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VLIN's KTP is featured by
• Large nonlinear optical coefficient
• Wide angular bandwidth and small walk-off angle
• Broad temperature and spectral bandwidth
• High electro-optic coefficient and low dielectric constant
• Large figure of merit
• Nonhydroscopic, chemically and mechanically stable
VLIN offers
· Strict quality control · large crystal size up to 20x20x40mm3 and maximum length of 60mm; · Quick delivery(2 weeks for polished only, 3 weeks for coated) · Unbeatable price and quantity discount · Technical support · AR-coating, mounting and re-polishing service
Table 1. Chemical and Structural properties
Crystal Structure
Orthorhombic, space group Pna21,point group mm2
Lattice Parameter
a=6.404?, b=10.616?, c=12.814?, Z=8
Melting Point
About 1172°C
Mohs Hardness
5
Density
3.01 g/cm3
Thermal Conductivity
13W/m/K
Thermal Expansion Coefficient
αx=11x10-6/°C, αy=9x10-6/°C, αz=0.6x10-6/°C
Table 2. Optical and Nonlinear Optical Properties
Transparency Range
350~4500nm
SHG Phase Matchable Range
497~1800nm (Type II)
Therm-optic Coefficients (/°C)
dnx/dT=1.1X10-5 dny/dT=1.3X10-5 dnz/dT=1.6X10-5
Absorption Coefficients
<0.1%/cm at 1064nm <1%/cm at 532nm
For Type II SHG of a Nd:YAG laser at 1064nm
Temperature Acceptance: 24°C-cm Spectral Acceptance: 0.56nm-cm Angular Acceptance: 14.2mrad-cm (φ);55.3mrad-cm (θ) Walk-off Angle: 0.55°
NLO Coefficients
deff(II)≈(d24-d15)sin2φsin2θ-(d15sin2φ + d24cos2φ)sinθ
Non-vanished NLO susceptibilities
d31=6.5 pm/V d24=7.6 pm/V d32=5 pm/V d15=6.1 pm/V d33=13.7 pm/V
Sellmeier Equations (λ in μm)
nx2=3.0065+0.03901/(λ2-0.04251)-0.01327λ 2 ny2=3.0333+0.04154/(λ 2-0.04547)-0.01408λ2 nz2=3.3134+0.05694/(λ 2-0.05658)-0.01682λ2
Applications for SHG and SFG of Nd: lasers
KTP is the most commonly used material for frequency doubling of Nd:YAG and other Nd-doped lasers, particularly when the power density is at a low or medium level. To date, extra- and intra-cavity frequency doubled Nd:lasers using KTP have become a preferred pumping source for visible dye lasers and tunable Ti:Sapphire lasers as well as their amplifiers. They are also useful green sources for many research and industry applications. * More than 80% conversion efficiency and 700mJ green laser were obtained with a 900mJ injection-seeded Q-switch Nd:YAG lasers by using extra-cavity KTP. * 8W green laser was generated from a 15W LD pumped Nd:YVO4 with intra-cavity KTP. * 200mW green outputs are generated from 1 W LD pumped Nd:YVO4 lasers by using CASTECH ’s 2x2x5mm KTP and 3x3x1mm Nd:YVO4. * 2-5mw green outputs are generated from 180mw LD pumped Nd:YVO4 and KTP glued crystals.For more details, please refer to Glued Crystals. KTP is also being used for intracavity mixing of 0.81μm diode and 1.064μm Nd:YAG laser to generate blue light and intracavity SHG of Nd:YAG or Nd:YAP lasers at 1.3μm to produce red light.
As an efficient OPO crystal pumped by a Nd:laser and its second harmonics, KTP plays an important role for parametric sources for tunable outputs from visible (600nm) to mid-IR (4500nm), as shown in Fig. 3 and Fig. 4.
The novel developed application is the non-critical phase-matched(NCPM) KTP OPO/OPA pumped by the X-cut KTP crystal. As shown in Fig.5, for pumping wavelength range from 0.7μm to 1 μm, the output can cover from 1.04μm to 1.45μm(signal) and from 2.15μm to 3.2μm(idler). More than 45% conversion efficiency was obtained with narrow output bandwidth and good beam quality.
Applications for E-O Devices In addition to unique NLO features, KTP also has promising E-O and dielectric properties that are comparable to LiNbO3These advantaged properties make KTP extremely useful to various E-O devices. Table 1 is a comparison of KTP with other E-O modulator materials commonly used:
Table 1. Electro-Optic Modulator Materials
Phase
Amplitude
Material
ε
N
R(pm/V)
k(10-6/°C)
N7r2/ε(pm/V)2
r(pm/V)
n7r2/ε(pm/V)2
KTP
LiNbO3
KD*P
LiIO3
15.42
27.9
48.0
5.9
1.80
2.20
1.47
1.74
35.0
8.8
24.0
6.4
31
82
9
24
6130
7410
178
335
27.0
20.1
1.2
11.7
42
8
15
3650
3500
124
Applications for Optical Waveguides Based on the ion-exchange process on KTP substrate, low loss optical waveguides developed for KTP have created novel applications in integrated optics. Table 2 gives a comparison of KTP with other optical waveguide materials. Recently, a type II SHG conversion efficiency of 20%/W/cm2 was achieved by the balanced phase matching, in which the phase mismatch from one section was balanced against a phase mismatch in the opposite sign from the second. Furthermore, segmented KTP waveguides have been applied to the type I quasi-phase-matchable SHG of a tunable Ti:Sapphire laser in the range of 760-960mm, and directly doubled diode lasers for the 400-430nm outputs.
Table 2. Electro-Optic Waveguide Materials
Materials
r (pm/V)
n
eeff (e11e33)1/2
n3r/eeff (pm/V)
KNbO3
BNN
BN
GaAs
BaTiO3
35
29
25
56
56-1340
28
1.86
2.17
2.22
3.6
2.36
13
37
30
86
119-3400
14
373
17.3
8.3
9.2
7.1
5.1-0.14
4.0
1.0
AR-coatings VLIN provides the following AR-coatings: · Dual Band AR-coating (DBAR) of KTP for SHG of 1064nm. low reflectance (R<0.2% at 1064nm and R<0.5% at 532nm ); high damage threshold (>300MW/cm2 at both wavelengths); long durability. · Broad Band AR-coating (BBAR) of KTP for OPO applications. · High reflectivity coating: HR1064nm&HT532nm, R>99.8%@1064nm, T>90%@532nm. · Other coatings are available upon request.