Pismo pulse pickers
The 
Pismo pulse picker system comprises two main parts – a control and power 
supply unit (CPSU) and a Pockels cell with a HV driver.
The CPSU realizes the following functions: synchronization to a femtosecond 
pulse train, amplifier pump laser start (flash-lamp or diode pumped with 
acoustooptical or electrooptical Q-switch) that is synchronous to the picked 
pulses, oscilloscope synchronization, streak-camera synchronization and other 
equipment that requires synching to a fs pulse train. The CPSU has 5 independent 
delay channels that are rigidly fixed to a fs pulse train (jitter <200 ps). The 
delay channels are used for starting Pockels cells, pump lasers and other 
equipment. One CPSU can manage up to 4 Pockels cells.
The Pockels cell consists of a HV pulse driver and an electrooptical crystal. 
The CPSU supplies necessary voltage to the HV driver (300-500 V, DC) and sends 
the start signal. The HV driver produces a bell-shaped HV pulse with duration of 
<10 ns at level 10 % from maximum (rise/fall time <4 ns). This pulse is then 
supplied to the DKDP electrooptical crystal.
 
Pockels cell can be purchased separately - request a quote

Typical Specifications
Pismo OG11/1 pulse picker system
Pulse picker system with synchronization and control electronics.
Pockels cell crystal: DKDP, 6x6x16 mm3, ARC 700-1000 nm (clear aperture – 5 mm), 
other apertures on request
HV pulse amplitude: up to 11 kV (HV pulse has the amplitude ~11kV with duration 
10 ns at level 10% of maximum)
Repetition rate: single-shot – 1 kHz
RF source: 30-120 MHz
RF input: optical (internal fiber coupled photodetector with 1.5 m length 
plastic fiber)
System transmission: >78%@full range; >85% @ 750-850nm
Contrast ratio: >1:1000
USB control with drivers and software included
Also included:
Two Glan-Taylor calcite air-spaced polarizers with mounts
1.5-meter optical fiber for synchronization
LabView-compatible software
request a quote - pdf brochure
As the name implies pulse pickers are used to selectively pick off pulses 
from the pulse train of a femtosecond or picosecond laser. Pismo pulse picker 
models are available as stand-alone devices that use a Pockels cell as an 
ultrafast shutter. These pulse pickers allow a wide range of control over the 
repetition rate of the pulse train. A single pulse can be selected from the 
pulse train at a fixed frequency, increasing the contrast of the signal. All 
models include a Pockels cell and synchronization unit, delay generator, and 
high voltage driver unit. The pulse picker operation is based on the linear 
electro-optic effect (Pockels effect). Pockels cells use an applied electric 
field produces a birefringence in the cell that is proportional to the electric 
field. The
Pockels cells included with the pulse pickers are made with a Deuterated 
Potassium Dihydrogen Phosphate (DKDP) crystal. DKDP is an optical material known 
for its wide transparency range and high optical damage threshold.
A pulse picker is used to pick out single optical pulses of picosecond or 
femtosecond duration from a sequence of pulses and for controlling femtosecond 
multipass and regenerative amplifiers.
Features:
• Single pulse selection from train of pulses
• External RF or optical signal trigger synchronization
• High voltage electrical pulse with adjustable delay
• High voltage electrical pulse with adjustable amplitude
• Two additional delayed pulses for measurement purposes
• Easy installation and alignment
• High efficiency and contrast ratio
• Rugged design
The Pismo control unit provides five output pulses with precise timing delays 
that can be synchronized with various signals. Each delay channel consists of a 
12 bit digital delay with 50MHz clock frequency and an approximately 40 ns range 
of continuous delay. 50 MHz delay oscillator is phase-triggered, so that no one 
period jitter occurs. In addition to the five delay channels, the control box 
contains two 12-bit frequency dividers with prescalers. All delays have a common 
start. The triggering signals for starting the delay can be chosen from two 
external inputs (TTL and wide range adjustable) and frequency dividers.
This triggering signal can be synchronized with an optical signal (built-in Si 
or InGaAs sensor with fiber-optic input), one of two external sources of RF, an 
internal 100MHz crystal or can stay unsynchronized. Delays function in one of 
five modes: free running, skipped, enabled, single shot asynchronous and single 
shot synchronous. In the free running mode every triggering
pulse causes a delayed output pulse at every channel, except when there is a 
frequency overrun. If the time between two triggering pulses is less then 
admissible, the second pulse will be ignored. In skipped mode some channels act 
every time, and some act only after a skipping signal edge takes place at the 
nearest subsequent triggering pulse. Enabled mode is like skipped mode, but 
output pulses are present if skipping signal has high level. In the single shot 
asynchronous mode delay, output pulses appear at the nearest subsequent to 
single shot command triggering pulse. The command can be given from an on-screen 
menu, from an external button (optional) or a trough RS-232C interface. Single 
shot synchronous mode, in contrast to asynchronous mode, gives output pulses 
only after first skipping signal following single shot command. Any delay 
channel can be separately turned into both skipped (behavior according to mode) 
and unskipped mode (output pulse at every triggering pulse). The control unit 
can also produce output pulse bursts with controlled length at every skipping 
signal edge or single pulse command. This option is available only in skipped 
and single pulse modes.
An electro-optical crystal (DKDP) is placed between two polarizers oriented at a 
90° angle to one another. Linearly polarized light passes through the first 
polarizer. By applying a high voltage (~ 10 kV) to the electrooptical crystal an 
induced birefringence occurs. When the birefringent phase difference reaches /2, 
polarization is rotated by 90° and linearly polarized light freely passes 
through the second polarizer. When no voltage is applied the polarization does 
not rotate and the second polarizer blocks the light.
Almost all of the device settings for the Pismo control unit are controlled with 
one knob on the front of the unit. Parameters of interest are selected with the 
help of
hierarchical menus, which appears at LCD display. The electro-optic Pockels cell 
is driven by high voltage pulses (duration ~ 6 ns at level 10% of maximum)
controlled by the electronics synchronization unit.
request a quote - pdf brochure
Pismo Pulse Pickers: Electro-Optical 
Ultrafast Shutters - pdf brochure -
typ.specs -
Pismo pulse picker 
for laser wavelength: 1025~1045 nm
Femtosecond Pulse Pickers Pismo Questions and 
Answers - 100kHz -
Pismo OG10B/100-1/DKDP 100kHz quote -
Pismo OG10B/100-1/BBO -
Pismo 8-1 Manual -
Pismo 8-10 -
Pismo 8-25 Manual -
QA1 
- QA2 
- QA3 -
QA4 -
QA5 - 
Pockels Cell -
selection of pulses from a ~ 
100 MHz, 20 fs Ti:Sapphire laser -
pulse selection for polarization 
flip - Pulse 
peaker for Chameleon Ultra I from Coherent
Pulse picker for Tsunami laser
Pulse 
Picker Pismo for Ti:Sapphire laser MIRA Optima 900-D (Femto,Pico) 76 MHz, 800 nm 
from Coherent -
Pulse picker for polarization control
Pockels cell based on Rubidium 
Titanyle Phosphate – RbTiOPO4 crystal
Ultrafast Shutter
Product news and updates - Training Workshops 
- Featured Customer - Other News
    ![]()  | 
      Trestles LH Ti:Sapphire 
    laser Trestles LH is a new series of high quality femtosecond Ti:Sapphire lasers for applications in scientific research, biological imaging, life sciences and precision material processing. Trestles LH includes integrated sealed, turn-key, cost-effective, diode-pumped solid-state (DPSS). Trestles LH lasers offer the most attractive pricing on the market combined with excellent performance and reliability. DPSS LH is a state-of-the-art laser designed for today’s applications. It combines superb performance and tremendous value for today’s market and has numerous advantages over all other DPSS lasers suitable for Ti:Sapphire pumping. Trestles LH can be customized to fit customer requirements and budget. Reserve a 
    spot in our Femtosecond lasers training 
    workshop in San Diego, California. Come to learn how to build a
    
    femtosecond laser from a kit  | 
  
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 DPSS DMPLH lasers  | 
  
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    New laser spectrometer 
    T&D-scan for research  that 
    demands high resolution and high spectral 
density in UV-VIS-NIR spectral domains - now available with 
    new pump option! The T&D-scan includes a CW ultra-wide-tunable narrow-line laser, high-precision wavelength meter, an electronic control unit driven through USB interface as well as a software package. Novel advanced design of the fundamental laser component implements efficient intra-cavity frequency doubling as well as provides a state-of-the-art combined ultra-wide-tunable Ti:Sapphire & Dye laser capable of covering together a super-broad spectral range between 275 and 1100 nm. Wavelength selection components as well as the position of the non-linear crystal are precisely tuned by a closed-loop control system, which incorporates highly accurate wavelength meter. Reserve a 
    spot in our CW lasers training 
    workshop in San Diego, California. Come to 
    learn how to build a
    CW 
    Ti:Sapphire laser from a kit  | 
  
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       Near IR viewers Ultraviolet viewers are designed to observe radiation emitted by UV sources.  | 
  
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 AOTF Infrared Spectrometer  | 
  
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 Open Microchannel Plate Detector 
MCP-MA25/2 -
now in stock!  | 
  
        
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    Hummingbird EMCCD camera  The digital Hummingbird EMCCD camera combines high sensitivity, speed and high resolution. It uses Texas Instruments' 1MegaPixel Frame Transfer Impactron device which provides QE up to 65%. Hummingbird comes with a standard CameraLink output. It is the smallest and most rugged 1MP EMCCD camera in the world. It is ideally suited for any low imaging application such as hyperspectral imaging, X-ray imaging, Astronomy and low light surveillance. It is small, lightweight, low power and is therefore the ideal camera for OEM and integrators. buy online  | 
  
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    Hatteras-D 
    
    femtosecond  transient absorption data acquisition system Future nanostructures and biological nanosystems will take advantage not only of the small dimensions of the objects but of the specific way of interaction between nano-objects. The interactions of building blocks within these nanosystems will be studied and optimized on the femtosecond time scale - says Sergey Egorov, President and CEO of Del Mar Photonics, Inc. Thus we put a lot of our efforts and resources into the development of new Ultrafast Dynamics Tools such as our Femtosecond Transient Absorption Measurements system Hatteras. Whether you want to create a new photovoltaic system that will efficiently convert photon energy in charge separation, or build a molecular complex that will dump photon energy into local heat to kill cancer cells, or create a new fluorescent probe for FRET microscopy, understanding of internal dynamics on femtosecond time scale is utterly important and requires advanced measurement techniques. Reserve a 
    spot in our Ultrafast Dynamics Tools 
    training workshop in San Diego, California.  | 
  
| 
     | 
    
 
Beacon Femtosecond Optically Gated Fluorescence Kinetic Measurement System 
-
request a quote  - 
pdf Reserve a 
    spot in our Ultrafast Dynamics Tools 
    training workshop in San Diego, California.  | 
  
    
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    Terahertz systems, set ups and components New band pass and long pass THz optical filters based on porous silicon and metal mesh technologies. Band pass filters with center wavelengths from 30 THz into GHz range and transmissions up to 80% or better. Standard designs with clear aperture diameters from 12.5 to 37.5 mm. Long pass filters with standard rejection edge wavelengths from 60 THz into GHz range. Maximum transmission up to 80% or better, standard designs at 19.0 and 25.4 mm diameters. Excellent thermal (from cryogenic to 600 K) and mechanical properties THz products: THz Spectrometer kit with Antenna THz transmission setup THz time domain spectrometer Pacifica fs1060pca THz time domain spectrometer Pacifica fs780pca THz detectors: Golay cell and LiTaO3 piroelectric detectors PCA - Photoconductive Antenna as THz photomixer Pacifica THz Time Domain Spectrometer - Trestles Pacifica Holographic Fourier Transform Spectrometer for THz Region Wedge TiSapphire Multipass Amplifier System - THz pulses generation Terahertz Spectroscopic Radar Mobile System for Detection of Concealed Explosives Band pass filters with center wavelengths from 30 THz into GHz range Long pass filters with standard rejection edge wavelengths from 60 THz into GHz range Generation of THz radiation using lithium niobate Terahertz crystals (THz): ZnTe, GaP, LiNbO3 - Wedge ZnTe  | 
  
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    iPCA - interdigital Photoconductive Antenna for terahertz waves Large area broadband antenna with lens array and high emitter conversion efficiency iPCA with LT-GaAs absorber, microlens array for laser excitation wavelengths l £ 850 nm, adjusted hyperhemispherical silicon lens with a high power conversion efficiency of 0.2 mW THz power / W optical power. The iPCA can be used also as large area THz detector. The two types iPCAp and iPCAs have the same active interdigital antenna area but different contact pad directions with respect to the electrical THz field. Interdigital Photoconductive Antenna for terahertz waves generation using femtosecond Ti:Sapphire laser THz books  | 
  
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    IntraStage lowers the cost 
    of test data management! Struggling with gigabytes or terabytes of test data? IntraStage easily transforms test data from disparate sources into web-based quality metrics and engineering intelligence you can use. 
    Contact 
us today to discuss your test management requirements and specifications of your 
    application.  | 
  
Training Workshops
| 
     | 
    Come to San Diego next summer! Attend one of our training workshops  in San Diego, California 
    during  summer 2011 Del Mar Photonics has presented training workshops for customers and potential customers in the past 3 years. Our workshops cover scientific basics, technical details and provide generous time for hands-on training. Each workshop is a three-day seminar conducted by professional lecturer from 10am to 4pm. It includes lunch, as well as a training materials. We have also reserved two days for Q&A sessions, one-on-one system integration discussions, social networking, and San Diego sightseeing. 
    The following training workshops will be offered during this 
    summer:  | 
  
Featured Customer
| 
     | 
    
 Trestles LH10-fs/CW laser system at UC Santa Cruz Center of Nanoscale Optofluidics 
Del 
    Mar Photonics offers new  
Trestles fs/CW laser system which can be easily 
    switched from femtosecond mode to CW and back. Having both modes of operation in one system dramatically increase a 
    number of applications that the laser can be used for, and makes it an ideal 
    tool for scientific lab involved in multiple research projects.   | 
  
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 Frequency-stabilized CW single-frequency ring Dye laser DYE-SF-007 pumped by DPSS DMPLH laser installed in the brand new group of Dr. Dajun Wang at the The Chinese University of Hong Kong. DYE-SF-077 features exceptionally narrow generation line width, which amounts to less than 100 kHz. DYE-SF-077 sets new standard for generation line width of commercial lasers. Prior to this model, the narrowest line-width of commercial dye lasers was as broad as 500 kHz - 1 MHz. It is necessary to note that the 100-kHz line-width is achieved in DYE-SF-077 without the use of an acousto-optical modulator, which, as a rule, complicates the design and introduces additional losses. A specially designed ultra-fast PZT is used for efficient suppression of radiation frequency fluctuations in a broad frequency range. DYE-SF-077 will be used in resaerch of Ultracold polar molecules, Bose-Einstein condensate and quantum degenerate Fermi gas and High resolution spectroscopy  | 
  
Other News
    
Optical Society of Southern California meeting at UCSD OSSC 2011-04-27
    Nd:YAG laser ordered by the University of Leon, UANL, Mexico
    
    Wedge 50 Multipass Amplifier pumped with a Darwin-527-30-M DPSS Laser 
    ordered by Hong Kong customer
    
    New 
    Trestles LH10-fs/CW femtosecond+CW laser ready for delivery to the 
    University of California Santa Cruz 
    Trestles femtosecond 
    Ti:Sapphire laser delivered to North Carolina State
    University
    
    
    Del Mar Photonics sponsor IONS (International OSA Network of Students) 
    conference IONS-NA-2 in Tucson, Arizona
    
    IONS-NA-2 
    website
    
    Best talk and best 
    poster awards at IONS-Moscow 2010 conference sponsored by Del Mar Photonics
    Watch Del Mar Photonics 
    videos!
Del Mar Photonics is now on Twitter!
Del Mar Photonics featured components
Del Mar Photonics continuously expands its components portfolio.
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    Solar 
    Prisms for Concentrating Photovoltaic Systems (CPV) Solar cells made of compound semiconductors such as gallium arsenide are very expensive. Usually very small cells are installed and various means such as mirrors, lenses, prisms, etc..are used to concentrate sunlight on the cells. Concentration photovoltaic technology (CPV) uses the solar radiation with an efficiency of 40%, double that of conventional solar cells Del Mar Photonics design custom Concentrating Photovoltaic Systems (CPV) and supply variety of the optical components for CPV such as solar prisms shown in the picture.  | 
  
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    Axicon Lens Axicon lens also known as conical lens or rotationally symmetric prism is widely used in different scientific research and application. Axicon can be used to convert a parallel laser beam into a ring, to create a non diffractive Bessel beam or to focus a parallel beam into long focus depth. Del Mar Photonics supplies axicons with cone angles range from 130° to 179.5° for use with virtually any laser radiation. We manufacture and supply axicons made from BK7 glass, fused silica and other materials. download brochure - request a quote  | 
  
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    Rutile (TiO2) coupling 
    prisms Del Mar Photonics offers optical elements made of high quality synthetically grown Rutile Titanium Dioxide crystals. Rutile’s strong birefringency, wide transmission range and good mechanical properties make it suitable for fabrication of polarizing cubes, prisms and optical isolators. Boules having high optical transmission and homogeneity are grown by proprietary method. Typical boules have 10 - 15 mm in dia. and up to 25 mm length. Optical elements sizes - from 2 x 2 x 1 mm to 12.7 x 12.7 x 12.7 mm. Laser grade polish quality is available for finished elements. So far we the largest elements that we manufactured are 12 x15 x 5 mm, in which optical axis is parallel to 15 mm edge, 5 mm is along beam path, 12 x 15 mm faces polished 20/10 S/D, one wave flatness, parallelism < 3 arc.min. (better specs. available on request). more details - download brochure - request a quote  | 
  
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    Vacuum viewport Del Mar Photonics offer a range of competitively priced UHV viewports , Conflat, ISO or KF including a variety of coatings to enhance performance. Del Mar Photonics viewports are manufactured using advanced techniques for control of special and critical processes, including 100 percent helium leak testing and x-ray measurements for metallization control. Windows Materials include: Fused silica, Quartz , Sapphire , MgF2, BaF2, CaF2, ZnSe, ZnS, Ge, Si, Pyrex. Standard Viewing diameters from .55" to 1.94 ". Coating - a range of custom coatings can applied - which include - Single QWOT - Broad Band AR - V coatings - ITO - DLC (Diamond like coating) more details - request a quote  | 
  
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    Hydrogen 
    Thyratrons are used in 
      such devices as radars with different power levels, high-power pulsed 
      technical, electrophysical, medical devices and lasers. Sophisticated 
      design and high quality ceramic-metal envelope determines long lifetime 
      and very accurate and reliable operation of hydrogen thyratrons under wide range of environmental 
      conditions.  Applications: - radars - pulsed lasers power supplies - medical apparatus - electrophysical instrumentation Triggered Three-Electrode Spark Gap Switches are ceramic-metal sealed off gas discharge trigatron-type devices with a co-axial trigger electrode. These Gas Discharge Tubes contain no mercury and, due to an advanced design, feature high reliability and a long lifetime being operating under wide range of environmental conditions. Applications: - pulsed installation for processing materials - installations with plasma focus - pulse power supplies for lasers and other pulse equipment - medical apparatus such as lithotriptors and defibrillators - processing systems for petroleum wells  | 
  
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    We are looking forward to hear from you and help you with your optical and crystal components requirements. Need time to think about it? Drop us a line and we'll send you beautiful Del Mar Photonics mug (or two) so you can have a tea party with your colleagues and discuss your potential needs. | 

Del Mar Photonics, Inc.
4119 Twilight Ridge
San Diego, CA 92130
tel: (858) 876-3133
fax: (858) 630-2376
    Skype: delmarphotonics
sales@dmphotonics.com