Sandra S. Eaton, Debbie G. Mitchell, Gareth R. Eaton
{"title":"群青蓝和青金石中 S3-的电子旋光弛豫","authors":"Sandra S. Eaton, Debbie G. Mitchell, Gareth R. Eaton","doi":"10.1007/s00723-024-01716-1","DOIUrl":null,"url":null,"abstract":"<p>The blue color that has made lazurite (lapis lazuli) a prized mineral is due to the same S<sub>3</sub><sup>−</sup> radical that is in synthetic ultramarine blue (UMB), which has been proposed as a CW EPR standard. Continuous wave and pulsed EPR spectra and relaxation times of S<sub>3</sub><sup>−</sup> are compared for three commercial sources of synthetic UMB, for samples of lapis lazuli from Afghanistan, Chile, Colorado USA, and Pakistan, and a solution in DMSO:dioxane. The spin concentrations in the UMB samples were high, in the range of 3 × 10<sup>20</sup> to 5 × 10<sup>20</sup> spins/g. The field-swept echo-detected spectra of UMB samples have lineshapes at 4.2 K that depend on the field at which phase adjustment is performed, indicating strong spin–spin interaction. The spectra of the minerals included large spectral contributions from Mn<sup>2+</sup>, in addition to S<sub>3</sub><sup>−</sup> for which the concentrations were 6 × 10<sup>18</sup> to 2.9 × 10<sup>19</sup> spins/g. Features in the spin-echo-detected spectra attributed to forbidden Mn<sup>2+</sup> transitions were confirmed by comparison with Mn<sup>2+</sup> spectra in CaO powder. Large distributions in relaxation times caused derived results to depend strongly on the experimental acquisition windows for echo decay and inversion-recovery curves. Short-phase memory times are attributed to spin–spin interactions and to motion of the S<sub>3</sub><sup>−</sup> in the lattices. Relatively weak temperature dependence of spin lattice relaxation rates below or around 25 K is attributed to substantial spin–spin interaction and cross relaxation. The strong spin–spin interaction is not present for 0.4 mM S<sub>3</sub><sup>−</sup> in DMSO:dioxane. The shorter <i>T</i><sub>1</sub> for S<sub>3</sub><sup>−</sup> than for SO<sub>2</sub><sup>−</sup> or SO<sub>3</sub><sup>−</sup> is attributed to stronger spin–orbit coupling.</p>","PeriodicalId":469,"journal":{"name":"Applied Magnetic Resonance","volume":"316 1","pages":""},"PeriodicalIF":1.1000,"publicationDate":"2024-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Electron-Spin Relaxation of S3− in Ultramarine Blue and Lapis Lazuli\",\"authors\":\"Sandra S. Eaton, Debbie G. Mitchell, Gareth R. Eaton\",\"doi\":\"10.1007/s00723-024-01716-1\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>The blue color that has made lazurite (lapis lazuli) a prized mineral is due to the same S<sub>3</sub><sup>−</sup> radical that is in synthetic ultramarine blue (UMB), which has been proposed as a CW EPR standard. Continuous wave and pulsed EPR spectra and relaxation times of S<sub>3</sub><sup>−</sup> are compared for three commercial sources of synthetic UMB, for samples of lapis lazuli from Afghanistan, Chile, Colorado USA, and Pakistan, and a solution in DMSO:dioxane. The spin concentrations in the UMB samples were high, in the range of 3 × 10<sup>20</sup> to 5 × 10<sup>20</sup> spins/g. The field-swept echo-detected spectra of UMB samples have lineshapes at 4.2 K that depend on the field at which phase adjustment is performed, indicating strong spin–spin interaction. The spectra of the minerals included large spectral contributions from Mn<sup>2+</sup>, in addition to S<sub>3</sub><sup>−</sup> for which the concentrations were 6 × 10<sup>18</sup> to 2.9 × 10<sup>19</sup> spins/g. Features in the spin-echo-detected spectra attributed to forbidden Mn<sup>2+</sup> transitions were confirmed by comparison with Mn<sup>2+</sup> spectra in CaO powder. Large distributions in relaxation times caused derived results to depend strongly on the experimental acquisition windows for echo decay and inversion-recovery curves. Short-phase memory times are attributed to spin–spin interactions and to motion of the S<sub>3</sub><sup>−</sup> in the lattices. Relatively weak temperature dependence of spin lattice relaxation rates below or around 25 K is attributed to substantial spin–spin interaction and cross relaxation. The strong spin–spin interaction is not present for 0.4 mM S<sub>3</sub><sup>−</sup> in DMSO:dioxane. The shorter <i>T</i><sub>1</sub> for S<sub>3</sub><sup>−</sup> than for SO<sub>2</sub><sup>−</sup> or SO<sub>3</sub><sup>−</sup> is attributed to stronger spin–orbit coupling.</p>\",\"PeriodicalId\":469,\"journal\":{\"name\":\"Applied Magnetic Resonance\",\"volume\":\"316 1\",\"pages\":\"\"},\"PeriodicalIF\":1.1000,\"publicationDate\":\"2024-09-10\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Applied Magnetic Resonance\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1007/s00723-024-01716-1\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"PHYSICS, ATOMIC, MOLECULAR & CHEMICAL\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Applied Magnetic Resonance","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1007/s00723-024-01716-1","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"PHYSICS, ATOMIC, MOLECULAR & CHEMICAL","Score":null,"Total":0}
Electron-Spin Relaxation of S3− in Ultramarine Blue and Lapis Lazuli
The blue color that has made lazurite (lapis lazuli) a prized mineral is due to the same S3− radical that is in synthetic ultramarine blue (UMB), which has been proposed as a CW EPR standard. Continuous wave and pulsed EPR spectra and relaxation times of S3− are compared for three commercial sources of synthetic UMB, for samples of lapis lazuli from Afghanistan, Chile, Colorado USA, and Pakistan, and a solution in DMSO:dioxane. The spin concentrations in the UMB samples were high, in the range of 3 × 1020 to 5 × 1020 spins/g. The field-swept echo-detected spectra of UMB samples have lineshapes at 4.2 K that depend on the field at which phase adjustment is performed, indicating strong spin–spin interaction. The spectra of the minerals included large spectral contributions from Mn2+, in addition to S3− for which the concentrations were 6 × 1018 to 2.9 × 1019 spins/g. Features in the spin-echo-detected spectra attributed to forbidden Mn2+ transitions were confirmed by comparison with Mn2+ spectra in CaO powder. Large distributions in relaxation times caused derived results to depend strongly on the experimental acquisition windows for echo decay and inversion-recovery curves. Short-phase memory times are attributed to spin–spin interactions and to motion of the S3− in the lattices. Relatively weak temperature dependence of spin lattice relaxation rates below or around 25 K is attributed to substantial spin–spin interaction and cross relaxation. The strong spin–spin interaction is not present for 0.4 mM S3− in DMSO:dioxane. The shorter T1 for S3− than for SO2− or SO3− is attributed to stronger spin–orbit coupling.
期刊介绍:
Applied Magnetic Resonance provides an international forum for the application of magnetic resonance in physics, chemistry, biology, medicine, geochemistry, ecology, engineering, and related fields.
The contents include articles with a strong emphasis on new applications, and on new experimental methods. Additional features include book reviews and Letters to the Editor.