Large transient magnetic fields for rare-earth ions recoiling in gadolinium and g-factors of high-spin states in 156, 158, 160Gd
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Cited by (59)
Nuclear Data Sheets for A=160
2021, Nuclear Data SheetsApparatus for in-beam hyperfine interactions and g-factor measurements: Design and operation
2020, Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated EquipmentCitation Excerpt :The analog output of an Ortec model 661 rate meter can be fed to the accelerator beam current metering system to assist with beam tuning. The requirements for the electromagnet design were that (i) it must be compact, (ii) the field applied to the target should be at least 0.07 T for targets with iron as the host [52], and of order 0.1 T for targets with gadolinium as the host [37,53], (iii) beam bending must be minimized. The present design was chosen on the basis of previous experience with several electromagnet designs and pole-piece geometries [11,54–56], along with detailed calculations using the Poisson Superfish software [57].
Nuclear Data Sheets for A=158
2017, Nuclear Data SheetsNuclear Data Sheets for A = 156
2012, Nuclear Data SheetsPerturbed angular correlations for Gd in gadolinium: In-beam comparisons of relative magnetizations
2006, Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and AtomsCitation Excerpt :Gadolinium foils are used extensively for in-beam measurements of hyperfine interactions and nuclear moments [1–13]. Magnetized gadolinium foils are used in preference to iron foils in many applications of the transient-field technique [5,13] to measure nuclear g factors because larger perturbations of the particle-γ correlations can be obtained under otherwise similar experimental conditions [6,7]. One disadvantage of gadolinium hosts, however, is that the magnetization is not well controlled, being sensitive to the crystalline structure of the foil and varying considerably with both the applied field and the temperature, even at temperatures well below the Curie temperature of 293 K [14].
Nuclear data sheets for A = 160
2005, Nuclear Data Sheets
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