| Code |
Types |
Wavelength |
Dimension |
Aperture |
Extinction Ratio |
Laser Damage Threshold |
Unit Price |
Delivery |
Cart |
| 2031-004 |
High ER |
Custom |
Ф15×18mm |
5mm |
>5000:1 |
500MW/cm^2 |
Inquire |
Inquire |
|
| 2031-005 |
Customized |
Custom |
Ф18x25mm |
6mm |
CP>2500:1; PP>1500:1 |
>800MW/cm^2 |
Inquire |
Inquire |
|
| 2031-001 |
Pin connectors |
1064nm |
Φ19x29mm |
8mm |
>2500:1 |
800MW/cm^2 |
$450.0 |
1 week |
|
| 2031-006 |
Customized |
Custom |
Ф18x25mm |
8mm |
CP>2500:1; PP>1500:1 |
>800MW/cm^2 |
Inquire |
Inquire |
|
| 2031-007 |
Compositive |
500-1100nm |
60x30x30mm |
8mm |
>2500:1 |
>800MW/cm^2 |
Inquire |
Inquire |
|
| 2031-025 |
High ER |
Custom |
Ф19x24mm |
8mm |
>5000:1 |
500MW/cm^2 |
Inquire |
Inquire |
|
| 2031-026 |
High ER |
Custom |
Ф19x24.7mm |
8mm |
>5000:1 |
500MW/cm^2 |
Inquire |
Inquire |
|
| 2031-008 |
High ER |
240-1400nm |
Ф19×24mm |
8mm |
>7000:1 |
750MW/cm^2 |
Inquire |
Inquire |
|
| 2031-009 |
High ER |
240-1400nm |
Ф19×24.7mm |
8mm |
>7000:1 |
750MW/cm^2 |
Inquire |
Inquire |
|
| 2031-002 |
Pin connectors |
1064nm |
Φ25x39mm |
10mm |
2500:1 |
800MW/cm^2 |
$500.0 |
1 week |
|
| 2031-010 |
Pin connectors |
500-1100nm |
Ф25.4x39mm |
10mm |
>2500:1 |
>800MW/cm^2 |
Inquire |
Inquire |
|
| 2031-027 |
High ER |
Custom |
Ф25.4x32mm |
10mm |
>5000:1 |
500MW/cm^2 |
Inquire |
Inquire |
|
| 2031-028 |
High ER |
Custom |
Ф25.4x39mm |
10mm |
>5000:1 |
750MW/cm^2 |
Inquire |
Inquire |
|
| 2031-011 |
High ER |
240-1400nm |
Ф25.4x32mm |
10mm |
>7000:1 |
750MW/cm^2 |
Inquire |
Inquire |
|
| 2031-012 |
High ER |
240-1400nm |
Ф25.4x39mm |
10mm |
>7000:1 |
750MW/cm^2 |
Inquire |
Inquire |
|
| 2031-013 |
High ER |
240-1400nm |
Ф28x33mm |
11mm |
>7000:1 |
750MW/cm^2 |
Inquire |
Inquire |
|
| 2031-003 |
Pin connectors |
1064nm |
Φ28x33mm |
12mm |
2500:1 |
800MW/cm^2 |
$600.0 |
1 week |
|
| 2031-024 |
755nm double connectors |
755nm |
Ф25.4x39mm |
12mm |
>2000:1 |
>850MW/cm^2 |
Inquire |
Inquire |
|
| 2031-014 |
755nm triple connectors |
755nm |
Custom |
12mm |
>2000:1 |
>850MW/cm^2 |
Inquire |
Inquire |
|
| 2031-015 |
Pin connectors |
500-1100nm |
Ф25.4x39mm |
12mm |
>2500:1 |
>800MW/cm^2 |
Inquire |
Inquire |
|
| 2031-016 |
694nm |
694nm |
Custom |
12mm |
>2500:1 |
>800MW/cm^2 |
Inquire |
Inquire |
|
| 2031-029 |
High ER |
Custom |
Ф34.5x41.2mm |
12mm |
>5000:1 |
500MW/cm^2 |
Inquire |
Inquire |
|
| 2031-030 |
High ER |
Custom |
Ф25.3x42.5mm |
13mm |
>5000:1 |
500MW/cm^2 |
Inquire |
Inquire |
|
| 2031-017 |
High ER |
240-1400nm |
Ф25.3x42.5mm |
13mm |
>7000:1 |
750MW/cm^2 |
Inquire |
Inquire |
|
| 2031-018 |
Large aperture |
1064nm |
Ф55x80mm |
25mm |
>1500:1 |
>850MW/cm^2 |
Inquire |
Inquire |
|
| 2031-019 |
Large aperture |
1064nm |
Ф55x80mm |
30mm |
>1000:1 |
>850MW/cm^2 |
Inquire |
Inquire |
|
| 2031-020 |
Large aperture |
1064nm |
Custom |
50mm |
>700:1 |
>850MW/cm^2 |
Inquire |
Inquire |
|
| 2031-021 |
Wire connector |
Custom |
Ф32x41mm |
Custom(<12mm) |
>2500:1 |
>800MW/cm^2 |
Inquire |
Inquire |
|
| 2031-022 |
Wire connector |
Custom |
Ф28x33mm |
Custom(<12mm) |
>2500:1 |
>800MW/cm^2 |
Inquire |
Inquire |
|
| 2031-023 |
Nitrogen encapsulated |
500-1100nm |
Ф25x36mm |
Custom(>10mm) |
>5000:1 |
>1GW/cm^2 |
Inquire |
Inquire |
|
DKDP or KD*P crystals stand out for their high electro-optic coefficients attributing to the high deuteration content, and the high e-o conversion efficiencies render them well-suited for pockels cells Q-switches applications. DKDP crystals also have good transmission at 0.3 to 1.1µm. The operation wavelength range of DKDP (KD*P) Pockels cells for Q-switching applications is 400 nm to about 1.1 μm. Most of the low repetition rate DPSS Nd:YAG lasers and commercial flashlamp-pumped Nd:YAG lasers are equipped with DKDP (KD*P) based Pockels cells for laser cavity Q-switching. With the distinguished merits of excellent mechanical and optical properties, DKDP Pockel cells are often used in lasers of large caliber, high power, and narrow pulse width.
Hangzhou Shalom EO offers the DKDP pockels cells with high deuteration (>98%), low capacitance and fast rise time, high transmission, and high extinction ratio. A largest aperture of 50mm is available.
Features:
- Low absorption and high deuteration
- Operates in the Longitudinal scheme, so applied voltage does not depend on crystal aperture, hence large apertures could be arranged without increasing the voltage
- High damage threshold dielectric AR coating options
- For fs applications due to low GVD
Applications:
- Pulse picking and Laser cavity dumping
- Q-switching of low repetition rate diode-pumped lasers and flashlamp-pumped high energy lasers
- OEM laser systems
- Medical/cosmetic lasers
- Versatile R&D laser platforms
- Military & aerospace lasers
Specifications:
| Deuteration of DKDP Crystals |
>98% |
Wavelength Range |
300nm to 1400nm |
| Aperture |
≦50mm |
Wavefront Distortion |
Lambda/8@633nm |
| Capacitance |
~3pF |
Quarter Wave Voltage |
~3200V |
| Transmission (@designed wavelength) |
>98% |
|
|
When it comes to practical applications of Pockels cells, one might need to take some additional side effects into account:
- Etalon effects might still exist and affect the optical performance if the beam direction is perpendicular to the faces of the crystal, Even when the end faces of the crystal are coated with high-quality AR coatings.
- The temperature could significantly affect the obtained phase changes. For example, a Pockels cell set to generate perfect high-contrast amplitude modulation might require readjustments of the operation voltages when the temperature changes. However, there are thermally compensated double-crystal designs that might circumvent the problem.
- For an operation with a large beam radius, it is worth paying attention to sort out an optimized design for electrodes (possibly with additional auxiliary electrodes for high uniformity of the generated electric field, as otherwise one may obtain a spatially varying modulation).
- Nonlinear crystals often exhibit substantial piezo-electric and electrooptic effects, which can have substantial influences on the performance at high modulation frequencies.
- Operating at high power levels, thermal effects may be induced by residual absorption of the crystal. Therefore materials with lower absorption are preferable for high-power applications
- The crystals used in Pockels cells are nonlinear crystal materials, they inherently demonstrate considerable optical nonlinearities. For instance, self-phase modulation and nonlinear self-focusing might occur for light pulses with substantial peak power.
Pockels Cell Comparison Chart:

Aperture 12mm 694nm DKDP Pockels Cells
Aperture 13mm high extinction ratio DKDP Pockels Cells
Aperture 25mm large Aperture DKDP Pockels Cells