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Properties of MoTe2

Properties of MoTe2 (Molybdenum ditelluride):

Compound NameMolybdenum ditelluride
Chemical FormulaMoTe2
Molar Mass351.16 g/mol

Chemical structure
MoTe2 (Molybdenum ditelluride) - Chemical structure
Lewis structure
3D molecular structure
Physical properties
Appearanceblack/lead-gray solid
Solubilityinsoluble
Density7.7000 g/cm³
Helium 0.0001786
Iridium 22.562

Alternative Names

molybdenum(IV) telluride
bis(tellanylidene)molybdenum

Elemental composition of MoTe2
ElementSymbolAtomic weightAtomsMass percent
MolybdenumMo95.96127.3266
TelluriumTe127.60272.6734
Mass Percent CompositionAtomic Percent Composition
Mo: 27.33%Te: 72.67%
Mo Molybdenum (27.33%)
Te Tellurium (72.67%)
Mo: 33.33%Te: 66.67%
Mo Molybdenum (33.33%)
Te Tellurium (66.67%)
Mass Percent Composition
Mo: 27.33%Te: 72.67%
Mo Molybdenum (27.33%)
Te Tellurium (72.67%)
Atomic Percent Composition
Mo: 33.33%Te: 66.67%
Mo Molybdenum (33.33%)
Te Tellurium (66.67%)
Identifiers
CAS Number12058-20-7
SMILES[Te]=[Mo]=[Te]
Hill formulaMoTe2

Related
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Oxidation state calculator

Molybdenum Ditelluride (MoTe₂): Chemical Compound

Scientific Review Article | Chemistry Reference Series

Abstract

Molybdenum ditelluride (MoTe₂) is an inorganic semiconducting compound belonging to the transition metal dichalcogenide class. It crystallizes in multiple polymorphic forms, primarily the hexagonal α-phase (2H-MoTe₂) and the monoclinic/orthorhombic β-phase (1T/1T'-MoTe₂). The compound exhibits a layered structure with strong covalent bonding within layers and weak van der Waals interactions between layers. Bulk α-MoTe₂ demonstrates an indirect band gap of 0.88 eV and a direct band gap of 1.02 eV at room temperature, transitioning to direct bandgap behavior in monolayer configurations. Physical properties include a density of 7.7 g/cm³, thermal conductivity of 2 W·m⁻¹·K⁻¹, and characteristic Raman spectra with prominent peaks at 171.4 cm⁻¹ (A1g mode) and 234.5 cm⁻¹ (E2g mode). Applications span electronics, optoelectronics, lubrication, catalysis, and emerging quantum materials research due to its tunable electronic structure and topological properties.

Introduction

Molybdenum ditelluride represents a significant 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 compound demonstrates particularly interesting polymorphic behavior and electronic properties that bridge semiconducting and metallic characteristics. Unlike its sulfide and selenide analogs, MoTe₂ exhibits closer energy proximity between different crystalline phases, enabling phase-controlled electronic applications. The compound's ability to exist in multiple structural forms with distinct electronic properties—semiconducting hexagonal (2H) and semimetallic monoclinic (1T') phases—makes it a compelling subject for fundamental materials research and technological applications in nanoelectronics and quantum computing.

Molecular Structure and Bonding

Molecular Geometry and Electronic Structure

Molybdenum ditelluride adopts a layered structure where each molybdenum atom coordinates with six tellurium atoms in trigonal prismatic geometry. In the hexagonal α-phase (2H-MoTe₂), the unit cell parameters measure a = 3.519 Å and c = 13.964 Å at room temperature, with space group P6₃/mmc (No. 194). The Mo-Te bond length measures 2.73 Å within the covalently bonded layers. The tellurium atoms in adjacent layers exhibit a separation of 3.95 Å, indicating van der Waals interactions between layers. The electronic configuration involves molybdenum in the +4 oxidation state with electron configuration [Kr]4d², while tellurium assumes the -2 oxidation state with electron configuration [Kr]4d¹⁰5s²5p⁴. The compound exhibits highly covalent bonding character despite formal ionic charges, with molecular orbital calculations indicating strong hybridization between molybdenum d-orbitals and tellurium p-orbitals.

Chemical Bonding and Intermolecular Forces

The intralayer bonding in MoTe₂ consists primarily of covalent interactions with partial ionic character. Bond angles within the layers include Te-Mo-Te angles of 80.7° within the same sublayer and 136.0° across sublayers. The interlayer interactions are dominated by van der Waals forces with a binding energy of approximately 40 meV per atom, significantly weaker than the intralayer covalent bonds exceeding 2 eV. The compound exhibits minimal dipole moment due to its centrosymmetric structure in the bulk form, though monolayer configurations lack inversion symmetry. The work function measures 4.1 eV, while the electron affinity ranges between 3.5-3.8 eV depending on crystalline phase and thickness.

Physical Properties

Phase Behavior and Thermodynamic Properties

Molybdenum ditelluride exists in three primary crystalline forms: hexagonal α-MoTe₂ (2H phase), monoclinic β-MoTe₂ (1T phase), and orthorhombic β'-MoTe₂ (1T' phase). The α-phase is thermodynamically stable at room temperature and transforms to the β-phase at 820°C under stoichiometric conditions. The compound appears as black or lead-gray crystalline solids with metallic luster. The density measures 7.7 g/cm³ for the α-phase and 7.5 g/cm³ for the β-phase. Thermal expansion coefficients demonstrate anisotropy with a-axis expansion from 3.492 Å at 100 K to 3.53 Å at 400 K, while c-axis expansion ranges from 13.67 Å at 100 K to 14.32 Å at 400 K. The heat of formation measures -84 kJ/mol for β-MoTe₂ and -6 kJ/mol for the α-β phase transformation. Decomposition occurs without melting at elevated temperatures, with tellurium vapor pressure following the relationship log PTe₂ = 8.398 - 11790/T for the α-phase.

Spectroscopic Characteristics

Raman spectroscopy of α-MoTe₂ reveals characteristic vibrational modes at 25.4 cm⁻¹, 116.8 cm⁻¹, 171.4 cm⁻¹ (A1g mode), and a doublet at 232.4-234.5 cm⁻¹ (E2g mode). The E2g mode frequency increases from 232.4 cm⁻¹ in bulk to 236.6 cm⁻¹ in monolayers, while the A1g mode decreases from 171.4 cm⁻¹ to 172.4 cm⁻¹. Infrared spectroscopy shows reflectivity of approximately 43% in the infrared region with absorption minima at 245.8 cm⁻¹ and maxima at 234.5 cm⁻¹. Photoluminescence spectroscopy reveals excitonic transitions at 1.10 eV (A exciton) and 1.48 eV (B exciton) at low temperatures. X-ray photoelectron spectroscopy shows molybdenum 3d peaks at 227.8 eV (3d5/2) and 231.0 eV (3d3/2), and tellurium 3d peaks at 572.5 eV (3d5/2) and 582.9 eV (3d3/2).

Chemical Properties and Reactivity

Reaction Mechanisms and Kinetics

Molybdenum ditelluride exhibits stability in non-oxidizing environments but decomposes under oxidizing conditions. The compound is insoluble in water and non-oxidizing acids but undergoes complete decomposition in dilute nitric acid. Oxidation in air proceeds gradually at room temperature, forming molybdenum dioxide (MoO₂) as an intermediate and ultimately yielding molybdenum trioxide and tellurium dioxide. The oxidation mechanism involves formation of intermediate tellurite compounds including Te₂MoO₇ and TeMo₅O₁₆. Thermal decomposition follows first-order kinetics with respect to tellurium vapor pressure, following the relationship log PTe₂ = 5.56 - 9879/T for the β-phase. The compound demonstrates resistance to hydrochloric acid attack but dissolves completely in concentrated sulfuric acid at 261°C.

Acid-Base and Redox Properties

Molybdenum ditelluride exhibits amphoteric behavior in strongly oxidizing environments. The compound demonstrates stability across a wide pH range in non-oxidizing conditions but undergoes oxidative decomposition in acidic oxidizing media. Standard reduction potentials for the MoTe₂/Te/Mo system measure approximately -0.1 V versus standard hydrogen electrode. The compound functions as a p-type semiconductor when synthesized with excess tellurium and as an n-type semiconductor when prepared with bromine transport agents. Electrochemical intercalation with alkali metals proceeds reversibly up to compositions of Li1.6MoTe₂ without structural degradation of the host lattice.

Synthesis and Preparation Methods

Laboratory Synthesis Routes

Stoichiometric synthesis of MoTe₂ involves direct combination of elemental molybdenum and tellurium at elevated temperatures. The standard method requires heating purified elements in a 1:2 molar ratio at 1100°C under vacuum or inert atmosphere for 48-72 hours. Chemical vapor transport using bromine as a transporting agent produces large single crystals of α-MoTe₂, with typical conditions involving 5 mg/cm³ bromine concentration and temperature gradients from 950°C (source) to 850°C (deposition zone). Vapor deposition methods utilizing tellurium vapor alone produce p-type material, while bromine-assisted transport yields n-type crystals. Thin film deposition employs tellurization of molybdenum films at 650°C, resulting in α-phase formation, or tellurization of molybdenum trioxide at 650°C, producing β-phase material. Sonochemical synthesis from molybdenum hexacarbonyl and tellurium in decalin produces amorphous MoTe₂ that crystallizes upon annealing.

Industrial Production Methods

Industrial production of molybdenum ditelluride utilizes scaled-up vapor transport methods with careful control of tellurium stoichiometry. Large-scale synthesis employs tube furnaces with multiple zones controlling temperature gradients within ±2°C. Tellurium-deficient compositions (MoTe1.94-MoTe1.95) demonstrate enhanced electrical conductivity and are produced by precise control of tellurium vapor pressure during synthesis. Quality control measures include X-ray diffraction analysis to verify phase purity and energy-dispersive X-ray spectroscopy to confirm stoichiometry. Production costs primarily derive from high-purity tellurium precursor materials and energy-intensive high-temperature processes.

Analytical Methods and Characterization

Identification and Quantification

X-ray diffraction provides definitive identification of crystalline phases through comparison with reference patterns (ICDD PDF #00-019-1462 for α-phase, #00-019-1463 for β-phase). Raman spectroscopy distinguishes between phases through characteristic frequency differences in the 230-240 cm⁻¹ region. Quantitative analysis employs inductively coupled plasma mass spectrometry with detection limits of 0.1 ppm for molybdenum and 0.2 ppm for tellurium. Stoichiometry determination requires thermogravimetric analysis under controlled atmosphere to measure tellurium content through mass loss during decomposition.

Purity Assessment and Quality Control

Phase purity assessment utilizes Rietveld refinement of X-ray diffraction patterns with impurity detection limits below 2%. Common impurities include unreacted elemental tellurium, molybdenum trioxide, and lower tellurides (Mo2Te3). Electrical characterization through Hall effect measurements verifies semiconductor type and carrier concentration, with specifications requiring carrier concentrations below 10¹⁷ cm⁻³ for electronic applications. Optical quality assessment employs photoluminescence quantum yield measurements with acceptance criteria exceeding 15% quantum efficiency for optoelectronic applications.

Applications and Uses

Industrial and Commercial Applications

Molybdenum ditelluride finds application as a solid lubricant in high-temperature vacuum environments, maintaining a coefficient of friction below 0.1 at temperatures up to 500°C. The compound serves as a catalyst for hydrogen evolution reactions, with the β-phase demonstrating Tafel slopes of 78 mV/decade and superior activity compared to the α-phase. Electronic applications include use as a channel material in field-effect transistors, with demonstrated electron mobility of 10-50 cm²/V·s and hole mobility of 5-20 cm²/V·s in thin-film configurations. Optoelectronic applications exploit the layer-dependent bandgap for photodetection in the near-infrared region (0.8-1.1 μm).

Research Applications and Emerging Uses

Research applications focus on quantum materials investigations, particularly the topological properties of the β'-phase which exhibits type-II Weyl semimetallic behavior and topological Fermi arcs. The compound serves as a platform for studying phase transitions between semiconducting and semimetallic states through electrostatic gating, strain, or laser excitation. Heterostructure devices combining MoTe₂ with other two-dimensional materials enable band engineering for novel electronic and optoelectronic functionality. Superconducting properties emerge in the β'-phase below 120 mK and in intercalated compounds below 2.8 K, providing systems for studying unconventional superconductivity. Emerging applications include surface-enhanced Raman spectroscopy substrates for biomarker detection and piezoelectric devices utilizing the non-centrosymmetric structure of monolayer configurations.

Historical Development and Discovery

Initial investigations of molybdenum telluride systems began in the early 20th century with phase diagram studies of the Mo-Te system. The compound's structural characterization advanced significantly in the 1960s with detailed X-ray diffraction studies identifying the hexagonal and monoclinic polymorphs. The development of chemical vapor transport methods in the 1970s enabled growth of large single crystals for detailed electronic property measurements. Renewed interest emerged in the 2010s with the discovery of topological properties in the β'-phase and the demonstration of phase-controlled electronic behavior. The recent development of chemical vapor deposition methods for large-area thin film growth has accelerated applications in electronics and optoelectronics.

Conclusion

Molybdenum ditelluride represents a versatile compound with unique polymorphic behavior and tunable electronic properties. The coexistence of semiconducting and semimetallic phases within the same chemical system enables phase-engineered devices and fundamental studies of phase transitions. The compound's strong covalent intralayer bonding and weak interlayer interactions facilitate fabrication of two-dimensional materials through mechanical exfoliation or direct growth. Applications span lubrication, catalysis, electronics, and quantum materials research. Future research directions include precise control of phase distributions in device geometries, enhancement of superconducting transition temperatures through chemical modification, and development of large-scale integration processes for commercial applications.

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