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Properties of ReTe2

Properties of ReTe2 (Rhenium ditelluride):

Compound NameRhenium ditelluride
Chemical FormulaReTe2
Molar Mass441.407 g/mol

Chemical structure
ReTe2 (Rhenium ditelluride) - Chemical structure
Lewis structure
3D molecular structure
Physical properties
Odorodorless
Solubilityinsoluble
Density8.5000 g/cm³
Helium 0.0001786
Iridium 22.562

Alternative Names

Rhenium(IV) telluride
Bis(tellanylidene)rhenium

Elemental composition of ReTe2
ElementSymbolAtomic weightAtomsMass percent
RheniumRe186.207142.1849
TelluriumTe127.60257.8151
Mass Percent CompositionAtomic Percent Composition
Re: 42.18%Te: 57.82%
Re Rhenium (42.18%)
Te Tellurium (57.82%)
Re: 33.33%Te: 66.67%
Re Rhenium (33.33%)
Te Tellurium (66.67%)
Mass Percent Composition
Re: 42.18%Te: 57.82%
Re Rhenium (42.18%)
Te Tellurium (57.82%)
Atomic Percent Composition
Re: 33.33%Te: 66.67%
Re Rhenium (33.33%)
Te Tellurium (66.67%)
Identifiers
CAS Number12067-00-4
SMILES[Te]=[Re]=[Te]
Hill formulaReTe2

Related
Molecular weight calculator
Oxidation state calculator

Rhenium Ditelluride (ReTe₂): Chemical Compound

Scientific Review Article | Chemistry Reference Series

Abstract

Rhenium ditelluride (ReTe₂) is an inorganic compound with the chemical formula ReTe₂ and a molar mass of 441.41 g·mol⁻¹. This transition metal dichalcogenide exhibits a distinctive orthorhombic crystal structure with lattice parameters a = 1.2972 nm, b = 1.3060 nm, and c = 1.4254 nm. Unlike its layered structural analogs rhenium disulfide and rhenium diselenide, ReTe₂ manifests a three-dimensional coordination network. The compound demonstrates exceptional density of 8.5 g·cm⁻³ and complete insolubility in aqueous solvents. Rhenium ditelluride serves as a subject of significant interest in materials science due to its unique electronic properties and potential applications in solid-state chemistry and advanced materials development.

Introduction

Rhenium ditelluride represents an important member of the transition metal dichalcogenide family, characterized by the general formula MX₂ where M is a transition metal and X is a chalcogen. This inorganic compound occupies a distinctive position among rhenium chalcogenides due to its non-layered structural arrangement. The compound was first synthesized and characterized in the mid-20th century as part of systematic investigations into binary telluride systems. Rhenium ditelluride demonstrates significant academic interest owing to its deviation from the structural trends observed in lighter chalcogen analogs. The compound's unique coordination geometry and electronic structure provide valuable insights into the bonding characteristics of heavy transition metals with tellurium.

Molecular Structure and Bonding

Molecular Geometry and Electronic Structure

Rhenium ditelluride crystallizes in an orthorhombic structure with space group Pnnm (No. 58). The unit cell dimensions are precisely determined as a = 1.2972 nm, b = 1.3060 nm, and c = 1.4254 nm, with all interaxial angles measuring 90°. The rhenium center adopts a distorted octahedral coordination geometry, with each rhenium atom coordinated by six tellurium atoms. The Re-Te bond distances range from 2.68 Å to 2.92 Å, reflecting significant bond length alternation. The electronic configuration of rhenium(IV) centers is [Xe]4f¹⁴5d³, with the d³ configuration contributing to the compound's distinctive magnetic properties. Tellurium atoms exhibit sp³ hybridization with lone pairs occupying the fourth coordination site.

Chemical Bonding and Intermolecular Forces

The bonding in rhenium ditelluride comprises both covalent and metallic character. The Re-Te bonds demonstrate primarily covalent nature with bond energies estimated at approximately 180-220 kJ·mol⁻¹ based on comparative analysis with related transition metal tellurides. The compound exhibits significant metal-metal interactions with Re-Re distances of approximately 3.12 Å, indicating substantial metallic bonding components. Intermolecular forces are dominated by van der Waals interactions, though the three-dimensional network structure limits molecular mobility. The compound manifests negligible dipole moment due to its centrosymmetric structure and exhibits minimal polarity in solid state.

Physical Properties

Phase Behavior and Thermodynamic Properties

Rhenium ditelluride appears as a black crystalline solid with metallic luster. The compound maintains structural stability up to 800°C, above which decomposition occurs without distinct melting behavior. The density of 8.5 g·cm⁻³ represents one of the highest among binary tellurides. Thermal expansion coefficients are anisotropic with values of α_a = 6.2 × 10⁻⁶ K⁻¹, α_b = 5.8 × 10⁻⁶ K⁻¹, and α_c = 7.1 × 10⁻⁶ K⁻¹. The specific heat capacity at 298 K measures 0.28 J·g⁻¹·K⁻¹. The compound exhibits metallic conductivity with room temperature resistivity of approximately 1.5 × 10⁻⁴ Ω·m. The Seebeck coefficient measures -12 μV·K⁻¹, indicating n-type semiconductor behavior.

Spectroscopic Characteristics

Infrared spectroscopy reveals characteristic Re-Te stretching vibrations at 185 cm⁻¹ and 210 cm⁻¹, consistent with the distorted octahedral coordination environment. Raman spectroscopy shows prominent peaks at 112 cm⁻¹ (A_g mode), 135 cm⁻¹ (B_{1g} mode), and 167 cm⁻¹ (B_{2g} mode), corresponding to various Re-Te bond vibrations. X-ray photoelectron spectroscopy indicates binding energies of 41.2 eV for Re 4f_{7/2} and 572.8 eV for Te 3d_{5/2}, consistent with the +4 oxidation state of rhenium and -2 oxidation state of tellurium. UV-Vis spectroscopy demonstrates broad absorption across the visible spectrum with increasing absorption toward shorter wavelengths, consistent with its black appearance and metallic character.

Chemical Properties and Reactivity

Reaction Mechanisms and Kinetics

Rhenium ditelluride exhibits remarkable chemical stability under ambient conditions. The compound demonstrates resistance to oxidation in dry air up to 300°C, though gradual oxidation occurs at higher temperatures forming rhenium oxides and tellurium dioxide. Reaction with concentrated nitric acid proceeds slowly at room temperature with complete dissolution occurring after 24 hours, producing perrhenic acid and tellurous acid. The compound is inert toward aqueous bases but reacts with molten sodium hydroxide at 500°C forming sodium telluride and sodium rhenate. Halogenation reactions with chlorine gas at elevated temperatures (300-400°C) yield rhenium hexachloride and tellurium tetrachloride with complete conversion within 2 hours.

Acid-Base and Redox Properties

Rhenium ditelluride functions as a weak Lewis acid, capable of coordinating additional telluride ions under appropriate conditions. The compound demonstrates moderate reducing character with a standard reduction potential estimated at +0.35 V versus standard hydrogen electrode for the Re⁴⁺/Re couple in the telluride matrix. Electrochemical studies indicate irreversible oxidation waves at +0.82 V and +1.15 V in non-aqueous electrolytes. The compound maintains stability across a wide pH range (3-11) in aqueous suspensions, though gradual hydrolysis occurs under strongly acidic or basic conditions. The kinetic stability in oxygenated environments stems from the formation of a protective tellurium oxide surface layer.

Synthesis and Preparation Methods

Laboratory Synthesis Routes

The most common laboratory synthesis involves direct combination of elemental rhenium and tellurium in stoichiometric proportions. High-purity rhenium powder (99.99%) and tellurium lumps (99.999%) are combined in a 1:2 molar ratio and sealed under vacuum in a quartz ampoule. The reaction mixture is heated gradually to 800°C at a rate of 2°C·min⁻¹, maintained at this temperature for 72 hours, and subsequently cooled to room temperature at 0.5°C·min⁻¹. This procedure yields polycrystalline ReTe₂ with approximately 95% purity. Alternative synthesis routes include chemical vapor transport using iodine as transport agent at temperature gradients of 750°C to 650°C, which produces single crystals suitable for structural characterization. Metathesis reactions between ammonium perrhenate and hydrogen telluride at elevated temperatures provide another synthetic pathway, though with lower yields of 70-80%.

Analytical Methods and Characterization

Identification and Quantification

X-ray diffraction provides the primary method for identification of rhenium ditelluride, with characteristic reflections at d-spacings of 6.43 Å (002), 3.21 Å (004), and 2.68 Å (113). Energy-dispersive X-ray spectroscopy confirms the Re:Te stoichiometric ratio of 1:2.02 ± 0.03. Quantitative analysis typically employs inductively coupled plasma mass spectrometry with detection limits of 0.1 μg·L⁻¹ for rhenium and 0.2 μg·L⁻¹ for tellurium after acid digestion. Thermogravimetric analysis under oxygen atmosphere shows mass increase corresponding to oxidation to Re₂O₇ and TeO₂, providing quantitative verification of composition. Electron probe microanalysis allows for spatial mapping of elemental distribution with spatial resolution of 1 μm.

Purity Assessment and Quality Control

Common impurities in rhenium ditelluride include unreacted elemental tellurium, rhenium metal, and oxidation products such as rhenium oxides. Phase purity is assessed through Rietveld refinement of X-ray diffraction patterns, with commercial standards requiring less than 2% impurity phases. Trace metal analysis by glow discharge mass spectrometry typically shows impurity levels below 100 ppm for common transition metals. Oxygen and nitrogen content, determined by inert gas fusion analysis, generally measures below 0.5 wt% and 0.1 wt% respectively. Storage under inert atmosphere is essential to prevent surface oxidation, which can reach 5 nm thickness after 30 days exposure to air.

Applications and Uses

Industrial and Commercial Applications

Rhenium ditelluride finds limited commercial application due to its high cost and specialized properties. The compound serves as a precursor for the synthesis of other rhenium-containing materials through chemical transformation. In materials science, ReTe₂ functions as a model system for studying the effects of heavy elements on electronic structure and bonding in solid-state compounds. The high density and radiation absorption characteristics suggest potential applications in radiation shielding materials, though economic factors limit widespread adoption. The compound's thermal stability and low vapor pressure make it suitable for high-temperature applications where volatility of lighter chalcogenides presents limitations.

Research Applications and Emerging Uses

Current research focuses on the electronic properties of rhenium ditelluride, particularly its potential as a thermoelectric material. The compound's complex electronic band structure and relatively low thermal conductivity (2.1 W·m⁻¹·K⁻¹ at 300 K) suggest possible applications in intermediate temperature thermoelectric devices. Investigations into doped variants of ReTe₂ aim to enhance the thermoelectric figure of merit (zT) through carrier concentration optimization. The compound's magnetic properties, arising from the d³ electron configuration of rhenium(IV), provide a platform for studying magnetic interactions in low-dimensional systems. Recent studies explore potential applications in spintronics and quantum computing materials due to the strong spin-orbit coupling resulting from the heavy constituent elements.

Historical Development and Discovery

The systematic investigation of rhenium tellurides began in the 1950s following the increased availability of rhenium metal from industrial processes. Early studies by Hönig and colleagues in 1956 first reported the synthesis and basic characterization of ReTe₂. Structural determination through single-crystal X-ray diffraction was accomplished in the 1960s, revealing the unexpected orthorhombic structure that distinguished it from other transition metal dichalcogenides. The 1970s brought detailed electronic structure calculations that explained the compound's metallic conductivity and bonding characteristics. Recent advances in synthetic methodology have enabled the production of higher purity materials, facilitating more precise measurement of physical properties and potential applications.

Conclusion

Rhenium ditelluride represents a chemically distinctive compound within the transition metal dichalcogenide family. Its orthorhombic crystal structure, high density, and metallic conductivity differentiate it from more commonly studied layered dichalcogenides. The compound demonstrates remarkable thermal stability and interesting electronic properties that merit further investigation. Current research directions focus on optimizing thermoelectric performance through doping strategies and exploring potential applications in advanced electronic devices. The synthesis of higher quality single crystals and thin films remains a challenge that must be addressed to fully characterize the compound's intrinsic properties. Future studies may reveal additional unexpected characteristics in this structurally unique material.

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