By H. Zingl, et al.,
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Additional resources for Few-Body Systems and Nuclear Forces I [Int'l Conf Graz, 1978]
025 for Δ/Γ. 00) × 10−2 is equal to the angle Δθ through which the AD of resonantly scattered gamma rays was rotated in the experiment being discussed. According to the correct theory of magnetic-ﬁeldÞ perturbed ADs, this angle is ðð2CþD CþDÞ Xs rather than Ωτ. In our case, we then have Δθ = 1478 Ωτ. 052. These measurements, performed by the present author together with Sorokin, were not published separately. Their results formed the content of Sorokin’s thesis completed in 1964 and presented for a diploma.
92), it was necessary to introduce a correction that would take into account the possible inﬂuence of the change in the magnetic-ﬁeld direction on detector operation. This correction, R00 , was determined experimentally as a quantity that was analogous to R0 , but which was measured under conditions where both the scatterer and the gamma source at rest were at room temperature. In that case, there was virtually no resonant scattering. 031. The results of that study, which was performed before the appearance of the article quoted in , were treated according to the theory that described perturbed angular correlations of sequentially emitted photons without allowance for the ratio of the width Δ of the spectrum of resonantly scattered gamma rays to the natural width Г of the nuclear level to be excited.
However, it remains unclear whether this also applies to the other results from  —in particular, the results for 182W. 4 keV. This is the same nucleus and the same transition as those studied by R. Mössbauer himself when he discovered in 1958 the 48 2 Experimental Study of Resonant Gamma-Ray Scattering phenomenon of recoilless gamma-ray emission and absorption [21, 22]. The ADs of resonantly scattered gamma rays of the 191Ir nucleus had not been measured by the time when we began our study.
Few-Body Systems and Nuclear Forces I [Int'l Conf Graz, 1978] by H. Zingl, et al.,