Er:YAG (Erbium-Doped Yttrium Aluminum Garnet) Crystal

Er:YAG (Erbium-doped Yttrium Aluminum Garnet) crystal, with the chemical formula Er:Y₃Al₅O₁₂, is created by doping Yttrium Aluminum Garnet (YAG) crystals with erbium (Er) atoms. It is widely used in the field of fiber optic communications due to its high birefringence coefficient and wide transmittance range, among other excellent optical properties.

Keywords:

Scintillation Crystals

Product Category:

  • Product Introduction
  • Key advantages
  • Application areas
  • Product Features
    • Commodity name: Er:YAG (Erbium-Doped Yttrium Aluminum Garnet) Crystal

    Er:YAG (Erbium-doped Yttrium Aluminum Garnet) crystal, with the chemical formula Er:Y₃Al₅O₁₂, is created by doping Yttrium Aluminum Garnet (YAG) crystals with erbium (Er) atoms. It is widely used in the field of fiber optic communications due to its high birefringence coefficient and wide transmittance range, among other excellent optical properties.

    Product Introduction

    Er:YAG (Erbium-doped Yttrium Aluminum Garnet) crystal, with the chemical formula Er:Y₃Al₅O₁₂, is created by doping Yttrium Aluminum Garnet (YAG) crystals with erbium (Er) atoms. It is widely used in the field of fiber optic communications due to its high birefringence coefficient and wide transmittance range, among other excellent optical properties.

     The base material for Er:YAG crystals is YAG itself—a crystalline substance with a cubic crystal structure. In this process, yttrium ions within the YAG lattice are partially replaced by erbium ions, resulting in an erbium-doped YAG crystal. These erbium ions are uniformly distributed throughout the crystal, enabling consistent gain in laser applications.  

    Er-YAG crystals belong to the cubic crystal system and are a promising solid-state laser material for the mid-infrared wavelength range. At room temperature, they can emit laser light at three distinct wavelengths: 1.64 μm, 1.78 μm, and 2.94 μm. Notably, the 1.64 μm and 1.78 μm wavelengths fall within the eye-safe spectral region. Meanwhile, Er-YAG’s emission wavelength of 2940 nm coincides with a strong water absorption peak, making it highly effective at being absorbed by water molecules—and thus ideal for targeting hydroxyl groups in biological tissues. As a result, Er-YAG lasers have become widely used in medical applications, including surgical procedures, dermatological treatments for skin rejuvenation and aesthetics, dental therapies, and even medical blood collection techniques. Moreover, the Er-YAG laser’s specific wavelength makes it an excellent choice for addressing a variety of skin concerns associated with aging and pigmentation issues, such as hyperpigmentation, photo-induced skin damage, solar elastosis, acne scars, and traumatic scarring. It’s also particularly effective for reducing fine lines, mild to moderate wrinkles, uneven skin texture, and loose, sagging skin.

     

    Key Advantages

    - Isotropic Crystals (cubic symmetry)  
    - High Thermal Conductivity  
    - Low Scattering Loss  
    - A Strong Absorption Bandwidth near 1470 nm, corresponding to the emission of InGaAsP/InP laser diodes  
    - The Emission Spectrum at 1617 nm shows no absorption in the atmosphere.

     

    Application Areas

    - Medical applications: 2.94µm laser for dermatology & aesthetics, oral surgery, dentistry (including implantology), and ENT procedures; also used for medical blood collection.  
    - Optical Communication 1600nm Laser  
    - Material processing, microfabrication, welding, and cutting  
    - High-efficiency, high-power thin-disk laser  
    - Continuous-wave and Q-switched, eye-safe (~1.6 μm) intracavity-pumped lasers for military applications, including lidar, telemetry, or active imaging

     

    Product Features

    Basic Material Properties

    Crystal Structure

    Cubic

    Melting Point

    1970°C

    Density

    4.56±0.04 g/cm³

    Specific Heat

    0.59 J/g·cm³

    Laser Wavelength

    2940 nm

    Main Pump Band Range

    600–800 nm

    Photon Energy

    6.75×10-20J@2940nm

    Launch Cross-section

    3×10-20cm²

    Mohs Hardness

    8.5 Mohs

    Poisson's Ratio

    0.3

    Tensile Strength

    0.13–0.26 GPa

    Thermal Expansion Coefficient

     

    <100>Direction:8.2×10 -6/10°C to 250°C

    <110>Direction:7.7×10 -6/10°C to 250°C

    <111>Direction:7.8×10 -6/10°C to 250°C

    Thermal Conductivity

     

    14 W/m/K at 20°C

    10.5 W/m/K at 100°C

    Thermal-Optic Coefficient

    dn/dT=7.3×10-6/k

    Refractive Index

    1.79@2940 nm

    Product Processing Indicators

    Oritentation

    <111>

    Doping Concentration

    0.2–50 atm%

    Effective Aperture

    >90%

    Size Range

    Diameter:1 mm–20 mm,

    Length:10 mm–1500 mm

    Dimensional Tolerance

    Φ:+0/-0.04 mm, L:+0.5/-0 mm

    Chamfer

    ≤0.2×45°

    Surface Quality

    10-5 S-D

    Flatness

    ≤λ/10@632.8 nm

    Wavefront Distortion

    ≤λ/8@633 nm

    Parallelism

    <20"

    Perpendicularity

    ≤10′

    Extinction Ratio

    ≥25 dB

    Coating

    AR:R≤0.20%@2940 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

Online Quotation Request

Please provide your phone number and email address, and we’ll get in touch with you as soon as possible.

操作
Submit