GL532TB (~50mW)
GL532TA (~300mW)
GL532TA with Fiber Coupler
GL532TA, SM/PM Fiber Coupled
GL532T1 (~200mW)
GL532T3 (~300mW)
GL532T3 with Fiber Coupler
GL532T8 (~1.5W, High Stability)
GL532T8 with Fiber Coupler
GL532T8M (1MHz Modulation)
GL532T6 (~2.5W, M2<1.1)
GL532T7 (~5W)
GL532T7A (~5W, TEM00)
GL532T9 (~20W)
GL532T10 (~18W, TEM00)
BLM445TA-E (Ellipse Beam)
BLM445TA-R (Round Beam)
BLM445TA, SM/PM Fiber Coupled
BLM450TA-E (Ellipse Beam)
BLM450TA-R (Round Beam)
BLM450TA, SM/PM Fiber Coupled
BLM445TA (up to 1.2W)
BLM445TA with Fiber Coupler
BLM450TA (up to 1.2W)
BLM450TA with Fiber Coupler
BLM445T3 (up to 1W)
BLM447T3 (up to 1W)
BLM450T3 (up to 1W)
BLM454T3 (up to 80mW)
RLM633TA-E (Ellipse Beam)
RLM633TA-R (Round Beam)
RLM633TA, SM/PM Fiber Coupled
RLM635TA-E (Ellipse Beam)
RLM635TA-R (Round Beam)
RLM635TA, SM/PM Fiber Coupled
RLM633TA (up to 300mW)
RLM633TA with Fiber Coupler
RLM635TA (up to 400mW)
RLM635TA with Fiber Coupler
RLM635T3 (up to 800mW)
RLM635T9 (up to 5000mW)
RLM622T3 (up to 50mW)
RLM627T3 (up to 100mW)
RLM633T3 (up to 100mW)
FCLS-635 (up to 1.2W)
FCLS-640 (up to 800mW)
FCLS-660 (up to 2W)
FCLS-785 (up to 1.5W)
FCLS-793 (up to 1.5W)
FCLS-808 (up to 10W)
FCLS-915 (up to 7W)
FCLS-940 (up to 10W)
FCLS-975 (up to 10W)
FCLS-980 (up to 10W)
FCLS-1450 (up to 400mW)
FCLS-1470 (up to 3W)
FCLS-1532 (up to 3W)
FCLS-1870 (up to 650mW)
FCLS-1908 (up to 650mW)
FCLS-1940 (up to 800mW)
FCLS-2200 (up to 350mW)
Laser for Raman Spectroscopy
GL532RA (up to 300mW)
GL532RA with Fiber Coupler
GL532RA, SM/PM Fiber Coupled
RLM658RA (up to 100mW)
RLM658RA, with Fiber Coupler
RLM658RA, SM/PM Fiber Coupled
IRM785RA (up to 500mW)
IRM785RA, with Fiber Coupler
IRM830RA (up to 500mW)
IRM830RA, with Fiber Coupler
Raman Probe
Accessories for Raman Spectra
P1 (up to 5mW)
RLM12-635C (Ф12mm, Cross)
P3 (up to 200mW)
RLM12-650L (Ф12mm, Line)
P5 (up to 200mW)
P1 (up to 5mW)
P3 (up to 500mW)
P1 (up to 5mW)
P3 (up to 500mW)
P1 (up to 2mW)
P8 (up to 20mW)
P2 (up to 5mW)
P8 (up to 80mW)
P2 (up to 5mW)
P8 (up to 80mW)
P6 (up to 50mW)
P7 (up to 50mW)
405nm Blue Laser Pointer
405nm Blue Portable Laser
808nm Laser Pointer
808nm Portable Laser
635nm Laser Pointer
635nm Portable Laser
655nm Laser Pointer
655nm Portable Laser
P8 (up to 500mW)
Laser Pointer
445nm Blue Laser Pointer
Laser Pens
445nm Blue Portable Laser
640nm Portable Laser
Laser Pointers
980nm Laser Pointer
P6 (up to 200mW)
P7 (up to 200mW)
980nm Portable Laser
P8 (up to 800mW)
DPSS Laser Principle |
Diode-pumped solid-state (DPSS) lasers are solid-state lasers made by pumping a solid gain medium, for example, a neodymium-doped YAG crystal, with a laser diode. DPSS lasers have advantages in compactness and efficiency over other types, and high power DPSS lasers have replaced ion lasers and flashlamp-pumped lasers in many scientific applications.

The most common DPSS laser in use is the 532nm wavelength green laser pointer. A powerful (>200 milliwatt) 808nm wavelength infrared laser diode pumps a neodymium doped yttrium orthvanadate (Nd:YVO4) crystal which produces 1064nm wavelength light. This is then frequency doubled using a nonlinear optical process in a KTP crystal, producing 532nm light. Green DPSS lasers are usually around 20% efficient, although some lasers have been reported to be 35% efficient. In other words, a green DPSS laser using a 2.5W pump diode would be expected to output around 500mW of 532 nm light.
Blue DPSS lasers use an extremely similar process, except that the 808nm light is being converted to 946nm light, which is then frequency-doubled to 473nm. Because of the lower gain for the materials, blue lasers are relatively weak, and are only around 3% efficient.
Yellow lasers use an even more complicated process. A 808nm pump is used to generate 1064nm and 1342nm light, which is summed to become 593.5nm. Yellow lasers are about as efficient as blue lasers, but due to their complexity and costs, most yellow DPSS lasers are only around 1% efficient.
