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BBO Crystals - Beta Barium Borate and Lithium Borate

(BBO and LBO)
(Table of Material Properties appears below)

Beta Barium Borate (BBO) and Lithium Triborate (LBO) single crystals combine unusually wide transparency, moderate to moderately large nonlinear coupling, high damage threshold and good mechanical/chemical properties.

BBO has band edges at 0.19 and 3.3um. Its useful transmission range (<5%/cm) is 0.21 to 2.1um and it has been demonstrated to be efficient for the generation of second harmonic radiation down to about 0.21um (3,14,15). It is also useful for broadly tunable optical parametric oscillators (OPOs) and amplifiers (OPAs). Autocorrelation applications may be performed down to 0.19um. Its exceptional IR transmission and wide thermal acceptance bandwidth allow high average power OPO/OPA operation, with minimal heating from long wavelength idler radiation.

BBO's relatively narrow angular acceptance bandwidth (especially in the UV) may limit its usefulness in certain applications involving lasers with less than diffraction limited beam quality. Its mild hygroscopicity should not limit its usefulness in most circumstances. Hermetically sealed housing are available.

BBO's broad phase-matchability makes it an excellent candidate for general use with Nd:YAG and other Q-switched/mode-locked solid-state lasers. Using a tunable Ti:sapphire, Alexandrite, or dye laser, BBO can be used to generate tunable radiation from the near IR to the UV. Such high power, widely tunable radiation would be useful for many applications, including spectroscopy, medicine, materials processing, nonlinear optics, LIDAR, remote sensing, and photochemistry. In the commercial market, solid state nonlinear systems based on BBO could compete with dye lasers, and have the advantage of lower operating cost and more convenient tuning over large frequency ranges.

LBO has band edges at 0.16(6) and 3.3um. Its useful transmission range (<5%/cm)is 0.21 to 2.3um. However, if higher absorption is acceptable, LBO compliments BBO by allowing deeper UV mixing. It also allows temperature-controllable non-critical phase matching (NCPM) for nominal 1.0-1.3um, Type I SHG(16). LBO also provides room temperature, quasi-NCPM (angle tune  while maintaining =90°) for Type II SHG(0.8-1.1um) and THG(0.95-1.2um), a unique capability attributable , in part, to its biaxiality. LBO's lower birefringence limits its UV phase matching to certain combinations of longer wavelength radiation, but it possesses significantly larger angular acceptance bandwidths, reducing the beam quality requirements for source lasers.


Properties of BBO and LBO (a)
 
Beta-BaB2O4 
(BBO)
LiB3O5 
(LBO)
Crystal Data
 
 
Crystal Symmetry and Class Rhombohedral, 3m(1) Orthorhombic, mm2(6)
Space Group R3c(1) Pbn21(6,j)
Lattice Constants (angstroms) a=12.726 +/-0.001(b) 
c=12.726 +/-0.001
a=7.3788 +/-0.0005(6,j)) 
b=8.4473 +/-0.0007(6,j) 
c=5.1395 +/-0.0005(6,j)
Density, g/cc 3.849 2.474
Cleavage (001) poor none observed
Optical Properties
 
 
Optical Transmission (um) 
50% transmission, t=3mm
0.196 to 2.2(c,2,3) 0.16 to 2.3(c,6)
Indices of refraction at (um) no(3), ne(3) nb=x(18,h), nc=y(18,h), na=z(18,h)
0.2537 ---,--- 1.6326,1.6577,1.6844
0.2660 1.7571,1.6146 1.6256,1.6597,1.6761
0.4358 1.6868,155638 1.5857,1.6147,1.6299
0.5461 1.6738,1.5547 1.5777,1.6056,1.6207
0.6328 1.6673,1.5500 1.5740,1.6014,1.6164
1.0642 1.6551,1.5425 1.5648,1.5904,1.6053
Thermooptic coefficient, dn/dT See (g) See (g)
Fresnel Refection Loss per surface
 
 
0.266um 7.5%,5.5% 5.7%,6.2%,.4%
1.06um 6.1%,4.1% 4.8%,5.2%,5.4%
Absorption Coeff.  (cm-1)
 
 
0.266um 0.04 to 0.15(1) ---
1.0um 0.001 to 0.002  --- 
2.09um e-ray: 0.0085
o-ray: 0.07
---
Laser Damage Threshold (GW/cm2)(f)
 
 
1.064um, 10ns pulse 4.6(10) ---
1.064um, 0.1ns pulse, 2.3J 15(6,i) 25(6,i)
NLO Susceptibility, pm/V 
SHG at 1.06um(e)  
[d31=d15 & d32=d24], Kleinman symmetry
 
 
d22 2.3(11,21) ---
d15 <=0.1(3,21) 0.85(21,j)
d24 =d15 by symmetry -0.67(21,j)
d33 unknown,irrelevant 0.04(21,j)
Phasematching Range (,um)
 
 
Type I SHG 0.4096 to 3+(3) 0.55 to 3.0
Type II SHG 0.53 to 3+(3) 0.79 to 2.2
Phasematching Angle ( j ) 
at max deff and 25°C
0.532um, Type I SHG 47.6°(4,g), 90° ---
0.532um, Type II SHG 81.0°(4,g), 0° ---
1.064um, Type I SHG 22.8°(4,g), 90° 11.4°(18,g), 0°
1.064um, Type II SHG 32.8°(4,g), 0° 90°, 69.1°(18,g)
Pockels Coeffs.(pm/V)(8)(0.5145um) 
(Linear Electro-Optic)
 
 
r22 2.7 +/-0.4 ---
r31 ~0 ---
r6 0.055 ---
Half Wave Voltage 87kV(3) ---
Mechanical Properties
 
 
Hardness, Mohs 4.5 6
Elastic Compliances, (TPa-1)(3,f)
 
 
s11 25.63 ---
s12 -14.85 ---
s13 -9.97 ---
s14 -63.97 ---
s33 37.21 ---
s44 331.3 ---
s66 81 ---
Young's Modulus, 1/s11E(GPa) 39 ---
Poisson's Ratio, -s12/s11 0.58 ---
Elastic Stiffnesses, (GPa)(3,f)
 
 
c11 123.8 ---
c12 60.3 ---
c13 49.4 ---
c14 12.3 ---
c33 53.3 ---
c44 7.8 ---
c66 31.8 ---
Thermal Properties
 
 
Melting point (°C) 1095( phase)(9) 834(peritectic)(19)
Thermal Expansion Coeff.(10-6/°C)(3)
 
 
a 4(3) 33.6(17,j)
b -- 108.2(17,j)
c 36(3) -88(17,j)
Phase transitions, °C 925 +/-5(9) none observed
Specific Heat (J/g/°C) 0.49 +/-0.02 1.06 +/-0.05
Thermal Conductivity (W/m/°C)
 
 
perpendicular to c 1.2 2.7 || to x
3.1 || to z
parallel to c 1.6 4.5 || to y(=c)
Electrical Properties
 
 
Resistivity (ohm-cm) >1011 >1011
Relative dielectric constant
 
 
11S/o 6.7(3) ---
33S/o 8.1(3) ---

Footnotes

a) Unreferenced data were determined at Cleveland Crystals, Inc.

b) The rhombohedral lattice constatns are a=8.387 angstroms, = 96.68°(1)

c) Fine structure is observed between ~2.2 and 3.28um

d) Calculated fom Sellmeier euqations, refs 4 and 18

e) Converted using d36(KDP)=0.39pm/V(20,21). Original papers sometimes report values relative to a different absolute scale.

f) Gpa=109N/m2. TPa=1012N/m2. GW=109J/s

g) Private communication from K. Kato

h) Measured at 20°C

i) Surface damage threshold(6)

j) Crystallographic axes abc and tensor reporting frame axes XYZ are designated here according to IEEE/ansi sTD 176-1987, which, for LBO, equates X=a=z, Y=b=x, Z=c=y, relative to principal optical axes xyz. Note that most literature designations [except in (21)] reverse a and b (also d31 and d32; also d15 and d24) from these conventions. For BBO and LBO, phase matching angle  is measured from x and  meausred from y towards z [see(21)].

k) UV absorption edge for LBO from ref 6, for BBO from ref 2.

l) Transmission is intensity dependent. (Unreferenced Cleveland Crystals data) 


References
 1) J. Liebertz and S. Stahr, Z. Krist. 165, 91
-3(1983)

 2) L.K. Cheng, W. Bosenberg, and C.L. Tang, J. Cryst.
Growth 89, 553-9(1988)

 3) D. Eimerl, L. Davis, S. Velsko, E.K. Graham, and A.
Zalkin, J. Appl. Phys. 62, 1968-83(1987)

 4) K. Kato, IEEE J. Quantum Electron. 22, 1013-4(1986)

 5) S.K. Kurtz, J. Jerphagnon, and M.M. Choy,
Landolt-Bornstein, New Series Vol.11, 671-4(1979);

    J. Jerphagnon, S.K. Kurtz and J.L. Oudar, ibid
Vol18, 456-7(1984)

 6) C. Chen, Y. Wu, A Jiang, B. Wu, G. You, R. Li, and S.
Lin, J. Opt. Soc. Am. B6, 616-21(1989)

 7) S.Zhao, C. Huang, and H. Zhang, J. Cryst. Growth 99,
809-10(1990)

 8) C.A Ebbers, Appl. Phys. Lett. 52, 1948-9(1988)

 9) C. CHen, B.Wu, A.Jiang, and G. You, Scientia Sinica B28,
235-43(1985)

10) B.S. Hudson, Spectroscopy 2(4), 33-5(1987)

11) R. Eckardt, H. Masuda, Y. Fan, and R. Beyer, IEEE J. Quantum
Electron. 26, 922-33(1990)

12) R.L. Beyer, "Optical parametric oscillators", in Treatise in
Quantum Electronics, H. Rabin,

    C.L. Tang, Editors, 587-702, Academic Press,
New York(1973)

13) "IEEE Standard on Piezoelectricity", IEEE/ANSI Std. 176-1987,
IEEE, Inc. 345 E. 47th St.,

     NY,NY 10017

14) W.R. Bosenberg, W.S. Pelouch, and C.L. Tang, Appl. Phys.
Lett. 55, 1952-4(1989)

15) C. Chen, B. Wu, G. You and Y. Huang, "High-efficiency and
wide-band second-harmonic

    generation of new crystal,
beta-BaB2O4" dig. Tech. Papers Xiii IQEC

    (1984), paper MCC5

16) T. Ukachi, R.J. Lane, W.R. Bosenberg, and C.L.Tang, Appl.
Phys. Lett 57, 980-2(1990)

17) Fujian Institute, private communication

18) K. Kato, IEEE J. Quantum Electron. 26, 1173-5(1990)

19) B.S.R. Sastry and F.A. Hummel, J. Am. Ceram. Soc. 41,
7-17(1958)

20) D. Eimerl, "Electro-optic, linear and nonlinear optical
properties of KDP and its isomorphs"

    ,Ferroelectrics Vol.72, 95-139(1987)

21)  D. A Roberts "Simplified Characterization of Uniaxial
and Biaxial Nonliner Optical

     Crystals: A plea for Standardization of
Nomenclature and Conventions", IEEE J. Quantum

     Electron, 28, 2057-74(1992). Reprints
available from Cleveland Crystals.


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