Nuclear reactions of silver with 25.2 GeV<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mmultiscripts><mml:mrow><mml:mi mathvariant="normal">C</mml:mi></mml:mrow><mml:mprescripts /><mml:mrow /><mml:mrow><mml:mn>12</mml:mn></mml:mrow><mml:mrow /><mml:mrow /></mml:mmultiscripts></mml:mrow></mml:math>ions and 300 GeV protons

Porile, N.; Cole, G. D.; Rudy, C.R.

doi:10.1103/physrevc.19.2288

Cited by 84 publications

(28 citation statements)

References 44 publications

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“…As the present experiments have been done with only one kind of projectile (12C), at only one incident energy (86 MeV/nucleon), it is difficult to extract precise information on the reaction mechanisms. Nevertheless, the present heavy fragments distributions exhibit similarities with previous results at high incident energies as for the 2~ at 8 GeV [11] or the 12c+natAg at 25 GeV [16] reactions. As in such cases a Monte Carlo intranuclear cascade model was able to generate the correct shape for high mass product distribution, the same approach has been performed on the present data, using both ISABELLE [17] and EVA [18] codes.…”

Section: Discussionsupporting

confidence: 89%

Heavy fragment energies and angular distributions in the reaction of 86 MeV/nucleon12C with medium-A targets

et al. 1983

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Using the thin target -thin catchers techniques, masses, mean recoil energies and angular distributions of target residues have been measured for 86 MeV/nucleon 12C induced reactions. Several different nuclear reaction processes, from peripheral to central collisions have been observed. Experimental results are partly reproduced by intranuclear cascade+evaporation calculations. Up to now, the production of the lightest masses (44

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Section: Discussionsupporting

confidence: 89%

Heavy fragment energies and angular distributions in the reaction of 86 MeV/nucleon12C with medium-A targets

et al. 1983

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“…This "memory" takes into account the difference in neutron excess between the projectile and the corresponding nuclei at the evaporation corridor [29]. Figure 2 (dashed line) clearly shows that the parameterization of this effect in EPAX is not optimal.…”

Section: Model Calculationsmentioning

confidence: 99%

Production of neutron-rich nuclei in fragmentation reactions of Sn132 projectiles at relativistic energies

Pérez–Loureiro¹,

Benlliure²,

Álvarez‐Pol³

et al. 2011

Physics Letters B

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The fragmentation of neutron-rich 132 Sn nuclei produced in the fission of 238 U projectiles at 950 MeV/u has been investigated at the FRagment Separator (FRS) at GSI. This work represents the first investigation of fragmentation of medium-mass radioactive projectiles with a large neutron excess. The measured production cross sections of the residual nuclei are relevant for the possible use of a two-stage reaction scheme (fission+fragmentation) for the production of extremely neutron-rich medium-mass nuclei in future rare-ion-beam facilities. Moreover, the new data will provide a better understanding of the "memory" effect in fragmentation reactions.

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“…It was found there that element distributions of IMF are rather well described in terms of a simple power law o-(Z) Z-N which was suggested to be a signature for the occurrence of statistical clustering near a critical point [2][3][4][5][6][7][8]. Similar element distributions were found later in reactions induced by the 3He, 12C, and heavier ions [9][10][11][12][13][14][15][16].…”

Section: Introductionmentioning

confidence: 62%