Nuclear Data Sheets for A = 125

Katakura, J.

doi:10.1016/s0090-3752(81)80054-3

Cited by 37 publications

(5 citation statements)

References 169 publications

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“…By the way, with the wave cross-section a~t = 2.85.10-19cm 2 for Sn-ll9me one gets from (1), (6) etc. the theoretical result e = 0.01% which contradicts the experimental value (73).…”

Section: -Experimentalmentioning

confidence: 98%

“…(7) and (25)). This experimental fact cannot be understood in the framework of the non-collective model based on (1), (6), (18)- (20), (26)-(38).…”

Section: -Experimentalmentioning

confidence: 98%

“…In 1984 [5] we observed the stimulated emission in Te-125mr Here 125~Te is the 144.772keV isomeric state 11/2 with a half-life of 60.2 days [6,7]. The gamma quanta were detected by a silicic BDRK-type semiconductor counter of low efficiency (ca.…”

Section: + Hvr~mentioning

confidence: 99%

“…And at 218.54keV there are no lines of spontaneous emission [6]. Therefore, a N 100% efficiency counter permits the absolute counting of stimulated-emission acts (5).…”

Section: + Hvr~mentioning

confidence: 99%

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New observations of stimulated emission of Mössbauer radiation in isomeric transitions $$^{125m_2 } Te \to ^{125m_1 } Te + hv(109.3 keV)$$ and $$^{123m_2 } Te \to ^{123m_1 } Te + hv(88.46 keV)$$

Скоробогатов

Dzevitskii

1995

Il Nuovo Cimento D

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Summary. --A sample of Be 125m2Te containing (4.9 _+ 1.5). 10 TM atoms/era 3 of 125"~Te was obtained in a reactor by neutron activation of polycrystalline beryllium telluride Be124Te. The ratio of the number of 109.27keV photons emitted in the 125~ZTe + hv--,125mlTe + 2hv transition due to attainment of the MSssbauer conditions (at T = 10 K) to the total number of photons produced in the sample at T = 300K was measured to be e~p = Ar162 = 0.0045 + 0.0030. Independent measurements of the intensity of the two-photon 218.54 keV line at 10 K in the same sample yielded a value of 0.0023 + 0.0004 for e~p. Under the conditions of our experiment in the moving-wave approximation (i.e. in the framework of non-stationary optics) the theory predicts the value etheo r =-~coh(10K)/-~non~oh (300 K) = 0.0018 + 0.0006 for the ratio of the superemission power of Te-125me nuclei at 10 K 2cob to the normal spontaneous emission power of these nuclei at 300 K -~non-coh-This value within the error coincides with e~p. The stimulated MSssbauer transition 123~Te + hv(88.46 keV)--~ 123miTe + 2hv(88.46 keV) in a polycrystalline sample of Mga TeO6 containing (3.4 -+ 0.7). 1019 atoms/cm 3 of 128~Te was also experimentally studied. The measured value e~p = (5 -+ 3). 10 -4 for this transition within the error coincides with a theoretical value ethc~r = 0.00023 obtained in the moving-wave approximation.

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“…By the way, with the wave cross-section a~t = 2.85.10-19cm 2 for Sn-ll9me one gets from (1), (6) etc. the theoretical result e = 0.01% which contradicts the experimental value (73).…”

Section: -Experimentalmentioning

confidence: 98%

“…(7) and (25)). This experimental fact cannot be understood in the framework of the non-collective model based on (1), (6), (18)- (20), (26)-(38).…”

Section: -Experimentalmentioning

confidence: 98%

Section: + Hvr~mentioning

confidence: 99%

“…And at 218.54keV there are no lines of spontaneous emission [6]. Therefore, a N 100% efficiency counter permits the absolute counting of stimulated-emission acts (5).…”

Section: + Hvr~mentioning

confidence: 99%

See 2 more Smart Citations

New observations of stimulated emission of Mössbauer radiation in isomeric transitions $$^{125m_2 } Te \to ^{125m_1 } Te + hv(109.3 keV)$$ and $$^{123m_2 } Te \to ^{123m_1 } Te + hv(88.46 keV)$$

Скоробогатов

Dzevitskii

1995

Il Nuovo Cimento D

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“…The values were determined in these works with relatively large uncertainties (2.2%, 10.2% and 8.7%, respectively) and furthermore, the data of [16] is available only in an unpublished thesis and the work of [14] provides only very limited experimental information. In the compilations before 1981 [17] the weighted average (45.2 ± 1 min) of the half-lives was given as the recommended value. However, this was changed -without any detailed explanation -in the compilations issued after 1993 [18] and the unweighted average of the three measurements [14,15,16] (46.7 min) was given.…”

Section: Available Half-life Valuesmentioning

confidence: 99%

High precision half-life measurement of 125Cs and 125Xe with γ-spectroscopy

et al. 2019

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In order to provide data for the simulation of the astrophysical γ-process, the cross section measurement of the 124 Xe(p,γ) 125 Cs reaction is in progress at MTA Atomki using the activation technique. Precise information on the decay characteristics of the reaction products is of crucial importance for measurements carried out using this method. The half-lives of the produced 125 Cs and its daughter 125 Xe are published in previous works, but with large uncertainties and ambiguous values. To make these nuclear parameters more precise, the half-lives have been re-measured with high precision using γ-spectroscopy. The obtained new half-life values are t 1/2 = 44.35 ± 0.29 minutes for 125 Cs and t 1/2 = 16.87 ± 0.08 hours for 125 Xe.

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