Standard
High spin levels in119Te. / Papadopoulos, C.T.; Vlastou, R.; Serris, M. et al.
In:
Zeitschrift für Physik A Hadrons and Nuclei, Vol. 352, No. 3, 1995, p. 243-244.
Research output: Contribution to Journal/Magazine › Journal article › peer-review
Harvard
Papadopoulos, CT, Vlastou, R, Serris, M, Hartas, HG, Fotiades, N, Kalfas, CA, Harissopoulos, S, Kossionides, S, Simpson, J, Paul, ES, Araddad, S, Beausang, CW, Bentley, MA
, Joyce, MJ & Sharpey-Schafer, JF 1995, '
High spin levels in119Te',
Zeitschrift für Physik A Hadrons and Nuclei, vol. 352, no. 3, pp. 243-244.
https://doi.org/10.1007/BF01289495APA
Papadopoulos, C. T., Vlastou, R., Serris, M., Hartas, H. G., Fotiades, N., Kalfas, C. A., Harissopoulos, S., Kossionides, S., Simpson, J., Paul, E. S., Araddad, S., Beausang, C. W., Bentley, M. A.
, Joyce, M. J., & Sharpey-Schafer, J. F. (1995).
High spin levels in119Te.
Zeitschrift für Physik A Hadrons and Nuclei,
352(3), 243-244.
https://doi.org/10.1007/BF01289495Vancouver
Papadopoulos CT, Vlastou R, Serris M, Hartas HG, Fotiades N, Kalfas CA et al.
High spin levels in119Te.
Zeitschrift für Physik A Hadrons and Nuclei. 1995;352(3):243-244. doi: 10.1007/BF01289495
Author
Papadopoulos, C.T. ; Vlastou, R. ; Serris, M. et al. /
High spin levels in119Te. In:
Zeitschrift für Physik A Hadrons and Nuclei. 1995 ; Vol. 352, No. 3. pp. 243-244.
Bibtex
@article{01dd87209a7c4df0b0e0fefd7adf7f3c,
title = "High spin levels in119Te",
abstract = "High spin levels in119Te have been populated following the96Zr (30Si, α 3n)119Te reaction at a beam energy of 135 MeV. The subsequentγ-ray deexcitation was studied usingγ-ray spectroscopic methods. New levels and several spin and parity assignments up toJπ=55/2− were established. The decay scheme at high-spin exhibits single-particle characteristics associated with the fully aligned ν(h11/2)3 π(g7/2)2 configuration for the 39/2− level, while the 55/2− level could be interpreted as fully aligned π(d5/2)2ν h 11 2/5 g 7 2/−2 ) configuration.",
author = "C.T. Papadopoulos and R. Vlastou and M. Serris and H.G. Hartas and N. Fotiades and C.A. Kalfas and S. Harissopoulos and S. Kossionides and J. Simpson and E.S. Paul and S. Araddad and C.W. Beausang and M.A. Bentley and M.J. Joyce and J.F. Sharpey-Schafer",
year = "1995",
doi = "10.1007/BF01289495",
language = "English",
volume = "352",
pages = "243--244",
journal = "Zeitschrift f{\"u}r Physik A Hadrons and Nuclei",
number = "3",
}
RIS
TY - JOUR
T1 - High spin levels in119Te
AU - Papadopoulos, C.T.
AU - Vlastou, R.
AU - Serris, M.
AU - Hartas, H.G.
AU - Fotiades, N.
AU - Kalfas, C.A.
AU - Harissopoulos, S.
AU - Kossionides, S.
AU - Simpson, J.
AU - Paul, E.S.
AU - Araddad, S.
AU - Beausang, C.W.
AU - Bentley, M.A.
AU - Joyce, M.J.
AU - Sharpey-Schafer, J.F.
PY - 1995
Y1 - 1995
N2 - High spin levels in119Te have been populated following the96Zr (30Si, α 3n)119Te reaction at a beam energy of 135 MeV. The subsequentγ-ray deexcitation was studied usingγ-ray spectroscopic methods. New levels and several spin and parity assignments up toJπ=55/2− were established. The decay scheme at high-spin exhibits single-particle characteristics associated with the fully aligned ν(h11/2)3 π(g7/2)2 configuration for the 39/2− level, while the 55/2− level could be interpreted as fully aligned π(d5/2)2ν h 11 2/5 g 7 2/−2 ) configuration.
AB - High spin levels in119Te have been populated following the96Zr (30Si, α 3n)119Te reaction at a beam energy of 135 MeV. The subsequentγ-ray deexcitation was studied usingγ-ray spectroscopic methods. New levels and several spin and parity assignments up toJπ=55/2− were established. The decay scheme at high-spin exhibits single-particle characteristics associated with the fully aligned ν(h11/2)3 π(g7/2)2 configuration for the 39/2− level, while the 55/2− level could be interpreted as fully aligned π(d5/2)2ν h 11 2/5 g 7 2/−2 ) configuration.
U2 - 10.1007/BF01289495
DO - 10.1007/BF01289495
M3 - Journal article
VL - 352
SP - 243
EP - 244
JO - Zeitschrift für Physik A Hadrons and Nuclei
JF - Zeitschrift für Physik A Hadrons and Nuclei
IS - 3
ER -
