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Tapered amplifier (TA) diodes combine the "best of both worlds": They amplify laser radiation into a nearly diffraction limited beam to powers that would destroy the facets of normal laser diodes. At the same time the spectral properties of the master laser are preserved. TOPTICA offers TA chips separately, but also integrates them into convenient laser systems (TA pro and BoosTA)

Distributed feedback (DFB) laser diodes feature a grating structure within the semiconductor and thus operate in both longitudinal and transverse single mode. Tuning is achieved by modulating either the laser current or the chip temperature. Mode-hop free tuning is maintained over several hundred GHz. Applications include alkaline spectroscopy, laser cooling, gas detection and the generation of tunable cw terahertz radiation.

TOPTICA Photonics is the number one supplier for laser diodes, providing the widest and most continuous coverage available within the optical spectrum. Our laser diodes have been thoroughly examined in an external cavity diode laser configuration. Based on our extensive testing we can ensure the highest quality to our valued customers.

TOPTICA Photonics is the number one supplier for laser diodes, providing the widest and most continuous coverage available within the optical spectrum. Our laser diodes have been thoroughly examined in an external cavity diode laser configuration. Based on our extensive testing we can ensure the highest quality to our valued customers.

The Collimation Module (C-Module) is a highly efficient means of reducing the divergence of diode lasers in the fast- and slow-axis simultaneously. The module consists of two micro-optics, fixed and aligned in one single module with high precision. Alongside its optimum collimation characteristics the module guarantees a simple and cost efficient assembly of diode lasers. The compact C-Module thus guarantees highest brightness of diode lasers in combination with minimum size. Please refer to our broad product spectrum of fast-axis and slow-axis collimators to combine your C-Module for your specific application. Advantages: efficient collimation optimized for highest brightness compact module easy to mount transmission up to 99% highest level of precision and uniformity long term stability optimized design

INGENERIC C-Module The Collimation Module (C-Module) is a highly efficient means of reducing the divergence of diode lasers in the fast- and slow-axis simultaneously. The module consists of two micro-optics, fixed and aligned in one single module with high precision. Alongside its optimum collimation characteristics the module guarantees a simple and cost efficient assembly of diode lasers. The compact C-Module thus guarantees highest brightness of diode lasers in combination with minimum size. Please refer to our broad product spectrum of fast-axis and slow-axis collimators to combine your C-Module for your specific application. Advantages efficient collimation optimized for highest brightness compact module easy to mount transmission up to 99% highest level of precision and uniformity long term stability optimized design

The INGENERIC beamPROP is a lens array which matches the beam parameter product (BPP) of the fast and slow axis of high power diode laser arrays. The beamPROP is a key component for the 1. fiber coupling of diode bars 2. dense wavelength beam combining. Both applications make high demands on the components, which are met by INGENERIC’s outstanding manufacturing technology, guaranteeing highest levels of efficiency for diode lasers. Achieve the highest beam quality through the four major features behind the beamPROP: - complete utilization of the aperture by minimized transition zones - minimum aberrations achieved by highest level of precision and uniformity of single lenslets - an exact rotation of the emitter is achieved through the defined center thickness accuracy - minimum pointing errors due to an exact position of front and back surfaces

INGENERIC beamPROP The INGENERIC beamPROP is a lens array which matches the beam parameter product (BPP) of the fast and slow axis of high power diode laser arrays. The beamPROP is a key component for the fiber coupling of diode bars dense wavelength beam combining. Both applications make high demands on the components, which are met by INGENERIC’s outstanding manufacturing technology, guaranteeing highest levels of efficiency for diode lasers. Achieve the highest beam quality through the four major features behind the beamPROP: complete utilization of the aperture by minimized transition zones minimum aberrations achieved by highest level of precision and uniformity of single lenslets an exact rotation of the emitter is achieved through the defined center thickness accuracy minimum pointing errors due to an exact position of front and back surfaces

The most important optical component in the beam shaping systems in high-power diode lasers is the Fast-Axis Collimation optic. The lenses are manufactured from high-quality glass and have an acylindrical surface. Their high numerical aperture permits the entire diode output to be collimated with outstanding beam quality. The high transmission and excellent collimation characteristics guarantee the highest levels of beam shaping efficiency for diode lasers. By means of an FAI lens, the emitter can be directly imaged into a fiber or a target plane. The design of INGENERIC’s FAI lenses is optimized for this specific application and allows an efficient and aberration-free imaging of the emitter. In order to offer the best solution for your application INGENERIC provides a broad spectrum of Fast-Axis Collimation optics from the shelf. Years of development allow us to provide optimized acylindrical lenses for different applications.

INGENERIC FAC The most important optical component in the beam shaping systems in high-power diode lasers is the Fast-Axis Collimation optic. The lenses are manufactured from high-quality glass and have an acylindrical surface. Their high numerical aperture permits the entire diode output to be collimated with outstanding beam quality. The high transmission and excellent collimation characteristics guarantee the highest levels of beam shaping efficiency for diode lasers. INGENERIC FAI By means of an FAI lens, the emitter can be directly imaged into a fiber or a target plane. The design of INGENERIC’s FAI lenses is optimized for this specific application and allows an efficient and aberration-free imaging of the emitter Product Spectrum In order to offer the best solution for your application INGENERIC provides a broad spectrum of Fast-Axis Collimation optics from the shelf. Years of development allow us to provide optimized acylindrical lenses for different applications. Based on...

The Slow-Axis Collimation optic is a highly efficient means of forming the beam in the slow-axis of diode lasers. It is available either as a monolithic array of cylindrical lenses or as a single lens. All of our optics are produced using high-quality optical glass. The exacting product tolerances guarantee efficient collimation of the light from all emitters and compatibility with laser bars and stacks In order to offer the best solution for your application INGENERIC provides a broad spectrum of Slow-Axis Collimation optics off the shelf. With respect to length or support structures the lenses can be tailored to your specific needs.

The first approach for the development of new processes and the research of scientific effects is the application of standardized laser systems. When the requirements on scientific research advance, they equally rise with regard to the laser systems. For optimum results in scientific research and development, diode lasers with very precise specifications are indispensable. Operating and monitoring the system with defined and fixed parameters such as the power distribution and wavelength is essential for the accurate collection and evaluation of data and will lead to reliable results. Provisioning an outright laser system will further enable scientists to actually focus on their actual research. As complete solution the system can furthermore be directly integrated into the security system, providing a safe operation for your team of experts.

INGENERIC SAC The Slow-Axis Collimation optic is a highly efficient means of forming the beam in the slow-axis of diode lasers. It is available either as a monolithic array of cylindrical lenses or as a single lens. All of our optics are produced using high-quality optical glass. The exacting product tolerances guarantee efficient collimation of the light from all emitters and compatibility with laser bars and stacks Product Spectrum In order to offer the best solution for your application INGENERIC provides a broad spectrum of Slow-Axis Collimation optics off the shelf. With respect to length or support structures the lenses can be tailored to your specific needs. Advantages transmission up to 99% minimized dead zones highest level of precision and uniformity customized solutions with small NRE-costs highly economical manufacturing process for large quantities reliable and stable quality

The optoNCDT BL models are equipped with a blue laser diode and are used when standard sensors with a red laser diode are operating at their performance limits. Due to its shorter wavelength, the blue laser does not penetrate the target surface, projecting a small light spot on the surface and therefore providing stable and precise results. As Blue Laser sensors are equipped with a special filter, they are insensitive to highly emitting objects such as glowing metals. Blue Laser sensors are preferably used with measurements on organic and (semi-)transparent objects, as well as for red-hot glowing metals.

ULTRATEST Technology™ Speed, Sensitivity and Reliability for Demanding Leak Detection Applications The INFICON UL1000 Mobile Helium Leak Detector is designed to meet the most demanding industrial leak detection applications. Providing fast, accurate and repeatable test results, testing flexibility, and high sensitivity in a low maintenance design, the UL1000 is ready to tackle the toughest leak detection jobs industry can offer. The UL1000 is optimized to provide quick, accurate results in any application from the leak checking of large vessels and systems to high-cycle, repetitive component testing - 24 hours / 7 days a week - in the toughest industrial environments. With the addition of the TC1000 Test Chamber accessory, the UL1000 Helium Leak Detector provides easy, fast and accurate testing of hermetically sealed parts like IC packages, quartz crystals and laser diodes (according to MIL-STD 883, Method 1014).

Due to their compact and flexible design, LS series laser machines guarantee an easy entry into the world of laser processing. We offer manual and automated solutions: - Palletising systems - Bar and coil feed systems - Pick-and-place systems - Robots You can realize the following laser material processing with the LS series: - laser machining for welding, clean welding, cutting, drilling, hardening, and structuring - micro processing - integration of CO2 , Nd: YAG, diode, fibre or disk-type lasers and ultra-short pulsed laser Please get furher information at Download.

The CryLaS Q series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. This consists of an Nd:YAG resonator with a directly coupled saturable absorber which works as a passive Q-switch. The compact housing and easy operation make the lasers an optimum light source for applications that require minimal housing dimensions with highest performance. Based on the 1064 nm fundamental, harmonics are generated using non-linear (NLO) crystals that allow a wide spectrum of laser wavelengths from 1064 nm to 213 nm. The FQSS213-Q4 laser emits pulses with approximately 1 ns pulse width at 213 nm, and can be modulated from single shot to 1 kHz. The pulse energy is 2.5 µJ. CryLaS lasers impress with their easy installation, service-free operation and long service life. This makes them ideal for OEM applications and demanding laboratory setups.

The CryLaS Q-series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. It consists of a Nd:YAG resonator with a directly coupled saturable absorber that works as a passive Q-switch. The compact housing and simple operation make the lasers an ideal light source for applications that require minimal housing dimensions with maximum performance. Based on the 1064 nm fundamental, non-linear optics (NLO optics) generate frequency multiples of this fundamental, covering a broad spectrum of laser wavelengths from 1064 nm to 213 nm. The DSS1064-Q2 laser emits pulses with a pulse width of approx. 1.5 ns at 1064 nm and can be modulated from single shot to 10 kHz. The pulse energy is 20 µJ. CryLaS lasers impress with their simple installation, service-free operation and long service life.

The CryLaS Q-series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. It consists of a Nd:YAG resonator with a directly coupled saturable absorber that works as a passive Q-switch. The compact housing and simple operation make the lasers an ideal light source for applications that require minimal housing dimensions with maximum performance. Based on the 1064 nm fundamental, non-linear optics (NLO optics) generate frequency multiples of this fundamental, covering a broad spectrum of laser wavelengths from 1064 nm to 213 nm. The DSS1064-Q1 laser emits pulses with a pulse width of approx. 1.5 ns at 1064 nm and can be modulated from single shot to 20 kHz. The pulse energy is 10 µJ. CryLaS lasers impress with their simple installation, service-free operation and long service life.

The CryLaS Q-series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. It consists of a Nd:YAG resonator with a directly coupled saturable absorber that works as a passive Q-switch. The compact housing and simple operation make the lasers an ideal light source for applications that require minimal housing dimensions with maximum performance. Based on the 1064 nm fundamental, non-linear optics (NLO optics) generate frequency multiples of this fundamental, covering a broad spectrum of laser wavelengths from 1064 nm to 213 nm. The FTSS355-Q1 laser emits pulses with a pulse width of approx. 1 ns at 355 nm and can be modulated from single shot to 20 kHz. The pulse energy is 0.3 µJ. CryLaS lasers impress with their simple installation, service-free operation and long service life.

The CryLaS Q-series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. It consists of a Nd:YAG resonator with a directly coupled saturable absorber that works as a passive Q-switch. The compact housing and simple operation make the lasers an ideal light source for applications that require minimal housing dimensions with maximum performance. Based on the 1064 nm fundamental, non-linear optics (NLO optics) generate frequency multiples of this fundamental, covering a broad spectrum of laser wavelengths from 1064 nm to 213 nm. The FTSS355-Q2 laser emits pulses with a pulse width of approx. 1 ns at 355 nm and can be modulated from single shot to 10 kHz. The pulse energy is 3 µJ. CryLaS lasers impress with their simple installation, service-free operation and long service life.

The CryLaS Q-series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. It consists of a Nd:YAG resonator with a directly coupled saturable absorber that works as a passive Q-switch. The compact housing and simple operation make the lasers an ideal light source for applications that require minimal housing dimensions with maximum performance. Based on the 1064 nm fundamental, non-linear optics (NLO optics) generate frequency multiples of this fundamental, covering a broad spectrum of laser wavelengths from 1064 nm to 213 nm. The FTSS355-Q3 laser emits pulses with a pulse width of approx. 1 ns at 355 nm and can be modulated from single shot to 2.5 kHz. The pulse energy is 15 µJ @ 1 kHz. CryLaS lasers impress with their simple installation, service-free operation and long service life.

The CryLaS Q-series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. It consists of a Nd:YAG resonator with a directly coupled saturable absorber that works as a passive Q-switch. The compact housing and simple operation make the lasers an ideal light source for applications that require minimal housing dimensions with maximum performance. Based on the 1064 nm fundamental, non-linear optics (NLO optics) generate frequency multiples of this fundamental, covering a broad spectrum of laser wavelengths from 1064 nm to 213 nm. The DSS1064-Q4 laser emits pulses with a pulse width of approx. 1.5 ns at 1064 nm and can be modulated from single shot to 1 kHz. The pulse energy is 90 µJ. CryLaS lasers impress with their simple installation, service-free operation and long service life.

The CryLaS Q-series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. It consists of a Nd:YAG resonator with a directly coupled saturable absorber that works as a passive Q-switch. The compact housing and simple operation make the lasers an ideal light source for applications that require minimal housing dimensions with maximum performance. Based on the 1064 nm fundamental, non-linear optics (NLO optics) generate frequency multiples of this fundamental, covering a broad spectrum of laser wavelengths from 1064 nm to 213 nm. The FDSS532-Q1 laser emits pulses with a pulse width of approx. 1 ns at 532 nm and can be modulated from single shot to 20 kHz. The pulse energy is 2 µJ. CryLaS lasers impress with their simple installation, service-free operation and long service life.

The CryLaS Q series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. This consists of an Nd:YAG resonator with a directly coupled saturable absorber which works as a passive Q-switch. The compact housing and easy operation make the lasers an optimum light source for applications that require minimal housing dimensions with highest performance. Based on the 1064 nm fundamental, harmonics are generated using non-linear (NLO) crystals that allow a wide spectrum of laser wavelengths from 1064 nm to 213 nm. The FQSS213-Q2 laser emits pulses with approximately 1 ns pulse width at 213 nm, and can be modulated from single shot to 10 kHz. The pulse energy is 0.1 µJ. CryLaS lasers impress with their easy installation, service-free operation and long service life. This makes them ideal for OEM applications and demanding laboratory setups.

The CryLaS Q-series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. It consists of a Nd:YAG resonator with a directly coupled saturable absorber that works as a passive Q-switch. The compact housing and simple operation make the lasers an ideal light source for applications that require minimal housing dimensions with maximum performance. Based on the 1064 nm fundamental, non-linear optics (NLO optics) generate frequency multiples of this fundamental, covering a broad spectrum of laser wavelengths from 1064 nm to 213 nm. The FDSS532-Q2 laser emits pulses with a pulse width of approx. 1 ns at 532 nm and can be modulated from single shot to 10 kHz. The pulse energy is 6 µJ. CryLaS lasers impress with their simple installation, service-free operation and long service life.

The CryLaS Q-series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. It consists of a Nd:YAG resonator with a directly coupled saturable absorber that works as a passive Q-switch. The compact housing and simple operation make the lasers an ideal light source for applications that require minimal housing dimensions with maximum performance. Based on the 1064 nm fundamental, non-linear optics (NLO optics) generate frequency multiples of this fundamental, covering a broad spectrum of laser wavelengths from 1064 nm to 213 nm. The FDSS532-Q3 laser emits pulses with a pulse width of approx. 1 ns at 532 nm and can be modulated from single shot to 2.5 kHz. The pulse energy is 20 µJ. CryLaS lasers impress with their simple installation, service-free operation and long service life.

The CryLaS Q-series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. It consists of a Nd:YAG resonator with a directly coupled saturable absorber that works as a passive Q-switch. The compact housing and simple operation make the lasers an ideal light source for applications that require minimal housing dimensions with maximum performance. Based on the 1064 nm fundamental, non-linear optics (NLO optics) generate frequency multiples of this fundamental, covering a broad spectrum of laser wavelengths from 1064 nm to 213 nm. The FDSS532-Q4 laser emits pulses with a pulse width of approx. 1 ns at 532 nm and can be modulated from single shot to 1 kHz. The pulse energy is 42 µJ. CryLaS lasers impress with their simple installation, service-free operation and long service life.

The CryLaS Q series lasers are diode-pumped solid-state lasers (DPSS lasers) based on a microchip design. This consists of an Nd:YAG resonator with a directly coupled saturable absorber which works as a passive Q-switch. The compact housing and easy operation make the lasers an optimum light source for applications that require minimal housing dimensions with highest performance. Based on the 1064 nm fundamental, harmonics are generated using non-linear (NLO) crystals that allow a wide spectrum of laser wavelengths from 1064 nm to 213 nm. The FQSS213-Q1 laser emits pulses with approximately 1 ns pulse width at 213 nm, and can be modulated from single shot to 20 kHz. The pulse energy is 0.05 µJ. CryLaS lasers impress with their easy installation, service-free operation and long service life. This makes them ideal for OEM applications and demanding laboratory setups.