Our femtosecond laser sources are based on robust and well-engineered designs, offering an excellent reliability with the low-noise performance from soliton mode-locking. Robust 24/7 operation, user-friendly and self-starting, our lasers have been made to facilitate OEM integration and enable customers’ applications.
Key Features:
Main Applications:
Key Specifications:
|
STMH-1550 |
STMH-1550+ |
Construction |
Oscillator, no amplifier |
With amplifier |
Average power |
>50mW |
Up to 2W |
Peak power |
>0.1kW |
Up to 4kW |
Pulse energy |
>0.05nJ |
Up to 1nJ |
Repetition rate |
Standard – 250, 500MHz, 1, 1.25, 2 or 2.5GHz. Custom design – 200MHz to 2.5GHz |
Standard – 250, 500MHz, 1, 1.25, 2 or 2.5GHz. Custom design – 200MHz to 2.5GHz |
Center wavelength |
1555nm +/- 10nm |
1555nm +/- 10nm |
Spectral bandwidth |
>10nm at 3dB |
>10nm at 3dB |
Pulse width |
<250fs, transform-limited |
<250fs, transform-limited |
Optical output port |
Fiber output (PM FC/APC), free-space |
Fiber output (PM FC/APC), free-space |
Beam quality |
TEM00, M2<1.05 |
TEM00, M2<1.05 |
Polarisation |
Linear (PER>23dB, >200:1) |
Linear (PER>23dB, >200:1) |
Amplitude noise |
<0.1% RMS (24h) |
<0.1% RMS (24h) |
Timing jitter |
<30fs (1kHz – 10MHz) |
<30fs (1kHz – 10MHz) |
Power supply |
5VDC/2A |
24VDC/2A |
Power consumption |
<10W |
<50W |
Cooling |
Passively air-cooled |
Passively air-cooled |
Warm-up time |
<10s (cold start) |
<10s (cold start) |
Laser head size/weight |
240x160x89mm/5kg |
240x160x89mm/5kg |
Control unit |
No control unit required |
No control unit required |
Operation temperature |
+5oC to +45oC |
+5oC to +45oC |
Storage temperature |
-10oC to +60oC |
-10oC to +60oC |
Relative humidity |
<80% (non-condensing) |
<80% (non-condensing) |
Analog interface |
Eg. Power mod, alarm, interlock, trigger, status |
Eg. Power mod, alarm, interlock, trigger, status |
Digital interface |
USA, RS232, ETHERNET, CAN |
USA, RS232, ETHERNET, CAN |
And find more about the full characterization of two versions of our lasers: STMH-1550 at 1 GHz laser and STMH-1550 at 250 MHz.
It is the first industrial-grade laser of its kind that operates at telecom wavelengths and achieves the lowest phase noise and timing jitter on the market. In this document, we report the full characterization of the product operating at a repetition rate of 1 GHz.
Key product specifications
Noise characterization (Free-running)
The free-running phase and amplitude noise of a STMH-1550 at 1 GHz is reported here. The phase noise was measured on the 10th harmonic, i.e., at 10 GHz.
Offset frequency (fc) |
Phase noise (dBc/Hz) 1 GHz carrier 10 GHz carrier |
Timing-jitter (fs) [fc – 10 MHz] |
Amplitude noise (RMS) [fc – 10 MHz] |
|
10 kHz |
< -150 |
< -130 |
< 1 |
< 0.01% |
1 kHz |
< -115 |
< -95 |
< 10 |
< 0.01% |
100 Hz |
< -90 |
< -70 |
< 100 |
< 0.01% |
1 Hz |
< -30 |
< -10 |
< 5000 |
< 0.02% |
Possibilities and options:
The STMH-1550 SERIES is the first industrial-grade laser of its kind that operates at telecom wavelengths and achieves the lowest phase noise and timing jitter on the market. In this document, we report the full characterization of the product operating at a repetition rate of 250 MHz.
Key product specifications
Noise characterization (Free-running)
The free-running phase and amplitude noise of a MENHIR-1550 at 250 MHz is reported here. The phase noise was measured on the 40th harmonic, i.e., at 10 GHz.
Offset frequency (fc) |
Phase noise (dBc/Hz) 1 GHz carrier 10 GHz carrier |
Timing-jitter (fs) [fc – 10 MHz] |
Amplitude noise (RMS) [fc – 10 MHz] |
|
10 kHz |
< -155 |
< -135 |
< 1 |
< 0.01% |
1 kHz |
< -140 |
< -110 |
< 2 |
< 0.01% |
100 Hz |
< -110 |
< -80 |
< 10 |
< 0.01% |
1 Hz |
< -50 |
< -20 |
< 1500 |
< 0.02% |
Possibilities and options:
The FSC1040 is an air-cooled, compact ultrafast laser.
Applications
Technical Overview
Features & Benefits
Part number |
FSC-1030-750 |
FSC-1040-2500 |
FSC-1040-3500 |
Output power |
Up to 750 mW |
>2.5W |
>3.5W |
Wavelength |
1030nm |
1040nm |
1040nm |
Pulse energy |
7.5nJ |
25nJ |
> 35nJ |
Pulse duration |
< 150fs |
||
Repetition frequency |
100MHz |
||
Beam parameters |
Free space, M2 < 1.3, Linearly polarized Divergence < 2mrad |
||
Beam diameter |
0.5 - 1.2 mm |
||
Control Interface |
Web browser interface. Ethernet & serial port (RS232) also available. |
||
Electrical |
Voltage 110 – 240V AC, Frequency 50 – 60Hz, Power 80W |
||
Dimensions |
426x250x108mm (laser head) 483x285x88mm (control unit – 19” 2U rack mount) |
Good News: FSC Series Ultrafast Lasers for Hire:
Hire one of our ultrafast lasers to experience their power and robustness first-hand. You can now use our femtosecond fiber lasers, or tunable optical parametric oscillators, to accelerate your research without incurring the total cost of ownership.
Our FSC-1040 laser and FSC series OPOs can be drop-shipped and installed remotely, without the presence of an onsite engineer. Our ultrafast lasers are easy-to-use and operational ready straight out of the box – so you spend less time running the equipment, and more time pioneering results.
Hire an ultrafast laser system and test drive our capabilities. Please send your email to us to receive details about hire costs and the availability of our demonstrator systems.
Applications
Technical Overview
Features & Benefits
Pumped by a PSC1040 ensures delivery of high quality ultrashort pulses in the green.
Part number |
FSC-532-500 |
FSC-532-1500 |
Configuration |
FSC1040 and internal SHG module |
FSC1040 and external SHG module |
Output power |
Up to 500mW |
Up to 1.5W |
Wavelength |
520 nm (1040 nm also available) |
520 nm (1040 nm also available) |
Pulse duration |
<150fs |
< 150fs |
Repetition frequency |
100MHz |
100MHz |
Beam parameters |
Free space, Linearly polarized Divergence < 2mrad |
Free space, Linearly polarized Divergence < 2mrad |
Beam diameter |
0.5-1.2mm |
0.5-1.2mm |
Control interface |
Web browser interface Ethernet & serial port (RS232) also available |
Web browser interface Ethernet & serial port (RS232) also available |
Electrical |
Voltage 110 – 240VAC, Frequency 50–60Hz, Power 80W |
Voltage 110 – 240VAC, Frequency 50 – 60Hz, Power 80W |
Dimensions (PSU) |
483x255x177mm |
483x255x177mm |
Dimensions (Laser head) |
526x250x108mm |
426x250x108mm SHG module 150x300mm |
Application Notes:
Measuring Picosecond Fluorescence Lifetimes using a FSC 520
Deep tissue cardiac imaging using the FSC 1040
SHG imaging in starch and collagen fibres using the FSC 1040
Two-photon fluorescence microscopy using the FSC 1040
Two-Photon Lightsheet Microscopy using the FSC 1040
Heating of Hybrid Gold-Iron Oxide Nanoparticles in Biological Media using the FSC 1040
Supercontinuum using FSC 1040
Two-Photon quantum interference and entanglement at 2.1μm using the FSC 1040 and Near-IR OPO
Active FTIR-based stand-off spectroscopy using a femtosecond optical parametric oscillator
White powder identification using broadband coherent light in the molecular fingerprint region
Stand-off identification of aerosols using mid-infrared backscattering Fourier-transform spectroscopy (Near-IR OPO)
Photon counting LIDAR at 2.3μm wavelength with superconducting nanowaves
Open-path multi-species remote sensing with a broadband optical parametric oscillator
Experimental observation of gain in a resonantly pumped Pr3+doped chalcogenide glass mid-infrared fibre amplifier
Dual-comb spectroscopy in the spectral fingerprint region using OPGaP optical parametric oscillators
Infrared fingerprint-region aerosol spectroscopy
Molecular fingerprint-region spectroscopy from 5 to 12μm using an orientation-patterned gallium phosphide optical parametric oscillator
The Femtosecond Mode Lock Fiber Laser is a compact, high-reliability laser featuring an all-fiber design (no bulk optics) with a center wavelength of 1030 nm at an average output power of 10mW, repetition rate of 25 MHz with pulse duration of 600 fs.
Applications
Features
Specifications
The 920nm and 1190nm are made up of two modules: 2RU pump module 440 x 343 x 92 (mm), and the Femtosecond Fiber Laser - 284 x 324 x 116 (mm).
The high-power Mode Locked Femtosecond Fiber Lasers operate at the 920nm and 1190 nm spectral range - which is traditionally covered by ultrafast Ti:Sapphire lasers and optical parametric oscillators. They generate linearly polarized nearly transformed-limited pulses with a pulse duration of 200 fs, at a repetition rate of 80 MHz, and an average power of 1 W.
Compact and maintenance-free, the lasers are fiber-based, have a very good beam profile, and do not require optical alignment.
The Femtosecond Fiber Laser is a natural product extension with its extensive suite of our visible fiber lasers developed for the microscopy industry, and its existing line of Picosecond Pulsed Mode Locked Fiber Lasers.
Features
Applications
Part number |
FSM-MLFL-920-femto |
FSM-MLFL-1190-femto |
|
Central Wavelength |
920 |
1190 |
nm |
Repetition Rate |
80 |
90 |
MHz |
Pulse Duration |
100 |
200 |
fs |
Average Output Power |
≥ 1 |
≥ 1 |
W |
Spec. Width |
10 |
10 |
nm |
Beam Diameter |
1 |
1 |
mm |
Polarization |
Linear, 99 |
Linear, 99 |
% |
FSF series high-power fs fiber laser is a 1030 nm high-power femtosecond fiber laser delivering up to 160µJ at 20W. With truly monolithic all-fiber front-end this laser provides fast warm-up time, unprecedented long-term stability and hands-free operation. Contrary to free space laser amplifiers, fiber amplifiers ensure unbeatable beam pointing stability even in harsh environment.
The laser is the right choice whenever there is a need for the high power and high pulse energy while maintaining a very short pulse duration. Some applications include:
Options:
If you require continues wavelength tuning, please contact us for more information.
|
FSF-1030-10 |
FSF-1030-20 |
FSF-1030-30 |
Maximum average power |
> 10 W |
> 20 W |
> 30 W |
Maximum pulse energy |
> 50 μJ |
> 50 μJ |
> 100 μJ |
System base repetition rate |
100 kHz – 25 MHz, selectable with control software |
||
Pulse duration |
< 250 fs (FWHM) |
||
Pulse duration tuning |
Option: Ask for details |
||
Central wavelength |
1030 ± 5 nm |
||
Optional wavelength outputs |
515 nm, 343 nm, 258 nm |
||
Built-in pulse picker |
Pulse on demand, any division of the base repetition rate |
||
Beam quality M2 |
< 1.3 |
||
Polarization |
Linear, vertical |
||
External gating trigger |
Included |
||
Laser control software |
Included |
||
Laser head size |
|||
Power supply size |
3U 19” rack unit: 485x376x132mm (LxWxD) |
||
Electrical |
100-240VAC, 50/60Hz, <250W |
||
Operating temperature |
15-35oC |
||
Operating humidity |
Non-condensing |
||
Chiller size |
3U 19” rack unit: 485x381x132mm (LxWxD) |
||
Electrical |
100-240VAC, 50/60Hz, <10A |
FSF series fiber laser is a compact, single-box, all-fiber femtosecond laser, specifically designed to meet the most demanding applications in the field of neuroscience, bio-photonics, microscopy and engineering. With pulses as short as < 180fs, average power up to 2W at 1030nm and option of second harmonic at 515nm, it is an irreplaceable tool in every lab that needs a reliable, turn-key, ultrafast light source. Thanks to its unique construction and SESAM-free technology it is a cost-effective solution that provides high pulse energy (up to 100nJ) with an excellent beam quality. Our industrial design facilitates easy integration with both experimental and commercial systems.
The laser can be used in applications that need pure and stable laser pulses. This includes:
Features:
Part number |
FSF-1030-0.7 |
FSF-1030-2 |
Maximum average power |
> 700mW |
> 2W |
Maximum pulse energy |
> 35nJ |
> 100nJ |
Pulse duration |
<200fs (<170fs option) |
<250fs FWHM |
System base repetition rate |
20 ± 2 MHz |
|
Central wavelength |
1030 ± 5 nm |
|
Optional wavelength outputs |
515 nm, 343 nm, 258 nm |
|
Beam quality M2 |
< 1.2 |
|
Polarization |
Linear, vertical |
|
Power supply |
Standard 24VDC |
|
Weight |
3kg |
|
Size |
350x230x60mm (LxWxD) |
|
Electrical |
100-240VAC, 50/60Hz, <50W |
|
Operating temperature |
15-35oC |
|
Operating humidity |
Non-condensing |
Laser control software included
Options:
The FSH series fiber lasers are stable and reliable femtosecond pulsed fiber lasers. This series of products adopts integrated optical and electrical design, pulse width less than 350fs, single pulse energy up to 200μJ, and supports Burst Mode, which can be widely used in semiconductor wafer processing, glass and other hard and brittle materials processing or Welding, processing and processing of polymer materials, medical device manufacturing, ceramics and polymer processing.
Part Number |
FSH-1064-35 |
Wavelength |
1035nm |
Average Power |
35W |
Pulse Energy |
200μJ @ 175 kHz |
Pulse Duration |
<350fs |
Peak Power |
>500MW |
Repetition Rate |
Single shot to 2MHz |
Beam Quality |
M2≤1.3 |
Beam Divergence |
<1mrad, 2θ |
Beam Circularity |
85% |
Beam Diameter |
4 ±2 mm, 1/e2 |
Polarization Ratio |
>100:1 |
Polarization Direction |
Vertical |
Pulse Energy Stability |
<2% RMS |
Power Stability |
<2% RMS |
External Control |
RS-232, Ethernet, USB |
Dimension |
FSH-Femto-NP (Narrow Pulse Width) series femtosecond fiber lasers can support the pulse width sub 150fs and average output power up to 5 W. Internal second harmonic generation module is also optional. The applications include micromachining, photo polymerization, Multiple photon excitation, Biological Imaging, ultrafast spectroscopy etc.
Feature:
|
FSH-Femto-NP-1 |
FSH-Femto-NP-1-SHG |
FSH-Femto-NP-5 |
Central wavelength |
1035±4nm |
517±2nm |
1035±4nm |
Average power |
>1W |
>400mW |
>5W |
Pulse duration |
<150fs |
<150fs |
<150fs |
Pulse repetition rate |
90-100MHz |
90-100MHz |
45±5MHz |
Beam quality |
M2<1.2 |
M2<1.2 |
M2<1.2 |
Beam divergence (full) |
<3mrad |
<3mrad |
<3mrad |
Beam circularity |
³90% |
³90% |
³90% |
Beam diameter |
3±1mm |
3±1mm |
3±1mm |
Polarization ratio |
>100:1 |
>100:1 |
>100:1 |
Pulse stability |
<2% RMS |
<2% RMS |
<2% RMS |
Power stability |
<1% RMS |
<1% RMS |
<1% RMS |
Operation temp. |
10 – 30 oC |
10 – 30 oC |
10 – 30 oC |
Dimension |
FSY series femtosecond fiber lasers have been widely used in the material micro-processing field. Our femtosecond fiber lasers offer >80W average power, >5MHz repetition rate with the pulse energy upto 100µJ.
Model |
FSY-1035-6 |
FSY-1035-10 |
FSY-1035-20 |
FSY-1035-50 |
FSY-1035-100 |
Center Wavelength |
1035nm |
1035nm |
1035nm |
1035nm |
1035nm |
Total power |
>6W |
>10W |
>20W |
>50W |
>100W |
Repetition rate |
80MHz |
1Hz - 5MHz |
1Hz - 5MHz |
1Hz - 5MHz |
1Hz - 5MHz |
Power stability |
<1% |
<1% |
<1% |
<1% |
<1% |
Pulse energy |
>10µJ |
>40µJ |
>100µJ |
>200µJ |
|
Number of burst pulse |
1 ~10 |
1 ~10 |
1 ~10 |
1 ~10 |
|
Burst pulse combinatintion energy |
>100µJ |
>120µJ |
>300µJ |
>400µJ |
|
Pulse width |
150fs |
400fs - 6ps |
400fs - 8ps |
400fs - 8ps |
400fs - 8ps |
Beam diameter |
3mm |
3mm |
3mm |
3mm |
3mm |
Beam pergence |
<1mrad |
<2mrad |
<2mrad |
<2mrad |
<2mrad |
Polarization |
Linear |
Linear |
Linear |
Linear |
Linear |
Sync (trigger) output |
SMA TTL pulse |
SMA TTL pulse |
SMA TTL pulse |
SMA TTL pulse |
SMA TTL pulse |
Power supply |
AC 100V - 240V, 50/60Hz, Rated output>960W |
AC 100V - 240V, 50/60Hz, Rated output>960W |
AC 100V - 240V, 50/60Hz, Rated output>960W |
AC 100V - 240V, 50/60Hz, Rated output>960W |
AC 100V - 240V, 50/60Hz, Rated output>960W |
Dimensions (L*W*H) |
680mm*480mm*212mm |
680mm*480mm*212mm |
680mm*480mm*212mm |
1200mm*410mm*141mm |
1200mm*410mm*141mm |
Control |
RS232 or DB25 |
RS232 or DB25 |
RS232 or DB25 |
RS232 or DB25 |
RS232 or DB25 |
IMPULSE is an all-diode-pumped, direct-diode-pumped, Yb-doped fiber oscillator/amplifier system capable of producing variable pulse energies up to 10μJ with user-selectable repetition rate between 200 kHz and 25 MHz. With 20 watts average power output at 2MHz, IMPULSETMoffers more than an order-of-magnitude higher power than has traditionally been available in a one-box ultrashort pulse laser design.
IMPULSETMis based on a revolutionary new concept in mode-locked oscillator/amplifier technology. The Yb-doped fiber oscillator/fiber-amplifier design combines the low noise performance of solid-state operation with high spatial mode quality of fiber lasers.
IMPULSETMis a compact, robust, one-box source of femtosecond to picosecond pulses with the ease-of-operation, stability and reliability you expect from a fiber source. All major parameters are computer controlled, enabling easy interface to workstation or experiment. IMPULSETMis even iPhone/ iPod2App enabled.
Optional accessories include multi-photon photo-polymerization, waveguide writing, micromachining, harmonic generation, and OPA/NOPA wavelength conversion for high S/N and rapid data acquisition in pump/probe experiments.
Remark:
The STKM-YFi laser series is a family of high average power, high repetition rate near-IR ultrafast fiber lasers. STKM-YFi products are based on a single rugged opto-mechanical platform and are engineered for hands-free operation.
STKM-YFi Outstanding Characteristics
The STKM-YFi system employs a patented all normal dispersion (ANDi) mode-locked fiber laser coupled with a fiber amplifier. This configuration offers numerous unique advantages, including:
The short, clean pulses of the STKM-YFi laser series deliver more peak intensity per mJ than competing products. We guarantees both pulse duration and pedestal energy content, verified with a FROG pulse measurement, to ensure each laser pulse is free of picosecond background that robs energy from the main short pulse. Thus, more of the laser output is truly usable, requiring less energy/average power and decreasing the probability of seeing collateral damage and other detrimental interactions.
Parameter |
STKM-YFi |
STKM-YFi HP |
STKM-YFi Ultra |
Pulse Width |
<150 fs (<120 fs typical) |
<170 fs |
<190 fs |
Compressor Dispersion Pre-compensation |
±20,000 fs2 |
±10,000 fs2 |
Inquire |
Centre Wavelength |
1035 ± 5 nm |
1035 ± 5 nm |
1035 ± 5 nm |
Pulse Energy |
> 0.45 µJ @ 10 MHz |
> 3 µJ @ 1 MHz |
> 40 µJ @ 1 MHz |
Beam Quality |
M2 < 1.2 |
M2 < 1.2 |
M2 < 1.2 |
Average Power |
> 4.5 W @ 10 MHz |
> 20 W @ 10 MHz |
> 50 W @ 10 MHz |
Repetition Rate |
0.5 - 15, 60 MHz |
0.5 - 15, 60 MHz |
0.5 - 15, 60 MHz |
Auto-Correlation Pedestal Content |
< 12%
|
< 15% |
< 20% |
Background content |
< 1.0% |
< 1.0% |
< 2.0% |
Pre-Pulse Contrast |
< 0.5% |
< 0.5% |
< 1% |
Post-Pulse Contrast |
< 0.5% |
< 0.5% |
< 1% |
Power Stability* |
<1% RMS over 12 hours after 30 min warm-up |
<1% RMS over 12 hours after 30 min warm-up |
<1% RMS over 12 hours after 30 min warm-up |
Pointing Stability* |
< 10 µRad RMS after 30 min warm-up |
< 10 µRad RMS after 30 min warm-up |
Inquire |
Operational Temp. Range |
16 - 26 °C |
16 - 26 °C |
16 - 26 °C |
Physical Configuration |
|||
Computer Interface |
Laptop provided, w/GUI |
Laptop provided, w/GUI |
Laptop provided, w/GUI |
SHG Power |
Inquire |
> 8 W @ 10 MHz |
Inquire |
SHG Pulse Duration |
Inquire |
< 150 fs |
Inquire |
*Ambient ± 0.5°C
|
|
STKM-YFi HP power and pointing stability over 50 hours, in typical lab conditions |
M-YFi HP clean 131 fs pulses at 20W output (2 mJ, 10 MHz), measured with frequency resolved optical grating (FROG). |
|
|
Average power measured over 20h showing fluctuations < 0.3% RMS |
Measured temporal pulse with a duration of 168 fs FWHM operating at 22 μJ at 1 MHz |
Coherent, EUV-wavelength light, made through high harmonic generation (HHG), has finally come of age. STKM-XUUS-5 is our fifth generation of EUV conversion platform designed to offer “black-box” conversion of ultra-short, infrared laser pulses into short wavelength, laser-like radiation. Our patented use of fiber-based HHG architecture ensures repeatable, highly-stable, bright and low gas-usage generation of EUV light.
STKM-XUUS-5 upconverts ultrafast laser pulses into the Extreme UV (EUV or XUV) or soft X-ray regions of the spectrum. Employing HHG processes, the output beam inherits the coherent properties of a driving laser such as the amplifier with wavelengths that can be tuned from ~10 to 50 nm. Moreover, customized systems can generate coherent beams with wavelengths as short as 6 nm. The STKM-XUUS-5 employs our patented hollow waveguide for the high harmonic up-conversion process.
The STKM-XUUS hollow-core fiber, or waveguide, architecture enables harmonics generated by the system to be distinguished from other HHG methods, guaranteeing your harmonics originate from the same point in space every time, minimizing any pointing drift. This architecture optimizes repeatability for your experiments. Additionally, the use of a fiber--rather than typical gas jet or semi-infinite gas cell target geometries--provides superior pressure tunability for phase-matched HHG. Now you can choose robustness without sacrificing flexibility.
Features
Applications
Specifications
Wavelength |
Flux* |
Repetition Rate |
Pointing Stability |
Power Stability |
30 nm |
>5x1012 ph/sec per harmonic |
1 - 20 |
<5 µrad RMS |
<5% RMS |
13 nm |
>1010 ph/sec per harmonic |
1 - 10 |
<5 µrad RMS |
<5% RMS |
6 nm |
>106 ph/sec per 10% BW |
1 |
<10 µrad RMS |
<10% RMS |
*Achievable when optimally coupled to our Ti:sapphire amplifier. Performance will vary with other driving lasers.
We provide bright femtosecond pulses at numerous wavelengths across the vacuum ultraviolet (VUV) region, from 6.0 eV (205 nm) to 10.8 eV (115 nm). The discrete tunability of the our STKM-Hyperion-VUV vacuum ultraviolet source enables researchers to study a wide range of materials and materials properties. A simple computer-selected change of photon energy provides a powerful capability, previously only available at a synchrotron; this ability to easily change the laser wavelength can enhance many experiments. For example, in angle-resolved photoemission (ARPES) experiments, this tunability allows researchers to distinguish surface effects from bulk effects. For time-of-flight (ToF) studies of molecules, the tunability can distinguish otherwise identical isomers.
STKM-Hyperion-VUV is also highly focusable, and the appropriate optics can be used to reach spot sizes below 10 microns. This ability will allow researchers to examine new types of samples, including materials that are polycrystalline, spatially inhomogeneous, faceted, or simply very small.
STKM-Hyperion-VUV produces pulses with durations below 250 femtoseconds, enabling scientists to probe ultrafast dynamics of molecules and materials. The 1 MHz repetition rate enables rapid data collection and avoids space-charge effects.
Additionally, STKM-Hyperion-VUV is “application ready,” including the appropriate focusing and beam-steering elements to enable fast integration with experimental apparatus. Importantly, STKM-Hyperion-VUV can be used with a window between the source and the experimental chamber, guaranteeing that applications demanding ultrahigh vacuum (such as ARPES) will remain contamination-free.
In addition to ARPES, STKM-Hyperion-VUV will enable breakthrough research in photoemission electron microscopy (PEEM), photoionization mass spectroscopy (PIMS) for combustion research, and other studies of next-generation materials and molecular systems.
STKM-Hyperion-VUV:
Applications:
Features that lead to significant benefits:
Tunable (computer-selected) photon energy between 6–10.8 eV enhances capabilities for laser ARPES experiments:
Tight focal spot provides greater sample flexibility, allowing the study of
A window provides complete isolation between Hyperion VUV and the experimental chamber, maintaining high vacuum
Femtosecond pulses enable time-resolved experiments
Hyperion VUV measures only 2.5 feet x 5 feet, bringing the power of the synchrotron to your lab
Photon energy (eV) |
User selectable: 6, 7.2, 8.4, 9.6, 10.8 |
|
Repetition rate |
1MHz |
|
Power stability |
<5% (RMS) |
|
Photon flux |
Full bandwidth (~40meV) |
Maderate bandwidth (<5meV) |
7.2eV |
1012 ph/s delivered |
5x1010 ph/s delivered |
10.8eV |
1010 ph/s delivered |
5x108 ph/s delivered |
Laser head size |
750x1500mm |
|
Electrical power |
110/230V 20A (x2) |
Femtosecond lasers enable high precision processing without any heat effect on the material. Despite the pristine quality they deliver, ultrashort pulsed micromachining often have the reputation of being “too slow” and therefore are not cost effective for industrial-grade applications.
We proudly announce that our game changer GHz femtosecond fiber lasers have up to 1000X higher processing speed ability while maintaining high precision.
Part number | STLM-DURO-GHz |
Wavelength |
1030 nm |
Pulse Duration |
<300 fs |
Burst Energy |
200 µJ |
Intra-Burst Repetition Rate |
4 GHz |
Burst Repetition Rate |
100 kHz |
Pulse Energy |
200 ~ 500 nJ |
Number of Pulse Inside Burst |
400 ~ 1000 Pulses |
Average Power |
20 W |
Burst Envelope Shaping |
available via analog modulation or laser user interface |
Power Stability |
<1% |
M2 |
<1.2 |
Polarization, PER |
Linear, 200:1 |
Power Consumption |
<300 W |
Electrical Requirements |
100 ~ 240 VAC, 50/60 Hz |
Cooling System |
Air Cooling |
External Interfaces |
USB 2.0, RS232 |
Software Interfaces |
User-friendly and Customizable GUI |
Pulse Repetition Control |
Amplifier Diode Modulation or Ext/Int AOM Both Available |
Pulse Duration Control |
Adjustable Between 300 fs to 10 ps |
Based on patented Fiber Chirped Pulse Amplification (FCPA) technology, the industry-leading FCPA μJewel™ series offers sufficient pulse energy for selected material processing at a near-infrared wavelength of 1045 nm. Harmonic generation packages, which convert its output to visible and UV wavelengths, are available . The FCPA architecture allows users to choose between high energy operation up to 50 μJ pulses at a repetition rate of 100 kHz or 200 kHz, and high average power of 10 W and 20 W at 1 MHz in the fundamental wavelength. The STIM-DE Series allow for material processing at faster rates, depending on the application requirements.
STIM-DE1050 | STIM-DE2020 | |
Wavelength | 1045 ± 5 nm | 1045 ± 5 nm |
Average Power | ≥ 10 W | ≥ 20 W |
Pulse Duration | ≤ 350 fs | ≤ 350 fs |
Pulse Energy | ≥ 50 μJ | ≥ 20 μJ |
M² | ≤ 1.3 | ≤ 1.3 |
Repetition Rate | 200 kHz 1 MHz | |
Beam Quality | M² ≤ 1.3 | |
Polarization | Horizontal with respect to baseplate | |
Power Stability | ≤ 1% rms after stabilization over ± 1 ˚C | |
Output Aperture | Height 55.4 mm | |
Laser Head Dimensions | 666 x 520 x 165 mm³ | |
Laser Head Weight | ≤ 45 kg | |
Head Heat Dissipation | Max. 100 W | |
Controller Dimensions | 433 x 483 x 222 mm³ | |
Controller Weight | ≤ 30 kg | |
Power Consumption | Max. 1200 W | |
Operating Voltage | 100-120 or 200-240 VAC | |
Output Trigger | TTL 100 ns pulse | |
Operating Temperature | 20-30 ºC | |
Storage Temperature | 0-50 ºC | |
Warm up time | ≤ 60 minutes | |
Cable Length | 3 m |
The most compact laser form based on patented Fiber Chirped Pulse Amplication (FCPA) technology. The STIM-DX Series lasers offer sufficient pulse energy for selected material processing at a near-infrared wavelength of 1045 nm with an ideal compact form factor. Harmonic generation packages, which convert its output to visible and UV wavelengths, are available. The FCPA architecture allows users to choose between high energy operation up to 40 μJ pulses, repetition rate up to 5 MHz, and average power up to 10 W depending on the specific source. The STIM-DX Series allow for material processing at fast rates in a light-weight package.
STIM-DX0210 | STIM-DX1010 | STIM-DX0320 | STIM-DX0330 | STIM-DX0540 | |
Wavelength | 1045 ± 5 nm | ||||
Pulse Energy | ≥ 10 μJ | ≥ 10 μJ | ≥ 20 μJ | ≥ 30 μJ | ≥ 40 μJ |
Pulse Duration | ≤ 450 fs | ||||
Average Power | ≥ 2 W | ≥ 10 W | ≥ 3 W | ≥ 3 W | ≥ 5 W |
M² | ≤ 1.3 | ||||
Repetition Rate | 100 kHz | 1000 kHz | 100 kHz | 100 kHz | 200 kHz |
Beam Quality | M² ≤ 1.3 | ||||
Polarization | Horizontal with respect to baseplate | ||||
Power Stability | ≤ 1% rms after stabilization over ± 1 ˚C | ||||
Output Aperture Height | 55.4 mm | ||||
Laser Head Dimensions | 550 x 400 x 149 mm³ | ||||
Laser Head Weight | ≤ 25 kg | ||||
Head Heat Dissipation | Max. 80 W | ||||
Controller Dimensions | 433 x 483 x 222 mm³ | ||||
Controller Weight | ≤ 30 kg | ||||
Power Consumption | Max. 600 W | ||||
Operating Voltage | 100-120 or 200-240 VAC | ||||
Output Trigger | TTL 100 ns pulse | ||||
Operating Temperature | 20-30 ºC | ||||
Storage Temperature | 0-50 ºC | ||||
Warm up time | ≤ 60 minutes | ||||
Cable Length | 3 m |
Proprietary Raman-shifting technology that creates a clean pulse shape and spectrum at the unique wavelength of 810 nm makes the STIM-FX series a convenient replacement for the ubiquitous Ti:Sapphire laser. This enables new possibilities for the use of femtosecond lasers in clinical and industrial settings. Since its introduction in 2005, the STIM-FX series has been a reliable workhorse in many applications. It is now available with powers up to 150 or 200 mW at 810 nm and 1620 nm. Target applications include Terahertz wave generation and detection, multiphoton fluorescence microscopy and second harmonic imaging.
Specification:
STIM-FX-100 | STIM-FX-150 | STIM-HX-150 | STIM-GX-200 | ||
Center Wavelength | 805 ± 15 nm | 810 ± 15 nm | 810 ± 15 nm | 1620 ± 40 nm | 1620 ± 40 nm |
Average Power | ≥ 100 mW | ≥ 150 mW | ≥ 150 mW | ≥ 200 mW | ≥ 200 mW |
Pulse Duration | ≤ 120 fs | ≤ 140 fs | ≤ 140 fs | ≤ 100 fs | ≤ 100 fs |
Dimensions (mm³) | 230 x 193 x 76 | ||||
Repetition Rate | 75 ± 10 MHz | ||||
Polarization | Horizontal with respect to baseplate | Horizontal* | |||
Power Stability | ≤ 1% rms after stabilization at 25 ˚C | ||||
Output Aperture Height | 43 mm | ||||
Laser Head Dimensions | 230 x 193 x 76 mm³ | ||||
Laser Head Weight | 2kg | 3kg | 2kg | ||
Head Heat Dissipation | <50 W | ||||
Controller Dimensions | 267 x 267 x 133 mm³ | ||||
Controller Weight | 3.5 kg | ||||
Power Consumption | <250 W | ||||
Operating Voltage | 100-240 VAC at 50-60 Hz | ||||
Operating Temperature | 20-30 ºC | ||||
Storage Temperature | 0-50 ºC | ||||
Warm up time | ≤ 15 minutes | ||||
Cable Length | 2 m |
Introduced in 2004, the STIM-Femtolite Ultra is the most compact, reliable Erbium-doped femtosecond fiber laser on the market. It is available in a range of wavelengths and power levels. The Ultra is the descendent of the first commercial femtosecond fiber laser. Together with earlier versions, hundreds of units have been sold around the world, with very low rates of return or failure. No other laser product has the same track record of reliable performance over such long time scales.
Specification:
STIM-AX-20 | STIM-BX-60 | STIM-CX-20 | STIM-FX-10 | ||
Center Wavelength | 780 ± 5 nm | 1560 ± 5 nm | 780 ± 5 nm | 1560 ± 10 nm | 810 ± 5 nm |
Average Power | ≥ 20 mW | ≥ 60 mW | ≥ 20 mW | ≥ 20 mW | ≥ 10 mW |
Pulse Duration | ≤ 100 fs | ≤ 110 fs | |||
Dimensions (mm³) | 142 x 96 x 38 | ||||
Repetition Rate | 50 ± 2 MHz | ||||
Polarization | Vertical with respect to baseplate | ||||
Power Stability | ≤ 1% rms after stabilization over ± 1 ˚C | ||||
Output Aperture Height | 23 mm | ||||
Laser Head Dimensions | 142 x 96 x 38 mm³ | ||||
Laser Head Weight | 0.8 kg | ||||
Head Heat Dissipation | Max. 80 W | ||||
Controller Dimensions | 215 x 200 x 89 mm³ | ||||
Controller Weight | 2 kg | ||||
Power Consumption | <50 W | ||||
Operating Voltage | 100-120 or 200-240 VAC | ||||
Operating Temperature | 20-30 ºC25-35 ºC | ||||
Storage Temperature | 0-50 ºC | ||||
Warm up time | ≤ 30 minutes | ||||
Cable Length | 2 m |
STIM-FD Series of laser is designed uniquely to deliver fs laser pulses via an optical fiber cable to user application. The laser application primarily targeting at the imaging application of proteins at 1045 nm. However, this product can serve many other applications where a handy delivery of fs pulses are required in flexible fashion. The first product of the STIM-FD Series, STIM-FD/D-FD-100S, offers over 1 W of average fiber delivered power with 200 fs along with high speed blanking function at less than 1 μs. All one-box design cooled by air allows for easy integration into workstations and laser machines. Target applications include microscopy and second harmonic imaging.
Center Wavelength | 1045 ± 5 nm |
Average Power | ≥ 1.0 W |
Pulse Duration | ≤ 200 fs |
Repetition Rate | 50 ± 5 MHz |
Power Modulation | internal AOM, <1μs |
Dimensions (mm³) | 500 x 540 x 270 |
STFC-Fetom series is a powerful industrial femtosecond lasers offering output powers up to 30W and pulse energies in excess of 160 µJ, with pulses shorter than 800 fs.
This series is the only ultrafast laser available integrating the Taranis Single Crystal Fiber (SCF) technology which enables high pulse energy and flexible repetition rate to meet requirements for both high throughput applications and high energy demanding applications.
This unique architecture provides excellent reliability and beam quality, all in a compact packaging.
Features
Applications
Specifications
Wavelength | 1030nm | |
Average Power | 30W | |
Pulse Repetition Rate | 100kHz to 1MHz | |
Spatial Mode TE00 | M² < 1.3 | |
Pulse Duration | <800s | |
Polarization Ratio | >100:1 | |
Electric Supply | 115 to 230VAC/ 50 to 60Hz | |
Beam Diameter | 2mm | |
Warm-Up Time | 95% 0f power in <10mm | |
Max Out Dimensions | 830x443x180mm³ | |
Laser specifications at Min/Max repetition rate | ||
Repetition rate | 100kHz | 1000kHz |
Average Power | 16W | 30W |
Pulse Energy | 160uJ | 30uJ |
Peak Power | 220MW | 42MW |
► GHz Low-noise 1555nm Femtosecond Laser, 2.8-3.5um Femtosecond Lasers, Pico-second Lasers, Ultrafast OPOs and OPAs