Pressure-induced superconductivity in SnSb2Te4
At a Glance
Section titled âAt a Glanceâ| Metadata | Details |
|---|---|
| Publication Date | 2020-02-17 |
| Journal | Journal of Physics Condensed Matter |
| Authors | Peng Song, Ryo Matsumoto, Zhufeng Hou, Shintaro Adachi, Hiroshi Hara |
| Institutions | National Institute for Materials Science, Fujian Institute of Research on the Structure of Matter |
| Citations | 12 |
| Analysis | Full AI Review Included |
Executive Summary
Section titled âExecutive SummaryâThis study reports the discovery and characterization of pressure-induced superconductivity in the phase change material (PCM) SnSb2Te4, providing a new avenue for exploring superconducting properties in chalcogenide compounds.
- New Superconductor: SnSb2Te4, typically a narrow-gap semiconductor (~0.26 eV), exhibits superconductivity when subjected to high pressure.
- Pressure-Induced Transition: Applied pressure causes a transition to metallic behavior, with the Fermi level crossing the valence bands at 10 GPa.
- Critical Temperature (Tc): Superconductivity onset (Tconset) was first detected at 2.1 K under 8.1 GPa.
- Maximum Performance: The maximum Tconset achieved was 7.4 K under the highest measured pressure of 32.6 GPa.
- Mechanism Insight: First-principles calculations suggest that pressure shrinks the Sn-Te and Sb-Te bond lengths, shifting anti-bonding states toward higher energy, which decreases the band gap and facilitates electron-phonon coupling (BCS mechanism).
- Material Potential: The high calculated Debye temperature (ÎR â 320 K) supports the materialâs potential for superconductivity under favorable conditions.
Technical Specifications
Section titled âTechnical Specificationsâ| Parameter | Value | Unit | Context |
|---|---|---|---|
| Maximum Superconducting Tc (onset) | 7.4 | K | Measured at 32.6 GPa |
| Minimum Pressure for Tc (onset) | 8.1 | GPa | Tc = 2.1 K |
| Pressure for Zero Resistivity (Tczero) | 10.2 | GPa | Tczero â 2.2 K |
| Maximum Pressure Measured | 32.6 | GPa | Resistance dependence study |
| Ambient Band Gap (Calculated) | ~0.26 | eV | GGA-PBE calculation at Z point |
| Ambient Crystal Structure | Trigonal (R-3m) | N/A | Layered structure |
| Ambient Lattice Constant (a=b) | 4.304(1) | A | Powder XRD data |
| Ambient Lattice Constant (c) | 41.739(3) | A | Powder XRD data |
| Calculated Debye Temperature (ÎR) | ~320 | K | Derived from Bloch-Gruneissen resistivity fitting (6K to 200K) |
| Stoichiometric Composition (EDS) | Sn1.01Sb1.98Te4 | N/A | Good agreement with nominal composition |
Key Methodologies
Section titled âKey MethodologiesâMaterial Synthesis (Conventional Melting-Growth Method)
Section titled âMaterial Synthesis (Conventional Melting-Growth Method)â- Precursor Preparation: Sn (99.9% powder), Sb (99.99% powder), and Te (99.9% grain) were combined in stoichiometric ratios (SnSb2Te4).
- Encapsulation: The mixture was sealed in an evacuated silica tube.
- Heating: Heated in a furnace up to 1010 K for 10 hours.
- Cooling: Slowly cooled to 873 K at a rate of 9.1 K h-1 and held at that temperature for 24 hours to grow single crystals.
Experimental Measurements
Section titled âExperimental Measurementsâ- Pressure Application: Resistance measurements under pressure were conducted using an originally designed Diamond Anvil Cell (DAC).
- Electrodes: Boron-doped diamond electrodes were used for electrical measurements.
- Structural Analysis: Room temperature Powder X-ray Diffraction (XRD) was performed using a Mini Flex 600 (Rigaku).
- Compositional Analysis: Energy Dispersive Spectroscopy (EDS) was used to confirm the material composition.
- Resistivity Fitting: Temperature-dependent resistivity (4.5 K to 296 K) was fitted using the Bloch-Gruneissen formula to determine the Debye temperature (ÎR).
Computational Methods (First-Principles Calculations)
Section titled âComputational Methods (First-Principles Calculations)â- Software: Quantum ESPRESSO software package (Projector Augmented Wave, PAW method).
- Functional: Generalized Gradient Approximation (GGA) of Perdew-Burke-Erzerhof (PBE) for exchange-correlation.
- Bonding Analysis: Crystal Orbital Hamilton Population (COHP) and its energy integral (ICOHP) were calculated using LOBSTER to analyze bonding states.
- Relaxation: Atomic positions and lattice parameters were relaxed using the Broyden-Fletcher-Goldfard-Shanno (BFGS) algorithm.
Commercial Applications
Section titled âCommercial ApplicationsâThe research on SnSb2Te4, a phase change material exhibiting pressure-induced superconductivity, has implications across several advanced technology sectors:
- Phase Change Memory (PCM): As a member of the Ge-Sb-Te family of PCMs, SnSb2Te4 is fundamentally relevant to high-density, nonvolatile data storage and rewriteable media.
- Pressure-Tunable Quantum Devices: The ability to induce a superconducting state (Tc up to 7.4 K) via pressure suggests potential for developing active quantum devices where electronic properties can be dynamically tuned by mechanical stress.
- Topological Electronics: Given that related compounds (like Sb2Te3) are topological insulators, the pressure-induced superconductivity in SnSb2Te4 may be topologically non-trivial, relevant for fault-tolerant quantum computing and spintronics.
- Thermoelectric Energy Conversion: The layered structure and narrow band gap at ambient pressure are favorable characteristics for high-performance thermoelectric materials, allowing for efficient conversion between heat and electrical energy.
- Advanced Sensor Technology: Materials that undergo sharp metal-insulator or metal-superconductor transitions under specific pressure ranges can be utilized in highly sensitive, miniaturized pressure transducers and gauges.
View Original Abstract
Here we firstly report the pressure-induced superconductivity in phase change materials SnSb<sub>2</sub>Te<sub>4</sub>. Single crystals of SnSb<sub>2</sub>Te<sub>4</sub> were grown using a conventional melting-down method. The resistance under pressure was measured using an originally designed diamond anvil cell with boron-doped diamond electrodes. The temperature dependence of the resistance under different pressures has been measured up to 32.6 GPa. The superconducting transition of SnSb<sub>2</sub>Te<sub>4</sub> appeared at 2.1 K ([Formula: see text]) under 8.1 GPa, which was further increased with applied pressure to a maximum onset transition temperature 7.4 K under 32.6 GPa.