Electrically Controlled Quantum Transition to an Anomalous Metal in 2D AITranslate
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The mechanism through which superconductivity is destroyed upon controlled disordering often holds the key to understanding the mechanism of the emergence of superconductivity. Here, we demonstrate an in-situ mechanism to control the fraction of disorder in a 2D superconductor. By controlling an electric field VG, we created an assembly of segregated superconducting nano-islands and varied the interisland distance to accomplish a quantum phase transition from a superconducting phase to a strange quantum anomalous metallic (QAM) phase at LaVO3/SrTiO3 interfaces. In the QAM phase, the resistivity dropped below a critical temperature (TCM) as if the system was approaching superconductivity and then saturated, indicating the destruction of global phase coherence and the emergence of a phase where metal-like transport of Bosons (a Bose metal) becomes a possibility. The unprecedented control over the island size is obtained through the control of nanometer-scale ferroelectric domains formed in the SrTiO3 side of the interface due to a low-temperature structural phase transition.
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DOI:https://doi.org/10.1021/acsaelm.3c00624
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The mechanism through which superconductivity is destroyed upon controlled disordering often holds the key to understanding the mechanism of the emergence of superconductivity. Here, we demonstrate an in-situ mechanism to control the fraction of disorder in a 2D superconductor. By controlling an electric field VG, we created an assembly of segregated superconducting nano-islands and varied the interisland distance to accomplish a quantum phase transition from a superconducting phase to a strange quantum anomalous metallic (QAM) phase at LaVO3/SrTiO3 interfaces. In the QAM phase, the resistivity dropped below a critical temperature (TCM) as if the system was approaching superconductivity and then saturated, indicating the destruction of global phase coherence and the emergence of a phase where metal-like transport of Bosons (a Bose metal) becomes a possibility. The unprecedented control over the island size is obtained through the control of nanometer-scale ferroelectric domains formed in the SrTiO3 side of the interface due to a low-temperature structural phase transition.
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| GB/T 7714-2015 | [1] Soumyadip Halder, Mona Garg, Shreekant Gawande, et al. ACS Applied Electronic Materials, 2023(5). DOI:10.1021/acsaelm.3c00624. |
| MLA | [1] Soumyadip Halder, et al., ACS Applied Electronic Materials, no. 5, 2023, https://doi.org/10.1021/acsaelm.3c00624. |
| APA | [1] Soumyadip Halder, Mona Garg, Shreekant Gawande, Nikhlesh Singh Mehta, Anamika Kumari, Suvankar Chakraverty, Sanjeev Kumar, & Goutam Sheet. (2023). ACS Applied Electronic Materials(5). https://doi.org/10.1021/acsaelm.3c00624 |
| IEEE | [1] Soumyadip Halder, Mona Garg, Shreekant Gawande, Nikhlesh Singh Mehta, Anamika Kumari, Suvankar Chakraverty, Sanjeev Kumar, and Goutam Sheet, ACS Applied Electronic Materials, no. 5, 2023, doi: 10.1021/acsaelm.3c00624. keywords: {oxide 2DEGs LaVO3/SrTiO3 interfaces superconductivity anomalous metal ferroelectricity networkresistor model} |
