|
All lasers operate in a single
transverse mode. Longitudinal mode refers to the spectral properties.
Model
No.
(with Temperature Control) |
Wavelength
(nm) |
Output Power
(mW) |
Mode
(long.) |
Applications |
|
L4 375M-15-TE/ESYS |
375 +/-5 |
15 |
M |
Excellent beam
quality for confocal microscopes,
Microlithography,
reprographics, direct write
Flow cytometry
Fluorescence excitation
Communications |
|
L4 405M-20-TE/ESYS |
405 +/-5 |
20 |
M |
|
L4 405M-50-TE/ESYS |
405 +/-5 |
50 |
M |
|
L4 405M-95-TE/ESYS |
405 +/-5 |
95-100 |
M |
|
L4 445M-40-TE/ESYS |
445 +/-5 |
40 |
M |
|
L4 473M-15-TE/ESYS |
473 +/-5 |
15 |
M |
|
L4 488M-48-TE/ESYS |
488 +/-5 (New) |
48-50 |
M |
|
L4 515M-20-TE/ESYS |
515 +/-5 (New) |
20 |
M |
|
|
L4 635S-12-TE/ESYS |
637 +/-5 |
12 |
S |
Low noise, excellent
beam quality. High power HeNe replacement.
Fluorescence
excitation and general purpose use. |
|
L4 638S-25-TE/ESYS |
638 +/-5 |
25 |
S |
|
L4 642S-48-TE/ESYS |
642 +3/-7 |
48 |
S |
|
L4 642S-120-TE/ESYS |
642 +/-4 |
120 |
S |
|
L4 660S-40-TE/ESYS |
660 +/-5 |
40 |
S |
High power HeNe
replacement
Photodynamic
therapy |
|
L4 660S-95-TE/ESYS |
660 +/-5 |
95 |
S |
|
L4 670S-8-TE/ESYS |
670 +/-10 |
8 |
S |
|
L4 685S-40-TE/ESYS |
685 +/-10 |
40 |
S |
|
L4 705S-32-TE/ESYS |
705 +/-10 |
32 |
S |
Highly permeable in living tissue,
low absorption by water and hemoglobin, photodynamic therapy |
|
L4 730S-32-TE/ESYS |
730 +/-10 |
32 |
S |
|
L4 760D-32-TE/ESYS |
760 +/-1 |
32 |
S |
Water absorption,
Sensors |
|
L4 785S-95-TE/ESYS |
784 +/-4 |
95 |
S |
Raman spectroscopy |
|
L4 783N-64-TE/ESYS |
783 +/-1 |
64 |
S |
|
L4 810S-40-TE/ESYS |
810 +/-5 |
40 |
S |
Ophthalmology
Dermatology
Raman spectroscopy
Cancer research, photodynamic therapy |
|
L4 810S-115-TE/ESYS |
810 +/-5 |
115 |
S |
|
L4 830S-40-TE/ESYS |
830 +/-10 |
40 |
S |
|
L4 830S-115-TE/ESYS |
830 +/-10 |
115 |
S |
|
L4 830S-150-TE/ESYS |
830 +/-10 |
150 |
S |
|
L4 850S-40-TE/ESYS |
852 +/-5 |
40 |
S |
|
L4 850S-115-TE/ESYS |
852 +/-5 |
115 |
S |
|
L4 852D-115-TE/ESYS |
852 +/-2 |
115 |
S |
Atomic Clocks,
Interferometry,
Raman spectroscopy |
|
L4 860D-115-TE/ESYS |
860 +/-2 |
115 |
S |
|
L4 905M-70-TE/ESYS |
905 +/-5 |
70 |
M |
Sensors |
|
L4 940M-150-TE/ESYS |
940 +/-5 |
150 |
M |
|
|
L4 975M-200-TE/ESYS |
975 +/-5 |
200 |
M |
Laser pump |
|
L4 976D-115-TE/ESYS |
976 +/-1 |
115 |
S |
|
L4 980M-200-TE/ESYS |
980 +/-5 |
200 |
M |
|
L4 1064M-70-TE/ESYS |
1064 +/-5 |
70 |
M |
YAG replacement |
|
L4 1064M-150-TE/ESYS |
1064 +/-5 |
150 |
M |
|
L4 1060D-115-TE/ESYS |
1060 +/-1 |
115 |
S |
|
L4 1310D-3-TE/ESYS |
1310 +/-10 |
3 |
S |
Communications, biophotonics |
|
L4 1550D-3-TE/ESYS |
1550 +/-10 |
3 |
S |
Communications |
2mm beam option is available
on all lasers.
Wavelength stabilized lasers
are also available. Please see our section Wavelength Stabilized.
Model number with a "D" in the part number uses a DFB
type laser with built in grating to stabilize the spectrum. This
results in no mode hops for the laser. Many other wavelengths
are available. Please call for your requirements. |
