Footenotes
J. P. Elliott andT. H. R. Skyrme:Proc. Roy. Soc., A232, 561 (1955).
L. J. Tassie andF. C. Barker:Phys. Rev.,111, 940 (1958);F. Palumbo: to be published.
C. Bloch andJ. Horowitz:Nucl. Phys. 8, 91 (1958).
F. Palumbo:Nucl. Phys.,99 A, 100 (1967).
F. Palumbo andD. Prosperi: inConference on Clustering Phenomena in Nuclei (Bochum, 1969).
M. H. Macfarlane: inProc. SIF, Course XL (New York, 1969);B. H. Brandow: inLectures in Theoretical Physics, Vol.11B (New York, 1969).
F. Palumbo andD. Prosperi:Nucl. Phys.,115 A, 296 (1968).
H. A. Bethe, B. H. Brandow andA. G. Petschek:Phys. Rev.,129, 225 (1963).
T. T. S. Kuo andJ. B. McGrory:Nucl. Phys.,134 A, 633 (1969).
J. S. Truelove andI. R. Nicholls:Austral. Journ. Phys.,23, 231 (1970);B. R. Barrett, R. G. L. Hewitt andR. J. McCarthy.Phys. Rev. C,2, 1199 (1970).
As has been discussed in ref. (4), in practicex 0 is not a free parameter. In fact the spaceP contains only a few linearly independent states of the c.m., so thatx 0 must be of ordermε2/h 2, where ε is the average difference of single-particle energy from shell to shell.
Author information
Authors and Affiliations
Rights and permissions
About this article
Cite this article
Palumbo, F. Nuclear centre-of-mass co-ordinate in the Bloch-Horowitz theory. Lett. Nuovo Cimento 2, 453–458 (1971). https://doi.org/10.1007/BF02804560
Received:
Published:
Issue Date:
DOI: https://doi.org/10.1007/BF02804560