76 TeV with ALICE. Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-43458-2_6.

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Conference papers on the topic "Antilambda"

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Yokosawa, A. "Polarization of antiprotons by antilambda decay." In AIP Conference Proceedings Volume 145. AIP, 1986. http://dx.doi.org/10.1063/1.35684.

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Hertzog, David W., P. D. Barnes, P. Birien, et al. "Lambda-antilambda decay asymmetries and CP violation." In HIGH−ENERGY SPIN PHYSICS/EIGHTH INTERNATIONAL SYMPOSIUM. AIP, 1989. http://dx.doi.org/10.1063/1.38251.

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Pochodzalla, Josef, and Stephan Pomp. "EXPLORING THE POTENTIAL OF ANTILAMBDAS IN NUCLEI WITH ANTIPROTONS." In Proceedings of the Sendai International Symposium. WORLD SCIENTIFIC, 2009. http://dx.doi.org/10.1142/9789814277860_0049.

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