Nd:GdVO₄ (Neodymium-doped Gadolinium Vanadate) Crystal

Nd:GdVO₄ (Neodymium-doped Gadolinium Vanadate) laser crystals exhibit properties similar to those of Nd:YVO₄ laser crystals, boasting excellent optical, physical, and mechanical characteristics. They are one of the ideal laser materials for diode-pumped, all-solid-state (DPSS) micro-laser systems.

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Scintillation Crystals

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  • Product Introduction
  • Key advantages
  • Application areas
  • Product Features
    • Commodity name: Nd:GdVO₄ (Neodymium-doped Gadolinium Vanadate) Crystal

    Nd:GdVO₄ (Neodymium-doped Gadolinium Vanadate) laser crystals exhibit properties similar to those of Nd:YVO₄ laser crystals, boasting excellent optical, physical, and mechanical characteristics. They are one of the ideal laser materials for diode-pumped, all-solid-state (DPSS) micro-laser systems.

    Product Introduction

    Nd:GdVO₄ (Neodymium-doped Gadolinium Vanadate) laser crystals share similar properties with Nd:YVO₄ laser crystals, boasting excellent optical, physical, and mechanical characteristics. They are an ideal laser medium for diode-pumped, all-solid-state (DPSS) micro-lasers—particularly compact ones. Compared to Nd:YAG, Nd:GdVO₄ exhibits higher slope efficiency, while offering superior thermal conductivity and enabling higher output power than Nd:VO₄. As a result, Nd:GdVO₄ delivers even better performance in high-power DPSS applications.

     

    Key Advantages

    - Large stimulated emission cross section 
    - High absorption coefficient and wide absorption bandwidth, with minimal dependence on the pump wavelength 
    - Excellent thermal conductivity 
    - Low laser threshold with high laser output slope efficiency 
    - High laser damage threshold 
    - The laser output has excellent polarization.

     

    Application Areas

    - Distance measurement 
    - Laser-diode-pumped all-solid-Sstate (DPSS) miniaturized laser 
    - Remote sensing 
    - Telemetry

     

    Product Features

    Material Properties

    Crystal Structure

    Tetragonal, Space Group D4h, a=b=7.21, c=6.35

    Lattice Constant

    a=7.21Å, c=6.35Å

    Density

    5.47 g/cm³

    Mohs Hardness

    5 Mohs

    Melting Point

    1780 °C

    Refractive Index (@1064 nm)

    no=1.972, ne=2.192

    Thermal Expansion Coefficient 

    aa=1.5×10-6/K, ac=7.3×10-6/K

    Thermal Conductivity <110>

    11.7 W/m/K

    Laser Wavelength

    1062.9 nm

    Emission Cross-Section (@1064 nm)

    7.6×10-19cm²

    Absorption Cross Section (@808 nm)

    4.9×10-19cm²

    Fluorescence Lifetime

    90 μs (1% Nd-doped)

    Absorption Coefficient (808 nm)

    74 cm-1

    Polarization

    Parallel to the c-axis

    Product Processing Indicators

    Nd Doping Concentration

    0.1~3.0 at.%

    Effective Aperture

    >90%

    Dimensional Tolerance

    (W±0.1 mm)×(H±0.1 mm)×(L+0.2/-0.1 mm)

    Chamfer

    ≤0.2×45°

    Surface Quality

    10-5 S-D

    Flatness

    ≤λ/8@632.8 nm

    Wavefront Distortion

    ≤λ/4@633 nm

    Parallelism

    <20"

    Perpendicularity

    ≤15′

    Angle Tolerance

    ≤0.5°

    Chipped Edge

    <0.1 mm

    Coating

    AR:R<0.2%@1064 nm

    HR: R>99.8% @1064 nm, T>95% @808 nm

  • - Excellent thermal conductivity
    - Multiple possible pump wavelengths (typically 532 nm)
    - Broad-wavelength tunability
    - Broadly Absorbing Pump Band
    - Outstanding output efficiency
    - Short-lived excited state (3.2 μm)
    - Narrow mode-locking width
    - High damage threshold

  • - Mode-locked laser with ultrashort pulses
    - Multi-channel Amplifiers and Regenerative Amplifiers
    - The tunable wavelength range allows Ti:Sapphire lasers to replace dye lasers in many applications.
    - By using ultra-thin, non-critically phase-matched crystals like BBO as frequency-doubling devices, Ti:Sapphire lasers can generate ultrashort pulses as short as below 10 fs, producing light in the ultraviolet to deep-ultraviolet range—down to as low as 193 nm.
    -Ti:Sapphire is also widely used as a pump source for optical parametric oscillators to broaden their tuning range.

  • Basic Material Properties
    Molecular formula Ti³⁺:Al₂O₃
    Crystal structure Hexagonal crystal system
    Lattice constant a = 4.758 Å, c = 12.991 Å
    Density 3.98g/cm3
    Melting point 2040°C
    Mohs Hardness 9Mohs
    Thermal conductivity 52W/m/k
    Specific heat 0.42J/g/K
    Laser generation Four-level system
    Fluorescence lifetime 3.2 μs (T = 300 K)
    Tuning range 660-1050nm
    Absorption range 400-600nm
    Emission peak 795nm
    Absorption peak 488nm
    Refractive index 1.76 @ 800 nm
    Peak cross-section 3–4 × 10⁻¹⁹ cm²
    Coefficient of thermal expansion 8.40 × 10⁻⁶/°C

     

    Product Processing Metrics
    Directional The C-axis is the optical axis direction, which is perpendicular to the crystal surface.
    Ti2O3 concentration 0.06–0.26 at.%
    Quality factor 100–300 units
    Effective Aperture >90%
    Surface Dimension Tolerance 0 / -0.1 mm
    Thickness Tolerance ±0.1 mm
    Protective Chamfer ≤0.2 × 45°
    End face Double parallel planes or Brewster-cut ends
    Surface finish 10-5 S-D
    Flatness ≤λ/8 @ 633 nm
    Transmitted Wavefront Distortion ≤λ/4 @ 633 nm
    Parallelism 30"
    Verticality ≤15′
    Custom film system services available

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