{"title":"利用低温光学显微镜揭示电荷转移Fe2Co2可切换分子材料的相变动力学。","authors":"Buqin Xu, Nour-El-Islam Belmouri, Longhe Li, Sadiya Sadiya, Guillaume Bouchez, Mouhamadou Sy, Geoffrey Gontard, Kamel Boukheddaden*, Yanling Li* and Rodrigue Lescouëzec*, ","doi":"10.1021/jacs.5c04906","DOIUrl":null,"url":null,"abstract":"<p >Understanding the phase transition mechanism in switchable materials is crucial to optimizing their properties. In this study, we present the thermal electron transfer-coupled spin transition (ETCST) mechanism, revealed through the cryogenic optical microscopy (OM) measurements on a cyanide-bridged square complex, {[Fe(Tp)(CN)<sub>3</sub>]<sub>2</sub>[Co(vbik)<sub>2</sub>]<sub>2</sub>}·2ClO<sub>4</sub>·2CH<sub>2</sub>Cl<sub>2</sub> (<b>1·ClO</b><sub><b>4</b></sub>), where Tp is tris(pyrazolyl)borate and vbik is bis(1-vinylimidazolyl)ketone. A one-step thermal ETCST of <b>1·ClO</b><sub><b>4</b></sub> is observed using conventional techniques such as single-crystal X-ray diffraction (SC-XRD) and bulk sample magnetic measurements. The ETCST is cooperative, with quite different transition temperatures for the single crystal (<i>T</i><sub>1/2</sub>↑ = 251.5 K for heating and <i>T</i><sub>1/2</sub>↓ = 243.5 K) and bulk sample (<i>T</i><sub>1/2</sub>↑ = 273 K and <i>T</i><sub>1/2</sub>↓ = 255 K). In contrast, the direct visualization of the thermal ETCST in the single crystal of <b>1·ClO</b><sub><b>4</b></sub> through OM and the subsequent image analysis disclose for the first time a phase transition of unexpected complexity. The ETCST progresses in three steps along the <i>a</i>, <i>b</i>, and <i>c</i> axes: (i) Initially, the strip domains form and rapidly extend along the <i>a</i>-axis. (ii) These domains then gradually widen in the <i>b</i>-axis covering the entire <i>ab</i> layer. (iii) The final step involves a layer-by-layer extension of ETCST along the <i>c</i>-axis. Structural analysis of <b>1·ClO</b><sub><b>4</b></sub> reveals that two types of intermolecular interactions govern the two preferential propagation directions of ETCST. The first type, mediated by the ClO<sub>4</sub><sup>–</sup> anion, drives the rapid propagation of ETCST along the <i>a</i> axis, occurring so rapidly that conventional methods like magnetometry and SC-XRD are unable to detect it. The second type, along the <i>b</i> axis, involves the π–π stacking of vbik ligands, which contributes to the slower ETCST propagation in this direction. This mechanistic insight into the anisotropic propagation patterns of ETCST in <b>1·ClO</b><sub><b>4</b></sub> underscores the role of intermolecular interactions in modulating the dynamics of molecular switching.</p>","PeriodicalId":49,"journal":{"name":"Journal of the American Chemical Society","volume":"147 31","pages":"27506–27514"},"PeriodicalIF":15.6000,"publicationDate":"2025-07-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Unveiling Phase Transition Dynamics Using Cryogenic Optical Microscopy in a Charge-Transfer Fe2Co2 Switchable Molecular Material\",\"authors\":\"Buqin Xu, Nour-El-Islam Belmouri, Longhe Li, Sadiya Sadiya, Guillaume Bouchez, Mouhamadou Sy, Geoffrey Gontard, Kamel Boukheddaden*, Yanling Li* and Rodrigue Lescouëzec*, \",\"doi\":\"10.1021/jacs.5c04906\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p >Understanding the phase transition mechanism in switchable materials is crucial to optimizing their properties. In this study, we present the thermal electron transfer-coupled spin transition (ETCST) mechanism, revealed through the cryogenic optical microscopy (OM) measurements on a cyanide-bridged square complex, {[Fe(Tp)(CN)<sub>3</sub>]<sub>2</sub>[Co(vbik)<sub>2</sub>]<sub>2</sub>}·2ClO<sub>4</sub>·2CH<sub>2</sub>Cl<sub>2</sub> (<b>1·ClO</b><sub><b>4</b></sub>), where Tp is tris(pyrazolyl)borate and vbik is bis(1-vinylimidazolyl)ketone. A one-step thermal ETCST of <b>1·ClO</b><sub><b>4</b></sub> is observed using conventional techniques such as single-crystal X-ray diffraction (SC-XRD) and bulk sample magnetic measurements. The ETCST is cooperative, with quite different transition temperatures for the single crystal (<i>T</i><sub>1/2</sub>↑ = 251.5 K for heating and <i>T</i><sub>1/2</sub>↓ = 243.5 K) and bulk sample (<i>T</i><sub>1/2</sub>↑ = 273 K and <i>T</i><sub>1/2</sub>↓ = 255 K). In contrast, the direct visualization of the thermal ETCST in the single crystal of <b>1·ClO</b><sub><b>4</b></sub> through OM and the subsequent image analysis disclose for the first time a phase transition of unexpected complexity. The ETCST progresses in three steps along the <i>a</i>, <i>b</i>, and <i>c</i> axes: (i) Initially, the strip domains form and rapidly extend along the <i>a</i>-axis. (ii) These domains then gradually widen in the <i>b</i>-axis covering the entire <i>ab</i> layer. (iii) The final step involves a layer-by-layer extension of ETCST along the <i>c</i>-axis. Structural analysis of <b>1·ClO</b><sub><b>4</b></sub> reveals that two types of intermolecular interactions govern the two preferential propagation directions of ETCST. The first type, mediated by the ClO<sub>4</sub><sup>–</sup> anion, drives the rapid propagation of ETCST along the <i>a</i> axis, occurring so rapidly that conventional methods like magnetometry and SC-XRD are unable to detect it. The second type, along the <i>b</i> axis, involves the π–π stacking of vbik ligands, which contributes to the slower ETCST propagation in this direction. This mechanistic insight into the anisotropic propagation patterns of ETCST in <b>1·ClO</b><sub><b>4</b></sub> underscores the role of intermolecular interactions in modulating the dynamics of molecular switching.</p>\",\"PeriodicalId\":49,\"journal\":{\"name\":\"Journal of the American Chemical Society\",\"volume\":\"147 31\",\"pages\":\"27506–27514\"},\"PeriodicalIF\":15.6000,\"publicationDate\":\"2025-07-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of the American Chemical Society\",\"FirstCategoryId\":\"92\",\"ListUrlMain\":\"https://pubs.acs.org/doi/10.1021/jacs.5c04906\",\"RegionNum\":1,\"RegionCategory\":\"化学\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"CHEMISTRY, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of the American Chemical Society","FirstCategoryId":"92","ListUrlMain":"https://pubs.acs.org/doi/10.1021/jacs.5c04906","RegionNum":1,"RegionCategory":"化学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
Unveiling Phase Transition Dynamics Using Cryogenic Optical Microscopy in a Charge-Transfer Fe2Co2 Switchable Molecular Material
Understanding the phase transition mechanism in switchable materials is crucial to optimizing their properties. In this study, we present the thermal electron transfer-coupled spin transition (ETCST) mechanism, revealed through the cryogenic optical microscopy (OM) measurements on a cyanide-bridged square complex, {[Fe(Tp)(CN)3]2[Co(vbik)2]2}·2ClO4·2CH2Cl2 (1·ClO4), where Tp is tris(pyrazolyl)borate and vbik is bis(1-vinylimidazolyl)ketone. A one-step thermal ETCST of 1·ClO4 is observed using conventional techniques such as single-crystal X-ray diffraction (SC-XRD) and bulk sample magnetic measurements. The ETCST is cooperative, with quite different transition temperatures for the single crystal (T1/2↑ = 251.5 K for heating and T1/2↓ = 243.5 K) and bulk sample (T1/2↑ = 273 K and T1/2↓ = 255 K). In contrast, the direct visualization of the thermal ETCST in the single crystal of 1·ClO4 through OM and the subsequent image analysis disclose for the first time a phase transition of unexpected complexity. The ETCST progresses in three steps along the a, b, and c axes: (i) Initially, the strip domains form and rapidly extend along the a-axis. (ii) These domains then gradually widen in the b-axis covering the entire ab layer. (iii) The final step involves a layer-by-layer extension of ETCST along the c-axis. Structural analysis of 1·ClO4 reveals that two types of intermolecular interactions govern the two preferential propagation directions of ETCST. The first type, mediated by the ClO4– anion, drives the rapid propagation of ETCST along the a axis, occurring so rapidly that conventional methods like magnetometry and SC-XRD are unable to detect it. The second type, along the b axis, involves the π–π stacking of vbik ligands, which contributes to the slower ETCST propagation in this direction. This mechanistic insight into the anisotropic propagation patterns of ETCST in 1·ClO4 underscores the role of intermolecular interactions in modulating the dynamics of molecular switching.
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