Bibliografías temáticas / Deep inelastic collisions

Literatura académica sobre el tema "Deep inelastic collisions"

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Publicado: 4 de junio de 2021
Última modificación: 29 de julio de 2024

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Artículos de revistas sobre el tema "Deep inelastic collisions"

1

Pappalardo, G. "Reaction times in deep inelastic collisions". Nuclear Physics A 488 (octubre de 1988): 395–408. http://dx.doi.org/10.1016/0375-9474(88)90277-1.

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Martinez, F. Guzman y R. Reif. "Incomplete deep-inelastic heavy-ion collisions". Nuclear Physics A 436, n.º 2 (abril de 1985): 294–310. http://dx.doi.org/10.1016/0375-9474(85)90200-3.

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Aguiar, C. E., V. C. Barbosa, L. F. Canto y R. Donangelo. "Fusion, deep-inelastic collisions, and neck formation". Physical Review C 38, n.º 1 (1 de julio de 1988): 541–42. http://dx.doi.org/10.1103/physrevc.38.541.

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Shen, W. Q., W. M. Qiao, W. L. Zhan, L. X. Ge, X. T. Zhu, S. Wenqing, G. Linxiao et al. "Analysis of deep inelastic collisions between16O and27Al". Zeitschrift f�r Physik A Atomic Nuclei 328, n.º 2 (junio de 1987): 219–26. http://dx.doi.org/10.1007/bf01290664.

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SKWIRA-CHALOT, I., K. SIWEK-WILCZYŃSKA y J. WILCZYŃSKI. "IMPACT-PARAMETER DEPENDENCE OF TERNARY AND QUATERNARY RESEPARATION OF HEAVY COLLIDING SYSTEMS". International Journal of Modern Physics E 19, n.º 04 (abril de 2010): 713–17. http://dx.doi.org/10.1142/s021830131001514x.

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Recently, we reported on the observation of a new reaction mechanism of fast collinear breakup of the 197 Au + 197 Au system into three and four fragments of comparable size. Here we present results of an additional analysis that shows that these ternary and quaternary breakup reactions occur at extremely deep-inelastic collisions corresponding to small values of the impact parameter, while more peripheral collisions lead to well known binary deep-inelastic reactions.
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SHVEDOV, L., J. BŁOCKI y J. WILCZYŃSKI. "TESTS OF THE DYNAMICS OF DEEP INELASTIC COLLISIONS". International Journal of Modern Physics E 14, n.º 03 (abril de 2005): 321–25. http://dx.doi.org/10.1142/s0218301305003065.

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A macroscopic dynamical model of deep-inelastic nucleus-nucleus collisions is presented. We solve Rayleigh-Lagrange equations of motion assuming the mechanism of one-body dissipation. Sensitivity of the model to the assumed strength of the dissipative Rayleigh force (relative to the one-body dissipation) is discussed.
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7

JENKOVSZKY, L. L., ANDREA NAGY, S. M. TROSHIN, JOLÁN TURÓCI y N. E. TYURIN. "CRITICAL PHENOMENA IN DEEP INELASTIC SCATTERING". International Journal of Modern Physics A 25, n.º 31 (20 de diciembre de 2010): 5667–82. http://dx.doi.org/10.1142/s0217751x10051104.

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Saturation in deep inelastic scattering and deeply virtual Compton scattering is associated with a phase transition between the partonic gas, typical of moderate x and Q2, and partonic fluid appearing at increasing Q2 and decreasing Bjorken x. In this paper we do not intend to propose another parametrization of the structure function; instead we suggest a new insight into the internal structure of the nucleon, as seen in deep inelastic scattering, and its connection with that revealed in high-energy nucleons and heavy-ion collisions.
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8

Krishan, K., S. K. Samaddar y J. N. De. "Spin dispersion and alignment in deep inelastic collisions". Journal of Physics G: Nuclear Physics 14, n.º 11 (noviembre de 1988): 1423–30. http://dx.doi.org/10.1088/0305-4616/14/11/013.

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Kanayama, N. "Effect of Mass Transfer in Deep Inelastic Collisions". Progress of Theoretical Physics 85, n.º 2 (1 de febrero de 1991): 335–42. http://dx.doi.org/10.1143/ptp/85.2.335.

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Adamian,1,2, G. G., R. V. Jolos,1, A. K. Nasirov,1,2 y A. I. Muminov2. "Friction coefficient for deep-inelastic heavy-ion collisions". Physical Review C 56, n.º 1 (julio de 1997): 373–80. http://dx.doi.org/10.1103/physrevc.56.373.

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Tesis sobre el tema "Deep inelastic collisions"

1

Gilmore, Jason R. "Search for contact interactions in deep inelastic scattering". Connect to this title online, 2002. http://rave.ohiolink.edu/etdc/view?acc%5Fnum=osu983824358.

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Thesis (Ph. D.)--Ohio State University, 2002.
Title from first page of PDF file. Document formatted into pages; contains xx, 143 p.; also contains graphics. Includes abstract and vita. Advisor: L. Stanley Durkin, Dept. of Physics. Includes bibliographical references (p. 137-143).
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2

Signal, Anthony Ian. "Deep inelastic scattering and bag model". Title page, abstract and contents only, 1988. http://web4.library.adelaide.edu.au/theses/09PH/09phs578.pdf.

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Valiente-Dobon, Jose Javier. "Studies of neutron-rich nuclei using deep inelastic collisions". Thesis, University of Surrey, 2003. http://epubs.surrey.ac.uk/843390/.

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A deep inelastic reaction between a thin self-supporting 19878Pt target and an 850MeV 13654Xe beam has been used to populate and study both neutron-rich nuclei around the beam and target masses and the reaction mechanism. An Ipi= 10+ isomeric state has been found in the N = 80 isotone 13656Ba with a measured half-life of 91 +/- 2ns. The structure of the predominantly (h11/2)-210+ isomer is discussed in terms of shell model and pair-truncated shell model calculations and compared to the even-Z, N = 80 isotones ranging from 13050Sn to 14868Er. A qualitative explanation of the observed dramatic decrease in the B(E2 : 10+ → 8+) value for the N = 80 isotones at 136Ba is given in terms of the increasing single-particle energy of the h11/2 neutron configuration as the proton sub-shell is filled. A 4-quasiparticle isomer has been observed in with a half-life of 188 +/- 38ns. The results are compared with blocked BCS Nilsson calculations which favour the Kpi= 15- interpretation. This isomer completes the even-A tungsten, 4-quasiparticle isomer systematics from A = 176 to 186. A high spin isomeric state has been found in the near spherical nucleus 19874W with a half-life of 36 +/- 2ns. The nature of this isomer has been interpreted from an examination of the systematics of platinum isotopes and neighbouring nuclei as a tentative Ipi= 12+ state from rotation-aligned, two neutron (i13/2)2configuration. Using prompt-delayed gamma-ray correlations, the complementary fragments of the reaction have been studied and used to identify new states in 19476Os. The angular momentum transfer to the binary fragments in the reaction has been investigated in terms of the average total gamma-ray fold versus the scattering angle of the recoils.
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Wilson, Emma. "Gamma spectroscopy of 207Tl126 populated in deep-inelastic collisions". Thesis, University of Surrey, 2015. http://epubs.surrey.ac.uk/807041/.

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Dunne, Gerald V. "Deep inelastic scattering and the EMC effect /". Title page, contents and introduction only, 1986. http://web4.library.adelaide.edu.au/theses/09SM/09smd923.pdf.

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Schilling, Frank-Peter. "Diffractive jet production in deep inelastic e+p collisions at HERA". [S.l. : s.n.], 2001. http://deposit.ddb.de/cgi-bin/dokserv?idn=961853298.

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Kant, David. "A study of the fragmentation of quarks in e-p collisions at HERA". Thesis, Queen Mary, University of London, 1996. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.338959.

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Campbell-Robson, Stephen. "A study of charm production in deep inelastic scattering in e'+p collisions". Thesis, University of Bristol, 1997. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.388016.

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Bass, Steven David. "Spin dependent effects in quantum chromodynamics /". Title page, contents and abstract only, 1992. http://web4.library.adelaide.edu.au/theses/09PH/09phb317.pdf.

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Thesis (Ph. D.)--University of Adelaide, Dept. of Physics and Mathematical Physics, 1993.
Copies of three of the author's previously published articles inserted as appendix B. Includes bibliographical references.
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10

Keksis, August Lawrence. "N/z equilibration in deep inelastic collisions and the fragmentation of the resulting quasiprojectiles". Texas A&M University, 2003. http://hdl.handle.net/1969.1/5886.

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When target and projectile nuclei have a difference in neutron to proton ratio (N/Z), the quasiprojectiles formed in a deep inelastic collision (DIC) should have a mean N/Z between the N/Z of the target and the N/Z of the projectile, depending on the amount of N/Z equilibration that occurred. Data from six reaction systems at two beam energies (32 and 45 MeV/nucleon) were collected. The systems in order of increasing difference between target and projectile N/Z (shown in parentheses) are 40Ar + 112Sn (∆N/Z = 0.018), 48Ca + 124Sn (∆N/Z = 0.080), 48Ca + 112Sn (∆N/Z = 0.160), 40Ca + 112Sn (∆N/Z = 0.240), 40Ar + 124Sn (∆N/Z = 0.258) and 40Ca + 124Sn (∆N/Z = 0.480). The quasiprojectile N/Z was determined by two techniques. The first technique used the isotopically resolved fragments to reconstruct the quasiprojectile N/Z. The second technique, developed in this thesis, used fragment yield ratios and a simple equation to simultaneously fit all six systems to determine the quasiprojectile N/Z. Simulations and a filter of the FAUST (Forward Array Using Silicon Technology) acceptance were used to calculate neutron loss; this accounted for the difference between the two techniques. To study the fragmentation of quasiprojectiles the fragment yields were used to calculate the isobaric, isotopic, fractional and mean N/Z yields. The results showed that as neutron richness increased, more neutron-rich fragments were produced. In addition observation showed evidence for an inhomogeneous distribution of N/Z between the light charged particles (LCPs Z less than 3) and intermediate mass fragments (IMFs Z greater than 2). The theoretical results, which used different values of the symmetry energy, were compared to experimental data to determine which symmetry energy best represents the experimental data. The comparison showed the experimental data was the overall best fit with a lower value of the symmetry energy. These results were not conclusive and further investigation is required.
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Libros sobre el tema "Deep inelastic collisions"

1

Zeuthen Workshop on Elementary Particle Theory: Deep Inelastic Scattering (1992 Teupitz, Germany). Deep inelastic scattering: Proceedings of the 1992 Zeuthen Workshop on Elementary Particle Theory : Deep Inelastic Scattering, Teupitz/Brandenburg, Germany, 6-10 April 1992. Amsterdam: North-Holland, 1992.

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2

Björkholm, Peter B. R. Measurement of the nucleon structure functions F2 and R in deep inelastic muon scattering. Uppsala, [Sweden]: [s.n.], 1995.

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Meyer, Herman. A spectator model for deep inelastic electron scattering. Amsterdam: Drukkerij GCA, 1992.

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4

Kruse, Andrés. Charged current interactions at HERA. [Amsterdam?: Universiteit van Amsterdam?], 1999.

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5

Aharon, Levy, ed. International Workshop on Deep Inelastic Scattering and Related Subjects: Eilat, Israel, 6-11 February, 1994. Singapore: World Scientific, 1994.

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Lettenström, Frans. A study of nuclear effects in deep inelastic muon scattering. Uppsala: Uppsala University, 1988.

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7

International Workshop on Deep Inelastic Scattering (13th 2005 Madison, Wis.). Deep inelastic scattering: 13th International Workshop on Deep Inelastic Scattering ; DIS 2005, Madison, Wisconsin (USA), 27 April - 1 May 2005. Editado por Smith Wesley H y Dasu Sridhara R. Melville, New York: American Institute of Physics, 2005.

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8

G, D'Agostini y Nigro A, eds. Deep inelastic scattering and related phenomena: DIS 96. Singapore: World Scientific, 1997.

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9

1939-, Boffi S., Ciofi Degli Atti C, Giannini M. M y Istituto nazionale di fisica nucleare., eds. 5th workshop on perspectives in nuclear physics at intermediate energies: ICTP, Trieste, Italy, May 6-10, 1991. Singapore: World Scientific, 1992.

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10

G, Roberts R. The structure of the proton: Deep inelastic scattering. Cambridge [England]: Cambridge University Press, 1990.

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Capítulos de libros sobre el tema "Deep inelastic collisions"

1

Kankeleit, Egbert. "Quasiatomic Spectroscopy as a Tool for Deep Inelastic Collisions". En Physics of Strong Fields, 359–71. Boston, MA: Springer US, 1987. http://dx.doi.org/10.1007/978-1-4613-1889-7_14.

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Adloff, Catherine. "Determination of the Gluon Structure Function Using Tagged Charm Events in Deep Inelastic EP Collisions". En NATO ASI Series, 365–70. Boston, MA: Springer US, 1997. http://dx.doi.org/10.1007/978-1-4899-0242-9_20.

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3

Fröbrich, P. y R. Lipperheide. "Deep-inelastic collisions. Phenomena and theory". En Theory of Nuclear Reactions, 363–403. Oxford University PressOxford, 1996. http://dx.doi.org/10.1093/oso/9780198537830.003.0011.

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Abstract So far we have been concerned with direct and compound-nucleus reactions. We shall now consider another type of reaction, the dissipative or deep-inelastic collisions (DIC), which display features of both of the former. Deep-inelastic collisions are special to heavy ions, and are the more pronounced the heavier the collision partners. They can be described in classical terms, and generally take place at intermediate impact parameters. For large impact parameters they go over into the direct or quasi-elastic reactions, and for small impact parameters into fusion.
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4

Fröbrich, P. y R. Lipperheide. "Analysis Of Deep-Inelastic Collisions, Fusion, And Heavy-Ion Induced Fission". En Theory of Nuclear Reactions, 404–62. Oxford University PressOxford, 1996. http://dx.doi.org/10.1093/oso/9780198537830.003.0012.

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Abstract In Chapter 11 we introduced friction and fluctuations in order to describe the dissipative processes occuring in deep-inelastic collisions. For the calculation of these effects we derived the Langevin and Fokker-Planck equations. We studied these equations for several simple examples and discussed general methods of solving them.
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Toki, Hiroshi y Hideo Suganuma. "Quark nuclear physics". En Nucleon—Hadron Many-Body Systems, 292–312. Oxford University PressOxford, 1999. http://dx.doi.org/10.1093/oso/9780198519003.003.0011.

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Abstract In traditional nuclear physics, protons and neutrons, the constituents of a nucleus, are assumed to be point particles and are described by a Hamiltonian with a kinetic term and an interaction term, possibly obtained from the Nucleon—Nucleon (NN) scattering data. The purpose is then to describe the binding energies of nuclei, their structures, decay properties, reaction rates, etc. The fundamental model used is the shell model [1]. About 20 years ago, other degrees of freedom were introduced to nuclear physics. The sensational one is pion condensation, in which the energy of pion becomes zero in nuclear matter, due to the interaction of pions with the nuclear medium, which includes also the delta isobar [2,3]. More recently, deep inelastic scattering has been used to probe the nucleons in nuclear medium and to study differences from their counterparts in free space, which is called the EMC effect [4]. A more drastic process is the production of high-density and high-temperature nuclear matter by relativistic heavy-ion collisions [5]. Such processes could even reduce nuclear matter from hadronic to a quark—gluon plasma phase.
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Actas de conferencias sobre el tema "Deep inelastic collisions"

1

Kovchegov, Yuri V. "Particle Production in p(d)A Collisions". En DEEP INELASTIC SCATTERING: 13th International Workshop on Deep Inelastic Scattering; DIS 2005. AIP, 2005. http://dx.doi.org/10.1063/1.2122040.

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Fries, R. J. "Forward Production in d+Au Collisions by Parton Recombination". En DEEP INELASTIC SCATTERING: 13th International Workshop on Deep Inelastic Scattering; DIS 2005. AIP, 2005. http://dx.doi.org/10.1063/1.2122041.

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Artru, X. "Transverse polarization in deep inelastic collisions". En Polarized Collider Workshop. AIP, 1991. http://dx.doi.org/10.1063/1.40477.

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Kniehl, Bernd A. "Charmonium production in two-photon collisions at next-to-leading order". En DEEP INELASTIC SCATTERING: 13th International Workshop on Deep Inelastic Scattering; DIS 2005. AIP, 2005. http://dx.doi.org/10.1063/1.2122166.

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Rakness, G. "Neutral Pion Suppression at Forward Rapidities in d+Au Collisions at STAR". En DEEP INELASTIC SCATTERING: 13th International Workshop on Deep Inelastic Scattering; DIS 2005. AIP, 2005. http://dx.doi.org/10.1063/1.2122039.

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Anthonis, Tinne. "Multiplicity structure in inclusive and diffractive deep inelastic e+p collisions at HERA". En DEEP INELASTIC SCATTERING: 13th International Workshop on Deep Inelastic Scattering; DIS 2005. AIP, 2005. http://dx.doi.org/10.1063/1.2122081.

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Jia, Jiangyong. "Jet properties from π± − h± correlation in p+p and d+Au collisions". En DEEP INELASTIC SCATTERING: 13th International Workshop on Deep Inelastic Scattering; DIS 2005. AIP, 2005. http://dx.doi.org/10.1063/1.2122157.

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Lim, Sanghoon. "PHENIX heavy-flavor results in d+Au collisions". En XXIII International Workshop on Deep-Inelastic Scattering. Trieste, Italy: Sissa Medialab, 2016. http://dx.doi.org/10.22323/1.247.0172.

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Awes, Terry C. "Production of Direct Photons, π0’s, and η’s in p+p and Au+Au Collisions at RHIC". En DEEP INELASTIC SCATTERING: 13th International Workshop on Deep Inelastic Scattering; DIS 2005. AIP, 2005. http://dx.doi.org/10.1063/1.2122156.

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Zhang, Chun. "Nuclear Modification Factors for Hadrons At Forward and Backward Rapidities in Deuteron-Gold Collisions at s[sub NN] = 200 GeV". En DEEP INELASTIC SCATTERING: 13th International Workshop on Deep Inelastic Scattering; DIS 2005. AIP, 2005. http://dx.doi.org/10.1063/1.2122038.

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