Featured inquiry:
I am interested in your OPO system (Product#: LP604).
I have a nanosecond pulse laser at 532 nm.
This laser has a pulse duration of 1.3 ns, a high-speed repetition rate of 50 –
600 kHz, and an averaged output power of 10 W at 600 kHz.
I want broad wavelength tuning with high-speed repetition rate.
Can I use your OPO system with my laser?
Del
Mar Photonics quote
Compact Pulsed Nd:YAG Lasers
Del Mar Photonics offers compact pulse Nd:YAG lasers with excellent beam
quality, high energy/efficiency and possibility of efficient PRR changes with no
significant degradation of the output beam parameters. No matter how you may
wish to use it — as a standalone laser or as a pump source for tunable lasers
and OPO — the Del Mar Photonics LQ529 laser provides a combination of high
operation parameters, reliability and reasonable price which could not be
achieved earlier.
Ring cavity design of the LQ529 oscillator ensures perfect balance of energy,
beam quality and reliability.
Excellent Beam Quality
Compensation of depolarization over the Nd:YAG rod crosssection together with
traditional advantages of ring cavities ensure excellent beam profile. Unique
optical design of the LQ529 not only makes losses and distortions caused by
induced birefringence almost negligible, but also minimizes thermal lensing
effect. The above allows the user to vary pulse repetition rate within a wide
range and requires no further cavity alignment to preserve high beam quality and
output energy.
LQ529 lasers provide smooth beam profile for all harmonics.
Figures show beam profile at 355nm/50Hz.
This constitutes a great advantage over lasers using expensive and
difficult to align Gaussian optics and thus demanding realignment and sometimes
even replacement of optical components in order to avoid dramatic worsening of
their output parameters if pulse repetition rate (PRR) has been changed.
Energy Through Efficiency
One of the main reasons for moderate efficiency of conventional Q-switched
lasers is birefringence induced in the Nd:YAG rod leading to depolarization of
laser output. Each time the beam passes through the cavity, depolarized lasing
is filtered by various polarization units and is dropped out of the cavity that
leads to decrease in laser operation efficiency. Optical design of the LQ529
laser cavity allows to practically eliminate energy losses caused by
depolarization and provides laser energy output with more than 2% wall-plug
efficiency of a laser system (total electrical-to-optical power efficiency). Such a high efficiency
allows the LQ529 to provide up to 600mJ output energy without using an amplifier.
Single rod and single flash lamp design is the determining factor for reduction
of the laser price and maintenance costs.
Supplementing the basic model with a onepass amplifier allows to provide up to
1500mJ output energy
in the fundamental (model LQ929) while preserving all the advantages of the
LQ529 model.
A power supply unit and a self-contained
water-to-air cooling system are integrated
into one compact package.
Remote controller with the tactile panel
and large LCD makes laser operating much
more convenient.
Stable And Reliable Operation
One of the obvious advantages of the laser is its absolute mechanical stability
and rigidity.
Pulse-to-pulse energy stability of LQ529C laser at 355nm (THG)
All optical components are mounted on the rigid optical bench which is
mechanically and thermally isolated from the laser housing. This ensures
exceptional alignment stability even under toughest conditions of
transportation and operation. All nonlinear crystals and Pockels cell are
temperature stabilized. Optical bench with cavity components is also
temperaturestabilized. High-precision termostabilization ensures minimal
pulsetopulse and longterm instability. Heating of optical components to the
temperature exceeding ambient totally eliminates any risk of condensation. This
feature along with dustproof housing protects the optics from damage and
minimizes the necessity in service. It should also be noted that the LQ529 laser
design eliminates the necessity of any laser alignments after flashlamp replacement, while the replacement procedure itself takes less than 10
minutes.
All Harmonics Available
All harmonic options — 532nm, 355nm, 266nm and 213nm — are available as
standard.
High-efficiency Harmonic Generators can be either built-in (except for the FiHG)
or supplied as separate units upon the customer’s request. For this reason all
the harmonics can be ordered with the laser or at later date.
Compact Intelligent Power Supply
A power supply unit and a selfcontained watertoair cooling system are
integrated into one compact package. Compact size and closed loop cooling system
which requires no external water, allow to place the power supply under the
optical bench or wherever convenient. Computer control using the optional RS232
interface allows integration into laboratory or industrial automated systems.
Highpower cooling system and automatic temperature control with 0.5°C precision
ensure stable laser operation at up to 30°C ambient temperature. A heater built
into the cooling system reduces warm-up time to several minutes even at 15°C
ambient temperature.
ACCESSORIES AND OPTIONS
* Built-in and External Harmonic Generators up to
5th Harmonic
* Solid State Raman Converter
* Solid State Optical
Parametric Oscillator OPO
* High Power Attenuator for All Harmonics
* Custom Configurations
SOLID-STATE NONLINEAR CONVERTERS |
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Case studies:
Raman
shifter for conversion from 1064 nm to 1328 nm
APPLICATIONS
Nonlinear optics
Excellent beam quality and high pulse energy allow to use the LQ529 laser for
nonlinear spectroscopy, plasma physics, nonlinear optics and harmonic
generation.
Spectroscopy
High pulse repetition rate allows to reduce data collecting time, while high
stability almost eliminates calibration drift troubles in Raman and
time-resolved spectroscopy.
Velocimetry
Critical for the success of PIV experimentation is stable, reliable compact
laser source. The LQ529 ideally suits for most PIV experements. Del Mar
Photonics offers several custom configurations for Particle Image Velocimetry
experiments based on the LQ529.
Pump source
The LQ529 ideally suits for tunable lasers and OPO pumping. Models LQ829 and
LQ929 are ideal pump lasers for terawatt class Ti:Sapphire amplifiers.
Material processing
Meets almost all major requirements made to lasers for industry applications.
Design features provide a highest reliability and low demands to operation
conditions. Low operating cost, fast and simple service are also significant
factors for industrial applications of the LQ529 Laser.
Mobile laser systems
Unique mechanical rigidity and resistance to mis-alignments, low electricity
consumption and air cooling make the LQ529 an ideal laser source for various
mobile measuring and monitoring systems which may be installed on any transport
means. Dust protected laser head design ensures long-term reliable operation of
laser optical components even in field conditions.
Nd:YAG laser models
Model | LQ529A | LG529B | LQ529C | LQ829 | LQ929 | ||
Configuration | Oscillator only | Oscillator + Amplifier | |||||
Pulse repetition rate, Hz | 5 | 10 | 10 | 20 | 50 | 10 | 10 |
Output energy, mJ | |||||||
at 1064 nm | 500 | 500 | 350 | 350 | 150 | 1000 | 1400 |
at 532 nm 1), 3) | 280 | 280 | 190 | 190 | 80 | 550 | 800 |
at 355 nm 1), 4) | 110 | 100 | 90 | 90 | 40 | 220 | 300 |
at 266 nm 1), 3) | 100 | 70 | 60 | 40 | 16 | 120 | 180 |
at 213 nm 2), 4) | 25 | 20 | 15 | 12 | 5 | 40 | 50 |
Pulsewidth, ns 5) | 10...13 | 8...11 | |||||
Beam diameter, mm | ≤8 | ≤6 | ≤5 | ≤10 | ≤11 | ||
Divergence, mrad | ~1.5 | ~1.3 | ~1.5 | ||||
Stability +/- % better than 5) | 2.5 | ||||||
Cooling | self-contained water-air cooling system | ||||||
Power consumption, less than, W (single phase, 220V+/- 10%, 50/60 Hz) |
400 | 600 | 600 | 800 | 1000 | 900 | 1000 |
Dimensions, mm | |||||||
Laser head | 575 x 180 x 100 | 600 x 220 x 115 | |||||
Power supply | 650 x 290 x 650 | 770 x 340 x 670 |
1) Harmonic generators built in laser head
2) When operating with external harmonic generator LG105
3) When SHG is optimized
4) When THG is optimized
5) At 1064 nm
* Excellent beam quality and stability
* All harmonics
up to 213 nm
* High pumping efficiency
* Turn-key operation
* Remote controller and
RS232 interface as standard
* No external water,
single phase mains operation
* Low maintenance
Nd:YAG Laser LQ929 is used as pump laser for second stage amplifier in Femtosecond Terawatt Ti:sapphire Laser System Teahupoo MPA-XL
pulsed Nd:YAG laser model LQ529C-TEM00 with aperture inside the cavity (TEM00)
Related Del Mar Photonics products
If you can't find information about the products that you are looking for just e-mail our Sales Team and we'll e-mail or call you back right away!
Trestles LH femtosecond lasers with integrated DPSS DMPLH laser pump - DPSS DMP LH series advantages
Trestles LH10-fs/CW laser system at UC Santa Cruz Center of Nanoscale Optofluidics
Del Mar Photonics Tresltes LH laser used for STED microscopy of nanodiamons
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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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. |
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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 |
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 |
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