The bound coherent neutron scattering lengths of the lanthanoids Pr, Nd, Sm, Eu, Yb and several of their isotopes as determined by neutron Bragg powder diffraction

We have determined the bound coherent neutron scattering lengthsbcof nuclides<sup>141</sup>Pr,<sup>iso</sup>Nd (iso = 142, 143, 144, 145, 146, 148, 150),<sup>iso</sup>Sm (iso = 147, 148, 150, 152, 154),<sup>153</sup>Eu,<sup>170</sup>Yb and<sup>174</sup>Yb as well as the natural elements<sup>nat</sup>Eu and<sup>nat</sup>Nd by using Bragg powder diffraction and analysing relative Bragg peak intensities with the Rietveld procedure. Some of these scattering lengths had never been determined before, to the best of our knowledge. Our investigations were carried out using different neutron diffractometers and different incident neutron energies (i.e. wavelengths) on chemically pure, crystalline, highly-enriched isotopic powder samples having different crystalline structures in order to ensure the consistency and robustness of the results and to reveal potential systematic errors. Our study led to final well-determined values ofbc(<sup>141</sup>Pr) = 4.44(4) fm,bc(<sup>142</sup>Nd) = 7.24(4) fm,bc(<sup>143</sup>Nd) = 17.51(6) fm,bc(<sup>144</sup>Nd) = 3.06(7) fm,bc(<sup>145</sup>Nd) = 10.40(12) fm,bc(<sup>146</sup>Nd) = 8.56(9) fm,bc(<sup>148</sup>Nd) = 4.44(13) fm,bc(<sup>150</sup>Nd) = 6.87(5) fm.bc(<sup>147</sup>Sm) = 6.68(5) fm,bc(<sup>148</sup>Sm) = 6.67(7) fm,bc(<sup>150</sup>Sm) = 10.05(10) fm,bc(<sup>152</sup>Sm) = -6.14(12) fm,bc(<sup>154</sup>Sm) = 9.34(9) fm,bc(<sup>153</sup>Eu) = 8.33(11) fm,bc(<sup>170</sup>Yb) = 4.83(3) fm,bc(<sup>170</sup>Yb) = 22.02(7) fm,bc(<sup>nat</sup>Nd) = 7.87(11) fm for thermal neutrons, and alsobc(<sup>nat</sup>Sm) = 5.29(5) fm for an incident neutron energy of 330.3(9) meV andbc(<sup>nat</sup>Eu) = 5.84(5) fm for an incident neutron energy of 168.10(5) meV. Based on the good precision and self-consistency of ourbcresults over so many isotopes, we advocate neutron Bragg powder diffraction as a method of choice for future studies to determine bound coherent neutron scattering lengths.

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Journal
Journal of Physics Condensed Matter
Published
2025-11-12
DOI
https://doi.org/10.1088/1361-648x/ae1ec0
Primary Topic
Nuclear Physics and Applications
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article
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article

The bound coherent neutron scattering lengths of the lanthanoids Pr, Nd, Sm, Eu, Yb and several of their isotopes as determined by neutron Bragg powder diffraction

Henry E. Fischer, Ralf Kautenburger, Kristina Brix, Thomas C. Hansen et al.
Journal of Physics Condensed Matter
Nuclear Physics and Applications
article

The bound coherent neutron scattering lengths of the lanthanoids Pr, Nd, Sm, Eu, Yb and several of their isotopes as determined by neutron Bragg powder diffraction

Henry E. Fischer, Ralf Kautenburger, Kristina Brix, Thomas C. Hansen, Florian Gehlhaar, Vanessa K. Peterson, Holger Kohlmann
article en

Abstract

We have determined the bound coherent neutron scattering lengthsbcof nuclides<sup>141</sup>Pr,<sup>iso</sup>Nd (iso = 142, 143, 144, 145, 146, 148, 150),<sup>iso</sup>Sm (iso = 147, 148, 150, 152, 154),<sup>153</sup>Eu,<sup>170</sup>Yb and<sup>174</sup>Yb as well as the natural elements<sup>nat</sup>Eu and<sup>nat</sup>Nd by using Bragg powder diffraction and analysing relative Bragg peak intensities with the Rietveld procedure. Some of these scattering lengths had never been determined before, to the best of our knowledge. Our investigations were carried out using different neutron diffractometers and different incident neutron energies (i.e. wavelengths) on chemically pure, crystalline, highly-enriched isotopic powder samples having different crystalline structures in order to ensure the consistency and robustness of the results and to reveal potential systematic errors. Our study led to final well-determined values ofbc(<sup>141</sup>Pr) = 4.44(4) fm,bc(<sup>142</sup>Nd) = 7.24(4) fm,bc(<sup>143</sup>Nd) = 17.51(6) fm,bc(<sup>144</sup>Nd) = 3.06(7) fm,bc(<sup>145</sup>Nd) = 10.40(12) fm,bc(<sup>146</sup>Nd) = 8.56(9) fm,bc(<sup>148</sup>Nd) = 4.44(13) fm,bc(<sup>150</sup>Nd) = 6.87(5) fm.bc(<sup>147</sup>Sm) = 6.68(5) fm,bc(<sup>148</sup>Sm) = 6.67(7) fm,bc(<sup>150</sup>Sm) = 10.05(10) fm,bc(<sup>152</sup>Sm) = -6.14(12) fm,bc(<sup>154</sup>Sm) = 9.34(9) fm,bc(<sup>153</sup>Eu) = 8.33(11) fm,bc(<sup>170</sup>Yb) = 4.83(3) fm,bc(<sup>170</sup>Yb) = 22.02(7) fm,bc(<sup>nat</sup>Nd) = 7.87(11) fm for thermal neutrons, and alsobc(<sup>nat</sup>Sm) = 5.29(5) fm for an incident neutron energy of 330.3(9) meV andbc(<sup>nat</sup>Eu) = 5.84(5) fm for an incident neutron energy of 168.10(5) meV. Based on the good precision and self-consistency of ourbcresults over so many isotopes, we advocate neutron Bragg powder diffraction as a method of choice for future studies to determine bound coherent neutron scattering lengths.

Journal of Physics Condensed MatterVol. 38(3)
Australian Nuclear Science and Technology Organisation (AU), Institut Laue-Langevin (FR), Saarland University (DE), Leipzig University (DE)
Openalex Percentile: Top 56%
Nuclear Physics and Applications
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