We present a femtosecond laser system at 920 nm delivering ultrashort pulses via a hollow-core photonic bandgap fiber (HC-PBGF). The laser system is designed to simplify two-photon microscopy applications and can be used for miniaturized two-photon microscopes. While previously presented solutions have been tailored to a specific length and dispersion coefficient of the HC-PBGF, we now show a compact and flexible scheme for dispersion compensation which is compatible with a wide range of fiber types and lengths.
In addition, this new approach fully maintains the capability of software-controlled dispersion compensation in the range from 0 to -40,000 fs2 after the pulse delivery fiber. Hence, the dispersion of common two-photon microscopes can be pre-compensated in order to obtain compressed pulses at the sample plane. Our newly developed system displays excellent long-term fiber coupling stability under varying environmental conditions. It is capable of polarization-preserving femtosecond pulse delivery at 920 nm and reaches Watt-level power after the delivery fiber, making it suitable for in-vivo brain imaging of GCaMP in mouse models.
We will present our latest innovations on high-power diode lasers and discuss their application in quantum technologies. We show that these laser sources are key not only to explore the magic world of quantum physics, but also to drive the commercialization of exciting new applications coming along with the second quantum revolution, such as quantum computers, -sensing, -metrology and optical clocks. Compared to other laser sources such as gas- or solid-state lasers, diode lasers offer key advantages for these applications, e.g. their compactness, low weight, low energy consumption and low cost of ownership.
We present time resolved measurements on low dimensional nanomaterials like individual (6,4) single-walled carbon nanotubes and monolayers of MoSe2 via transient interferometric scattering (TiSCAT) microscopy. For this a novel fiber laser system was developed comprising a tunable probe arm and low noise performance. The sensitivity of the measurement is demonstrated for very low excitation powers to prevent photodamage of the sample. Signal variations close to the shot-noise limit can be resolved even with low excitation powers in the order of 1 μW. In combination with the tunability of the laser system the absorption spectrum of a single SWCNT was determined.
Simulation of grating spectrometers constitutes the problem of propagating a spectrally broad light field through a
macroscopic optical system that contains a nanostructured grating surface. The interest of the simulation is to quantify
and optimize the stray light behaviour, which is the limiting factor in modern high end spectrometers. In order to
accomplish this we present a simulation scheme that combines a RCWA (rigorous coupled wave analysis) simulation of
the grating surface with a selfmade GPU (graphics processor unit) accelerated nonsequential raytracer. Using this, we are
able to represent the broad spectrum of the light field as a superposition of many monochromatic raysets and handle the
huge raynumber in reasonable time.
In the last decades, diode laser systems conquered the spectral range step-by-step from conventional gas lasers, wherever
they can match or outperform in optical specifications. Although highly anticipated in the ultraviolet wavelength range,
for instance in high-resolution lithography, biological and medical fluorescence applications or holography, cw single
frequency operation of sufficient power has been a challenge for diode or other solid state laser systems. Currently this
scope is still dominated by the HeCd gas laser, emitting at 325 nm with powers of up to 100 mW.
In this paper we present a diode laser system emitting at 325 nm offering the same output power by efficient second
harmonic generation (SHG) of a master oscillator power amplifier (MOPA) at 650 nm.
For the master oscillator a ridge waveguide diode is anti-reflection coated and used in an external cavity diode laser
(ECDL) with grating feedback in Littrow configuration. This setup features a MHz line width (coherence length of
100m), a coarse tuning range from 649 nm to 657 nm and a mode hope free tuning of 20 GHz. In a second step, we use a
tapered amplifier to boost the output from the ECDL to a level of 400 mW, for powering an efficient second harmonic
generation process in an enhancement cavity. Faraday isolators on both ends of the amplifier stage prevent back
reflection and stabilize the single mode operation of the system. Together with astigmatism compensation this yields to a
high spatial quality (M2<1.5) of the amplified beam. The frequency doubling is achieved by using a four mirror bow-tie
enhancement resonator fitted with a Beta-Barium Borate (BBO) crystal. The cavity length is actively locked to the laser
frequency using the Pound-Drever-Hall method.
With this set-up, stable and reliable laser operation is achieved. After a few minutes warm-up time, fixed frequency and
tunable UV output power of more than 100 mW could be generated, opening this important wavelength range for future
product development.
High-brightness tapered lasers and amplifiers at 670 nm with output powers up to 1 W and nearly diffraction limited
beam quality were realised. The devices consist of a 750 &mgr;m long straight section and a 1250 &mgr;m long tapered
section. Devices with a taper angle of 2°, 3° and 4° were manufactured.
The material quality was studied in a long-term test for ridge-waveguide lasers. Devices with 7.5 &mgr;m ridge width
show reliable operation at 100 mW output power over more than 10000 h.
At a temperature of 15°C a tapered lasers with an angle of 4° reached an output power of 1 W at a current of 2.1 A.
The highest conversion efficiency for this device was 24%, the peak wavelength of the emission was 668 nm and the
spectral width was smaller than 0.2 nm. The beam propagation factor was M2 = 1.7 (1/e2) and M2 = 3.0 (second
moments).
At 500 mW output power, master-oscillator power-amplifier (MOPA) devices showed also a nearly diffraction
limited beam quality with M2 < 1.5 and reliable operation with degradation rates as low as 7x10-6 h-1 over 1200 h.
The spectral line-width in this arrangement is determined by the master oscillator and is suitable for high-resolution
spectroscopy.
A master oscillator power amplifier system operating around 670 nm is presented. For the master laser an
external cavity diode laser is used with an output power of 25 mW at tunable wavelength and with narrow line
width. A tapered amplifier boosts the power up to 970 mW while maintaining the spectral characteristics and
keeping the beam quality close to the diffraction limit. The performance of the laser system is presented and a
Lithium spectrum depicting the suitability of the system for Lithium spectroscopy, cooling and trapping.
Gain-switching of laser diodes might be the most convenient way to generate picosecond laser pulses. The outstanding features of gain-switched laser diodes are a rich choice of wavelength and an easy synchronization to an external trigger source. To broaden the field of applications we pushed the peak power to the 10 W level while maintaining the essential characteristics of the laser source. In a master oscillator power amplifier (MOPA) configuration a tapered amplifier is used to increase the output from 10 mW to 160 mW average power. Second harmonic generation is demonstrated in a single pass setup, which results in 6.5 mW average power at 532 nm with a repetition rate of 80 MHz.
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