CLBO

CLBO

CLBO (Cesium Lithium Borate, CsLiB6O10) is a new type of nonlinear crystal. It has a wide transparent spectral range (175~2800 nm), a high nonlinear coefficient, 2.2 times that of KDP, and a small dispersion angle.

The laser damage threshold is high, up to 26GW/cm2, and the multiplicative conversion efficiency is 60% (SHG). It can work at room temperature and is well suited for Nd: YAG lasers to produce 4w (266 nm) and 5w (213 nm) octave light output. It can be used for UV parametric oscillation (OPG) and parametric amplification (OPA).

Features of CLBO Nnonlinear Crystal:

  • Small discrete angle
  • Low absorption coefficient
  • High frequency conversion efficiency
  • Easy-to-grow single crystal
  • High laser damage threshold
  • Efficient nonlinear optical coefficients
  • Its uv absorption edge reaches 180 nm
  • Larger angle, spectral and temperature bandwidth values

Physical and Chemical Properties

AttributeNumerical
Chemical FormulaCsLiB6O10
Crystal StructureTetragonal Negative Uniaxial Crystal,42 m
Lattice Constanta=10.494Å,c = 8.939Å,Z=4
Mass Density2.461 g/cm3
Mohs Hardness5.5
Melting Point1118 K
Molecular Mass364.706
Thermal Conductivity1.25 W/m K

Nonlinear Optical Properties

Attribute数值
NLO Coefficientdeff(I)=d36sinθmsin(2φ)
 deff(II)=d36sin(2θm)cos(2φ)
Thermal Coefficient of Lightdno/dT=-1.9*10-6/℃
 dne/dT=-0.5*10-6/℃
Damage Threshold26 GW/cm2
Wavelength(nm)532 + 532 = 266
1064 + 266 = 213
Phase Supporting Frame(°)61.7
68.4
Flow Rate(pm / V)0.84
0.87
Angle Tolerance(mrad·cm)0.49
0.42
Declination(°)1.83
1.69
Spectral Acceptability(nm·cm)0.13
0.16
Temperature Acceptability(℃·cm)8.3
4.6

Linear Optical Properties

AttributeValue
Transparent Range180-2750 nm
Absorption Coefficient 0.0013 cm−1
Refractive Index
1.064 micronn= 1.4340, n= 1.4838
0.532 micronn= 1.4445, n= 1.4971
Sellmeier Equation (λinμm)no= 2.2104+0.01018/(λ2-0.01424)-0.01258λ2
ne= 2.0588+0.00838/(λ2-0.01363)-0.00607λ2

Experimental Value of Refractive Index

λ[µm]none
0.421.50581.4517
0.451.5031.4493
0.481.50061.4474
0.51.49911.4462
0.5321.49711.4445
0.561.49571.4434
0.591.49431.4422
0.611.49351.4414
0.63281.49281.4409
0.671.49151.4398
0.71.49071.4392
0.721.49021.4387
1.0641.48381.434

Experimental Values ​​for Phase Matching Temperature, Internal Angle and Temperature Bandwidth

Interaction Wavelength[μm]θpm [deg]T [◦C]Δθint [deg]ΔT [◦C]
SHG, o + o ⇒ e
0.946 ⇒ 0.47390-15 5
0.5235 ⇒0.2617565.8~160  
0.5321 ⇒ 0.2660562~140  
61.4200.236.2
1.0642 ⇒0.532129.5200.04352.7
1.3382 ⇒ 0.669127.720 68.7
SFG, o + o ⇒ e
1.0642 + 0.26605 ⇒ 0.2128467.320 3.6
1.547 + 0.221 ⇒0.1933861.7150  
1.9079 + 0.2128 ⇒ 0.19145520 1.2
1.0642 + 0.35473 ⇒ 0.2660550.620 6.1
1.0642 + 0.5321 ⇒ 0.3547339.120 18
SHG, e + o ⇒ e
1.0642 ⇒0.532142.420 49.4
SFG, e + o ⇒ e
1.9079 + 0.2128 ⇒ 0.191457.420 1.1
1.0642 + 0.5321 ⇒ 0.3547348.920 17

Spectrum

CLBO nonlinear crystal Calculation CRYLINKCLBO nonlinear crystal transmission CRYLINK
The second harmonic conversion efficiency is calculated as a function of input basic pulse energyCLBO transmission spectrum
CLBO nonlinear crystal index CRYLINKCLBO nonlinear crystal angle CRYLINK
Refractive index dispersionThe phase of type I and II varies with the length of the fundamental wave

References

[1]  Kawamura T ,  Yoshimura M ,  Shimizu Y , et al. Crystal growth of CsLiB6O10CsLiB6O10 in a dry atmosphere and from a stoichiometric melt composition[J]. Journal of Crystal Growth, 2010, 312(8):1118-1121.
[2] AE Kokh,  Kononova N G ,  Lisova I A , et al. CsLiB6O10 crystal: forth and fifth-harmonic generation in Nd:YAP laser[J]. Proceedings of SPIE – The International Society for Optical Engineering, 2001, 4268.
[3]  Lv X ,  Yuan J L ,  Dai Y , et al. Study on Ultra-Precise Machining of CLBO Crystal[J]. Key Engineering Materials, 2006, 304-305:398-402.
[4]  Mori Y ,  Kuroda I ,  Nakajima S , et al. New nonlinear optical crystal: Cesium lithium borate[J]. Applied Physics Letters, 1995, 67(13):1818-1820.
[5]  Ryu G ,  Yoon C S ,  Han T , et al. Growth and characterisation of CsLiB6O10 (CLBO) crystals[J]. Journal of Crystal Growth, 1998, 191(3):492-500.
[6]  Sasaki T ,  Mori Y ,  Kuroda I , et al. Caesium Lithium Borate: a New Nonlinear Optical Crystal[J]. Acta Crystallographica, 2010, 51(11):2222-2224.
[7]  Sekine T ,  Sakai H ,  Takeuchi Y , et al. High efficiency 12.5 J second-harmonic generation from CsLiB6O10 nonlinear crystal by diode-pumped Nd:glass laser[J]. Optics Express, 2013, 21(7):8393-8400.
[8]  Yu X ,  Hu Z G . Flux growth of CsLiB6O10 crystals[J]. Journal of Crystal Growth, 2010, 312(16-17):2415-2418.
[9]  Yuan X ,  Shen G ,  Wang X , et al. Growth and characterization of large CLBO crystals[J]. Journal of Crystal Growth, 2006, 293(1):97-101.
[10]  Bhar G C ,  Kumbhakar P ,  Chatterjee U , et al. Widely tunable deep ultraviolet generation in CLBO[J]. Optics Communications, 2000, 176(1-3):199-205.
[11]  Ono R ,  Kamimura T ,  Fukumoto S . Effect of crystallinity on the bulk laser damage and UV absorption of CLBO crystals[J]. Journal of Crystal Growth, 2002, 237:645-648.
[12]  Mori Y ,  Kuroda I ,  Nakajima S , et al. Growth of a nonlinear optical crystal: cesium lithium borate[J]. Journal of Crystal Growth, 1995, 156(3):307-309.
[13]  Mirov S B ,  Fedorov V V ,  Boczar B , et al. All-solid-state laser system tunable in deep ultraviolet based on sum-frequency generation in CLBO[J]. Optics Communications, 2001, 198(4-6):403-406.
[14]  Pylneva N A ,  Kononova N G ,  Yurkin A M , et al. Top-seeded solution growth of CLBO crystals[J]. Proceedings of SPIE – The International Society for Optical Engineering, 1999, 3610:148-155.
[15]  Yap Y K ,  Inagaki M ,  Nakajima S , et al. High-power fourth- and fifth-harmonic generation of a Nd:YAG laser by means of a CsLiB(6)O(10).[J]. Optics Letters, 1996, 21(17):1348.
[16]  Sakuma J ,  Asakawa Y ,  Obara M . Generation of 5-W deep-UV continuous-wave radiation at 266 nm by an external cavity with a CsLiB6O10 crystal[J]. Optics Letters, 2004, 29(1):92-4.
[17] Trnovcova, V, Fedorov, et al. Electrical and dielectric properties of b-BaB2O4 (BBO) and CsLiB6O10 (CLBO) crystals[J]. Journal of Physics & Chemistry of Solids, 2007.
[18]  Yap Y K ,  Inoue T ,  Sakai H , et al. Long-term operation of CsLiB6O10 at elevated crystal temperature[J]. Optics Letters, 1998, 23(1):34.
[19]  Yap Y K ,  Haramura S ,  Taguchi A , et al. CsLiB6O10 crystal for frequency doubling the Nd:YAG laser – ScienceDirect[J]. Optics Communications, 1998, 145( 1–6):101-104.
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[21]  Mori Y ,  Yap Y K ,  Kamimura T , et al. Recent development of nonlinear optical borate crystals for UV generation[J]. Optical Materials, 2002, 19(1):1-5.
[22]  Bai K ,  Jung S T . Growth and characterization of pure and Er-doped CsLiB 6O 10 single crystals[J]. Journal of Crystal Growth, 1998, 186(4):612-615.
[23]  Chandra S ,  Allik T H ,  Hutchinson J A , et al. Tunable ultraviolet laser source based on solid-state dye laser technology and CsLiB6O10 harmonic generation[J]. Optics Letters, 1997, 22(4).
[24]  Zhou W L ,  Mori Y ,  Sasaki T , et al. High-efficiency intracavity continuous-wave ultraviolet generation using crystals CsLiB~6O~1~0, -BaB~2O~4 and LiB~3O~5[J]. OPTICS COMMUNICATIONS, 1996, 123(4).
[25]  Yushi K ,  Yarborough J M ,  Li L , et al. Continuous-wave all-solid-state 244 nm deep-ultraviolet laser source by fourth-harmonic generation of an optically pumped semiconductor laser using CsLiB6O10 in an external resonator[J]. Optics Letters, 2008, 33(15):1705-7.
[26]  Petrov V ,  Noack F ,  Rotermund F . Sum-Frequency Generation of Femtosecond Pulses in CsLiB(6)O(10) Down to 175 nm.[C]// Conference on Lasers & Electro-optics. 2000.
[27]  Sakuma J ,  Finch A ,  Ohsako Y , et al. High-power narrowband DUV laser source by frequency mixing in CLBO[J]. International Society for Optics and Photonics, 2000, 3889:516-523.
[28]  Nishioka M ,  Kanoh A ,  Yoshimura M , et al. Growth of CsLiB 6O 10 crystals with high laser-damage tolerance[J]. J.cryst.growth, 2005, 279(1-2):76-81.

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