LiNbO3 crystal has been widely used in optical waveguide and optical communication technology because of its excellent electro-optical properties. It is an ideal substrate material for many integrated optoelectronic devices. Because of the large electro-optic coefficient of LiNbO3, the half-wave voltage is low. The electro-optic effect of LiNbO3 crystal is usually used to modulate the optical signal. Electro-optic modulation is divided into longitudinal and transverse, and LiNbO3 is mainly used in transverse modulation. It has been widely used in medium and low power solid-state lasers.
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Number
|
Size(mm) | Length(mm) | Orientation | Coating |
Price
|
Delivery
(week)
|
Order
|
| LN001 |
9*9
|
25
|
z-cut | AR/AR @ 1064 nm, with gold electrodes | 510 |
1-2
|
 |
| LN002 |
6*6
|
25
|
z-cut | AR/AR @ 1065 nm, with gold electrodes | 570 |
1-2
|
|
| LN003 |
Ø80
|
0.6
|
z-cut | Uncoated | 140 |
1-2
|
|
| LN004 |
25.6*25.6
|
0.5
|
0/0 |
Uncoated | 90 |
1-2
|
|
| LN005 |
Ø50
|
0.5
|
0/0 | Uncoated | 110 |
1-2
|
|
| LN006 |
Ø100
|
0.8
|
z-cut | Uncoated | 330 |
1-2
|
|
| LN007 |
3*3
|
10
|
z-cut | AR/AR/AU/AU | 80 |
1-2
|
|
| LN008 |
9*9
|
20
|
z-cut | AR/AR/AU/AU | 80 |
1-2
|
|
| LN009 |
Ø50
|
0.5
|
0/0 | Uncoated | 110 |
1-2
|
|
| LN010 |
Ø50
|
3
|
0/0 | Uncoated | 110 |
1-2
|
|
| NLO Coefficients | d33 = 34.4 pm/V |
| d31 = d15 = 5.95 pm/V | |
| d22 = 3.07 pm/V | |
| Efficiency NLO Coefficients | deff =5.7 pm/V or ~14.6 x d36 (KDP) for frequency doubling 1300 nm; |
| deff =5.3 pm/V or ~13.6 x d36 (KDP) for OPO pumped at 1064 nm; | |
| deff =17.6 pm/V or ~45 x d36 (KDP) for quasi-phase-matched structure. | |
| Electro-Optic Coefficients | gT33 = 32 pm/V, gS33 = 31 pm/V, |
| gT31 =10 pm/V, gS31=8.6 pm/V, | |
| gT22 = 6.8 pm/V, gS22= 3.4 pm/V, | |
| Half-Wave Voltage, DC Electrical field||z, light ^z: Electrical field||x or y, light||z: |
3.03 KV |
| 4.02 KV | |
| Damage Threshold | 100 MW/cm2 (10 ns, 1064nm) |
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