1T-TaS2 块状晶体中的斜坡反向记忆

Avital Fried, Ouriel Gotesdyner, Irena Feldman, Amit Kanigel, Amos Sharoni
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引用次数: 0

摘要

斜坡反向记忆(RRM)是一种非易失性记忆效应,以前曾在表现出温度驱动的金属-绝缘转变(MIT)的相关氧化物中观察到过。从本质上讲,当显示 RRM 的系统被加热到 MIT 体系内的特定温度(金属和绝缘域共存),然后通过反向温度斜坡进行冷却时,电阻会在随后的加热循环中增加。重要的是,这种增加只发生在逆转温度附近,表明系统 "记住 "了这个温度。然而,这种记忆会在下一个加热循环中被消除。虽然这种效应有可能在各种系统中表现出来,但迄今为止,只有相关过渡金属氧化物薄膜中出现过这种现象,包括 VO2、V2O3 和 NdNiO3。在这项工作中,我们报告了在层状材料1T-TaS2的宏观晶体中观察到的RRM,该晶体在190 K附近沿着电荷密度波转变发生了MIT。我们的研究结果提供了令人信服的证据,证明RRM是一种普遍现象,其范围超出了之前研究的氧化物。有趣的是,TaS2 中的 RRM 显示出明显不同的特征:它是在从冷却到加热(而不是从加热到冷却)的逆转过程中观察到的,而且其幅度(代表记忆的 "强度")几乎比相关氧化物中的大一个数量级。虽然我们讨论了TaS2中RRM的潜在机制,但仍然缺乏一个全面的第一原理模型。我们希望这项研究能促使我们进一步研究斜坡反向记忆的基本机制,从而加深我们对这一有趣现象的理解。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Ramp reversal memory in bulk crystals of 1T-TaS2
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.
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