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| Products
-> Crystal -> BBO |
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| BBO
Beta Barium Borate
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| BBO
(beta-BaB2O4 ) is a nonlinear optical crystal which combines a number of
unique features. These features include wide transparency and phase matching
ranges, large nonlinear coefficient, high damage threshold and excellent
optical homogeneity. Therefore, BBO provides an attractive solution for
various nonlinear optical applications. |
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| BBO
crystal is also an excellent electro-optic crystal for high power applications
at the wavelength range from 200nm to 2500nm. It can be used for Q-Switching
in a CW diode pumped Nd:YAG laser with average power>50W. |
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| Main
Features |
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- Good
mechanical and physical properties
- Broad
phase-matchable second-harmonic-generation (SHG) range from 409.6 nm
to 3500 nm
- Wide
transmission region from 190 nm to 3500 nm
- Large
effective SHG coefficient
- High
damage threshold of 10 GW/cm2 for 100 ps
pulse-width at 1064 nm
- High
optical homogeneity with Δn=10-6/cm
- Wide
temperature-bandwidth of about 55℃
(for type I SHG 1064 nm)
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| Typical
Applications |
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- Second, third,
fourth and fifth harmonic generation of Nd:YAG and Nd:YLF laser
- Frequency-doubling,
-tripling and -mixing of Dye lasers
- Second, third and
fourth harmonic generation of Ti:Sapphire and Alexandrite lasers
- Optical parametric
amplifier (OPA) and optical parametric oscillators (OPO)
- Frequency-doubling
of Argon ion, Cu-vapor and Ruby lasers
- Research and development
for advanced laser techniques, including all-solid state wide-tunable
lasers, ultrafast pulse lasers, and DUV lasers
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| Specifications |
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| Dimension
Tolerance |
(W±0.1mm)
x (H±0.1mm) x (L±0.2mm) |
| Angle
Tolerance |
Δθ<
0.5°, ΔΦ< 0.5° |
| Surface
Flatness |
<λ/8@633
nm |
| Surface
Quality |
Better
than 20/10 Scratch and Dig |
| Parallelism |
<
20 arc seconds |
| Perpendicularity |
<
5 arc minutes |
| Clear
Aperture |
>
90% Central |
| Wavefront
Distortion |
<λ/4@633
nm |
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| Physical
and Optical Properties |
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| Crystal Structure |
trigonal, space group
R3c |
| Cell Parameters |
a = b = 12.532Å,
c = 12.717Å, Z = 6 |
| Melting Point |
1095±5oC |
| Transition Temperature |
925±5oC |
| Optical Homogeneity |
10-6/cm |
| Mohs Hardness |
4.5 |
| Density |
3.85 g/cm3 |
| Linear Absorption
Coefficient |
< 0.1%/cm (at
1064 nm) |
| Hygroscopic
Susceptibility |
low |
| Resistivity |
> 1011 ohm/cm |
| Relative Dielectric
Constant |
eT11/e0: 6.7,
eT33/e0:
8.1
Tan d, < 0.001 |
| Thermal Expansion
Coefficients(in the range of 25-900℃) |
^c, 4 x 10-6/K
||c, 36 x 10-6/K |
| Thermal Conductivity |
^c,
1.2 W/m/K; ||c, 1.6 W/m/K |
| Transparency
Range |
189
- 3500 nm |
| Therm-Optic
Coefficients |
dno/dT
= - 9.3 x 10-6/0C;dne/dT = -16.6
x 10-6/0C |
| NLO
coefficients |
d11
= 5.8 x d36(KDP)
d31 = 0.05 x d11, d22<
0.05 x d11 |
| Electro-Optic
Coefficients |
g11
= 2.7 pm/V, g22,
g31<
0.1 g11 |
| Half-Wave
Voltage |
48
KV (at 1064 nm) |
| Phase-matchable
SHG range |
189-1750nm |
| Damage
Threshold |
@1.064
mm |
5
GW/cm2 (10 ns); 10 GW/cm2 (1.3 ns) |
| @0.532
mm |
1
GW/cm2 (10 ns); 7 GW/cm2 (250 ps) |
| @0.266
mm |
120
MW/cm2 (8ns) |
| Sellmeier
Equations(l in mm) |
no2(l)
= 2.7359+0.01878/(l2-0.01822)-0.01354 l 2
ne2(l) = 2.3753+0.01224/(l2-0.01667)-0.01516 l 2 |
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| Standard
Parameter for Different Application |
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| 1)
Harmonic generations of Nd:YAG lasers: |
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| 1064nm
SHG-> 532nm:
Type I, Theta=22.8deg, Phi=0deg |
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| 1064nm
THG-> 355nm:
Type I, Theta=31.3deg, Phi=0deg |
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Type II, Theta=38.6deg, Phi=30deg |
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| 1064nm
4HG-> 266nm:
Type I, Theta=47.6deg, Phi=0deg |
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| 1064nm
5HG-> 213nm:
Type I, Theta=51.1deg, Phi=0deg |
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| 2)
OPO and OPA pumped by harmonics of Nd:YAG lasers |
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| 532nm
Pump-> 680-2600nm:
Type I, Theta=21deg, Phi=0deg |
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| 355nm
Pump-> 410-2600nm:
Type I, Theta=30deg, Phi=0deg |
| Type
II, Theta=37deg, Phi=30deg |
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| 266nm
Pump-> 295-2600nm:
Type I, Theta=39deg, Phi=0deg |
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| 3)
Frequency doubling of dye lasers |
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| 670-530nm
SHG-> 355-260nm: Type I, Theta=40deg, Phi=0deg |
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| 600-440nm
SHG-> 300-220nm: Type I, Theta=55deg, Phi=0deg |
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| 444-410nm
SHG-> 222-205nm: Type I, Theta=80deg, Phi=0deg |
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| 4)
Harmonic generations of Ti:Sapphire lasers |
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| 700-1000nm
SHG-> 350-500nm:
Type I, Theta=28deg, Phi=0deg |
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| 700-1000nm
THG->240-330nm:
Type I, Theta=42deg, Phi=0deg |
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| 700-1000nm
FHG-> 210-240nm:
Type I, Theta=28deg, Phi=0deg |
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| 5)
Frequency doubling and tripling of Alexandrite lasers. |
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| 720-800nm
SHG-> 360-400nm:
Type I, Theta=31deg, Phi=0deg |
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| 720-800nm
THG-> 240-265nm:
Type I, Theta=48deg, Phi=0deg |
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| 6)
Intracavity SHG of Ar+ laser with Brewster angle cut BBO |
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| 514nm
SHG-> 257nm:
Type I, Theta=51deg, Phi=0deg |
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| 488nm
SHG-> 244nm:
Type I, Theta=55deg, Phi=0deg |
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| Standard
Product Series |
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Part
No. |
Size(mm) |
θ |
Φ |
Coating |
Type |
Unit
Price |
BBO101 |
4x4x7 |
22.8° |
0° |
AR/AR@1064&532nm |
I |
$408 |
BBO102 |
4x4x7 |
47.6° |
0° |
AR/AR@532&266nm |
I |
$408 |
BBO103 |
4x4x10 |
22.8° |
0° |
AR/AR@1064&532nm |
I |
$518 |
BBO104 |
4x4x10 |
47.6° |
0° |
AR/AR@532&266nm |
I |
$518 |
BBO105 |
5x5x2 |
29.2° |
0° |
AR/AR@800&400nm |
I |
$338 |
BBO106 |
5x5x1 |
29.2° |
0° |
AR/AR@800&400nm |
I |
$368 |
BBO107 |
5x5x0.3-0.5 |
29.2° |
0° |
AR/AR@800&400nm |
I |
$398 |
BBO108 |
5x5x0.1 |
29.2° |
0° |
AR/AR@800&400nm |
I |
$450 |
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