ADOPTED LEVELS for 71Kr

Authors: Balraj Singh and Jun Chen |  Citation: Nucl. Data Sheets 188, 1 (2023) |  Cutoff date: 17-Jan-2023 

 Full ENSDF file | Adopted Levels (PDF version) 


Q(β-)=-14040 keV SYS(n)= 13300 keV SYS(p)= 2.19×103 keV 13Q(α)= -2.17×103 keV 15
Reference: 2021WA16

General Comments:

Mass measurement: 2011Tu02, HIRFL-CSR, Cooler Storage Ring at the Heavy Ion Research Facility in Lanzhou.

1981Ew01: 71Kr produced and identified in 93Nb(p,X) at 1 GeV, chemical mass separation, measured half-life

1995Bl23: fragmentation of 78Kr beam at 73 MeV/nucleon with a carbon target. SISSI/LISE spectrometer at GANIL. Energy loss and time-of-flight techniques.

1997Oi01: 93Nb(p,X) at 1 GeV, ISOLDE-CERN facility, measured γ, β, delayed protons, coincidences between different types of radiation

2002Lo13 (also 2002Bl17): fragmentation of 78Kr beam at 73 MeV/nucleon with a carbon target. SISSI/LISE spectrometer at GANIL. Energy loss and time-of-flight techniques.

2008NaZR: Ca(32S,X) and Ca(33S,X), recoil-β+ decay tagging method to identify γ rays in 71Kr. The details are not available

2014Ro14: 71Kr produced in the fragmentation of 70 MeV/nucleon 78Kr beam with nickel target. Fragments selected with the LISE3 separator at GANIL and identified by time-of-flight and energy loss. Measured half-life of 71Kr ground-state decay by (fragment)β, (fragment)γ correlations using four Si detectors (an energy loss ΔE detector, a degrade, DSSD and Si(Li)) for particles surrounded by four HPGe Clover detectors, three EXOGAM, and one mini-clover Ge detector for γ rays.

2018Wi08: intense production (see Fig. 1 in the paper) of beam of 71Kr nuclei in 9Be(78Kr,X),E-345 MeV/nucleon at RIBF-RIKEN

2019Si33: 71Kr produced at the RIBF-RIKEN facility in the 9Be(124Xe,X) reaction at E=345 MeV/nucleon. Fragments were separated in the first stage of BigRIPS and then identified by measuring ΔE, tof and Bρ using BigRIPS and the ZeroDegree spectrometer, followed by implantation of products into the beta-counting system WAS3ABi, consisting of a double-sided silicon-strip detector. Measured time distribution of (implanted ions)β+-correlated events, and deduced half-life of 71Kr decay

2022Wa34: 71Kr produced in 9Be(92Mo,X),E=140 MeV/nucleon reaction, followed by separation of ions of interest using A1900 fragment separator and a Radio Frequency Fragment Separator (RFFS) at the Coupled Cyclotron Facility of NSCL-MSU. The ions in the cocktail beam were implanted into the β-counting station (BCS), which consisted of a stack of PIN detector (PIN2) and Double-Sided Silicon-Strip Detector (DSSSD) for detection of implants, surrounded by the SeGA array of 16 HPGe detectors for γ detection. Measured Eγ, Iγ, (implants)β-coin, (implants)(β-delayed protons)-coin, (implants)γγ-coin, (implants)βγ-coin, T1/2 of decay of 71Kr. Deduced absolute (per 100 decays of parent) number of βγ-coin events, β events, absolute (per 100 decays of parent) intensities of γ rays, and intensities of β-delayed protons.

1964Fl03: 70-72Br or 70-72Kr claimed to have been produced in Ni(20Ne,X) E=140 MeV reaction and a delayed proton group of 2.5 MeV with a half-life of 23 s 4. It is not possible to associate this observation with a presently known activity

Theoretical structure calculations:

2012Bh10: calculated S(2n), β2, S(p), binding energy using microscopic-macroscopic model with Wigner-Kirkwood expansion.

2001Sa67: calculated Gamow-Teller strength distributions, Q(ε), T1/2, deformation, using self-consistent Hartree-Fock approach.

1998Ur03: calculated levels, Jπ, Gamow-Teller strengths using Hartree-Fock approach.

1972Di03: calculated potential energy surface, deformation energy using Strutinsky formalism

Q-value: ΔQ(β-)=420, ΔS(n)=240 (syst,2021Wa16)

Q-value: S(2n)=30330 330 (syst), S(2p)=4470 130, Q(εp)=8310 130, Q(ε)=10180 130 (2021Wa16)





E(level)
(keV)
Jπ(level) T1/2(level)
  0 (5/2)- 94.9 ms 4 
% ε = 100
% εp = 3.06 27

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Additional Level Data and Comments:

E(level)Jπ(level)T1/2(level)Comments
  0(5/2)- 94.9 ms 4 
% ε = 100
% εp = 3.06 27
%εp=3.06 27 (2022Wa34, measurement of β-delayed proton spectrum correlated with implants, Monte-Carlo analysis used for separation of charged particles into positron and protons). Others: %εp=2.1 7 (1997Oi01), 5.2 6 (1995Bl23). Due to much higher statistics and a refined analysis in 2022Wa34, value from this work is preferred over those from 1997Oi01 and 1995Bl23.
E(level): %εp=3.06 27 (2022Wa34, measurement of β-delayed proton spectrum correlated with implants, Monte-Carlo analysis used for separation of charged particles into positron and protons). Others: %εp=2.1 7 (1997Oi01), 5.2 6 (1995Bl23). Due to much higher statistics and a refined analysis in 2022Wa34, value from this work is preferred over those from 1997Oi01 and 1995Bl23.

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