Florian Gehlhaar, Henry E Fischer, Hartmut Lemmel, Kristina Brix, Ralf Kautenburger, Thomas C Hansen, Vanessa Peterson, Holger Kohlmann
{"title":"用中子Bragg粉末衍射和中子干涉法重新研究锂及其同位素的束缚相干中子散射长度。","authors":"Florian Gehlhaar, Henry E Fischer, Hartmut Lemmel, Kristina Brix, Ralf Kautenburger, Thomas C Hansen, Vanessa Peterson, Holger Kohlmann","doi":"10.1088/1361-648X/add3a6","DOIUrl":null,"url":null,"abstract":"<p><p>The quality of neutron scattering studies relies upon accurately determined bound coherent neutron scattering lengths<i>b</i><sub>c</sub>, whose standard tabulated values can be in need of review. We have measured integrated Bragg peak intensities via neutron diffraction from LiF powders, as well as scattering-length densities via neutron interferometry on LiF aqueous solutions, to accurately redetermine the<i>b</i><sub>c</sub>values for the lithium isotopes<sup>6</sup>Li and<sup>7</sup>Li, as well as that for naturally occurring elemental Li as a mix of these two isotopes. As compared to earlier studies going back to 1986, our measurements make use of considerably improved instrumentation, and careful attention was given to the experimental procedure as well as to data analysis, in particular to aspects of systematic error. From the neutron diffraction measurements we obtain<i>b</i><sub>c</sub>(<sup>6</sup>Li)<sub>NPD</sub>= 2.27(2) fm,<i>b</i><sub>c</sub>(<sup>7</sup>Li)<sub>NPD</sub>= -2.28(2) fm and<i>b</i><sub>c</sub>(<sup>nat</sup>Li)<sub>NPD</sub>= -1.94(2) fm, in excellent agreement with our interferometry results of<i>b</i><sub>c</sub>(<sup>6</sup>Li)<sub>INT</sub>= 2.28(4) fm,<i>b</i><sub>c</sub>(<sup>7</sup>Li)<sub>INT</sub>= -2.28(3) fm and<i>b</i><sub>c</sub>(<sup>nat</sup>Li)<sub>INT</sub>= -1.93(3) fm, allowing to average them together and to propose recommended values of<i>b</i><sub>c</sub>(<sup>6</sup>Li)<sub>Rec</sub>. = 2.27(2) fm,<i>b</i><sub>c</sub>(<sup>7</sup>Li)<sub>Rec</sub>. = -2.28(2) fm and<i>b</i><sub>c</sub>(<sup>nat</sup>Li)<sub>Rec</sub>= -1.93(2) fm, where all values correspond to pure isotopes or the standard terrestrial isotopic composition of<sup>nat</sup>Li. Compared to standard literature values of<i>b</i><sub>c</sub>(<sup>6</sup>Li)<sub>Lit.</sub>= 2.0(1) fm,<i>b</i><sub>c</sub>(<sup>7</sup>Li)<sub>Lit.</sub>= -2.22(2) fm, and<i>b</i><sub>c</sub>(<sup>nat</sup>Li)<sub>Lit.</sub>= -1.90(3) fm, we note in particular that our recommended value for<i>b</i><sub>c</sub>(<sup>6</sup>Li) is 14% greater in magnitude, which is well outside of experimental uncertainties. Having obtained nearly identical results using two independent experimental techniques with qualitatively different possible sources of systematic error, we have confidence in our recommended<i>b</i><sub>c</sub>values. We discuss reasons for the observed discrepancies with respect to previously tabulated values, as well as the relative merits of the various methods to measure bound coherent neutron scattering lengths.</p>","PeriodicalId":16776,"journal":{"name":"Journal of Physics: Condensed Matter","volume":" ","pages":""},"PeriodicalIF":2.6000,"publicationDate":"2025-05-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Reinvestigation of the bound coherent neutron scattering lengths of lithium and its isotopes using neutron Bragg powder diffraction and neutron interferometry.\",\"authors\":\"Florian Gehlhaar, Henry E Fischer, Hartmut Lemmel, Kristina Brix, Ralf Kautenburger, Thomas C Hansen, Vanessa Peterson, Holger Kohlmann\",\"doi\":\"10.1088/1361-648X/add3a6\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>The quality of neutron scattering studies relies upon accurately determined bound coherent neutron scattering lengths<i>b</i><sub>c</sub>, whose standard tabulated values can be in need of review. We have measured integrated Bragg peak intensities via neutron diffraction from LiF powders, as well as scattering-length densities via neutron interferometry on LiF aqueous solutions, to accurately redetermine the<i>b</i><sub>c</sub>values for the lithium isotopes<sup>6</sup>Li and<sup>7</sup>Li, as well as that for naturally occurring elemental Li as a mix of these two isotopes. As compared to earlier studies going back to 1986, our measurements make use of considerably improved instrumentation, and careful attention was given to the experimental procedure as well as to data analysis, in particular to aspects of systematic error. From the neutron diffraction measurements we obtain<i>b</i><sub>c</sub>(<sup>6</sup>Li)<sub>NPD</sub>= 2.27(2) fm,<i>b</i><sub>c</sub>(<sup>7</sup>Li)<sub>NPD</sub>= -2.28(2) fm and<i>b</i><sub>c</sub>(<sup>nat</sup>Li)<sub>NPD</sub>= -1.94(2) fm, in excellent agreement with our interferometry results of<i>b</i><sub>c</sub>(<sup>6</sup>Li)<sub>INT</sub>= 2.28(4) fm,<i>b</i><sub>c</sub>(<sup>7</sup>Li)<sub>INT</sub>= -2.28(3) fm and<i>b</i><sub>c</sub>(<sup>nat</sup>Li)<sub>INT</sub>= -1.93(3) fm, allowing to average them together and to propose recommended values of<i>b</i><sub>c</sub>(<sup>6</sup>Li)<sub>Rec</sub>. = 2.27(2) fm,<i>b</i><sub>c</sub>(<sup>7</sup>Li)<sub>Rec</sub>. = -2.28(2) fm and<i>b</i><sub>c</sub>(<sup>nat</sup>Li)<sub>Rec</sub>= -1.93(2) fm, where all values correspond to pure isotopes or the standard terrestrial isotopic composition of<sup>nat</sup>Li. Compared to standard literature values of<i>b</i><sub>c</sub>(<sup>6</sup>Li)<sub>Lit.</sub>= 2.0(1) fm,<i>b</i><sub>c</sub>(<sup>7</sup>Li)<sub>Lit.</sub>= -2.22(2) fm, and<i>b</i><sub>c</sub>(<sup>nat</sup>Li)<sub>Lit.</sub>= -1.90(3) fm, we note in particular that our recommended value for<i>b</i><sub>c</sub>(<sup>6</sup>Li) is 14% greater in magnitude, which is well outside of experimental uncertainties. Having obtained nearly identical results using two independent experimental techniques with qualitatively different possible sources of systematic error, we have confidence in our recommended<i>b</i><sub>c</sub>values. We discuss reasons for the observed discrepancies with respect to previously tabulated values, as well as the relative merits of the various methods to measure bound coherent neutron scattering lengths.</p>\",\"PeriodicalId\":16776,\"journal\":{\"name\":\"Journal of Physics: Condensed Matter\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":2.6000,\"publicationDate\":\"2025-05-20\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physics: Condensed Matter\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1088/1361-648X/add3a6\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, CONDENSED MATTER\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics: Condensed Matter","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1088/1361-648X/add3a6","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, CONDENSED MATTER","Score":null,"Total":0}
Reinvestigation of the bound coherent neutron scattering lengths of lithium and its isotopes using neutron Bragg powder diffraction and neutron interferometry.
The quality of neutron scattering studies relies upon accurately determined bound coherent neutron scattering lengthsbc, whose standard tabulated values can be in need of review. We have measured integrated Bragg peak intensities via neutron diffraction from LiF powders, as well as scattering-length densities via neutron interferometry on LiF aqueous solutions, to accurately redetermine thebcvalues for the lithium isotopes6Li and7Li, as well as that for naturally occurring elemental Li as a mix of these two isotopes. As compared to earlier studies going back to 1986, our measurements make use of considerably improved instrumentation, and careful attention was given to the experimental procedure as well as to data analysis, in particular to aspects of systematic error. From the neutron diffraction measurements we obtainbc(6Li)NPD= 2.27(2) fm,bc(7Li)NPD= -2.28(2) fm andbc(natLi)NPD= -1.94(2) fm, in excellent agreement with our interferometry results ofbc(6Li)INT= 2.28(4) fm,bc(7Li)INT= -2.28(3) fm andbc(natLi)INT= -1.93(3) fm, allowing to average them together and to propose recommended values ofbc(6Li)Rec. = 2.27(2) fm,bc(7Li)Rec. = -2.28(2) fm andbc(natLi)Rec= -1.93(2) fm, where all values correspond to pure isotopes or the standard terrestrial isotopic composition ofnatLi. Compared to standard literature values ofbc(6Li)Lit.= 2.0(1) fm,bc(7Li)Lit.= -2.22(2) fm, andbc(natLi)Lit.= -1.90(3) fm, we note in particular that our recommended value forbc(6Li) is 14% greater in magnitude, which is well outside of experimental uncertainties. Having obtained nearly identical results using two independent experimental techniques with qualitatively different possible sources of systematic error, we have confidence in our recommendedbcvalues. We discuss reasons for the observed discrepancies with respect to previously tabulated values, as well as the relative merits of the various methods to measure bound coherent neutron scattering lengths.
期刊介绍：
Journal of Physics: Condensed Matter covers the whole of condensed matter physics including soft condensed matter and nanostructures. Papers may report experimental, theoretical and simulation studies. Note that papers must contain fundamental condensed matter science: papers reporting methods of materials preparation or properties of materials without novel condensed matter content will not be accepted.
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