Er:Yb:Glass (Erbium-doped Glass)

Er:Yb:glass (erbium glass) is a well-known and widely used active medium—a phosphate glass co-doped with erbium (Er³⁺) and ytterbium (Yb³⁺)—employed for lasers emitting in the eye-safe 1.5–1.6 µm wavelength range.

Keywords:

Scintillation Crystals

Product Category:

  • Product Introduction
  • Key advantages
  • Application areas
  • Product Features
    • Commodity name: Er:Yb:Glass (Erbium-doped Glass)

    Er:Yb:glass (erbium glass) is a well-known and widely used active medium—a phosphate glass co-doped with erbium (Er³⁺) and ytterbium (Yb³⁺)—employed for lasers emitting in the eye-safe 1.5–1.6 µm wavelength range.

    Product Introduction

    Er:Yb:glass (erbium glass) is a well-known and widely used active medium—a phosphate glass co-doped with erbium (Er³⁺) and ytterbium (Yb³⁺)—employed for lasers emitting in the eye-safe 1.5–1.6 µm wavelength range.

    Er:Yb:Glass (Erbium-Ytterbium co-doped phosphate glass) is a rare-earth-doped laser material based on a phosphate glass matrix. It boasts a long fluorescence lifetime and is relatively safe for human eyes. As an eye-safe wavelength laser, the Er3+/Yb3+-co-doped phosphate glass laser has garnered significant attention due to its compact design and cost-effectiveness—particularly in applications like laser generation and signal amplification. The 1540 nm wavelength happens to fall precisely within both the eye-safe range and the optical fiber communication window. This material is widely used in laser ranging and tracking, fiber-optic communications, optoelectronic countermeasures, high-power laser damage applications, laser-based medical treatments, and laser cosmetic procedures. It also excels in optical waveguide amplification and offers high-gain characteristics when employed in fiber amplifiers.

     

    Key Advantages

    - High laser efficiency 
    - Low laser threshold 
    - Eye-safe 
    - Low power loss 
    - Energy transfer efficiency from high-Yb to Er 
    - Long fluorescence lifetime

     

    Application Areas

    - Military individual long-range targeting, tank and armored vehicle targeting 
    - Drone micro-pod, missile laser guidance 
    - Laser ranging and tracking 
    - Laser medical treatments and laser beauty procedures 
    - Fiber-optic communication

     

    Product Features

    Material Properties

    Erbium Glass Properties

    Erbium Glass Specifications

    EAT14

    WM4

    The Cross-section for Stimulated Emission

    0.8 10-20 cm²

    0.75 10-20 cm²

    Density

    3.06 g/cm³

    2.83 g/cm³

    Melting Point

    1970 °C

    1970 °C

    Thermal Expansion Coefficient (20100°C)

    87 10-7/K

    82 10-7/K

    Thermal Expansion Coefficient (100300°C)

    95 10-7/K

    96 10-7/K

    Thermal Coefficient of Optical Path Length (20 100°C)

    2.9 10-6/K

    1.4 10-6 /K

    Thermal Conductivity (25°C) 

    0.7 W/m·K

    0.7 W/m·K

    Central Laser Wavelength

    1535 nm

    1535 nm

    Refractive Index

    1.524@1535 nm

    1.528@1535 nm

    Refractive Index 

    1.532@589.3 nm

    1.536@589.3 nm

    Abbe Number

    66

    66

    Softening Temperature

    605 °C

    573 °C

    Transition Temperature

    556 °C

    530 °C

    Fluorescence Lifetime

    7.78.0 ms

    7.78.2 ms

    Product Processing Indicators

    Orientation Tolerance

    <0.5°

    Effective Aperture

    >90%

    Maximum Size

    ∅(3 12.7)×(3 150) mm²

    Dimensional Tolerance

    ±0.05 mm

    Chamfer

    ≤0.2×45°

    Surface Quality

    10-5 S-D

    Flatness

    ≤λ/8@632.8 nm

    Wavefront Distortion

    ≤λ/4@632.8 nm

    Parallelism

    <10"

    Perpendicularity

    ≤15′

    Chipped Edge

    <0.1 mm

  • - 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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