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Lithium Triborate (LBO) Crystal is a...
HM2818
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Lithium Triborate (LBO) Crystal is a high-performance nonlinear optical crystal known for its excellent optical uniformity, broad transmission range, high conversion efficiency, and high laser damage threshold. It is ideal for frequency-doubling applications. Heeger Materials is a professional supplier and manufacturer of high-quality LBO Crystal, offering competitive prices.
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Density | 2.47 g/cm³ |
Materials | LBO |
Melting Piont | 834 ℃ |
Molecular Formula | LiB3O5 |
Lithium Triborate (LBO) Crystal is widely used for frequency doubling and other nonlinear optical processes. It offers a broad transmission range, a high laser damage threshold, and excellent optical uniformity. With stable chemical properties, high mechanical hardness, and low birefringence compared to BBO, LBO limits the spectral range of phase matching for improved efficiency. Heeger Materials (HM) provides high-quality LBO crystals for advanced applications.
Dimensions Tolerance | (W±0.1 mm)×(H±0.1 mm)×(L+0.5/-0.1 mm) (L≥2.5 mm) (W±0.1 mm)×(H±0.1 mm)×(L+0.1/-0.1 mm) (L<2.5 mm) |
Effective Aperture | 90% of the central region diameter |
Flatness | λ/8 @ 633 nm |
Transmitted Wavefront Distortion | λ/8 @ 633 nm |
Surface Quality | 10/5 per MIL-PRF-13830B standard |
Parallelism | 20″ |
Perpendicularity | 15′ |
Angle Deviation | Δθ≦0.25°, ΔФ≦0.25° |
Chamfer | ≤0.2 mm×45° |
Edge Chip | ≤0.1 mm |
Damage Threshold | >10 GW/cm² @ 1064 nm, 10 ns, 10 Hz (polished) |
>1 GW/cm² @ 1064 nm, 10 ns, 10 Hz (AR coating) | |
>0.5 GW/cm² @ 532 nm, 10 ns, 10 Hz (AR coating) |
Size | Length (mm) | Theta | PHI | Coating | Application |
6x6 mm | 0.1, 0.5, 1 | 29.2° | 90° | P/P@400-800NM | SHG@800NM, Type I |
10x10 mm | 0.1, 0.5, 1 | 29.2° | 90° | P/P@400-800NM | SHG@800NM, Type I |
6x6 mm | 0.1, 0.5, 1 | 44.3° | 90° | P/P@400-800/266 nm | THG@800NM, Type I |
10x10 mm | 0.1, 0.5, 1 | 44.3° | 90° | P/P@400-800/266 nm | THG@800NM, Type I |
6x6 mm | 0.5, 1, 1.5 | 23.4° | 90° | AR/Ar@515+1030 nm | SHG@1030NM, Type I |
6x6 mm | 0.15, 0.25, 0.55 | 32.5° | 90° | AR/Ar@1030+515/343 nm | THG@1030, Type I |
10x10 mm | 0.5, 1 | 23.4° | 90° | AR/Ar@515+1030 nm | SHG@1030NM, Type I |
Crystal Structure | Orthorhombic, space group Pna21, point group mm2 |
Unit Cell Parameters | a=8.4473 Å, b=7.3788 Å, c=5.1395 Å, Z=4 |
Melting Point | ~834 ℃ |
Mohs Hardness | 6 Mohs |
Density | 2.47 g/cm³ |
Thermal Conductivity | 3.5 W/m/K |
Thermal Expansion Coefficient | αx=10.8×10^-5 /K, αy=-8.8×10^-5 /K, αz=3.4×10^-5 /K |
Transmission Range | 160-2600 nm |
SHG Phase Matching Range | 551-2600 nm (TypeⅠ), 790-2150 nm (Type Ⅱ) |
Thermal Optic Coefficient (/℃, λ in μm) | dnx/dT=-9.3×10⁻⁶ dny/dT=-13.6×10⁻⁶ dnz/dT= (-6.3-2.1λ)×10⁻⁶ |
Absorption Coefficient | <0.1%/cm @ 1064 nm, <0.3%/cm @ 532 nm |
Acceptance Angle | 6.54 mrad·cm (Ф, Type Ⅰ, 1064 SHG) 15.27 mrad·cm (θ, Type Ⅱ, 1064 SHG) |
Temperature Bandwidth | 4.7℃·cm (Type Ⅰ, 1064 SHG) 7.5℃·cm (Type Ⅱ, 1064 SHG) |
Acceptance Spectral Width | 1.0 nm·cm (Type Ⅰ, 1064 SHG) 1.3 nm·cm (Type Ⅱ, 1064 SHG) |
Walk-off Angle | 0.60° (Type Ⅰ, 1064 SHG) 0.12° (Type Ⅱ, 1064 SHG) |
NLO Coefficients | deff (Ⅰ)=d32cosФ (Type Ⅰ, XY plane) deff (Ⅰ)=d31cos2θ+d32sin2θ (Type Ⅰ, XZ plane) deff (Ⅱ)=d31cosθ (Type Ⅱ, YZ plane) deff (Ⅱ)=d31cos2θ+d32sin2θ (Type Ⅱ, XZ plane) |
Non-zero Nonlinear Optical Coefficients | d31=1.05±0.09 pm/V d32=-0.98±0.09 pm/V d33=0.05±0.006 pm/V |
Sellmeier Equations (λ in μm) | nx² = 2.454140 + 0.011249 / (λ² - 0.011350) - 0.014591 λ² - 6.60 × 10⁻⁵ λ⁴ ny² = 2.539070 + 0.012711 / (λ² - 0.012523) - 0.018540 λ² + 2.00 × 10⁻⁴ λ⁴ nz² = 2.586179 + 0.013099 / (λ² - 0.011893) - 0.017968 λ² - 2.26 × 10⁻⁴ λ⁴ |
LBO crystals can be used for second and third-harmonic generation (SHG and THG) phase matching of Nd: YAG and Nd: YLF lasers, supporting both Type I and Type II phase matching. At room temperature, within the broad wavelength range of 551 nm to 2600 nm, Type I phase matching with the highest effective nonlinear optical coefficients can be achieved on the XY and XZ planes, while the optimal Type II phase matching for LBO crystals occurs on the YZ and XZ planes. As shown in the figure below:
LBO Crystal SHG Tuning Curve
SHG Characteristics of Type I NCPM for 1064 nm Light | |
NCPM Temperature | 148 ℃ |
Acceptance Angle | 52 mrad•cm |
Walk-off Angle | 0 |
Temperature Bandwidth | 4 ℃•cm |
Effective SHG Coefficient | 2.69×d36 (KDP) = 1.18 pm/V |
Type I OPO Tuning Curve of LBO Crystals Type II OPO Tuning Curve of LBO Crystals
LBO crystals can achieve both angle-tuning NCPM and spectral-tuning NCPM (SNCPM). These spectral characteristics of LBO crystals are particularly suitable for frequency doubling of broadband coherent radiation around 1.3 μm, such as certain diode lasers and OPA/OPO outputs without linewidth narrowing components.
1. Frequency Doubling:
2. Frequency Tripling
Lithium Triborate (LBO) Crystal will be securely packaged in sturdy containers with cushioning materials to prevent movement or damage during shipping. This careful packaging ensures that the product arrives in perfect condition, maintaining its high-quality standards throughout the delivery process.
Heeger Materials Inc., a professional supplier and manufacturer of high-quality Nonlinear Crystals products including Lithium Triborate (LBO) Crystal, leverages extensive expertise in supply and export to offer competitive prices. We provide customized solutions to meet specific requirements, ensuring exceptional quality and customer satisfaction.
Heeger Materials Inc. was established in 2016 in Colorado, USA. We specialize in premium-grade metals, alloys, ceramics, powders, and other materials catering to research, development, and large-scale industrial production in scientific and industrial sectors.
Nonlinear Crystal Type | BBO, ß-BaB₂O₄ | KTP, KTiOPO₃ | LBO, LiB₃O₅ | BIBO, BiB₃O₆ | CLBO, CsLiB₆O₁₀ |
Transmission Range (nm) | 190-3500 | 350-4500 | 160-2600 | 286-2500 | 180-2750 |
SHG Phase-Matching Range (nm) | 409.6-3500 (Type I) 25-3500 (Type II) | 994-2000 (Type II) | 551-2600 (Type I) 790-2150 (Type II) | 574-2480 | 473-2750 (Type I) 636-2750 (Type II) |
Effective Nonlinear Coefficient deff SHG 1064 nm [pm/V] | 2.14 (Type I) 1.47 (Type II) | 4.03 (Type II) | 0.82 (Type I) | 3.34 | 0.9 (Type I, 4HG) 1.19 (Type I, 5HG) 0.95 (Type II) |
Absorption Coefficient [%/cm] | <0.1@1064nm <1@532nm | <0.1@1064nm <1@532nm | <0.1@1064nm <0.3@532nm | <0.1@1064nm | <0.03@1064nm <0.1@532nm |
Acceptance Angle SHG 1064 nm [mrad/cm] | 0.8 (Type I) 1.27 (Type II) | 14.2 (φ) 55.3 (θ) | 6.54 (Type I) 15.27 (Type II) | 1.03 (ee-o) | 0.45 (Type I, 4HG) 0.42 (Type I, 5HG) 1.90 (Type II) |
Walk-off Angle SHG 1064 nm [mrad] | 55.6 (Type I) 69.4 (Type II) | 4.87 (Type II) | 6.7 (Type I) 6.4 (Type II) | 24.5 (Type I) | 7.85 (Type I, 4HG) 7.33 (Type I, 5HG) 33.1 (Type II) |
Acceptance Temperature SHG 1064 nm [°C/cm] | 70 | 24 | 6.7 (Type I) 7.5 (Type II) | 2.17 | 8.30 (Type I, 4HG) 4.60 (Type I, 5HG) 43.1 (Type II) |
Acceptance Spectrum | 1.1 | 0.56 | 1.0 (Type I) 1.3 (Type II) | 0.96 (ee-o) | 0.13 (Type I, 4HG) 0.16 (Type I, 5HG) 5.60 (Type II) |
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