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Concerning the time dependence of the decay rate of 137Cs.

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It is found that the PTB measurements of the decay rate of (137)Cs show no evidence of an annual oscillation, in agreement with the recent report by Bellotti et al., and is consistent with the finding that different nuclides have different sensitivities to whatever external influences are responsible for the observed periodic variations.
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This article is published in Applied Radiation and Isotopes.The article was published on 2013-04-01 and is currently open access. It has received 26 citations till now. The article focuses on the topics: Nuclide.

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Comparative study of beta-decay data for eight nuclides measured at the Physikalisch-Technische Bundesanstalt

TL;DR: In this article, the results of time-series analyses of data, kindly provided by the Physikalisch-Technische Bundesanstalt, concerning the beta-decays of Ag108, Ba133, Cs137, Eu152 and Eu154, Kr85, Ra226, and Sr90 were presented.
References
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Journal ArticleDOI

Evidence of correlations between nuclear decay rates and Earth–Sun distance

TL;DR: In this paper, the decay rates of 32 Si and 226 Ra have been investigated at Brookhaven National Laboratory (32 Si) and at the Physikalisch-Technische-Bundesanstalt in Germany (226 Ra).
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Precise measurement of the solar neutrino day-night and seasonal variation in Super-Kamiokande-I

Michael B. Smy, +132 more
- 30 Jan 2004 - 
TL;DR: The time variation of the elastic scattering rate of solar neutrinos with electrons in Super-Kamiokande-I was fit to the variations expected from active two-neutrino oscillations as discussed by the authors.
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Half-life of32Si

TL;DR: In this paper, the decay rate was determined from the 32Si/36Cl ratio of counts, based on the analysis of 53 points taken in 48 months, the valueT1/2 = 172(4) yr is adopted for the half-life of 32Si.
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Frequently Asked Questions (9)
Q1. What are the contributions in "Concerning the time dependence of the decay rate of 137 cs" ?

In this paper, the authors present new data for 133Ba and 137Cs, which were measured on the same detector system for the same time period, for which no annual oscillatory behavior was observed. 

This result, in addition to the results of decay experiments listed in Table 1, indicates that the failure to observe the annual ( or other ) periodicity in one isotope does not exclude that possibility in others. In light of Table 1, the authors can state in general that their studies to date suggest the following: ( a ) not all nuclides exhibit variability in decay constants ; ( b ) among nuclides that do exhibit this variability, the patterns of variability ( e. g., amplitude and phase of any oscillation ) are not all the same ; and ( c ) for nuclides that do exhibit variability, the patterns themselves may vary over time. 

The authors have also analyzed the PTB measurements in terms of ‘‘phasegrams,’’ which are analogous to spectrograms, displaying the power as a function of time and phase for an assumed annual oscillation. 

One of the significant factors leading to the selection of ionization chambers in these types of measurements is their inherent stability with respect to systematic and environmental effects. 

The rod was placed in the neutron irradiator for 5 min, activated, and then was placed in the counting bed and counted for fifteen minutes. 

The 137Cs standard set referenced above, which was used to determine system stability and calibration, consisted of nineindividual sources of 0:5 mCi each. 

Over a six month period of initial set-up and calibration, as reported in Cohn et al. (1969), the standard deviation of the 137Cs counts was 0.54%, implying good stability, and the background over the same period was 2:32 10470:56% counts/min over a 2:5 MeV spectrum window. 

Based on the care and thorough effort in the design, construction and calibration of the counting system in the Ellis experiment, aimed at reducing possible background and systematic variations, it seems probable that the observed differences in the fluctuations in the measured decay rates are intrinsic to the 56Mn and 137Cs decays themselves. 

This counting system was utilized in conjunction with a broad beam neutron irradiator (Cohn et al., 1972), for the in vivo NAA experiments described in Ellis (1990), as mentioned above.