{"title":"准二维有机金属 (EDT-TTF)4[Hg3I8]1-x (x = 0 和 0.027) 的光学研究--相位声子模型内的比较分析","authors":"B. V. Petrov, M. P. Volkov","doi":"10.1134/S0030400X2304015X","DOIUrl":null,"url":null,"abstract":"<p>Reflection spectra of quasi-two-dimensional organic conductors (EDT–TTF)<sub>4</sub>[Hg<sub>3</sub>I<sub>8</sub>]<sub>1–<i>x</i></sub>, are considered, which, depending on the composition, demonstrate different phase transitions: <i>x</i> = 0.027—metal–superconductor with <i>T</i><sub><i>c</i></sub> = 8.1 K, <i>x</i> = 0—metal–insulator at a temperature of <i>T <</i> 35 K. The polarized reflection spectra were analyzed using the “phase phonons” model, which takes into account the electronic-vibrational interaction. Using this model, the optical functions of both compounds were adequately described and the energy parameters of the π-electron system were obtained. It is shown that for the compound with <i>x</i> = 0.027 these parameters change monotonically with temperature, while for <i>x</i> = 0 they show a jump at the phase transition temperature. A comparison of the model parameter Δ (the value of the periodic potential) for crystals with different stoichiometric coefficients <i>x</i> = 0 and 0.027 was carried out and an assumption was made about the dependence of the periodic potential on the average charge of one EDT molecule.</p>","PeriodicalId":723,"journal":{"name":"Optics and Spectroscopy","volume":null,"pages":null},"PeriodicalIF":0.8000,"publicationDate":"2024-03-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Optical Studies of Quasi-Two-Dimensional Organic Metals (EDT–TTF)4[Hg3I8]1–x (x = 0 and 0.027)—Comparative Analysis within the Phase Phononsmodel\",\"authors\":\"B. V. Petrov, M. P. Volkov\",\"doi\":\"10.1134/S0030400X2304015X\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Reflection spectra of quasi-two-dimensional organic conductors (EDT–TTF)<sub>4</sub>[Hg<sub>3</sub>I<sub>8</sub>]<sub>1–<i>x</i></sub>, are considered, which, depending on the composition, demonstrate different phase transitions: <i>x</i> = 0.027—metal–superconductor with <i>T</i><sub><i>c</i></sub> = 8.1 K, <i>x</i> = 0—metal–insulator at a temperature of <i>T <</i> 35 K. The polarized reflection spectra were analyzed using the “phase phonons” model, which takes into account the electronic-vibrational interaction. Using this model, the optical functions of both compounds were adequately described and the energy parameters of the π-electron system were obtained. It is shown that for the compound with <i>x</i> = 0.027 these parameters change monotonically with temperature, while for <i>x</i> = 0 they show a jump at the phase transition temperature. A comparison of the model parameter Δ (the value of the periodic potential) for crystals with different stoichiometric coefficients <i>x</i> = 0 and 0.027 was carried out and an assumption was made about the dependence of the periodic potential on the average charge of one EDT molecule.</p>\",\"PeriodicalId\":723,\"journal\":{\"name\":\"Optics and Spectroscopy\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.8000,\"publicationDate\":\"2024-03-14\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Optics and Spectroscopy\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://link.springer.com/article/10.1134/S0030400X2304015X\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q4\",\"JCRName\":\"OPTICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Optics and Spectroscopy","FirstCategoryId":"101","ListUrlMain":"https://link.springer.com/article/10.1134/S0030400X2304015X","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q4","JCRName":"OPTICS","Score":null,"Total":0}
引用次数: 0
摘要
摘要 研究了准二维有机导体(EDT-TTF)4[Hg3I8]1-x 的反射光谱,根据组成的不同,它们表现出不同的相变:x = 0.027-金属-超导体,Tc = 8.1 K;x = 0-金属-绝缘体,温度为 T < 35 K。偏振反射光谱采用 "相声子 "模型进行分析,该模型考虑了电子-振动相互作用。利用该模型,两种化合物的光学函数都得到了充分的描述,并获得了 π 电子系统的能量参数。结果表明,对于 x = 0.027 的化合物,这些参数随温度的变化呈单调变化,而对于 x = 0 的化合物,这些参数在相变温度时会出现跃变。对具有不同化学计量系数 x = 0 和 0.027 的晶体的模型参数 Δ(周期电势值)进行了比较,并假设周期电势取决于一个 EDT 分子的平均电荷。
Optical Studies of Quasi-Two-Dimensional Organic Metals (EDT–TTF)4[Hg3I8]1–x (x = 0 and 0.027)—Comparative Analysis within the Phase Phononsmodel
Reflection spectra of quasi-two-dimensional organic conductors (EDT–TTF)4[Hg3I8]1–x, are considered, which, depending on the composition, demonstrate different phase transitions: x = 0.027—metal–superconductor with Tc = 8.1 K, x = 0—metal–insulator at a temperature of T < 35 K. The polarized reflection spectra were analyzed using the “phase phonons” model, which takes into account the electronic-vibrational interaction. Using this model, the optical functions of both compounds were adequately described and the energy parameters of the π-electron system were obtained. It is shown that for the compound with x = 0.027 these parameters change monotonically with temperature, while for x = 0 they show a jump at the phase transition temperature. A comparison of the model parameter Δ (the value of the periodic potential) for crystals with different stoichiometric coefficients x = 0 and 0.027 was carried out and an assumption was made about the dependence of the periodic potential on the average charge of one EDT molecule.
期刊介绍:
Optics and Spectroscopy (Optika i spektroskopiya), founded in 1956, presents original and review papers in various fields of modern optics and spectroscopy in the entire wavelength range from radio waves to X-rays. Topics covered include problems of theoretical and experimental spectroscopy of atoms, molecules, and condensed state, lasers and the interaction of laser radiation with matter, physical and geometrical optics, holography, and physical principles of optical instrument making.