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Correlated structural and electronic phase transformations in transition metal chalcogenide under high pressure

MetadataDetails
Publication Date2016-04-04
JournalJournal of Applied Physics
AuthorsChunyu Li, Feng Ke, Qingyang Hu, Zhenhai Yu, Jinggeng Zhao
InstitutionsCarnegie Institution for Science, Geophysical Laboratory
Citations7
AnalysisFull AI Review Included

6CCVD Technical Documentation: High-Pressure Semiconductor Physics

Section titled “6CCVD Technical Documentation: High-Pressure Semiconductor Physics”

This research investigates the structural and electronic properties of chromium sesquisulfide ($\text{Cr}_2\text{S}_3$), a key layered transition metal chalcogenide, under extreme pressure using Diamond Anvil Cell (DAC) methodologies. The findings are highly relevant to engineers optimizing thermoelectric and semiconductor materials for high-stress environments.

  • Application Focus: Comprehensive study of high-pressure structural (XRD) and electrical transport properties up to 36.3 GPa, supporting the development of advanced thermoelectric materials.
  • Core Achievement: Observation of a structural phase transition in rhombohedral $\text{Cr}_2\text{S}_3$ at approximately 16.5 GPa, confirmed via synchrotron angle dispersive X-ray diffraction (AD-XRD).
  • Electronic Transformation: Detection of a pressure-induced semiconductor-to-metal transition, characterized by a steep decrease in electrical resistance by an order of three across the 7 GPa to 15 GPa range.
  • Methodology: Utilized specialized DACs with 300 ”m culets for pressure application and a custom four-electrode setup on the diamond surface for in-situ resistance measurements.
  • Material Implication: The necessity for highly stable, optically clear (for XRD), and electrically customized diamond anvils underscores the demand for 6CCVD’s Single Crystal (SCD) and Boron-Doped (BDD) diamond solutions.
  • DAC Engineering: The experiment required precision fabrication, including 300 ”m culets and custom diamond surface modification for thin-film electrode integration.

The following hard data points were extracted from the experimental results and setup descriptions:

ParameterValueUnitContext
Maximum Applied Pressure36.3GPaLimit of high-pressure AD-XRD experiment
Structural Phase Transition Pressure16.5GPaObserved onset of phase change via AD-XRD
Semiconductor-to-Metal Transition Range14.4 to 17GPaInferred from change in resistance temperature coefficient ($\text{dR}/\text{dT}$)
Electrical Resistance ReductionOrder of three (10Âł factor)N/AResistance drop observed between 7 GPa and 15 GPa
Isothermal Bulk Modulus ($\text{B}_0$)59.8(6)GPaFor the low-pressure (LP) phase of $\text{Cr}_2\text{S}_3$
Ambient Unit Cell Volume ($\text{V}_0$)511.41(9)ųCalculated from 3rd-order Birch-Murnaghan fit
Resistance Measurement Temp Range300 to 400KUsed for characterizing temperature dependence of resistance
Diamond Anvil Culet Size300”mUsed for Symmetric DAC (XRD experiments)
Sample Chamber Diameter (XRD)120”mPre-indented stainless steel gasket size
Sample Chamber Diameter (Resistance)150”mHole diameter used for resistance measurement setup
Synchrotron Wavelength (X17C BNL)0.4075ÅUsed for AD-XRD patterns

The experiment relied on high-precision DAC fabrication and specialized in-situ measurement techniques:

  1. High-Pressure X-Ray Diffraction (AD-XRD):
    • Symmetric DACs utilized single crystal diamond anvils with a 300 ”m culet size to achieve pressures up to 36.3 GPa.
    • Sample chambers (120 ”m diameter) were formed in pre-indented 45 ”m thick stainless steel gaskets.
    • Silicone oil was employed as the pressure transmitting medium for XRD, calibrated using ruby fluorescence.
    • AD-XRD patterns were collected using focused synchrotron beams ($\lambda = 0.4075$ Å).
  2. In-situ Electrical Resistance Measurement:
    • Performed using a four-electrode method, requiring highly customized diamond anvils where electrodes were set up directly on the diamond surface.
    • A 150 ”m sample chamber was drilled into the gasket.
    • Insulation for the electrodes was achieved by filling the chamber with compacted cubic Boron Nitride (c-BN) powder and covering the remaining gasket area with insulating gel.
    • Measurements were conducted on a temperature-controlled hot plate (300 K to 400 K) without a pressure transmitting medium, introducing deviatoric stress (noted as a cause for differing transition pressures compared to XRD).
  3. First-Principles Calculations:
    • Density Functional Theory (DFT) utilized the VASP package, employing the generalized gradient approximation (GGA) plus Hubbard U ($\text{U} = 3.2$ eV) method.
    • Calculations confirmed the transition nature and predicted structural changes by applying hydrostatic pressure (Pulay stress) to fully optimize the unit cell.

The successful replication and extension of high-pressure studies like this rely fundamentally on the quality, customizability, and electrical properties of the diamond anvils. 6CCVD provides the specialized CVD diamond products required for next-generation DAC experiments.

Research Requirement6CCVD Recommended SolutionKey Capability Alignment
High Purity/High Stress AnvilsOptical Grade Single Crystal Diamond (SCD)Provides maximum mechanical strength and optical transmission necessary for synchrotron XRD and high-pressure stability (>36 GPa). 6CCVD supplies SCD up to 500 ”m thick.
Robust Electrical PathwaysBoron-Doped Diamond (BDD) SubstratesFor high-P transport studies, BDD offers stable, known conductivity, essential for eliminating signal noise associated with c-BN insulation. Available in SCD or PCD formats.
Electrode FabricationCustom Metalization ServicesRequired for the four-electrode setup. 6CCVD offers in-house deposition of thin films including Ti, Pt, Au, W, or Cu onto polished diamond surfaces, enabling precise electrical contacting on small culet sizes (300 ”m).
Precision Anvil ShapingCustom Laser Cutting ServicesNecessary for producing highly symmetric diamond anvils and precise culet sizes (300 ”m) critical for achieving homogeneous pressure distribution.
Surface QualityPrecision PolishingEnsures optimal surface contact between the metal electrodes and the sample. 6CCVD guarantees ultra-low roughness: $\text{Ra} < 1$ nm for SCD, and $\text{Ra} < 5$ nm for inch-size PCD.

The observed differences in transition pressures between the XRD (hydrostatic/quasi-hydrostatic) and resistance (non-hydrostatic, no PCM) experiments highlight the complexity of material behavior under deviatoric stress.

6CCVD’s in-house PhD engineering team specializes in the fabrication and selection of diamond materials optimized for complex high-pressure research. We can assist researchers in selecting the ideal material (e.g., optical SCD vs. heavy BDD) and configuring custom metalization patterns for transport studies in similar semiconductor or thermoelectric phase transformation projects.

For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly. We offer global shipping (DDU default, DDP available) to ensure reliable delivery of highly customized diamond components.

View Original Abstract

Here, we report comprehensive studies on the high-pressure structural and electrical transport properties of the layered transition metal chalcogenide (Cr2S3) up to 36.3 GPa. A structural phase transition was observed in the rhombohedral Cr2S3 near 16.5 GPa by the synchrotron angle dispersive X-ray diffraction measurement using a diamond anvil cell. Through in situ resistance measurement, the electric resistance value was detected to decrease by an order of three over the pressure range of 7-15 GPa coincided with the structural phase transition. Measurements on the temperature dependence of resistivity indicate that it is a semiconductor-to-metal transition in nature. The results were also confirmed by the electronic energy band calculations. Above results may shed a light on optimizing the performance of Cr2S3 based applications under extreme conditions.