StanisŁaw K. Hoffmann, Wojciech Hilczer, Janina Goslar
{"title":"铜(II)掺杂硒酸三甘氨酸晶体的电子自旋-晶格弛豫和德拜温度","authors":"StanisŁaw K. Hoffmann, Wojciech Hilczer, Janina Goslar","doi":"10.1006/jmra.1996.0171","DOIUrl":null,"url":null,"abstract":"<div><p>Single-crystal rotational data of CW-EPR and two-pulse field-swept ESE collected at room and low temperatures lead to the spin-Hamiltonian parameters<em>g</em><sub><em>z</em></sub>= 2.2596,<em>g</em><sub><em>y</em></sub>= 2.0647,<em>g</em><sub><em>x</em></sub>= 2.0529,<em>A</em><sub><em>z</em></sub>= 151.2 × 10<sup>−4</sup>cm<sup>−1</sup>,<em>A</em><sub><em>y</em></sub>= 2.5 × 10<sup>−4</sup>cm<sup>−1</sup>, and<em>A</em><sub><em>x</em></sub>= 42.2 × 10<sup>−4</sup>cm<sup>−1</sup>which are temperature independent. The parameters and Cu<sup>2+</sup>ion site in the crystal unit cell are very similar to those in the triglycine sulfate crystal. Electron-spin-echo measurements of the spin–lattice relaxation time<em>T</em><sub>1</sub>in the temperature range 4.2–90 K gave identical results for inversion- and saturation-recovery methods, indicating a negligible spectral-diffusion contribution. The<em>T</em><sub>1</sub>decreases from 275 μs at 15 K to 1.7 μs at 83 K and the temperature dependence is governed by the direct (one-phonon) process at low temperatures and two-phonon Raman process at higher temperatures. A new analytical form of the<em>I</em><sub>8</sub>transport integral of the Raman term is proposed. The best fit to the theoretical expression was found for the Debye temperature ϑ<sub>D</sub>= 168 ± 3 K which is comparable to ϑ<sub>D</sub>= 171 K calculated from the elastic constants of the crystal.</p></div>","PeriodicalId":16165,"journal":{"name":"Journal of Magnetic Resonance, Series A","volume":"122 1","pages":"Pages 37-41"},"PeriodicalIF":0.0000,"publicationDate":"1996-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1006/jmra.1996.0171","citationCount":"16","resultStr":"{\"title\":\"EPR, Electron Spin–Lattice Relaxation, and Debye Temperature of Cu(II)-Doped Triglycine Selenate Crystal\",\"authors\":\"StanisŁaw K. Hoffmann, Wojciech Hilczer, Janina Goslar\",\"doi\":\"10.1006/jmra.1996.0171\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>Single-crystal rotational data of CW-EPR and two-pulse field-swept ESE collected at room and low temperatures lead to the spin-Hamiltonian parameters<em>g</em><sub><em>z</em></sub>= 2.2596,<em>g</em><sub><em>y</em></sub>= 2.0647,<em>g</em><sub><em>x</em></sub>= 2.0529,<em>A</em><sub><em>z</em></sub>= 151.2 × 10<sup>−4</sup>cm<sup>−1</sup>,<em>A</em><sub><em>y</em></sub>= 2.5 × 10<sup>−4</sup>cm<sup>−1</sup>, and<em>A</em><sub><em>x</em></sub>= 42.2 × 10<sup>−4</sup>cm<sup>−1</sup>which are temperature independent. The parameters and Cu<sup>2+</sup>ion site in the crystal unit cell are very similar to those in the triglycine sulfate crystal. Electron-spin-echo measurements of the spin–lattice relaxation time<em>T</em><sub>1</sub>in the temperature range 4.2–90 K gave identical results for inversion- and saturation-recovery methods, indicating a negligible spectral-diffusion contribution. The<em>T</em><sub>1</sub>decreases from 275 μs at 15 K to 1.7 μs at 83 K and the temperature dependence is governed by the direct (one-phonon) process at low temperatures and two-phonon Raman process at higher temperatures. A new analytical form of the<em>I</em><sub>8</sub>transport integral of the Raman term is proposed. The best fit to the theoretical expression was found for the Debye temperature ϑ<sub>D</sub>= 168 ± 3 K which is comparable to ϑ<sub>D</sub>= 171 K calculated from the elastic constants of the crystal.</p></div>\",\"PeriodicalId\":16165,\"journal\":{\"name\":\"Journal of Magnetic Resonance, Series A\",\"volume\":\"122 1\",\"pages\":\"Pages 37-41\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1996-09-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://sci-hub-pdf.com/10.1006/jmra.1996.0171\",\"citationCount\":\"16\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Magnetic Resonance, Series A\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S1064185896901710\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Magnetic Resonance, Series A","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S1064185896901710","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
EPR, Electron Spin–Lattice Relaxation, and Debye Temperature of Cu(II)-Doped Triglycine Selenate Crystal
Single-crystal rotational data of CW-EPR and two-pulse field-swept ESE collected at room and low temperatures lead to the spin-Hamiltonian parametersgz= 2.2596,gy= 2.0647,gx= 2.0529,Az= 151.2 × 10−4cm−1,Ay= 2.5 × 10−4cm−1, andAx= 42.2 × 10−4cm−1which are temperature independent. The parameters and Cu2+ion site in the crystal unit cell are very similar to those in the triglycine sulfate crystal. Electron-spin-echo measurements of the spin–lattice relaxation timeT1in the temperature range 4.2–90 K gave identical results for inversion- and saturation-recovery methods, indicating a negligible spectral-diffusion contribution. TheT1decreases from 275 μs at 15 K to 1.7 μs at 83 K and the temperature dependence is governed by the direct (one-phonon) process at low temperatures and two-phonon Raman process at higher temperatures. A new analytical form of theI8transport integral of the Raman term is proposed. The best fit to the theoretical expression was found for the Debye temperature ϑD= 168 ± 3 K which is comparable to ϑD= 171 K calculated from the elastic constants of the crystal.