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Newlight's LBO features

 WB01158_1.GIF (255 bytes) Very broad transparency range from 160nm to 2600nm
 WB01158_1.GIF (255 bytes) High optical homogeneity (δn ~ 10-6/cm) and  free of defects
 WB01158_1.GIF (255 bytes) Moderate effective SHG coefficient (about three times that of KDP)
 WB01158_1.GIF (255 bytes) High damage threshold (18.9 GW/cm2 for a 1.3ns Nd laser )
 WB01158_1.GIF (255 bytes) Wide acceptance angle and small angular walkoff
 WB01158_1.GIF (255 bytes) Both Type I and Type II non-critical phase matching (NCPM) in a wide wavelength
   range is possible.
 WB01158_1.GIF (255 bytes) Spectral NCPM near 1300nm

LBO  is a negative biaxial crystal, with the dielectric axes X, Y, and Z (nz>ny>nx) parallel to the crystallographic axes a, c, and b, respectively.

Structural and Physical Properties

Crystal Structure Orthorhombic, Space group Pna21, Point group mm2
Cell Parameters a=8.4473Å, b=7.3788Å, c=5.1395Å, Z=2
Melting Point ~834°C
Mohs Hardness 6
Density  2.47 g/cm3
Hygroscopic Susceptibility Low
Thermal Expansion Coefficients αx=10.8x10-5/K,αy= -8.8x10-5/K,αz=3.4x10-5/K
Thermal Conductivity 3.5W/M/K

Linear Optical Properties

Transparency Range 160 - 2600nm
Thermo-optic Coefficient
(1/°C, λ in µm)
dnx/dT = (-3.76λ+2.30) x 10-6
dny/dT = (6.01λ-19.40) x 10-6
dnz/dT = (1.50λ-9.70) x 10-6
Optical Homogeneity δn ~10-6/cm
Bulk Absorption Coefficient < 100ppm/cm at 1064nm,  < 150ppm/cm at 532 nm
Sellmeier  Equations
(λ in µm)
nx2=2.454140+0.011249/(λ2-0.011350)-0.014591λ2-6.60x10-5λ4
n
y2=2.539070+0.012711/(λ2-0.012523)-0.018540λ2+2.00x10-4λ4
n
z2=2.586179+0.013099/(λ2-0.011893)-0.017968λ2-2.26x10-4λ4
Refractive Indices:
              @ 1064 nm
              @ 532 nm
              @ 266 nm

nx = 1.5656, ny = 1.5905, nz=1.6055
nx = 1.5785, ny = 1.6065, nz=1.6212
nx = 1.5973, ny = 1.6286, nz=1.6444

Nonlinear Optical Properties

SHG Phase Matchable Range 551 ~ 2600nm  (Type I); 790-2150nm (Type II)
NLO Coefficients

d31=1.05 ± 0.09 pm/V
d
32= -0.98 ± 0.09 pm/V
d
33=0.05 ± 0.006 pm/V

Effective Nonlinearity Coefficients dooe=d32cosφ(in XY plane)
d
eeo=d31cos2θ+d32sin2θ (in XZ plane)
d
oeo=d31cosθ(in YZ plane)
d
eoe=d31cos2θ+d32sin2θ (in XZ plane)
Damage Threshold (Bulk)
@ 1064nm
@ 532nm

9GW/cm
2 (9 ns); 19 GW/cm2 (1.3 ns)
2.2 GW/cm
2 (10 ns); 45 GW/cm2 (100ps)
NCPM Temperature 148oC for SHG@1064nm,  
162
oC for SHG@1053nm
172
oC for SHG@1047nm

Damage Threshold

LBO has the highest bulk damage threshold among all known nonlinear optical crystals and is the crystal of choice for high power second and third harmonic generations  of Nd:YAG, Nd:YLF, and Nd:YVO4  lasers.

Comparison of bulk damage threshold (@1064nm, 1.3ns)

Crystal Energy Fluence (J/cm2) Power Density (GW/cm2)
KTP 6.0 4.6
KDP 10.9 8.4
BBO 12.9 9.9
LBO 24.6 18.9

Application Examples

 WB01158_1.GIF (255 bytes) SHG, SFG for a broad range of wavelength:  phase matching cutoff wavelength: SHG-
     554 nm, THG-794 nm, SFM-down to 160 nm
 WB01158_1.GIF (255 bytes) SHG and THG for middle and high power Nd: lasers at 1064nm for medical, industrial
     and military applications
 WB01158_1.GIF (255 bytes) SHG for Ti:Sapphire, Alexandrite and Cr:LiSAF lasers
 WB01158_1.GIF (255 bytes) SHG and THG of high power Nd: lasers at 1342nm & 1319nm for red and blue laser
 WB01158_1.GIF (255 bytes) SHG for the Nd: Lasers at 914nm & 946nm for blue laser.
 WB01158_1.GIF (255 bytes) The VUV output at 187.7 nm is obtained by sum-frequency generation.
 WB01158_1.GIF (255 bytes) NCPM SHG over a broad wavelength range from 900nm -1700nm was measured.
 WB01158_1.GIF (255 bytes) Optical Parametric Amplifiers (OPA) and Oscillators (OPO) application.

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 in a wide wavelength range from 551nm to about 3000nm. LBO is the first choice for making doubler or tripler for lasers such as Nd:YAG where high power density, high stability, and long time operation are required. 

SHG tuning curves of LBO 

NCPM temperature tuning curves of LBO 

 

 WB01158_1.GIF (255 bytes) 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.
 WB01158_1.GIF (255 bytes) Over 80W green output is obtained by SHG of a Q-switched Nd:YAG laser in a Type
   II phase matching  18mm long LBO crystal.
 WB01158_1.GIF (255 bytes) The frequency doubling of a diode pumped Nd:YLF laser (>500mJ @ 1047nm, <7ns,
   1-10KHz) reaches a conversion efficiency over 40% in a 9mm long LBO crystal.
 WB01158_1.GIF (255 bytes) The VUV output at 187.7 nm is obtained by sum-frequency generation in LBO.
 WB01158_1.GIF (255 bytes) 2mJ/pulse diffraction-limited beam at 355nm is obtained by intracavity frequency
   tripling a Q-switched Nd:YAG laser.  

Non-Critical Phase-Matching at Raised Temperature

 WB01158_1.GIF (255 bytes) Non-Critical Phase-Matching (NCPM) of LBO is featured by zero walk -off, very wide
   acceptance angle and maximized effective coefficient. Type I NCPM and Type II NCPM
   are along x-axis (θ=90°, φ=0°) and z-axis (θ=0°, φ=0°), respectively.

 WB01158_1.GIF (255 bytes) Over 11W of average power at 532nm was obtained by extracavity SHG of a 25W
   Antares mode-locked Nd:YAG laser (76MHz, 80ps).

 WB01158_1.GIF (255 bytes) 20W green output was generated by frequency doubling a multimode Q-switched
   medical Nd:YAG laser.

LBO can reach both temperature NCPM and spectral NCPM (with a very wide spectral bandwidth) at 1300nm. This is favorable to the SHG of very broadband or ultrafast pulses at ~ 1300nm.   

Properties for type I NCPM SHG at 1064nm

NCPM Temperature 148°C
Acceptance Angle 52 mrad-cm1/2
Walk-off Angle 0
Temperature Bandwidth 4°C-cm
Effective SHG Coefficient 2.69 x d36(KDP)

OPO and OPA with LBO

LBO is an excellent NLO crystal for OPOs and OPAs with a widely tunable wavelength range and high powers. The unique properties of type I and type II phase matching as well as the NCPM leave a big room in the research and applications of LBO's OPO and OPA.

 

 WB01158_1.GIF (255 bytes) A high overall conversion efficiency and 540-1030nm tunable wavelength range
   were obtained with OPO pumped at 355nm.
 WB01158_1.GIF (255 bytes) Type I OPA pumped at 355nm with the pump-to-signal energy conversion
   efficiency of 30% has been reported.
 WB01158_1.GIF (255 bytes) 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.
 WB01158_1.GIF (255 bytes) 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°C to 148.5°C.
 WB01158_1.GIF (255 bytes) 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
   pumped by a 4.8mJ, 30ps laser at 354.7nm. Wavelength tuning range from
   482.6nm to 415.9nm was covered by increasing the temperature of LBO and
   rotating BBO.

 

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