Scanning Fabry-Perot interferometers (FPI) 
Observations with the FPI consist of successive acquisition of a few dozen images of interference rings from the object (or from a calibration lamp) when changing the optical path between the parallel plates. The radius of the rings is a
function of wavelength and gap between the plates of the interferometer. The complete set of such images
which fills the free spectral range of the interferometer is called 'a scanning cycle'. 
After data reduction  images are  collected  in a data cube. Control of the scanning (change of the gap between flat reflecting plates) is managed by  the  controller    CS100  IC Optical Systems Ltd., connected with a computer.   The description of observations and data reduction is presented in the papers: 
- Moiseev A.V. 2002,   Bull. SAO, 54, 77 (English PDF, Русский PS)
 
 - Moiseev A.V., Egorov O.V.,   2008, Astrophy. Bull., 63, 181 (English PDF, Russian PDF)
 
Moiseev A.V.,  2015, Astrophy. Bull., 70, 494; ( Russian PDF  ; arXiv:1511.03886); 
   
SCORPIO-2 has a set of bandpass filters which cut the desired narrow spectral range around    the emission lines H-alpha, [OIII]5007, [NII]6548,6583, [SII]6717,6731. You can use this  IDL-programm  for chose an optimal filter for desired  systemic velocities of target galaxies.
The piezoelectric interferometers were mad by   IC Optical Systems Ltd. (early name - Queensgate).
 
 
The main parameters of FPI (in the H-alpha spectral range). 
 
|      | 
 IFP20  |  IFP186  |  IFP501 |  IFP751 |  
| Order  | 20 | 186 | 501 | 751 |  
| Interfringe  | 328 A |  35 A  (~1600) km/s) |  13 A   (~600 km/s) |  8.7 A   (~390 km/s) |  
| Sp. resolution  | 20 |    1.7 A |  0.8A | 0.4A |  
| Finesse  | 16 |    21 |  16 | 20 |  
| Number of spectral channels  |   tunable filter | 40 |  36  | 40 |  
 
  
The photo shows  IFP751 mounted into  SCORPIO-2 during tuning procedures
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