Del Mar Photonics - Newsletter
Subject: RFQ for Actively frequency-stabilized CW single-frequency ring Ti:Sapphire laser TIS-SF-777
I need a quote for this laser.
I'll need the highest power available and less than 100 kHz linewidth.
What is the power output at 780 for the middle optics set? I want to be able to operate at 780 nm, 800 nm, 850 nm, or 920 nm with several Watts of power.
Please include shipping/freight and installation. Do you have a service plan? Please include the details and price if you do.
Also, you mention locking to an atomic line: Can I choose the line? How would I change it later if I wanted to lock somewhere else?
Del Mar Photonics reply and quote
Actively frequency-stabilized CW single-frequency ring Ti:Sapphire laser TIS-SF-777
request a quote
Unique TIS-SF-777 laser has more narrow linewidth for Ti:Sa lasers on the present market. TIS-SF-777 laser has super-narrow linewidth (< 5 kHz/sec) and unique Auto Re-lock function which is extremely useful in a work with frequency stabilized laser.
Ring design, three wavelength selectors: birefringent filter, thin and thick etalons, elec-tronically controlled thick etalon to ensure laser operation in a single longitudinal-cavity mode.
Ultra-narrow line width up to < 5 kHz rms (1 sec): active frequency stabilization to an external reference cavity, special fast PZT actuator with extended response bandwidth.
Unique function Smart Auto-Relock that allows uninterrupted laser operation in the fre-quency stabilisation mode under arbitrary external perturbations.
Actively thermostated high-finesse reference cavity, frequency drift <40MHz/hr.
External lock capability for stabilization to an absolute reference (e.g. iodine saturated absorption line).
Wavelength range, power
Laser optimized at factory for primary operation wavelength around 759 nm
Output power at 759nm+/-10nm 1,4W or better with 10W pump (DPSS, 532 nm, TE-Moo).
TEMoo mode, linear polarization.
Most of the mounts are placed on a horizontal base plate, which is also the top element of the compact rigid 3-D frame made from three invar rods that ensures high stability of the optical element positions.
Ease of adjustment, simplified laser alignment in the ring configuration because of pre-liminary optimisation of the elements in the linear cavity, exceptionally accurate alignment of the pump beam position.
Premium Ti:Sapphire crystal (FOM > 500).
Enclosed cavity with nitrogen purge port.
Ergonomical and reliable electronic control unit featuring a built-in generator for smooth scanning of the laser frequency.
Actively frequency-stabilized, continuous-wave, single-frequency ring Titanium-Sapphire laser, model TIS-SF-777:
Wavelength ranges: 700-770 nm
Linewidth: < 10 kHz/sec rms
Output power: > 1,4W@759+/-10nm at 10W pump (532 nm, TEMoo)
Smooth scanning: > 5 GHz
Frequency drift: < 40 MHz/hour
Polarization: horizontally polarized output
Auto-Relock function, external lock capability for stabilization to an absolute reference
Price of the TIS-SF-07 laser with above mentioned specifications, including delivery, installation and 12-months warranty period: Request a quote
Accessories & Options:
Extra optics set (695-770 nm or 850-950 nm or 950-1050 nm): request a quote
Smooth scanning > 18 GHz: request a quote
Standard delivery time: 12 weeks ARO.
Recommended pump laser:
DPSS DMPLH lasers
Nice tool for alignment:
Near IR viewers
Ultraviolet viewers are designed to observe radiation emitted by UV sources.
|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.
spot in our
CW lasers training
workshop in San Diego, California. Come to
learn how to build a
Ti:Sapphire laser from a kit
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
TIF-SF-777 support - thick etalon adjustment
High-energy Yb-doped all-fiber femto-, pico-, nano-second laser, model Tourmaline Ytterbius-Master
T&D Scan high resolution Laser Spectrometer based on broadly tunable CW laser
CW single-frequency ring Dye laser
Delmar-Tekhnoscan - resonant doubler - atom cooling - Yb:KYW - BIBO - Adiabatic frequency conversion of quantum optical information in atomic vapor - Ultra-narrow-linewidth combined CW Ti:Sapphire/Dye laser for atom cooling and high-precision spectroscopy - Vortex-Lattice Dynamics in Rotating Spinor Bose-Einstein Condensates. Vortex Dynamics in and around the Lowest Landau Level - Characterization of atomic coherence decay for the storage of light - Decoherence of electromagnetically-induced transparency in atomic vapor - Diluted maximum-likelihood algorithm for quantum tomography - Efficiency limits for linear optical processing of single photons and single-rail qubits - Electronic noise in optical homodyne tomography - Interconvertibility of single-rail optical qubits - Mark Kasevich: Atom optics and interferometry and the study of quantum many-body effects in dilute atomic vapors - Mark Kasevich: Laser cooling and trapping and Bose-Einstein condensation studies - Preparation and probing of the ground state coherence in rubidium - Pulsed squeezed light: simultaneous squeezing of multiple modes - Raman adiabatic transfer of optical states in multilevel atoms - Resonant doubler with a 2-THz automatic quasi-smooth scan range for widely tunable CW single-frequency lasers - CW single-frequency ring Ti:Sapphire and dye lasers for atom cooling, trapping, quantum manipulation and high resolution spectroscopy, nanostructures analysis and fabrication - Trapping, Spectroscopy, and Collisions of Ultracold Atoms and Molecules - Diode-pumped femtosecond master Yb:KYW laser for multi-terawatt Nd-glass facility PROGRESS-P
|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.|