Monocrom manufactures high quality, accurate laser systems for use in Spectroscopy: low power, single frequency diode lasers, ideal for the most common Raman spectroscopy set-ups and high energy diode-pumped solid state lasers (HiEN-PULS) to step into all coherent Raman spectroscopy applications as well as remote Raman spectroscopy.
We offer different types of laser sources for spectrometers covering the range from 532 nm to NIR.
Monocrom is an OEM manufacturer. but also offering standard products in short lead time. We adapt to customers needs with a high degree of flexibility and versatility for their developments.
Applications
- Raman Spectroscopy
- LIBS Spectroscopy
- Cavity ring-down Spectroscopy (CRDS)
Related articles: Raman spectroscopy and Monocrom products
Technical Specifications
wdt_ID Raman Spectroscopy LIBS Cavity ring-down Spectroscopy
5
narrow remove space
single or dual wavelength 532 nm / 1064 nm
narrow remove space (and tunable system)
680 nm – 1064 nm (depending on the trace gas)
diode laser as well as diode-pumped solid-state-laser
6
532 nm / 785 nm / 1064 nm
>10 mJ to create a plasma Q-switched diode-pumped solid-state-laser
760-765 nm oxygen detection
7
< 1 W for microscopy application
767 nm K-Spectroscopy (D2)
8
high energy solid-state-laser for remote Raman spectroscopy
780 nm Rb-Spectroscopy (D2)
9
diode laser as well as diode-pumped solid-state-laser
795 nm Rb-Spectroscopy (D1)
10
852 nm CS-Spectroscopy (D2)
11
922 nm Sr-Spectroscopy
12
953 nm Yb-Spectroscopy
13
953 nm Water-Spectroscopy
14
narrow line width
single or dual wavelength 532 nm / 1064 nm
narrow linewidth (and tunable system)
680 nm – 1064 nm (depending on the trace gas)
diode laser as well as diode-pumped solid-state-laser
15
532 nm / 785 nm / 1064 nm
single or dual wavelength 532 nm / 1064 nm
< 10 mJ to create a plasma Q-switched diode-pumped solid-state-laser
760-765 nm oxygen detection
16
< 1 W for microscopy application
767 nm K-Spectroscopy (D2)
17
high energy SSL for remote Raman spectroscopy
780 nm Rb-Spectroscopy (D2)
18
diode laser as well as diode-pumped solid-state-laser
795 nm Rb-Spectroscopy (D1)
19
852 nm CS-Spectroscopy (D2)
20
922 nm Sr-Spectroscopy
21
953 nm Yb-Spectroscopy
22
953 nm Water-Spectroscopy
23
narrow line width
single or dual wavelength 532 nm / 1064 nm
narrow linewidth (and tunable system)
680 nm – 1064 nm (depending on the trace gas)
diode laser as well as diode-pumped solid-state-laser
24
532 nm / 785 nm / 1064 nm
single or dual wavelength 532 nm / 1064 nm
< 10 mJ to create a plasma Q-switched diode-pumped solid-state-laser
760-765 nm oxygen detection
25
< 1 W for microscopy application
767 nm K-Spectroscopy (D2)
26
high energy solid-state-laser for remote Raman spectroscopy
780 nm Rb-Spectroscopy (D2)
27
diode laser as well as diode-pumped solid-state-laser
795 nm Rb-Spectroscopy (D1)
28
852 nm CS-Spectroscopy (D2)
| wdt_ID | Raman Spectroscopy | LIBS | Cavity ring-down Spectroscopy |
|---|---|---|---|
| 5 | narrow remove space | single or dual wavelength 532 nm / 1064 nm | narrow remove space (and tunable system) 680 nm – 1064 nm (depending on the trace gas) diode laser as well as diode-pumped solid-state-laser |
| 6 | 532 nm / 785 nm / 1064 nm | >10 mJ to create a plasma Q-switched diode-pumped solid-state-laser | 760-765 nm oxygen detection |
| 7 | < 1 W for microscopy application | 767 nm K-Spectroscopy (D2) | |
| 8 | high energy solid-state-laser for remote Raman spectroscopy | 780 nm Rb-Spectroscopy (D2) | |
| 9 | diode laser as well as diode-pumped solid-state-laser | 795 nm Rb-Spectroscopy (D1) | |
| 10 | 852 nm CS-Spectroscopy (D2) | ||
| 11 | 922 nm Sr-Spectroscopy | ||
| 12 | 953 nm Yb-Spectroscopy | ||
| 13 | 953 nm Water-Spectroscopy | ||
| 14 | narrow line width | single or dual wavelength 532 nm / 1064 nm | narrow linewidth (and tunable system) 680 nm – 1064 nm (depending on the trace gas) diode laser as well as diode-pumped solid-state-laser |
| 15 | 532 nm / 785 nm / 1064 nm | single or dual wavelength 532 nm / 1064 nm |
760-765 nm oxygen detection |
| 16 | < 1 W for microscopy application | 767 nm K-Spectroscopy (D2) | |
| 17 | high energy SSL for remote Raman spectroscopy | 780 nm Rb-Spectroscopy (D2) | |
| 18 | diode laser as well as diode-pumped solid-state-laser | 795 nm Rb-Spectroscopy (D1) | |
| 19 | 852 nm CS-Spectroscopy (D2) | ||
| 20 | 922 nm Sr-Spectroscopy | ||
| 21 | 953 nm Yb-Spectroscopy | ||
| 22 | 953 nm Water-Spectroscopy | ||
| 23 | narrow line width | single or dual wavelength 532 nm / 1064 nm | narrow linewidth (and tunable system) 680 nm – 1064 nm (depending on the trace gas) diode laser as well as diode-pumped solid-state-laser |
| 24 | 532 nm / 785 nm / 1064 nm | single or dual wavelength 532 nm / 1064 nm |
760-765 nm oxygen detection |
| 25 | < 1 W for microscopy application | 767 nm K-Spectroscopy (D2) | |
| 26 | high energy solid-state-laser for remote Raman spectroscopy | 780 nm Rb-Spectroscopy (D2) | |
| 27 | diode laser as well as diode-pumped solid-state-laser | 795 nm Rb-Spectroscopy (D1) | |
| 28 | 852 nm CS-Spectroscopy (D2) |
Product Carousel Tabs
Single Emitters
Single Emitters: Laser diode modules based on single emitters.
Wavelengths between 375 nm – 1550 nm are available in a range of power that starts below 1mW and scales up to some watts.
We can add optics, mechanics and electronics to fit customer’s demands.
Fiber-coupled Lasers
Fiber-coupled Lasers
Highly efficient fiber coupled diode lasers with Monocrom Solder-free laser bar Clamping™ technology. The lack of a “smile” effect results in an optimum coupling efficiency to the optical fiber. We also provide wavelength stabilized fiber-coupled laser modules with a grating for wavelength locking. Having a low smile results in an exceptionally well-controlled feedback, which increases the locking efficiency and production repeatability.
For the most demanding applications of high brightness (radiance), we offer fiber-coupled high power diode laser systems capable of delivering 1 kW in power in continuous wave (CW) at a single wavelength.
HiEN Puls x5400-YAG
HiEN Puls x5400-YAG
High energy pulsed solid state laser solution for material processing, LIBS/RAMAN/IR Spectroscopy, OPO/DYE/Ti: Sa optical pumping, LiDAR & wind LiDAR
HiEN Puls x5400-YLF
HiEN Puls x5400-YAG
High energy pulsed solid state laser solution for material processing, LIBS/RAMAN/IR Spectroscopy, OPO/DYE/Ti: Sa optical pumping, LiDAR & wind LiDAR
CW Pumping Source PH120 – PH300
CW Pumping Source PH120 – PH300
Pump heads for laser pumping, pumped with 120 W – 300 W at continuos wave (CW).
We offer all of them with Nd:YAG or Nd:YLF rod material.
The cylindrical symmetry of these pumping units allows rotation of the pumping chamber giving flexibility during the production and optimization of a laser system. The pumping laser diode bars are mounted using our patented solder-free clamping technology. Exclusively used by Monocrom.
QCW Pumping Source PH450-PH1800
Reliable laser pumping units that operate in quasi continous wave (QCW).
A cylindrical symmetry design allows rotation of the pumping chamber giving flexibility during the production and optimization of a laser system.
The pumping laser diode bars are mounted using our patented solder-free Clamping™ technology.
No mechanical stress Our patented solder-free technology is used in our diode bars stacks. Thanks to it clamped bars expand and contract freely during the thermal cicles of the pulsed regime avoiding mechanical stress.