VLIN’s BBO is featured by
•
Broad phase matchable range from 409.6 nm to 3500 nm;
•
Wide transmission region from 190 nm to 3500 nm;
•
Large effective second-harmonic-generation (SHG) coefficient
about 6 times greater than that of KDP
crystal;
•
High damage threshold;
•
High optical homogeneity with
dn
»10-6/cm;
•
Wide temperature-bandwidth of about 55°C.
VLIN offers BBO of
• Strict
quality control;
• Crystal
length from 0.02mm to 25mm and size up to 15x15x15 mm3;
• P-coatings,
AR-coatings, mounts and re-polishing services;
• A
large quantity of crystals in stock
• Fast
delivery (15 days for polished only,20 days for AR-coated).
Basic Properites of BBO
Table 1.Chemical and Structural properties of BBO
Crystal Structure:
|
Trigonal, space group R3c
|
Lattics Parameters:
|
a=b=12.532Å, c=12.717Å, Z=6
|
Melting point
|
About 1095℃
|
Mohs Hardness
|
4
|
Density
|
3.85g/cm3
|
Thermal Conductivity
|
1.2W/m/K(┴c):
1.6W/m/K(//c)
|
Thermal Expansion Coefficients
|
a11=4x10-6/K;
a33=36x10-6/K
|
Table
2.Optical and Nontinear Optical Properties Of BBO
Transparency
Range:
|
190-3500nm
|
SHG Phase Matchable Range
|
409.6-3500nm(Type I)
525-3500nm(Type II)
|
therm-optic Coefficients(/℃)
|
dno/dT=-16.6X10-6
dne/dT=-9.3X10-6
|
Absorption Coefficients
|
<0.1%/cm at 1064nm
<1%/cm at 532nm
|
Angle Acceptance
|
0.8mrad-cm (θ, Type I,1064
SHG)
1.27mrad-cm
(θ, Type II,1064 SHG)
|
Temperature Acceptance
|
55℃-cm
|
Spectral Acceptance
|
1.1nm-cm
|
Walk-off Angle
|
2.7° (Type I 1064 SHG)
3.2° (Type II 1064 SHG)
|
NLO Coefficients
|
deff (I)=d31sinθ+(d11cosΦ-d22sin3Φ)cosθ
deff (II)=(d11sin3Φ+d22cos3Φ)cos2θ
|
Non-vanished NLO
susceptibilities
|
d11=5.8xd36(KDP)
d31=0.05xd11
d22<0.05xd11
|
sellmeier Equations(λ in μm )
|
no2=2.7359+0.01878
/ (λ2-0.01822)
-0.01354 λ2
ne2=2.3753+0.01224
/ (λ2-0.01667)
-0.01516 λ2
|
Electro-optic coefficients:
|
r22=2.7pm/V
|
Half-wave voltage:
|
7KV (at 1064nm,3*3*20mm3)
|
Resistivity:
|
>1011 ohm-cm
|
Relative Dielectric Constant:
|
εs11/εo:6.7
εs33/εo:8.1
Tan δ<0.001
|
BBO
is a negative uniaxial crystal,with ordinary refractive-index(no)
larger than extraordinary refractive-index(ne).Both
type I and type II phase-matching can be reached by angle-tuning.The
phase matching angles of frequency doubling are shown in Fig.2.
Application in Nd:YAG Lasers
BBO
is an efficient NLO crystal for the second, third and fourth
harmonic generation of Nd:YAG lasers,and the best NLO crystal
for the fifth harmonic generation at 213nm. Conversion
efficiencies of more than 70% for SHG,60% for THG and 50% for
4HG,and 200mW output at 213 nm(5HG)have been
obtained,respectively.
BBO
is also an efficient crystal for the intracavity SHG of high
power Nd:YAG lasers. For the intracavity SHG of an acousto-optic
Q-switched Nd:YAG laser, more than 15 W average power at 532 nm
was generated in a VLIN AR-coated BBO crystal. When pumped by
the 600 mW SHG output of a mode-locked Nd:YLF laser, 66 mW
output at 266 nm was produced from a Brewster-angle-cut BBO in
an external enhanced resonant cavity.
Because of a small acceptance angle and large walk-off, good
laser beam quality (small divergence, good mode condition,etc.)
is the key for BBO to obtain high conversion efficiency. Tight
focus of laser beam is not recommended by VLIN's engineers.
Applications in Tunable Lasers
1.Dye lasers
Efficient UV output (205nm-310nm) with a SHG efficiency of over
10% at wavelength of ≥206nm was obtained in type I BBO, and 36%
conversion efficiency was achieved for a XeC1-laser pumped Dye
laser with power 150KW which is about 4-6 times higher than that
in ADP. The shortest SHG wavelength of 204.97 nm with efficiency
of about 1% has been generated in BBO.
VLIN’s BBO is widely used in the Dye lasers. With type I
sum-frequency of 780-950 nm and 248.5 nm (SHG output of 495 nm
dye laser) in BBO, the shortest UV outputs ranging from 188.9nm
to 197 nm and the pulse energy of 95 mJ at 193 nm and 8 mJ at
189 nm have been obtained in BBO, respectively.
2.Ultrafast Pulse Laser
Frequency-doubling and -tripling of ultrashort-pulse lasers are
the applications in which BBO shows superior properties to KDP
and ADP crystals. Now, VLIN can provide as thin as 0.01mm BBO
for this purpose. A laser pulse as short as 10 fs can be
efficiently frequency-doubled with a thin BBO, in terms of both
phase-velocity and group-velocity matching.
3.Ti:Sapphire and Alexandrite lasers
UV output in the region 360nm -390nm with pulse energy of 105 mJ(31%
SHG efficiency) at 378 nm, and output in the region 244nm-259nm
with 7.5 mJ(24% mixing efficiency) have been obtained for type I
SHG and THG of an Alexandrite laser in BBO crystal.
More than 50% of SHG conversion efficiency in a Ti:Sapphire
laser has been obtained in BBO. High conversion efficienies have
been also obtained in BBO for the THG and FHG of Ti:Sapphire
lasers.
4. Argon Ion and Copper-Vapor lasers
By employing the intracavity frequency-doubling technique in an
Argon Ion laser with all lines output power of 2W, maximum 33 mW
at 250.4 nm and thirty-six lines of deep UV wavelengths ranging
from 228.9 nm to 257.2 nm were generated in a Brewster-angle-cut
BBO crystal.
Up to 230 mW average power was generated in BBO at 255.3 nm with
maximum 8.9% conversion efficiency was achieved for the SHG of a
Copper-Vapor laser at 510.6 nm.
BBO’s OPO and OPA
The OPO and OPA of BBO are powerful tools for generating a
widely tunable coherent radiation from the UV to IR. The tuning
angles of type I and type II BBO OPO and OPA have been
calculated, with the results shown in Fig.3and Fig.4,
respectively.
1.OPO pumped at 532 nm
An OPO output ranging from 680 nm to 2400 nm with the peak power
of 1.6MW and up to 30% energy conversion efficiency was obtained
in a 7.2 mm long type I BBO. The input pump energy was 40 mJ at
532nm with pulse-width 75ps. With a longer BBO crystal, higher
conversion efficiency is expected.
2.OPO and OPA pumped at 355 nm
In the case of Nd:YAG pumping,BBO’s OPOs can generate more than
100mJ,with wavelength tunable from 400nm to 2000nm. Using VLIN’s
BBO crystal, the OPO system covers a tuning range from 400nm to
3100nm which guarantees a maximum of 30% and more than 18%
conversion efficiency, over the wavelength range from 430nm to
2000nm.
Type II BBO can be used to decrease linewidth near the
degenerate points. A linewidth as narrow as 0.05nm and usable
conversion efficiency of 12% were obtained. However, a longer
(>15mm) BBO should normally be used to decrease the oscillation
threshold when employing the type II phase-matching scheme.
Pumping with a picosecond Nd:YAG at 355nm, a
narrow-band(<0.3nm), high energy (>200μJ) and wide tunable
(400nm to 2000nm) pulse has been produced by BBO’s OPAs. This
OPA can reach as high as more than 50% conversion efficiency,
and therefore is superior to common Dye lasers in many respects,
including efficiency, tunable range, maintenance, and easiness
in design and operation. Furthermore, coherent radiation from
205 nm to 3500 nm can be also generated by BBO’s OPO or OPA plus
a BBO for SHG.
3.Others
A tunable OPO with signal wavelengths between 422 nm and 477 nm
has been generated by angle tuning in a type I BBO crystal
pumped by the fourth harmonic of a Nd:YAG laser (at 266 nm) has
been observed to cover the whole range of output wavelengths 330
nm -1370nm.
When pumped by a 1mJ, 80fs Dye laser at 615 nm,the OPA with two
BBO crystal yields more than 50μJ (maximum 130μJ),<200fs
ultrashort pulse, over 800 nm-2000 nm.
BBO`s E-O Applications
BBO
can also be used for E-O applications.It has wide transmission
range from UV to about 3500nm and it has much higher damage
threshold than KD*P or LiNbO3, More than 80W output
power and 50KHz repitition rate have been reached by using
VLIN`s E-O BBO crystal and Nd:YVO4 crystal as gain
media. At 5KHz,its pulse has width as short as 6.4ns,and energy
of 5.7mJ or peak power of 900 KW.It has advantages over the
commercial A-O Q-switched one , including a very short
pulse,high beam quality and size compact as well. Although it
has a relative small electro-optic coefficient,the Half-wave
voltage is high (7KV at 1064nm,3*3*20mm3),long and thin BBO can
reduce the voltage requirements.VLIN now can supply 25mm long
and 1mm thin high optical quality BBO crystal with Z-cut,
AR-coated and Gold/Chrome plated on the side faces.
Coatings of BBO
VLIN provides BBO with the following AR-coatings:
·
Dual Band AR-coating (DBAR)of BBO for SHG of 1064nm
low reflectance (R<0.2% at 1064nm and R<0.5% at 532nm);
high damage threshold (>300MW/cm2 at both wqvelengths);
long durability;
·
Broad Band AR-coating (BBAR) of BBO for SHG of tunable lasers.
·
Broad Band P-coating of BBO for OPO applications.
·
Other coatings are available upon request.
VLIN Warranty on BBO Specifications
·
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% or 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: ≤0.2mmx45°
·
Chip: ≤0.1mm
·
Scratch/Dig code: better than 10/5 to
MIL-PRF-13830B
·
Parallelism: ≤20 arc seconds
·
Perpendicularity:≤5 arc minutes
·
Angle tolerance:≤0.25°
·
Damage threshold[GW/cm2]:
>1 for 1064nm,TEM00,10ns,10HZ (polished only),
>0.5 for 1064nm,TEM00,10ns,10HZ(AR-coated) ;
>0.3 for 532nm,TEM00,10ns,10HZ(AR-coatd)
·
Quality Warranty Period: one year under proper use.
Notes
1.
BBO has a low susceptibility to the moisture. The user is
advised to provide dry conditions for both the use and preservation of BBO.
2.
BBO is relatively soft and therefore requires precautions to
protect its polished surfaces.
3.
When angle adjusting is necessary, keep in mind that the
acceptance angle of BBO is small.
4. VLIN engineers can select and design the best BBO crystal, if
the main parameters of your laser are provided, such as energy per pulse, pulse width and repetition
rate for a pulsed laser, power for a cw laser,
laser beam diameter, mode condition, divergence, wavelength
tuning range, etc.
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