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Нелинейные оптические кристаллы NLO Crystal литиевый триборат LBO для SHG
- Категории: Crystals, Oscillators and Resonators >>>
- Поставщик: Hangzhou,Brandnew,Technology,Co.,Ltd.
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Product Description
Nonlinear Optical NLO Crystal Lithium Triborate LBO Crystals for SHG THG
Lithium Triborate (LiB3O5 or LBO) is an excellent nonlinear optical crystal
Features
• Broad transparency range from 160nm to 2600nm (see Figure 1);
• High optical homogeneity (δn≈10-6/cm) and being free of inclusion;
• Relatively large effective SHG coefficient (about three times that of KDP);
• High damage threshold;
• Wide acceptance angle and small walk-off;
• Type I and type II non-critical phase matching (NCPM) in a wide wavelength range;
• Spectral NCPM near 1300nm.
• Broad transparency range from 160nm to 2600nm (see Figure 1);
• High optical homogeneity (δn≈10-6/cm) and being free of inclusion;
• Relatively large effective SHG coefficient (about three times that of KDP);
• High damage threshold;
• Wide acceptance angle and small walk-off;
• Type I and type II non-critical phase matching (NCPM) in a wide wavelength range;
• Spectral NCPM near 1300nm.
Specification
Chemical and Structural Properties | ||
Crystal Structure | Orthorhombic, Space group Pna21, Point group mm2 | |
Lattice Parameter | a=8.4473Å,b=7.3788Å,c=5.1395Å,Z=2 | |
Melting Point | About 834℃ | |
Mohs Hardness | 6 | |
Density | 2.47g/cm3 | |
Thermal Expansion Coeficients | αx=10.8x10-5/K, αy=-8.8x10-5/K,αz=3.4x10-5/K | |
Thermal Conductivity Coefficients | 3.5W/m/K | |
Optical and Nonlinear Optical Properties | ||
Transparency Range | 160-2600nm | |
SHG Phase Matchable Range | 551-2600nm (Type I) 790-2150nm (Type II) | |
Therm-optic Coefficient (/℃, λ in μm) | dnx/dT=-9.3X10-6 dny/dT=-13.6X10-6 dnz/dT=(-6.3-2.1λ)X10-6 | |
Absorption Coefficients | <0.1%/cm at 1064nm <0.3%/cm at 532nm | |
Angle Acceptance | 6.54mrad·cm (φ, Type I,1064 SHG) 15.27mrad·cm (θ, Type II,1064 SHG) | |
Temperature Acceptance | 4.7℃·cm (Type I, 1064 SHG) 7.5℃·cm (Type II, 1064 SHG) | |
Spectral Acceptance | 1.0nm·cm (Type I, 1064 SHG) 1.3nm·cm (Type II, 1064 SHG) | |
Walk-off Angle | 0.60° (Type I 1064 SHG) 0.12° (Type II 1064 SHG) | |
NLO Coefficients | deff(I)=d32cosΦ (Type I in XY plane) deff(I)=d31cos2θ+d32sin2θ (Type I in XZ plane) deff(II)=d31cosθ (Type II in YZ plane) deff(II)=d31cos2θ+d32sin2θ (Type II in XZ plane) | |
Non-vanished NLO susceptibilities | 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)-0.014591λ2-6.60×10-5λ4 ny2=2.539070+0.012711/(λ2-0.012523)-0.018540λ2+2.00×10-4λ4 nz2=2.586179+0.013099/(λ2-0.011893)-0.017968λ2-2.26×10-4λ4 | |
Transparency curve of LBO
• Dimension tolerance: (W±0.1mm)x(H±0.1mm)x(L+0.5/-0.1mm) (L≥2.5mm)
(W±0.1mm)x(H±0.1mm)x(L+0.1/-0.1mm) (L<2.5mm)
• Clear aperture: central 90% of the diameter
• No visible scattering paths or centers when inspected by a 50mW green laser
• Flatness: less than λ/8 @ 633nm
• Transmitting wavefront distortion: less than λ/8 @ 633nm
• Chamfer: ≤0.2mm x 45°
• Chip: ≤0.1mm
• Scratch/Dig code: better than 10/ 5 to MIL-PRF-13830B
• Parallelism: better than 20 arc seconds
• Perpendicularity: ≤5 arc minutes
• Angle tolerance: △θ≤0.25°, △φ≤0.25°
• Damage threshold[GW/cm2 ]: >10 for 1064nm, TEM00, 10ns, 10HZ (polished only)
>1 for 1064nm, TEM00, 10ns, 10HZ (AR-coated)
>0.5 for 532nm, TEM00, 10ns, 10HZ (AR-coated)
(W±0.1mm)x(H±0.1mm)x(L+0.1/-0.1mm) (L<2.5mm)
• Clear aperture: central 90% of the diameter
• No visible scattering paths or centers when inspected by a 50mW green laser
• Flatness: less than λ/8 @ 633nm
• Transmitting wavefront distortion: less than λ/8 @ 633nm
• Chamfer: ≤0.2mm x 45°
• Chip: ≤0.1mm
• Scratch/Dig code: better than 10/ 5 to MIL-PRF-13830B
• Parallelism: better than 20 arc seconds
• Perpendicularity: ≤5 arc minutes
• Angle tolerance: △θ≤0.25°, △φ≤0.25°
• Damage threshold[GW/cm2 ]: >10 for 1064nm, TEM00, 10ns, 10HZ (polished only)
>1 for 1064nm, TEM00, 10ns, 10HZ (AR-coated)
>0.5 for 532nm, TEM00, 10ns, 10HZ (AR-coated)
AR-coatings:
BrandNew provides the following AR-coatings:
• Dual Band AR-coating (DBAR) of LBO for SHG of 1064nm.
low reflectance (R<0.2% at 1064nm and R<0.5% at 532nm), super low reflectivity of R<0.05% at 1064nm and R<0.1% at 532nm is available upon request; high damage threshold (＞500MW/cm2 at both wavelengths); long durability.
• Broad Band AR-coating (BBAR) of LBO for SHG of tunable lasers.
• Other coatings are available upon request.
BrandNew provides the following AR-coatings:
• Dual Band AR-coating (DBAR) of LBO for SHG of 1064nm.
low reflectance (R<0.2% at 1064nm and R<0.5% at 532nm), super low reflectivity of R<0.05% at 1064nm and R<0.1% at 532nm is available upon request; high damage threshold (＞500MW/cm2 at both wavelengths); long durability.
• Broad Band AR-coating (BBAR) of LBO for SHG of tunable lasers.
• Other coatings are available upon request.
Applications
SHG and THG at Room Temperature:
LBO is phase matchable for the SHG and THG of Nd:YAG and Nd:YLF lasers, using either type I or type II interaction. For the SHG at room temperature, type I phase matching can be reached and has the maximum effective SHG coefficient in the principal XY and XZ planes (see Fig. 2) in a wide wavelength range from 551nm to about 2600nm (the effective SHG coefficient see Table 2).
The optimum type II phase matching falls in the principal YZ and XZ planes (see Fig. 2), (the effective SHG coefficient see Table 2).
SHG conversion efficiencies of more than 70% for pulse and 30% for cw Nd:YAG lasers, and THG conversion efficiency over 60% for pulse Nd:YAG laser have been observed by using CASTECH's LBO crystals.
LBO is phase matchable for the SHG and THG of Nd:YAG and Nd:YLF lasers, using either type I or type II interaction. For the SHG at room temperature, type I phase matching can be reached and has the maximum effective SHG coefficient in the principal XY and XZ planes (see Fig. 2) in a wide wavelength range from 551nm to about 2600nm (the effective SHG coefficient see Table 2).
The optimum type II phase matching falls in the principal YZ and XZ planes (see Fig. 2), (the effective SHG coefficient see Table 2).
SHG conversion efficiencies of more than 70% for pulse and 30% for cw Nd:YAG lasers, and THG conversion efficiency over 60% for pulse Nd:YAG laser have been observed by using CASTECH's LBO crystals.
SHG tuning curves of LBO
Applications:
• More than 480mW output at 395nm is generated by frequency doubling a 2W mode-locked Ti:Sapphire laser (<2ps, 82MHz). The wavelength range of 700-900nm is covered by a 5x3x8mm3 LBO crystal.
• Over 80W green output is obtained by SHG of a Q-switched Nd:YAG laser in a type II 18mm long LBO crystal.
• The frequency doubling of a diode pumped Nd:YLF laser (>500μJ @ 1047nm,<7ns, 0-10KHz) reaches over 40% conversion efficiency in a 9mm long LBO crystal.
• The VUV output at 187.7 nm is obtained by sum-frequency generation.
• 2mJ/pulse diffraction-limited beam at 355nm is obtained by intracavity frequency tripling a Q-switched Nd:YAG laser.
Non-Critical Phase Matching:
As shown in Table 3, Non-Critical Phase Matching (NCPM) of LBO is featured by no walk-off, very wide acceptance angle and maximum effective coefficient. It promotes LBO to work in its optimal condition. SHG conversion efficiencies of more than 70% for pulse and 30% for cw Nd:YAG lasers have been obtained, with good output stability and beam quality.
As shown in Fig.3, type I and type II non-critical phase matching can be reached along x-axis and z-axis at room temperature, respectively.(CASTECH develops an assembly of oven and temperature controller for NCPM applications. Please refer to Page 69 for more technical data).
• More than 480mW output at 395nm is generated by frequency doubling a 2W mode-locked Ti:Sapphire laser (<2ps, 82MHz). The wavelength range of 700-900nm is covered by a 5x3x8mm3 LBO crystal.
• Over 80W green output is obtained by SHG of a Q-switched Nd:YAG laser in a type II 18mm long LBO crystal.
• The frequency doubling of a diode pumped Nd:YLF laser (>500μJ @ 1047nm,<7ns, 0-10KHz) reaches over 40% conversion efficiency in a 9mm long LBO crystal.
• The VUV output at 187.7 nm is obtained by sum-frequency generation.
• 2mJ/pulse diffraction-limited beam at 355nm is obtained by intracavity frequency tripling a Q-switched Nd:YAG laser.
Non-Critical Phase Matching:
As shown in Table 3, Non-Critical Phase Matching (NCPM) of LBO is featured by no walk-off, very wide acceptance angle and maximum effective coefficient. It promotes LBO to work in its optimal condition. SHG conversion efficiencies of more than 70% for pulse and 30% for cw Nd:YAG lasers have been obtained, with good output stability and beam quality.
As shown in Fig.3, type I and type II non-critical phase matching can be reached along x-axis and z-axis at room temperature, respectively.(CASTECH develops an assembly of oven and temperature controller for NCPM applications. Please refer to Page 69 for more technical data).
NCPM temperature tuning curves of LBO
Properties of type I NCPM SHG at 1064nm | ||
NCPM Temperature | 148℃ | |
Acceptance Angle | 52 mrad·cm | |
Walk-off Angle | 0 | |
Temperature Bandwidth | 4℃·cm | |
Effective SHG Coefficient | 2.69 x d36(KDP) | |
Applications:
• Over 11W of average power at 532nm was obtained by extra-cavity SHG of a 25W Antares mode-locked Nd:YAG laser (76MHz, 80ps).
• 20W green output was generated by frequency doubling a medical, multi-mode Q-switched Nd:YAG laser. Higher green output is expected with higher input power.
LBO's OPO and OPA:
LBO is an excellent NLO crystal for OPOs and OPAs with a widely tunable wavelength range and high powers. These OPO and OPA which are pumped by the SHG and THG of Nd:YAG laser and XeCl excimer laser at 308nm have been reported. The unique properties of type I and type II phase matching as well as the NCPM leave a large room in the research and applications of LBO's OPO and OPA. Fig.4 shows the calculated type I OPO tuning curves of LBO pumped by the SHG, THG and 4HG of Nd:YAG laser in XY plane at the room temperature. And Fig. 5 illustrates type II OPO tuning curves of LBO pumped by the SHG and THG of Nd:YAG laser in XZ plane.
• Over 11W of average power at 532nm was obtained by extra-cavity SHG of a 25W Antares mode-locked Nd:YAG laser (76MHz, 80ps).
• 20W green output was generated by frequency doubling a medical, multi-mode Q-switched Nd:YAG laser. Higher green output is expected with higher input power.
LBO's OPO and OPA:
LBO is an excellent NLO crystal for OPOs and OPAs with a widely tunable wavelength range and high powers. These OPO and OPA which are pumped by the SHG and THG of Nd:YAG laser and XeCl excimer laser at 308nm have been reported. The unique properties of type I and type II phase matching as well as the NCPM leave a large room in the research and applications of LBO's OPO and OPA. Fig.4 shows the calculated type I OPO tuning curves of LBO pumped by the SHG, THG and 4HG of Nd:YAG laser in XY plane at the room temperature. And Fig. 5 illustrates type II OPO tuning curves of LBO pumped by the SHG and THG of Nd:YAG laser in XZ plane.
Type I OPO tuning curves of LBO
Type II OPO tuning curves of LBO
Applications:
• A quite high overall conversion efficiency and 540-1030nm tunable wavelength range were obtained with OPO pumped at 355nm.
• Type I OPA pumped at 355nm with the pump-to-signal energy conversion efficiency of 30% has been reported.
• Type II NCPM OPO pumped by a XeCl excimer laser at 308nm has achieved 16.5% conversion efficiency, and moderate tunable wavelength ranges can be obtained with different pumping sources and temperature tuning.
• By using the NCPM technique, type I OPA pumped by the SHG of a Nd:YAG laser at 532nm was also observed to cover a wide tunable range from 750nm to 1800nm by temperature tuning from 106.5℃ to 148.5℃.
• By using type II NCPM LBO as an optical parametric generator (OPG) and type I critical phase-matched BBO as an OPA, a narrow linewidth (0.15nm) and high pump-to-signal energy conversion efficiency (32.7%) were obtained when it is pumped by a 4.8mJ, 30ps laser at 354.7nm. Wavelength tuning range from 482.6nm to 415.9nm was covered either by increasing the temperature of LBO or by rotating BBO.
LBO's Spectral NCPM:
Not only the ordinary non-critical phase matching (NCPM) for angular variation but also the non-critical phase matching for spectral variation (SNCPM) can be achieved in the LBO crystal. As shown in Fig.2, the phase matching retracing positions are λ1 =1.31μm with θ =86.4°, φ=0° for Type I and λ2=1.30 μm with θ =4.8°, φ=0° for Type II. The phase matching at these positions possess very large spectral acceptances Δλ. The calculated Δλ at λ1 and λ2 are 57nm·cm and 74nm·cm respectively, which are much larger than that of other NLO crystals. These spectral characteristics are very suitable for doubling broadband coherent radiations near 1.3 μm, such as those from some diode lasers, and some OPA/OPO output without linewidth-narrowing components.
• A quite high overall conversion efficiency and 540-1030nm tunable wavelength range were obtained with OPO pumped at 355nm.
• Type I OPA pumped at 355nm with the pump-to-signal energy conversion efficiency of 30% has been reported.
• Type II NCPM OPO pumped by a XeCl excimer laser at 308nm has achieved 16.5% conversion efficiency, and moderate tunable wavelength ranges can be obtained with different pumping sources and temperature tuning.
• By using the NCPM technique, type I OPA pumped by the SHG of a Nd:YAG laser at 532nm was also observed to cover a wide tunable range from 750nm to 1800nm by temperature tuning from 106.5℃ to 148.5℃.
• By using type II NCPM LBO as an optical parametric generator (OPG) and type I critical phase-matched BBO as an OPA, a narrow linewidth (0.15nm) and high pump-to-signal energy conversion efficiency (32.7%) were obtained when it is pumped by a 4.8mJ, 30ps laser at 354.7nm. Wavelength tuning range from 482.6nm to 415.9nm was covered either by increasing the temperature of LBO or by rotating BBO.
LBO's Spectral NCPM:
Not only the ordinary non-critical phase matching (NCPM) for angular variation but also the non-critical phase matching for spectral variation (SNCPM) can be achieved in the LBO crystal. As shown in Fig.2, the phase matching retracing positions are λ1 =1.31μm with θ =86.4°, φ=0° for Type I and λ2=1.30 μm with θ =4.8°, φ=0° for Type II. The phase matching at these positions possess very large spectral acceptances Δλ. The calculated Δλ at λ1 and λ2 are 57nm·cm and 74nm·cm respectively, which are much larger than that of other NLO crystals. These spectral characteristics are very suitable for doubling broadband coherent radiations near 1.3 μm, such as those from some diode lasers, and some OPA/OPO output without linewidth-narrowing components.
Company Profile
Cooperated with Institute of semiconductors Chinese academy of sciences and Zhejiang University, Today, over 60 technicians and 2 scientists, 20 technicians are with PHD degree. Production space is 10000 Class Lab Clean Room with 2000 square meters.
BrandNew's strengths are in talent employees, quality engineering,Process control, product development and volume manufacturing.
BrandNew's strengths are in talent employees, quality engineering,Process control, product development and volume manufacturing.
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