Alpha-decay branching ratios to high-lying excited-states of the 242 Cm → 238 Pu → 234 U → 230 Th → 226 Rn decay chain

2009 ◽  
Vol 33 (9) ◽  
pp. 764-768
Author(s):  
Zhang Jin-Juan ◽  
Xu Chang ◽  
Ren Zhong-Zhou
1973 ◽  
Vol 28 (10) ◽  
pp. 1635-1641 ◽  
Author(s):  
A. G. de Pinho ◽  
M. Weksler

The X-ray spectra resulting from the internal conversion of electric quadrupole transitions following the alpha decay of Th230 and Ra226 were analysed with a Si (Li) spectrometer. From the knowledge of the Coster-Kronig and fluorescence yields, the internal conversion coefficients of the E2 transitions from the first excited states in Ra226 and Rn222 could be deduced. Results are in good agreement with theoretical values.


2005 ◽  
Vol 72 (5) ◽  
Author(s):  
M. Coreno ◽  
K. C. Prince ◽  
R. Richter ◽  
M. de Simone ◽  
K. Bučar ◽  
...  

2007 ◽  
Author(s):  
S. N. Liddick ◽  
R. Grzywacz ◽  
C. Mazzocchi ◽  
R. D. Page ◽  
K. P. Rykaczewski ◽  
...  
Keyword(s):  

2019 ◽  
Vol 28 (06) ◽  
pp. 1950045 ◽  
Author(s):  
B. Nandana ◽  
R. Rahul ◽  
S. Mahadevan

[Formula: see text]-value and half-life of elements in alpha decay chain of [Formula: see text]117, [Formula: see text]117, [Formula: see text]116 and [Formula: see text]116 were calculated using the Nuclear potential generated by double folding procedure and using the WKB method treating the alpha decay as a tunneling problem. The nuclear potential was parameterized using Woods–Saxon potential. Using this approach, the [Formula: see text]-value and half-life of next heaviest element in the alpha decay chain of element [Formula: see text]116 is predicted. It is proposed to use this to predict the [Formula: see text]-value and half-life of other higher elements in different alpha decay chains.


2012 ◽  
Vol 21 (06) ◽  
pp. 1250055 ◽  
Author(s):  
M. RASHDAN

The NL-RA1 effective interaction of the relativistic mean field theory is employed to study the structure of deformed and superheavy nuclei, using an axially deformed harmonic oscillator basis. It is found that a fair agreement with the experimental data is obtained for the binding energies (BE), deformation parameters and charge radii. Comparison with NL-Z2, NLSH and NL3 interactions show that NL-Z2 gives good binding but larger radii, while NL-SH gives good radii but larger binding. The NL-RA1 interaction is also tested for the new deformed superheavy element with Z≥98. Excellent agreement with the experimental binding is obtained, where the relative error in BEs of Cf, Fm, No, Rf, Sg and Ea (Z = 110) isotopes are found to be of the order ~0.1%. The NL3 predicted larger binding and larger relative errors ~0.2–0.5%. Furthermore, the experimental Q-values of the alpha-decay of the superheavy elements 270110, 288114 and 292116 are satisfactory reproduced by NL-RA1 interaction, where the agreement is much better than that predicted by the phenomenological mass FRDM model. Furthermore, the alpha-decay chain of element 294118 are also better reproduced by NL-RA1 interaction.


2005 ◽  
Vol 22 (4) ◽  
pp. 843-845 ◽  
Author(s):  
Tai Fei ◽  
Chen Ding-Han ◽  
Xu Chang ◽  
Ren Zhong-Zhou

2011 ◽  
Vol 850 (1) ◽  
pp. 34-52 ◽  
Author(s):  
K.P. Santhosh ◽  
Sabina Sahadevan ◽  
Jayesh George Joseph

1994 ◽  
Vol 117 ◽  
pp. 1-15
Author(s):  
Hirokazu Tamura ◽  
Ryugo S. Hayano ◽  
Haruhiko Outa ◽  
Toshimitsu Yamazaki

We summarize studies of Λ hypernuclei with stopped K− reaction carried out at KEK. The π− momentum spectra in the (stopped K−, π−) reaction were measured with light nuclear targets (4He, 7Li, 9Be, 12C and 16O). The ground and excited states of Λ4He, Λ12C and Λ16O were identified and their formation probabilities were measured. The branching ratios of π0-mesonic decay of Λ4He, Λ11B and Λ12C were measured for the first time with π0 coincidence. The lifetime of Λ4H was also determined with an improved accuracy. The π− peak intensity from Λ4H→4He+π− decay gave the Λ4H formation probabilities on these targets, where Λ4H is produced as hyperfragment except for the case of the 4He target. Concerning the formation mechanism of hyperfragments and their application to hypernuclear γ-ray spectroscopy, the running experiments and future prospects are also described.


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