He-Ne Lasers of Visible Range
Plasma, JSC, offers 25 models of He-Ne lasers of HN and LGN series with
emission power from 0.5 to 70 mW in single mode or from 5 to 100 mW in multimode
regime. There are models with polarized and non-polarized emission.
Model | Wavelength, um | Power, mW | Spectral structure | Polarization | Downloads | |
GN-0.5 | 0.63 | 0.5 | TEMoo | 1:1 | ||
GN-1 | 0.63 | 1.0 | TEMoo | 1:1 | ||
GN-2P | 0.63 | 2.0 | TEMoo | 100:1 | ||
GN-3 | 0.63 | 3.0 | TEMoo | 1:1 | ||
GN-5 | 0.63 | 5.0 | TEMoo | 1:1 | ||
GN-5P | 0.63 | 5.0 | TEMoo | 100:1 | ||
GN-5M | 0.63 | 5.0 | TEMmn | 1:1 | ||
GN-10M | 0.63 | 8.0 | TEMmn | 1:1 | ||
GN-15 | 0.63 | 15.0 | TEMoo | 1:1 | ||
GN-15-1 | 0.63 | 15.0 | TEMoo | 100:1 | ||
GN-25 | 0.63 | 25.0 | TEMoo | 1:1 | ||
GN-25-1 | 0.63 | 25.0 | TEMoo | 100:1 | ||
GN-40 | 0.63 | 40.0 | TEMmn | 1:1 | ||
GN-50 | 0.63 | 50.5 | TEMmn | 1:1 | ||
GN-50-1 | 0.63 | 50.0 | TEMoo | 100:1 | ||
GN-60 | 0.63 | 60.0 | TEMmn | 1:1 | ||
GN-70 | 0.63 | 70.0 | TEMmn | 1:1 | ||
GN-80 | 0.63 | 80.0 | TEMmn | 1:1 | ||
LGN-225A | 0.63 | 2.0 | TEMoo | 1:1 | ||
LGN-226A | 0.63 | 1.5 | TEMoo | 100:1 | ||
LGN-223 | 0.63 | 10.0 | TEMoo | 1:1 | ||
LGN-223-1 | 0.63 | 10.0 | TEMoo | 100:1 | ||
LGN-115 | 0.63 | 15.0 | TEMmn | 1:1 | ||
LGN-118 | 0.63 | 25.0 | TEMmn | 1:1 | ||
LGN-220 | 0.63 | 70.0 | TEMoo | 500:1 | ||
LGN-220M | 0.63 | 100.0 | TEMmn | 500:1 | ||
LGN-220SF | 0.63 | 40 | single-frequency | 500:1 |
He-Ne Lasers of IR Range
The series of He-Ne lasers of IR range includes 11 models with emission power
of multimode emission from 1 to 25 mW at wavelengths 1.15, 3.39, 3.5, 5.4
mm. He-Ne lasers possess all the advantages of low-power
monochromatic emission at the new spectral lines, coinciding with the lines of
absorption of a series of ecologically hazardous wastes produced by industrial
facilities.
Model | Wavelength, um | Power, mW | Spectral structure | Polarization | Downloads | |
GNIK-3-1 | 3.3922 | 3 | TEMmn | 100:1 | ||
GNIK-3-1A | 3.3912 | 1 | TEMmn | 100:1 | ||
GNIK-3-2 | 3.3922 | 9 | TEMmn | 100:1 | ||
GNIK-3-2A | 3.3912 | 4 | TEMmn | 100:1 | ||
GNIK-3-3 | 3.3922 | 14 | TEMmn | 100:1 | ||
GNIK-3-3A | 3.3912 | 7 | TEMmn | 100:1 | ||
GNIK-3-4 | 3.3922 | 24 | TEMmn | 100:1 | ||
GNIK-3-4A | 3.3912 | 10 | TEMmn | 100:1 | ||
GNIK-3-K | 3.5 | 12 | TEMmn | 100:1 | ||
GNIK-1-1 | 1.15 | 1.5 | TEMoo | 100:1 | ||
GNIK-1-2 | 1.15 | 3.0 | TEMmn | 100:1 | ||
GNIK-5 | 5.4 | 1.5 | TEMoo | 100:1 |
Multiline He-Ne lasers
You can also purchase lasers operating either in the mode of simultaneous
generation on 2 lines, or in modes of separate generation at any of operating
wavelengths. At the tuning from one wavelength to another the position of the
emission axis does not change.
Model | Wavelength, um | Power, mW | Spectral structure | Polarization | Downloads | |
LGN-118-2V | 0.63/1.15 | 10/5 | TEMmn | 100:1 | ||
LGN-118-3V | 0.63/1.15/3.39 | 10/5/5 | TEMmn | 100:1 |
Stabilized He-Ne Lasers
We produce and sell single- and dual-frequency stabilized He-Ne lasers.
Dual-frequency lasers with Zeeman frequency splitting and wide range of the
difference frequency values (from 1.5 MHz to 4.5 MHz) of the optical emission
components. High stability of emission frequency is provided by active and
passive methods of stabilization. Linear and orthogonal emission polarizations
provide for the wide opportunities of the application in control-measurement
systems with the highest accuracy.
Model | Wavelength, um | Power, mW | Spectral structure | Polarization | Downloads | |
LGN-212-1 | 0.63 | 0.2 | double-frequency | 2 orthogonally polarized components | ||
LGN-303 | 0.63 | 1 | single-frequency | 100:1 | ||
LGN-303-1 | 0.63 | 1 | double-frequency | 100:1 | ||
LGN-302 | 0.63 | 0.7 | single-frequency | 100:1 | ||
LGN-212-1M | 0.63 | 0.2 | double-frequency | linear | ||
LGN-212-1-MF | 0.63 | 0.2 | double-frequency | linear |
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