ensdf evaluation for a=260-265
DESCRIPTION
ENSDF evaluation for A=260-265. M. Gupta Manipal University, Manipal, India T. W. Burrows National Nuclear Data Center, Brookhaven National Laboratory, USA. Motivation for evaluation. α -decay mass chains from some heavier nuclei (A≥266) end in this region update of this region is due - PowerPoint PPT PresentationTRANSCRIPT
M. Gupta, 20th IAEA-NSDD, Kuwait, 27-31 January, 2013
ENSDF evaluation forA=260-265
M. Gupta Manipal University, Manipal, India
T. W. BurrowsNational Nuclear Data Center,
Brookhaven National Laboratory, USA
M. Gupta, 20th IAEA-NSDD, Kuwait, 27-31 January, 2013
α-decay mass chains from some heavier nuclei (A≥266) end in this region
update of this region is due Earlier evaluations of these nuclides in : 1999Ar21,
1999Ak02 and 2001Ak11 265Rf : 2000Fi12
the same evaluation methodology adopted for (distant) ancestors could be usefully extended to descendents within an α-decay chain for consistency and uniformity of treatment
New results / chemistry
Motivation for evaluation
M. Gupta, 20th IAEA-NSDD, Kuwait, 27-31 January, 2013
Chart of Nuclides showing Chart of Nuclides showing A=260-265 regionA=260-265 region
Cold fusion
Hot fusion
A=265
A=260
Physics interest:
Deformed shell region
N ~162-164
M. Gupta, 20th IAEA-NSDD, Kuwait, 27-31 January, 2013
Guidelines for evaluation:
As established in 2005Gu33:
International Union of Pure and Applied Chemistry, Trans-fermium Working Group (IUPAC-TWG-JWP):
R. C. Barber et. al., Prog. Part. Nucl. Phys., v29, p453-530, 1992
IUPAC/IUPAP - TWG is concerned with the discovery of a new element ENSDF evaluations seek primarily to adopt the best set of data for a
given isotope
Priority of discovery for elements in the A=260-265 region already established by IUPAC/IUPAP-TWG/JWP
Guidelines serve well to re-visit older data and evaluate new data within a consistent framework
M. Gupta, 20th IAEA-NSDD, Kuwait, 27-31 January, 2013
Data checked for:• Measurement of excitation functions• Cross-bombardments: changing the relative yields of xn-evaporation channels by
varying mass number of Projectile or Target (useful in “hot fusion”)• Independent verification by another laboratory • Redundancy and internal consistency of data• Estimates of randomness• Consistency of assignments of daughters: secured connection to known descendents; (“cold-fusion”) presence of elemental signatures such as x-rays (in the absence of mass measurements);
direct measurements of nuclei in the decay chain by independent chemical studies determination of Z• T1/2 : larger statistics, better value (results can be ‘combined’)
M. Gupta, 20th IAEA-NSDD, Kuwait, 27-31 January, 2013
Statistical determination of uncertainties
Where not quoted or for combining /including new data
Method of K.-H. Schmidt et. al., Z. Phys. A316, 19, 1984
τu = Upper limit (estimate); τl = lower limit (estimate)
tm = average mean time; z = 1 for 68% confidence level;
n = # of eventsExpected accuracy of approximation: within 10%
M. Gupta, 20th IAEA-NSDD, Kuwait, 27-31 January, 2013
“Viola-Seaborg” Phenomenology
V. E. Viola and G. T. Seaborg, J. Inorg. Nucl. Chem., v28, p741, 1966
‘Dubna’ parameter set, obtained by a fit to 65
even-even nuclei:
M. Gupta, 20th IAEA-NSDD, Kuwait, 27-31 January, 2013
A=260-265 Available data for 31 observed nuclides considered
A = 265 (4); 264 (3); 263 (6); 262 (5); 261 (6); 260 (7)
Experimental details include: Differences in interpretation of observations for parents and
daughters e.g. 265/266Sg 261/262Rf
Cross-sections including revisions in cross-sections following re-interpretation
of data (e.g. 262/263Db) Reassignments --- existing data
noted in both original and “re-assigned” data sets SF: TKE, mass distributions, n-multiplicity Chemical properties
M. Gupta, 20th IAEA-NSDD, Kuwait, 27-31 January, 2013
Chemical studies: A=260-265 region ~40% nuclides studied using chemistry Reporting of experimental uncertainties in chemical studies
varies with: Specific chemical techniques used (e.g. parent half-life not
measured in some cases) Motivation for experiment (e.g. measurement for presence or
absence of nuclide rather than accurate half-life) Interpretation of half-lives (e.g. upper or lower limits?)
Properties derived from chemical studies supported if same nuclides are also studied by “physical” techniques
Re-assignments possible due to ambiguities in data
M. Gupta, 20th IAEA-NSDD, Kuwait, 27-31 January, 2013
Conclusions Uniform criteria used to evaluate A=260 – 294 region Evaluation methodology is internally consistent
Re-visiting ‘old’ data yields useful information Reveals important experimental parameters vital to
adopting the best data set in the absence of mass measurements e.g. cross-sections / excitation function measurements
Atomic properties revealed by chemistry Chemical methods:
Increased statistics Independent verification