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	<title>Key Photonics &#187; Pockels Cells | Q-Switches | Electro-Optic Modulators</title>
	<atom:link href="http://www.key-photonics.co.uk/category/electro-optics/pockels-cells/feed/" rel="self" type="application/rss+xml" />
	<link>http://www.key-photonics.co.uk</link>
	<description>Photonic equipment products &#38; accessories</description>
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		<title>LOW VOLTAGE LIGHT MODULATORS &#8211; 3079 SERIES</title>
		<link>http://www.key-photonics.co.uk/electro-optics/low-voltage-light-modulators-3079-series/</link>
		<comments>http://www.key-photonics.co.uk/electro-optics/low-voltage-light-modulators-3079-series/#comments</comments>
		<pubDate>Wed, 21 Oct 2009 16:08:18 +0000</pubDate>
		<dc:creator>keyphuser</dc:creator>
				<category><![CDATA[Electro-Optics]]></category>
		<category><![CDATA[Pockels Cells | Q-Switches | Electro-Optic Modulators]]></category>
		<category><![CDATA[Transverse field KD*P modulator]]></category>

		<guid isPermaLink="false">http://key-photonics.co.uk/products/?p=172</guid>
		<description><![CDATA[<p></p>
<p>Series 3079 Low Voltage modulators are Pockels effect devices that operate in the transverse field mode. This well characterized and &#8230;]]></description>
				<content:encoded><![CDATA[<p><img class="alignleft size-medium wp-image-173" title="low voltage light modulator- 3079" src="http://key-photonics.co.uk/products/wp-content/product_images/2009/10/low-voltage-light-modulator-3079-300x235.jpg" alt="low voltage light modulator- 3079" width="300" height="235" /></p>
<p>Series 3079 Low Voltage modulators are Pockels effect devices that operate in the transverse field mode. This well characterized and proven design is utilized as an extra-cavity intensity modulator. The Series 3079 is widely used in research and industrial applications and is modestly priced in comparison to competitive devices. The high deuteration level KD*P (KD2PO4) crystals are mounted in a sealed housing available with or without index matching fluid. The EOM-3079 incorporates an outer metal housing which provides R.F. shielding and great mounting rigidity. The design features electrically floating, center fed crystals for low parasitic capacitance and maximum frequency response, replaceable windows, high contrast ratio, and integrally mounted accessories, such as wave plates, filters and polarizers.</p>
<p>3079 Modulators are RoHS and CE compliant.</p>
<p><a href="http://www.fastpulse.com/pdf/3079.pdf">3079 SERIES</a><a href="http://www.fastpulse.com/pdf/3079.pdf"> LOW VOLTAGE LIGHT MODULATORS DATA SHEET (PDF)</a></p>
]]></content:encoded>
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		<item>
		<title>BBO POCKELS CELL Q-SWITCHES &#8211; 1150 SERIES</title>
		<link>http://www.key-photonics.co.uk/electro-optics/bbo-pockels-cell-q-switches-1150-series-2/</link>
		<comments>http://www.key-photonics.co.uk/electro-optics/bbo-pockels-cell-q-switches-1150-series-2/#comments</comments>
		<pubDate>Wed, 21 Oct 2009 15:56:21 +0000</pubDate>
		<dc:creator>keyphuser</dc:creator>
				<category><![CDATA[BBO Pockels Cells]]></category>
		<category><![CDATA[Electro-Optics]]></category>
		<category><![CDATA[Pockels Cells | Q-Switches | Electro-Optic Modulators]]></category>

		<guid isPermaLink="false">http://key-photonics.co.uk/products/?p=167</guid>
		<description><![CDATA[BBO (Beta Barium Borate) is noted for its excellent optical quality and low strain birefringence. This
results in high extinction ratios and low wavefront distortion. Low absorption provides excellent
transmission efficiency in the UV and near IR.]]></description>
				<content:encoded><![CDATA[<p><img class="alignleft size-medium wp-image-163" title="modulator-q-switch rtp 1147" src="http://key-photonics.co.uk/products/wp-content/product_images/2009/10/modulator-q-switch-rtp-1147-300x203.jpg" alt="modulator-q-switch rtp 1147" width="300" height="203" /></p>
<ul>
<li>Wide Spectral Range 250 nm to 1100 nm</li>
</ul>
<ul>
<li> High Extinction Ratio</li>
</ul>
<ul>
<li> Negligible Piezoelectric Response</li>
</ul>
<ul>
<li> High Damage Threshold</li>
</ul>
<ul>
<li> High Average Power Capability</li>
</ul>
<ul>
<li> Single &amp; Double Crystal Configurations</li>
</ul>
<p>BBO (Beta Barium Borate) is noted for its excellent optical quality and low strain birefringence. This<br />
results in high extinction ratios and low wavefront distortion. Low absorption provides excellent<br />
transmission efficiency in the UV and near IR. Qswitches fabricated from BBO can be operated at<br />
high repetition rates and high average power.<br />
Operation of BBO modulators and Q-switches from single shot to repetition rates of more than 50 kHz<br />
is possible with negligible piezoelectric response.<br />
Series 1150 devices are compatible with FastPulse’s Laser Pulse Gating Systems. They are<br />
used in regenerative laser amplifiers for seeding and gating, Laser Pulse Chopping and Polarization<br />
Rotation applications. One advantage of BBO devices is that they do not induce significant<br />
piezoelectric ringing on the transmitted laser beam.<br />
BBO has a useful optical wavelength range from 250 nm to 2100 nm. Transmittance, in the 350 to<br />
1100 nm range, with “V” type narrow band, high efficiency Anti-Reflection coated windows is<br />
approximately 98.5%.<br />
Typical intrinsic extinction ratios of single crystal BBO devices are greater than 1000:1 (&gt;30 db)<br />
measured at 633 nm. Single pass wavefront distortion is &lt;1/8 wave at 633 nm. Thermal<br />
stability is excellent over a broad temperature range. BBO crystals are slightly hygroscopic and in<br />
many applications must be enclosed in a sealed housing. In a dry, appropriately clean, dust-free,<br />
enclosure, all devices within the series can be used without protective windows.<br />
The damage threshold of BBO is of the same order as deuterated KD*P and RTP, approximately 850<br />
MW/cm2 for a 10 nanoseconds wide Q-switched pulse at 1064 nm. In gating applications with<br />
laser pulses &lt;100 picoseconds, the damage threshold is in the 10 GW/cm2 range.<br />
Driving voltages required for BBO crystals to attain 1/4 or ½ wave retardation can be significantly<br />
higher than for KD*P, Lithium Niobate and RTP crystal devices. Reduced voltage operation is<br />
attained by use of a transverse field configuration where required drive voltage becomes a function<br />
of crystal dimensions: the ratio of width between electrodes to overall crystal length.<br />
The 1150 Series has an industry standard 35 mm diameter, convenient for optical mounts. The<br />
physical size is identical with FastPulse’s Series Q1059P KD*P and 1147 RTP devices and may<br />
easily replace them in many of the company’s E-O systems. Series 1150 devices are being used in<br />
the company’s Models 5046, 5057 and 5100 Series Laser Pulse Extraction/ Chopping Systems,<br />
as well as the 5048, 5056, and 5060 Q-switching Systems and 8025S HV Generator. All of these<br />
drivers provide pulsed high voltages with zero DC voltage applied to the crystal.</p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>RTP ELECTRO-OPTIC MODULATORS AND Q-SWITCHES &#8211; 1147 SERIES</title>
		<link>http://www.key-photonics.co.uk/electro-optics/rtp-electro-optic-modulators-and-q-switches-1147-series/</link>
		<comments>http://www.key-photonics.co.uk/electro-optics/rtp-electro-optic-modulators-and-q-switches-1147-series/#comments</comments>
		<pubDate>Wed, 21 Oct 2009 15:40:23 +0000</pubDate>
		<dc:creator>keyphuser</dc:creator>
				<category><![CDATA[Electro-Optics]]></category>
		<category><![CDATA[Pockels Cells | Q-Switches | Electro-Optic Modulators]]></category>
		<category><![CDATA[RTP Pockels Cells]]></category>

		<guid isPermaLink="false">http://key-photonics.co.uk/products/?p=160</guid>
		<description><![CDATA[RTP (rubidium titanyl phosphate - RbTiOPO4), used in the company’s 1147 Series Pockels cells, is a very desirable crystal material for electrooptic modulators and Q-switches.]]></description>
				<content:encoded><![CDATA[<p><img class="alignleft size-medium wp-image-163" title="modulator-q-switch rtp 1147" src="http://key-photonics.co.uk/products/wp-content/product_images/2009/10/modulator-q-switch-rtp-1147-300x203.jpg" alt="modulator-q-switch rtp 1147" width="300" height="203" /></p>
<ul>
<li>No Piezoelectric Ringing</li>
</ul>
<ul>
<li>High Damage Threshold</li>
</ul>
<ul>
<li> High Extinction Ratio</li>
</ul>
<ul>
<li>Low Insertion Loss</li>
</ul>
<ul>
<li>Non-Hygroscopic</li>
</ul>
<ul>
<li>Thermally Compensated</li>
</ul>
<p>RTP (rubidium titanyl phosphate &#8211; RbTiOPO4), used in the company’s 1147 Series Pockels cells,<br />
is a very desirable crystal material for electrooptic modulators and Q-switches. It combines<br />
several features of KD*P and Lithium Niobate and has one major advantage over both: RTP exhibits<br />
virtually no piezo-electric effect with electrical signals between DC and 100 kHz. There is no<br />
ringing superimposed on the transmitted optical beam passing through the crystal. Modulators<br />
and Q-switches made with RTP can be utilized with high power lasers operating at high repetition rates.<br />
Freedom from piezoelectric ringing enables the use of RTP devices in high repetition rate mode<br />
locked laser pulse extraction, laser pulse slicing, chopping and gating systems as well as in Qswitching<br />
applications. Tests conducted at up to 100 kHz reveal no ringing in the optical waveform.<br />
RTP has a useful optical wavelength range from 350 nm to 4300 nm. Transmittance, in the 400<br />
to 1100 nm range, with hard, “V” type high efficiency Anti-Reflection coatings is 98.5%.<br />
Standard AR wavelengths, at the present time, are 1064 nm and 700-900 nm. A-R coatings for other wavelengths are available.<br />
Typical extinction ratios of RTP devices are greater than 200:1 (&gt;20 db) measured at 633<br />
nm. Wavefront distortion is &lt;1/8 Wave at 633 nm. Thermal stability is excellent over a broad<br />
temperature range. The electro-optic coefficient for RTP is temperature insensitive from about 10<br />
0C to more than 50 0C. Because RTP crystals are not hygroscopic, in an appropriately clean, dustfree,<br />
enclosure, all devices within the series can be used without protective windows.</p>
<p>The damage threshold of RTP is of the same order as deuterated KD*P, approximately 850 MW/cm2<br />
for a 10 nanoseconds wide Q-switched pulse at 1064 nm. In gating applications with laser pulses<br />
&lt;100 picoseconds, the damage threshold is in the 10 GW/cm2 range.<br />
Operating voltages for the 1147 Series are lower than those experienced for KD*P and BBO in the<br />
same aperture sizes. A typical device (Model 1147-6-1064) with a 5.5 mm clear aperture and<br />
AR coatings for 1064 nm has a half wave retardation voltage of 2400 Volts. Capacitance is<br />
also low: for the Series 1147, it is about 5 picofarads. RTP has a high (&gt;1011 Ohms)<br />
resistivity and does not exhibit “gray track” laser damage.<br />
The 1147 Series has an industry standard 35 mm diameter, convenient for optical mounts. The size<br />
is compatible with the company’s Series 1059 KD*P devices and may be easily replace them in<br />
many of the company’s E-O systems.<br />
Series 1147 devices are being used in the FastPulse Technology’s Models 5046E, 5046SC,<br />
and 5057 Laser Pulse Extraction / Chopping Systems, as well as the 5048, 5056, and 5060<br />
Q-switching Systems and 8025S HV Generator.</p>
<p><a href="http://www.fastpulse.com/pdf/1147.pdf">1147 SERIES</a><a href="http://www.fastpulse.com/pdf/1147.pdf"> RTP ELECTRO-OPTIC MODULATORS AND Q-SWITCHES DATA SHEET (PDF)</a></p>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>POCKELS CELL ELECTRO-OPTIC Q-SWITCHES &#8211; 1145 SERIES</title>
		<link>http://www.key-photonics.co.uk/electro-optics/pockels-cell-electro-optic-q-switches-1145-series/</link>
		<comments>http://www.key-photonics.co.uk/electro-optics/pockels-cell-electro-optic-q-switches-1145-series/#comments</comments>
		<pubDate>Wed, 21 Oct 2009 14:01:19 +0000</pubDate>
		<dc:creator>keyphuser</dc:creator>
				<category><![CDATA[Electro-Optics]]></category>
		<category><![CDATA[KD*P Pockels Cells]]></category>
		<category><![CDATA[Pockels Cells | Q-Switches | Electro-Optic Modulators]]></category>

		<guid isPermaLink="false">http://key-photonics.co.uk/products/?p=155</guid>
		<description><![CDATA[<p></p>
<p>Series 1145 Q-switches are miniature electro-optic devices (Pockels cells) intended for use with the latest compact size lasers. They are &#8230;]]></description>
				<content:encoded><![CDATA[<p><img class="alignleft size-full wp-image-156" title="Electro-optic Q-switch 1145 -image" src="http://key-photonics.co.uk/wp-content/product_images/2009/10/electro-optic-q-switch-1145-image.jpg" alt="Electro-optic Q-switch 1145 -image" width="236" height="236" /></p>
<p>Series 1145 Q-switches are miniature electro-optic devices (Pockels cells) intended for use with the latest compact size lasers. They are useful for Q-switching, cavity dumping and laser pulse extraction in regenerative amplifiers. Other applications include polarization rotation, laser beam chopping,slicing and pulse picking. They accommodate the most demanding high peak power laser applications. All models within the series utilize a rugged internal crystal support and hermetic sealing system. The devices incorporate highest quality crystals, fused quartz windows and high damage threshold antireflection coatings.</p>
<p><a href="http://www.fastpulse.com/pdf/1145.pdf">1145 SERIES</a><a href="http://www.fastpulse.com/pdf/1145.pdf"> POCKELS CELL ELECTRO-OPTIC Q-SWITCHES DATA SHEET (PDF)</a></p>
]]></content:encoded>
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		<slash:comments>0</slash:comments>
		</item>
		<item>
		<title>PICOSECOND POCKELS CELLS &#8211; MODELS 1111 / 1112</title>
		<link>http://www.key-photonics.co.uk/electro-optics/picosecond-pockels-cells-models-1111-1112/</link>
		<comments>http://www.key-photonics.co.uk/electro-optics/picosecond-pockels-cells-models-1111-1112/#comments</comments>
		<pubDate>Wed, 21 Oct 2009 13:41:21 +0000</pubDate>
		<dc:creator>keyphuser</dc:creator>
				<category><![CDATA[Electro-Optics]]></category>
		<category><![CDATA[KD*P Pockels Cells]]></category>
		<category><![CDATA[Pockels Cells | Q-Switches | Electro-Optic Modulators]]></category>

		<guid isPermaLink="false">http://key-photonics.co.uk/products/?p=148</guid>
		<description><![CDATA[<p></p>
<p>Lasermetrics Models 1111 and 1112 are the fastest switching Pockels Cell Electro-Optic
Modulators currently available. The Model 1111, a single crystal &#8230;]]></description>
				<content:encoded><![CDATA[<p><img class="size-medium wp-image-151 alignleft" title="pico second pockels cell 1111- 1112" src="http://key-photonics.co.uk/products/wp-content/product_images/2009/10/pico-second-pockels-cell-1111-1112-300x206.jpg" alt="Pico Second Pockels Cell" width="300" height="206" /></p>
<p>Lasermetrics Models 1111 and 1112 are the fastest switching Pockels Cell Electro-Optic<br />
Modulators currently available. The Model 1111, a single crystal device and the 1112, a dual<br />
crystal model have demonstrated rise times of 40 picoseconds and 85 picoseconds<br />
respectively. They attain, within a few percent, the maximum theoretical speed possible for<br />
devices of their physical clear aperture.</p>
<p>The Model 1112 operates at one half the voltage required by the single crystal Model 1111 by using two crystals optically in series and electrically in parallel. Both devices are configured to present a 50 Ohm impedance to<br />
the electrical driving pulse.<br />
These Pockels Cells are made from carefully screened KD*P crystals with &gt;98.5%<br />
deuteration, having a computer optimized cylindrical ring electrode geometry. The design<br />
minimizes drive voltage and switching speed and optimizes optical performance. Crystals are<br />
mounted in a rugged aluminum housing sealed with fused quartz windows. The design permits<br />
use of index matching fluid to minimize reflections from internal optical surfaces. This<br />
feature, in combination with high efficiency, multilayer antireflection coatings on the<br />
protective window surfaces, can provide a transmission of efficiency as high as 98%.</p>
<p>The 1111 and 1112 were designed for use as fast shutters for pulse chopping and isolation, and in<br />
modelocked pulse selection systems where only a single picosecond or femtosecond pulse must be<br />
gated from the pulse train. Total optical path length of the 1111 is 15 mm and that of the 1112 is 22 mm,<br />
which minimizes temporal dispersion. The devices find use in many other laser system applications<br />
requiring the ultimate in switching speed. This series is intended for use with pulsed voltages only since the<br />
equivalent electrical transmission line circuit presents a 50 Ohm impedance load to the driving voltage<br />
source.</p>
<p><a href="http://www.fastpulse.com/pdf/1111-1112.pdf">MODELS 1111 / 1112</a><a href="http://www.fastpulse.com/pdf/1111-1112.pdf"> PICOSECOND POCKELS CELLS DATA SHEET (PDF)</a></p>
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		<item>
		<title>ELECTRO-OPTIC Q-SWITCHES -1059 SERIES</title>
		<link>http://www.key-photonics.co.uk/electro-optics/electro-optic-q-switches-1059-series/</link>
		<comments>http://www.key-photonics.co.uk/electro-optics/electro-optic-q-switches-1059-series/#comments</comments>
		<pubDate>Wed, 21 Oct 2009 13:26:36 +0000</pubDate>
		<dc:creator>keyphuser</dc:creator>
				<category><![CDATA[Electro-Optics]]></category>
		<category><![CDATA[KD*P Pockels Cells]]></category>
		<category><![CDATA[Pockels Cells | Q-Switches | Electro-Optic Modulators]]></category>

		<guid isPermaLink="false">http://key-photonics.co.uk/products/?p=141</guid>
		<description><![CDATA[<p></p>
<p>Lasermetrics 1059 E-O Modulator/Q-switches are electro-optic devices that are used in many laser
systems world-wide. The 1059 Series originated in 1970 &#8230;]]></description>
				<content:encoded><![CDATA[<p><img class="alignleft size-medium wp-image-144" title="Pockels Cell 1059" src="http://key-photonics.co.uk/products/wp-content/product_images/2009/10/Pockels-Cell-1059-300x121.jpg" alt="Pockels Cell 1059" width="300" height="121" /></p>
<p>Lasermetrics 1059 E-O Modulator/Q-switches are electro-optic devices that are used in many laser<br />
systems world-wide. The 1059 Series originated in 1970 and have been continuously upgraded and<br />
improved. They will accommodate the most demanding high peak power laser applications. All<br />
models within the series utilize an enhanced internal crystal support and superior sealing system. The<br />
devices incorporate highest quality crystals, fused quartz windows and high damage threshold<br />
antireflection coatings.<br />
E-O performance of the 1059 Series is based on highly deuterated (98+%D)-KDP (KD*P) crystals,<br />
selected for the absence of strain and stria, lowest residual birefringence and wavefront distortion. A<br />
cylindrical ring electrode-crystal configuration produces the most uniform retardation field<br />
currently available. Crystals are mounted in durable and mechanically stable thermoplastic housings.<br />
Stainless steel aperture plates are used in all models. Windows are bubble and strain-free fused<br />
quartz with high efficiency antireflection coatings.</p>
<p>Sol Gel antireflection coatings can be applied to the crystal for highest peak and average power<br />
applications. Sol Gel coatings are extremely efficient, having reflectance losses of about 0.05%.<br />
Damage threshold for Sol Gel coatings is at least as high as that of the KD*P crystal material<br />
While Sol Gel crystal coatings have largely replaced Index Matching Fluid (IMF) for the visible through<br />
Near IR, these coatings are not efficient in the UV range below 400 nm. For UV applications, when<br />
IMF is required to minimize reflection losses at the window-crystal interfaces, we recommend our<br />
Series 1040 and Model 1058 Pockels cells.</p>
<p>A variety of antireflection coatings options are available. A key feature of the 1059 Series is the<br />
user’s ability to adjust the alignment of the fused quartz windows. This may be done while the<br />
device is in position in the laser optical train.<br />
Simple hex wrench adjustments can tilt each window to be precisely on or off-axis by as much<br />
as 2 degrees. The Q1059P model can be specified with wedged or parallel window surfaces and with<br />
the crystal cut at a desired off-axis or wedge angle.<br />
In very fast pulse gating applications, with laser pulses widths less than 100 picoseconds, the 1059<br />
Series has a nominal damage threshold of 20 Gigawatts/cm2. In Q-switching the devices will<br />
tolerate in excess of 850 Megawatts/cm2 at less than 10 nanoseconds pulse width.<br />
Lasermetrics Q-switch drivers 5055, 5056, 5060, and Laser Extraction/Chopping Systems 5046,<br />
5057 and 8025RS can be used with all 1059 models within the series.<br />
Q1059P Series devices are guaranteed against defects in materials and workmanship for one year.</p>
<p><a href="http://www.fastpulse.com/pdf/1059.pdf">1059 SERIES</a><a href="http://www.fastpulse.com/pdf/1059.pdf"> ELECTRO-OPTIC Q-SWITCHES DATA SHEET (PDF)</a></p>
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		<item>
		<title>ELECTRO-OPTIC Q-SWITCH &#8211; 1058 SERIES</title>
		<link>http://www.key-photonics.co.uk/electro-optics/electro-optic-q-switch-1058-series/</link>
		<comments>http://www.key-photonics.co.uk/electro-optics/electro-optic-q-switch-1058-series/#comments</comments>
		<pubDate>Tue, 20 Oct 2009 14:08:17 +0000</pubDate>
		<dc:creator>keyphuser</dc:creator>
				<category><![CDATA[Electro-Optics]]></category>
		<category><![CDATA[KD*P Pockels Cells]]></category>
		<category><![CDATA[Pockels Cells | Q-Switches | Electro-Optic Modulators]]></category>

		<guid isPermaLink="false">http://key-photonics.co.uk/products/?p=86</guid>
		<description><![CDATA[<p></p>
<p>Lasermetrics 1058 Q-switches are large aperture
electro-optic devices that are used in high energy
lasers having beam diameters up to 20 mm
diameter. &#8230;]]></description>
				<content:encoded><![CDATA[<p><img class="alignleft size-medium wp-image-88" title="Pockels cell 1058" src="http://key-photonics.co.uk/products/wp-content/product_images/2009/10/Pockels-cell-10581-300x200.jpg" alt="Pockels cell 1058" width="300" height="200" /></p>
<p>Lasermetrics 1058 Q-switches are large aperture<br />
electro-optic devices that are used in high energy<br />
lasers having beam diameters up to 20 mm<br />
diameter. The 1058 Series was used in the<br />
earliest Ruby and Nd:YAG medical lasers and the<br />
latest, improved versions are presently used in<br />
several medical laser systems marketed<br />
throughout the world. They will reliably<br />
accommodate the most demanding high peak<br />
power laser applications.</p>
<p>All models within the series utilize an enhanced internal crystal support and superior sealing system. The devices<br />
incorporate highest quality crystals, fused quartz windows and high damage threshold<br />
antireflection coatings.<br />
1058 Series E-O performance is based on highly deuterated (98+%)D-KDP (KD*P)<br />
crystals, selected for the absence of strain and stria, lowest residual birefringence and wavefront<br />
distortion. A cylindrical ring electrode-crystal configuration produces the most uniform<br />
retardation field currently available. Crystals are mounted in durable and mechanically stable<br />
aluminum housings. . Stainless steel aperture plates are used in all models. Windows are<br />
bubble and strain-free fused quartz with high efficiency antireflection coatings.<br />
Sol Gel antireflection coatings can be applied to the crystal for highest peak and average power<br />
applications in the wavelength range of 650 nm to 1100 nm. Sol Gel coatings are extremely<br />
efficient, having reflectance losses of .0.05%.</p>
<p>Damage threshold for Sol Gel coatings is at least as high as that of the KD*P crystal material.<br />
For many low repetition rate applications index matching fluid is employed in the hermetically<br />
sealed, vacuum tested housing to minimize reflection losses at the window-crystal interfaces.<br />
A variety of antireflection coatings and index matching fluid options are available. A key<br />
feature of the 1058 Series is the user’s ability to adjust the alignment of the fused quartz<br />
windows. This may be done while the device is in position in the laser optical train. Simple hex<br />
wrench adjustments can tilt each window to be precisely on or off-axis by as much as 2 degrees.<br />
All models can be specified with wedged or parallel window surfaces and with the crystal cut<br />
at a desired off-axis or wedge angle.<br />
In fast pulse gating applications, with laser pulses less than 100 picoseconds width, the 1058<br />
Series has a damage threshold of greater or equal to 20 Gigawatts/cm2. In Q-switching the devices will<br />
tolerate in excess of 850 Megawatts/cm2 at less than 20 nanoseconds pulse width.<br />
Lasermetrics Q-switch drivers 5048, 5055SC, 5056, 8006; 8025S pulse choppers; 5046E and<br />
5046SC pulse extractors, can be used with all 1058 models within the series. The 1058<br />
models have been used with the 8403 HV Amplifiers in polarization and circular dichroism<br />
studies.</p>
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		<title>POCKELS CELL: ELECTRO-OPTIC LIGHT MODULATORS &#8211; 1040 SERIES</title>
		<link>http://www.key-photonics.co.uk/electro-optics/pockels-cell-electro-optic-light-modulators-1040-series/</link>
		<comments>http://www.key-photonics.co.uk/electro-optics/pockels-cell-electro-optic-light-modulators-1040-series/#comments</comments>
		<pubDate>Tue, 20 Oct 2009 11:59:38 +0000</pubDate>
		<dc:creator>keyphuser</dc:creator>
				<category><![CDATA[Electro-Optics]]></category>
		<category><![CDATA[KD*P Pockels Cells]]></category>
		<category><![CDATA[Pockels Cells | Q-Switches | Electro-Optic Modulators]]></category>

		<guid isPermaLink="false">http://key-photonics.co.uk/products/?p=79</guid>
		<description><![CDATA[<p></p>
<p>1040 Series Pockels cell light modulators are designed for high speed laser shutter and pulse chopper applications external or internal &#8230;]]></description>
				<content:encoded><![CDATA[<p><img class="alignleft size-medium wp-image-80" title="Pockels Cell 1040" src="http://key-photonics.co.uk/products/wp-content/product_images/2009/10/Pockels-Cell-1040-300x142.jpg" alt="Pockels Cell 1040" width="300" height="142" /></p>
<p>1040 Series Pockels cell light modulators are designed for high speed laser shutter and pulse chopper applications external or internal to the laser cavity. They are also utilized as Q-Switches, cavity dumpers and polarization rotators. The basic mechanical design is</p>
<p>configured to accept a variety of connection devices to meet most system requirements.</p>
<p><a href="http://fastpulse.com/pdf/1040.pdf"><br />
</a></p>
<p><a href="http://fastpulse.com/pdf/1040.pdf">1040 SERIES</a><a href="http://fastpulse.com/pdf/1040.pdf"> POCKELS CELL ELECTRO-OPTIC LIGHT MODULATORS DATA SHEET (PDF)</a></p>
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