Pockels Cells & Q Switches

Pockels Cells

Overview

 


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Pockels Cells


Pockels Cells are electro-optic devices used to switch the polarization direction of light beams. Their operating principle is based on the Pockels Effect, by which an applied electric field produces linear changes in the refractive index of non-centrosymmetric crystalline materials. Because their switching behavior largely depends on the drive electronics, Pockels Cells offer a much faster response time than acousto-optic devices.





Applications


Common applications for Pockels Cells include:

  • Q-switching of laser cavities
  • Coupling light in and out of regenerative amplifiers
  • Light intensity modulation, when used in conjunction with a pair of polarizers

Pockels Cells can also be used for phase modulation—by imprinting sidebands onto the frequency of the transmitted light at multiples of the cell’s drive frequency. This electro-optic approach, however, modulates phase less efficiently than devices that rely on optimized crystal orientation and electric field direction. 

Optical Specifications

Inrad Optics Pockels Cells Specifications

Model Crystal Type
Aperture (mm)
Wavelength Range (nm)
Transmission (%T)
@ specific λ
Capacitance (pF)
Quarterwave Voltage
@ 1064 nm
Extinction Ratio
@ 1064 nm
Damage Threshold (MW/cm2)
PKC21 KD*P
9.5, 12, 15, 20, 25 .30 - 1.32 µm FC > 96 % 8, 9, 10, 14, 17 3.3 kV > 1000:1
For ≤ 15mm aperture
FC> 500
.25 - 1.32 µm SG> 99 % SG> 800
PKC02 9, 15, 20
.30 - 1.32 µm FC > 95 % 14, 22, 28
1.65 kV
> 1000:1
For ≤ 15mm aperture
FC> 500
.25 - 1.32 µm SG > 96 % SG> 800
PKC24 9 .25 - 1.32 µm SG > 99 % 8 3.3 kV   > 1000:1 > 800
PKC26
PLC01 LiNbO3
8.5 1.0 - 3.8 µm > 98 % 20   1.65 kV   > 600:1 > 300
PLCX1 3.5 1.0 - 3.8 µm > 98 % 4   1.0 kV   > 900:1 > 300
PBCX1 BBO
2.5, 3.5 .22 - 2.1 µm > 98 % 3 3.6, 4.8 kV > 1000:1 > 500
PBC05
PBC06 3.5, 4.5, 5.5 .22 - 2.1 µm  > 97 % 5 2.4, 3.1, 3.6 kV > 500:1 > 500

Cells by Crystal Type

 BBO ~ KD*P ~ LiNbO3

 


 

BBO Pockels Cells

Model Description Aperture
PBCX1-DC03 Compact BBO Pockels Cell, with AR coated crystal
and windows, dry cell
2.5 mm
PBCX1-DC04 BBO Pockels Cell, with AR coated crystal and windows, dry cell 3.5 mm

PBC05-DC03

BBO Pockels Cell, dual crystal, with AR coated crystal
and windows, dry cell

2.5 mm

PBC05-DC04

3.5 mm

PBC06-DC04

BBO Pockels Cell, dual crystal, with AR coated windows, dry cell

 3.5 mm

PBC06-DC06

5.5 mm

Note: Standard wavelengths for BBO Pockels Cells are 1064nm, 532nm, 355nm and 266nm.
Custom wavelengths are available.

 

BBO Pockels Cells

MODEL
PBC05-DC04
PBCX1-DC04 
PBC05-DC03
PBCX1-DC03 
PBC06-DC06 PBC06-DC04
Aperture Diameter
3.5 mm  2.5 mm
5.5 mm  3.5 mm
Number of Crystals
one
two

Quarter-Wave Voltage
@ 1064 nm

4.8 kV

 3.6 kV

 3.6 kV 

2.4 kV

Intrinsic Contrast
@ 1064 nm

> 1000 : 1

> 500 : 1

Optical Transmission > 98% T > 97% T
Damage Threshold*
(Nanosecond Pulses)
> 500 MW / cm2
Damage Threshold*
(cw Power)
> 3 kW / cm2
Waterfront Distortion
@1064 nm
< λ / 8

Electrical Contacts

two, electrically floating, miniature banana plugs

Typical Capacitance

3 pF   3 pF  4.5 pF   5 pF

Outline Dimensions

  PBC05: Diameter x 2" Long Cylinder
PBCX1: Diameter x 1.5" Long Cylinder 

1.25" Diameter x 2.7" Long Cylinder

*Damage Threshold values for reference only and are not guaranteed.



KD*P Pockels Cells, Single Crystal

Model Description Aperture Notes
PKC21-FC09 KD*P Pockels Cell, with AR coated windows, filled with
FC-43 fluid.
9.5 mm Windows are wedged, customer must select between net 0º or 1º wedge for the device
PKC21-FC12 12 mm
PKC21-FC15
15 mm
PKC21-SG09 KD*P Pockels Cell, with AR coated windows, with sol-gel coated crystal.   9.5 mm
PKC21-SG12   12 mm
PKC21-SG15   25 mm
PKC21-SG20
20 mm
PKC21-SG25
25 mm
PKC21-SG35
35 mm
PKC21-SG50
50 mm

 

KD*P Pockels Cells, Single Crystal, Compact

Model Description Aperture Notes
PKC24-SG09 KD*P Pockels Cell, with AR coated windows, with sol-gel coated crystal,
OD 0.75"
9 mm Windows are wedged, customer must select between net 0º or 1º wedge for the device
PKC26-SG09 KD*P Pockels Cell, with AR coated windows, with sol-gel coated crystal,
OD 25mm
  9 mm

Windows are wedged,  net 0º wedge for the device

 

KD*P Pockels Cells, Dual Crystal

Model Description Aperture Notes
PKC02-FC09 KD*P Dual Crystal Pockels Cell, with AR coated windows, filled with
FC-43 fluid.
9 mm Windows are not wedged
PKC02-FC15 15 mm
PKC02-SG09 KD*P Dual Crystal Pockels Cell, with AR coated windows, with
sol-gel coated crystal.
  9 mm
PKC02-SG15   15 mm
PKC02-SG20   20 mm

 


Standard wavelengths for KD*P Pockels cells are 
1064nm,700-900nm,755nm,694nm,532nm, and 355nm. 
Custom wavelengths are available.

 


 


LiNbO3 Pockels Cells

Model Description Aperture Notes
PLCX1-DC04 LiNbO3 Pockels Cell, with crystal and windows AR coated, dry cell. 3.5 mm Windows are not wedged
PLC01-DC08 LiNbO3 Pockels Cell, with crystal and windows AR coated, dry cell, damped. 8.5 mm

PLC01-DC10.5

LiNbO3 Pockels Cell, with crystal and windows AR coated, dry cell. 10.5 mm

Standard wavelengths for LiNbO3 are 1064nm, 1320nm and 2100 nm.
Custom wavelengths are available.

 

 

Q Switch Crystals

 


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Q-Switch Crystals


The ideal crystalline medium for Q-Switch Crystals depends on operating wavelength laser beam size, damage threshold, average power handling, contrast ratio, extinction ratio and repetition rate. Here’s an overview of different types of Q-Switch Crystals:

  • KD*P Pockels Cells are routinely used for Q-switching applications with wavelengths from the UV to approximately 1.1 µm. Beyond 1.1 µm, absorption limits KD*P’s use in active cavities unless the application can tolerate a few percent of absorption.
  • LiNbO3 Pockels Cells address wavelengths of at least 1.064 µm. With an electric field applied transverse to the direction of light propagation, LiNBO3 cells can be configured to operate at a lower voltage than comparable KD*P cells. LiNbO3 can also be a good choice for infrared wavelengths as long as 4.0 µm, though half-wave voltage increases at those wavelengths.
  • BBO Pockels Cells target operating wavelengths from the UV to roughly 2 µm. BBO crystal handles high average powers better than either KD*P or LiNbO3. Since it has a relatively small electro-optic coefficient, BBO tends to require higher voltages than the other two crystal mediums. The voltage required in a given application will depend on the crystal length, thickness and size of the clear aperture.

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