1969
DOI: 10.1103/physrev.188.1837
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Resonance Fluorescence Measurements ofIn115Transition Strengths below 3 MeV

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Cited by 26 publications
(5 citation statements)
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“…Good correspondence is observed for the 1.608 MeV level measured by Cauchois et al [21], while the deviations for the 1.497 MeV transition are discussed above. The results of Alston [19] agree within errors for the 2.480 and the 2.740 MeV transitions, but are significantly smaller for the 2.283 MeV and the 2.443 MeV transitions. Above E~ = 3.8 meV no transitions belonging to 115In could be identified.…”
Section: Resultssupporting
confidence: 50%
See 1 more Smart Citation
“…Good correspondence is observed for the 1.608 MeV level measured by Cauchois et al [21], while the deviations for the 1.497 MeV transition are discussed above. The results of Alston [19] agree within errors for the 2.480 and the 2.740 MeV transitions, but are significantly smaller for the 2.283 MeV and the 2.443 MeV transitions. Above E~ = 3.8 meV no transitions belonging to 115In could be identified.…”
Section: Resultssupporting
confidence: 50%
“…[19][20][21] and other information on the level properties available in the literature [18]. Unlike the case of even-even nuclei where the ratio of results obtained at 90 ~ and 127 ~ permits a distinction between dipole and quadrupole transitions, the angular distributions W(O) are much more isotropic in odd-even nuclei.…”
Section: Resultsmentioning
confidence: 99%
“…[13] at 940 keV coincides with the excited states in 115 In located at 934 keV with J π = 7/2 + , and at 941 keV with J π = 5/2 + , the latter indicating that E2 excitations could play a role. Quadrupole excitations have also been identified in nuclear resonance fluorescence measurements on 115 In [12][13][14][15][16][17][18]. Earlier photoexcitation work performed by Booth and Brownson [19] which led to the identification of IS below 2 MeV excitation energy is in general consistent with the findings of Ref.…”
Section: Introductionsupporting
confidence: 76%
“…(Auch die Hinzunahme des yon Alston [5] [5] als gegeben annimmt. Auch bier ist, wie bei der (158-1 133)keV-Kaskade, die Mehrzahl aller Spinkombinationen nach unseren A2, A4-Koeffizienten erlaubt.…”
Section: Die Mebergebnisseunclassified
“…Dietrich et al [9] linden durch modelltheoretische Uberlegungen j~--13/2 +, w~ihrend Atalay und Chiao-Yap [10] nach dem Unified Model in intermedifirer Kopplung j~=9/2 + erwarten. Der 1291 keVZustand zerf~illt unter Emission einer 1291 keV-Strahlung (~2>2,0) [5] in den Grundzustand und durch einen 158 keV-~bergang, fiber dessen Multipolarit~it bisher keine experimentellen Ergebnisse vorliegen, in das 1 133 keV-Niveau. Aus modelltheoretischen Uberlegungen fordern Dietrich et al [9], dab dieser 158 keV-~bergang vom Typ M1 sein sollte.…”
unclassified