Avital Fried, Ouriel Gotesdyner, Irena Feldman, Amit Kanigel, Amos Sharoni
{"title":"1T-TaS2 块状晶体中的斜坡反向记忆","authors":"Avital Fried, Ouriel Gotesdyner, Irena Feldman, Amit Kanigel, Amos Sharoni","doi":"arxiv-2409.11977","DOIUrl":null,"url":null,"abstract":"The ramp reversal memory (RRM) is a non-volatile memory effect previously\nobserved in correlated oxides exhibiting temperature-driven metal-insulator\ntransitions (MITs). In essence, when a system displaying RRM is heated to a\nspecific temperature within the MIT regime - where metallic and insulating\ndomains coexist - and then cooled by reversing the temperature ramp, the\nresistance increases in the subsequent heating cycle. Crucially, this increase\noccurs only in the vicinity of the reversal temperature, indicating that the\nsystem 'remembers' this temperature. However, this memory is erased in the next\nheating loop. While such an effect could potentially manifest in various\nsystems, to date, it has only been reported in thin films of correlated\ntransition metal oxides, including VO2, V2O3, and NdNiO3. In this work, we\nreport the observation of RRM in macroscopic crystals of the layered material\n1T-TaS2, which undergoes an MIT near 190 K along charge-density wave\ntransitions. Our findings provide compelling evidence that RRM is a general\nphenomenon, extending beyond the previously studied oxides. Interestingly, the\nRRM in TaS2 displays significantly different characteristics: it is observed\nwhen reversing from cooling to heating (as opposed to heating to cooling), and\nits magnitude - representing the 'strength' of the memory - is nearly an order\nof magnitude larger than in correlated oxides. While we discuss potential\nmechanisms for the RRM in TaS2, a comprehensive first-principles model is still\nlacking. We hope that this study will prompt further investigation into the\nunderlying mechanisms of ramp reversal memory, enhancing our understanding of\nthis intriguing phenomenon.","PeriodicalId":501171,"journal":{"name":"arXiv - PHYS - Strongly Correlated Electrons","volume":"30 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Ramp reversal memory in bulk crystals of 1T-TaS2\",\"authors\":\"Avital Fried, Ouriel Gotesdyner, Irena Feldman, Amit Kanigel, Amos Sharoni\",\"doi\":\"arxiv-2409.11977\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The ramp reversal memory (RRM) is a non-volatile memory effect previously\\nobserved in correlated oxides exhibiting temperature-driven metal-insulator\\ntransitions (MITs). In essence, when a system displaying RRM is heated to a\\nspecific temperature within the MIT regime - where metallic and insulating\\ndomains coexist - and then cooled by reversing the temperature ramp, the\\nresistance increases in the subsequent heating cycle. Crucially, this increase\\noccurs only in the vicinity of the reversal temperature, indicating that the\\nsystem 'remembers' this temperature. However, this memory is erased in the next\\nheating loop. While such an effect could potentially manifest in various\\nsystems, to date, it has only been reported in thin films of correlated\\ntransition metal oxides, including VO2, V2O3, and NdNiO3. In this work, we\\nreport the observation of RRM in macroscopic crystals of the layered material\\n1T-TaS2, which undergoes an MIT near 190 K along charge-density wave\\ntransitions. Our findings provide compelling evidence that RRM is a general\\nphenomenon, extending beyond the previously studied oxides. Interestingly, the\\nRRM in TaS2 displays significantly different characteristics: it is observed\\nwhen reversing from cooling to heating (as opposed to heating to cooling), and\\nits magnitude - representing the 'strength' of the memory - is nearly an order\\nof magnitude larger than in correlated oxides. While we discuss potential\\nmechanisms for the RRM in TaS2, a comprehensive first-principles model is still\\nlacking. We hope that this study will prompt further investigation into the\\nunderlying mechanisms of ramp reversal memory, enhancing our understanding of\\nthis intriguing phenomenon.\",\"PeriodicalId\":501171,\"journal\":{\"name\":\"arXiv - PHYS - Strongly Correlated Electrons\",\"volume\":\"30 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-18\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Strongly Correlated Electrons\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.11977\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Strongly Correlated Electrons","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.11977","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The ramp reversal memory (RRM) is a non-volatile memory effect previously
observed in correlated oxides exhibiting temperature-driven metal-insulator
transitions (MITs). In essence, when a system displaying RRM is heated to a
specific temperature within the MIT regime - where metallic and insulating
domains coexist - and then cooled by reversing the temperature ramp, the
resistance increases in the subsequent heating cycle. Crucially, this increase
occurs only in the vicinity of the reversal temperature, indicating that the
system 'remembers' this temperature. However, this memory is erased in the next
heating loop. While such an effect could potentially manifest in various
systems, to date, it has only been reported in thin films of correlated
transition metal oxides, including VO2, V2O3, and NdNiO3. In this work, we
report the observation of RRM in macroscopic crystals of the layered material
1T-TaS2, which undergoes an MIT near 190 K along charge-density wave
transitions. Our findings provide compelling evidence that RRM is a general
phenomenon, extending beyond the previously studied oxides. Interestingly, the
RRM in TaS2 displays significantly different characteristics: it is observed
when reversing from cooling to heating (as opposed to heating to cooling), and
its magnitude - representing the 'strength' of the memory - is nearly an order
of magnitude larger than in correlated oxides. While we discuss potential
mechanisms for the RRM in TaS2, a comprehensive first-principles model is still
lacking. We hope that this study will prompt further investigation into the
underlying mechanisms of ramp reversal memory, enhancing our understanding of
this intriguing phenomenon.