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 es un fabricante OEM. pero también ofrece productos estándar en plazos de entrega cortos. Nos adaptamos a las necesidades de los clientes con un alto grado de flexibilidad y versatilidad para sus desarrollos.
Aplicaciones
- Raman Spectroscopy
- LIBS Spectroscopy
- Cavity ring-down Spectroscopy (CRDS)

Related articles: Espectroscopia Raman y productos Monocrom
Especificaciones técnicas
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) |
Fichas de carrusel de productos
Emisores individuales
Emisores únicos: Módulos de diodos láser basados en emisores únicos.
Las longitudes de onda entre 375 nm y 1550 nm están disponibles en una gama de potencias que empieza por debajo de 1mW y llega hasta algunos vatios.
Podemos añadir óptica, mecánica y electrónica para adaptarnos a las demandas del cliente.
Láseres de fibra óptica
Láseres de fibra óptica
Láseres de diodo acoplados a fibra de alta eficiencia con tecnología de barra láser Monocrom Solder-free Clamping™. La ausencia de efecto "sonrisa" se traduce en una eficiencia de acoplamiento óptima a la fibra óptica. También proporcionamos módulos láser acoplados a fibra estabilizados en longitud de onda con una rejilla para el bloqueo de la longitud de onda. Al tener una sonrisa baja, se consigue una retroalimentación excepcionalmente bien controlada, lo que aumenta la eficacia del bloqueo y la repetibilidad de la producción.
Para las aplicaciones más exigentes de alto brillo (luminosidad), ofrecemos sistemas láser de diodo de alta potencia acoplados a fibra capaces de suministrar 1 kW de potencia en onda continua (CW) a una sola longitud de onda.
HiEN Puls x5400-YAG
HiEN Puls x5400-YAG
Solución láser de estado sólido pulsado de alta energía para procesamiento de materiales, Espectroscopia LIBS/RAMAN/IR, OPO/DYE/Ti: bombeo óptico Sa, LiDAR y LiDAR eólico
HiEN Puls x5400-YLF
HiEN Puls x5400-YAG
Solución láser de estado sólido pulsado de alta energía para procesamiento de materiales, Espectroscopia LIBS/RAMAN/IR, OPO/DYE/Ti: bombeo óptico Sa, LiDAR y LiDAR eólico
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.
En 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.
Fuente de bombeo QCW PH450-PH1800
Unidades de bombeo láser fiables que funcionan en onda cuasi continua (QCW).
Un diseño de simetría cilíndrica permite la rotación de la cámara de bombeo, lo que aporta flexibilidad durante la producción y optimización de un sistema láser.
Las barras de diodos láser de bombeo se montan utilizando nuestra tecnología patentada sin soldadura Clamping™.
Sin tensión mecánica En nuestras pilas de barras de diodos se utiliza nuestra tecnología patentada sin soldadura. Gracias a ella las barras apiladas se expanden y contraen libremente durante los ciclos térmicos del régimen pulsado evitando tensiones mecánicas.