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NEW OPPORTUNITIES FOR ATMOSPHERIC MONITORING !
Two-Channel Laser System
 

Two-Channel
Laser System

  With the progress of the human technological potential, elimination or minimization of the effects of global atmospheric pollution has become a must for the absolute majority of states in their environmental activity. The acquisition of on-line information about the state of the atmospheric layer is an integral part of both global and regional atmospheric monitoring. Lidar systems utilizing laser radiation sources become more and more often integrated into the systems of atmospheric monitoring.
  The SOLAR TII two-channel laser system is specially designed for use in lidar complexes to monitor the aerosol component, to determine the level of the atmospheric pollution with gases (NH3 , SO2 , NOx , O3 , or others), to monitor the vertical distribution of ozone in stratosphere, as well as in other applications.

     Features

  • Simultaneous lasing at several wavelengths
  • Broad spectral range (235 to 1064 nm)
  • Generation of narrow-linewidth (down to 35 pm) radiation
  • A wide range of output energies (1 to 650 mJ)
  • Automatic setting and control of output parameters
  • Energy and wavelength control for each output pulse in both of the channels in the real time scale
  • Heat/Impact-resistant construction & stable parameters
  • Completely automatic system for measuring each pulse parameters
  • High noise-immunity
  • Control and data transfer via fiber optics

 

Specifications

LASER PARAMETERS
  Wavelength
    Channel I
      Nd:YAG laser:
      Ti:Sapphire laser
        at fundamental:
        at second harmonic:
        at third harmonic:
      Channel II
        Nd:YAG laser:
        Ti:Sapphire laser
          at fundamental:
          at second harmonic:
          at third harmonic:
        Laser line-width (max)
          Nd:YAG laser:
          Ti:Sapphire laser:
        Max. wavelength stability
        (with 8hrs-continuous laser running):
        Beam diameter (before output telescope)
          Nd:YAG laser:
          Ti:Sapphire laser:

532 nm, 266 nm

700-950 nm
350-475 nm
235-315 nm

1064 nm, 355 nm

700-950 nm
350-475 nm
235-315 nm

0,005 nm
0,035 nm

0,02 nm

</= 7,5 mm
</= 3,0 mm

ENERGY CHARACTERISTICS
  Pulse energy (before output telescope)
    Nd:YAG laser
      1064 nm:
      532 nm:
      355 nm:
      266 nm:
    Ti:Sapphire laser
      at fundamental:
      at second harmonic (450 nm):
      at third harmonic (300 nm):

650 mJ
400 mJ
150 mJ
120 mJ

75 mJ
30 mJ
10 mJ

SPATIAL CHARACTERISTICS
  Max. beam divergence:
  Telescopes:
  Separation between channel optic axes:

0,5 mrad
achromatic 8x
350 mm

TIME CHARACTERISTICS
  Max. pulse width (1064 nm):
  Pulse repetition rate:

16 ns
10 Hz (20 Hz)

PULSE PARAMETERS MEASURED AND MEASUREMENT ACCURACY
  Pulse energy measurement
    measurement range:
    measurement accuracy:
  Wavelength measurement
    measurement range:
    measurement accuracy
      700-950 nm:
      350-475 nm:
      235-315 nm:

1-650 mJ
+/- 3%

230-959 nm

0,04 nm
0,02 nm
0,013 nm

ELECTRIC CHARACTERISTICS
  Power requirements:

  External synchronization:

single phase, 220V +/-20%,
50-60 Hz, 1850 W (max)
TTL level (+5V)

OVERALL SIZE, WEIGHT
  Laser heads module:
  Power & Cooling unit:

1500x1200x250 mm, 385 kg
420x510x1080 mm, 96 kg

 
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