Study of 9Be + 12C elastic scattering at energies near the Coulomb barrier
References (26)
Nucl. Phys. A
(2009)- et al.
Phys. Rep.
(2006) - et al.
Nucl. Phys. A
(2006) Nucl. Phys. A
(1995)- et al.
Phys. Rep.
(1975) Nucl. Instrum. Methods A
(2001)Comp. Phys. Rep.
(1988)Phys. Lett. B
(2009)Nucl. Phys. A
(1999)Nucl. Phys. A
(2004)
Nucl. Phys. A
Nucl. Phys. A
Nucl. Phys. A
Cited by (15)
Threshold anomalies in <sup>9</sup>Be + <sup>12</sup>C
2024, Nuclear Physics AEnergy dependence of the optical potential of the weakly bound <sup>9</sup>Be projectile on the <sup>197</sup>Au target
2020, Nuclear Physics ACitation Excerpt :On the other hand, the data for the elastic scattering of the 7Li projectile on 59Co [16], 80Se [14], 138Ba [11], 144Sm [15] and 208Pb [17] show the presence of the usual TA. Finally, no conclusions could be extracted regarding any of these anomalies for the cases of 6Li on 27Al [8], 64Ni [9], 112,116Sn [10], 138Ba [11], 7Li + 28Si [29] and 9Be on 12C [22], 27Al [32], 120Sn [24] and 144Sm [19]. These results expose the necessity for further experimental data, especially for energies close to the barrier, where the elastic scattering is dominated by the Coulomb interaction.
Breakup threshold anomaly in the elastic scattering of the <sup>9</sup>Be + <sup>80</sup>Se system
2018, Nuclear Physics ACitation Excerpt :Finally, in several other reactions involving these stable weakly bound projectiles, no definite conclusions could be drawn regarding any of these two types of behavior. This includes the cases of 6Li on 27Al [4], 64Ni [5], 112Sn, 116Sn [6], 138Ba [7], 7Li + 28Si [14], and 9Be on 12C [20], 27Al [16], 120Sn [25] and 144Sm [17]. Among the main experimental limitations for establishing the character of the anomaly is the difficulty to obtain enough experimental data near and below the barrier.
Energy levels of light nuclei A = 12
2017, Nuclear Physics ACitation Excerpt :Discussion on polarization measurements is given in [1995CH12,1995CH44,2005CH58,2006SV01,2010WE06]. For Optical Potential analyses see [1990NI02,1991SH08,1997EL13,2001KA58,2009WE04,2011JA09,2011RA34,2012JA03,2012PA09,2015GH04,2016AL14,2016XU07]; for Coupled Channels analyses see [2003AM08,2005CA16,2006SV01]; for other analyses see [1990BE54,1991BA39,1992GA26,1992KA14,1992KA21,1994IS08,1994XI04,1996CH33,1996CH49,1996GO48,1997HA21,1998SU23,1999SU01,2000CH31,2000KE13,2005PI16,2008FR02,2008FR11,2008GE04,2009AL05,2009AL10,2010NA18,2016AR13,2016FR09]. For theoretical analysis of elastic and inelastic scattering see [1990TA13,1990TA16,1991LI07,1991TA01,1992WA19,1993BY02,1993DE33,1995MA23,1996BE25,1997DO02,1997TE14,1998GI01,1998GU13,1998KI17,1998SU23,1999GU17,1999NA43,2000CH31,2000DE37,2000LO20,2004YA24,2005PI16,2006GU23,2008FR02,2013WE05,2015TO11].
Recent developments in fusion and direct reactions with weakly bound nuclei
2015, Physics Reports