About this site

This site is in permanent work. It will take infinite time until I put what I intend on it.
Please be patient. In the meantime you can consult Wiki on interferometry at
http://starryridge.com/mediawiki-1.9.1/index.php?title=Main_Page
Vladimir

Polarizers in Phase Shift Interferometry

Bath Phase Shift  Interferometer  (BPSI) requires several polarizing components. Two of them are linear polarizers, one is circular poarizer  aka quarter wave plate (QWP) and one is polarizing cube beam splitter.  All optics in the interferometer must be very clean, free from scratches, in order to introduce least amount of wavefront deformations. Most used polarizing  filters are plastic films and their surface is not particularily good or resistant to scratches. One source of good polarizing filters are filters for photographic cameras. They are made of polarizing films sendwiched between two glass plates. That makes them well protected and easy for cleaning. Used filters of this kind can be obtained cheep and are recomended for amateur use. I have got mine for 2 euro apice.  Morower polarizing filters for camera objectives come in holders  which are screwed to the objective  and can be rotated which makes them particularly suitable for PSI Bath. Poalrizing filters for cameras  come in two varieties. Old style (film) cameras use linerily polarized filters, while digital cameras use circularly polarizing filters because linear polarizers get in way of automatic exposure determination. Those circular filters are also used in Bath PSI  and  can be obtained much cheeper than similar filters sold by optics companies.

Camera Focusing in Bath Interferometer

In Bath interferometer camera must be focused on the mirror under test. Usually this is done by placing some well illuminated printed text on the mirror under test and camera is focused until the text is sharp.

Focusing can be done also in other way where separate illumination is not required and laser from interferometer is used for this purpose.

The beam splitter cube is removed so that there is no reference beam. Test beam diverged by the lens is illuminating the mirror and reflected light is directed to the camera via flat mirror. If an object (mask) is placed on the mirror under test, its outline can be used for focusing. First picture shows the outline of such object (mask) in interferogram

 

and second picture how it looks  with proposed setup.

If the beam splitter cube can not be easily removed, the same method can be used if reference spot on the mirror under test is blocked by the same object (mask) used for focusing (in other words, reference beam spot should fall on the mask and thus can not be reflected).  This picture shows the resulting image.

XYZ translation stage for Bath interferometer

The stahe is based on flexural hinges for x and z  (horizontal) translations, and 3 screws for y (vertical) translations. Flexures are  spring wires 1 mm diameter. For size estimate, the spltter cube is 15 mm on side.

xyz stage for Bath interferometer

xyz stage, exploded view

Ray tracing the Bath Interferometer

This is the Bath interferometer consisting of the 10 mm beam splitter cube , a flat front surface mirror and  diverging lens of 10 mm focal length, 7 mm diameter and  1.5 index of refraction,  used in testing the 850 mm ROC  spherical mirror. Laser beam width is 2 mm.The interferograms associated with each interferometer-mirror setting are synthesized as a Young two point source interference pattern corresponding to the actual position of final foci of the test and reference beams as seen on the each image text. In rendering images, refraction on the beam splitter cube sides was not considered.  refraction in lens and reflections on the splitter diagonal was used in ray tracing of the light beams . Real case differs because the conics, other than spheres, usually paraboloids, have spherical aberration when tested from ROC which is modifying  the interference patterns.

Quantitative values of changed positions of the mirror, relative to the interferometer and resulting change in interferograms are instructive to get feeling for the amount of adjustments required in xyz translational stages on which the interferometer usually rests. It also demonstrates that adjustments can be divided so that for example longitudinal movement (z- axis) is done on interferometer and transversal (x,y axes) by the moving the mirror under test (or some other combination). Please note the difference in sensitivity to transversal movement compared to  the longitudinal.

The interferogram analysis program OpenFringe (from Dale Eason) is offering  several methods.  Most recent is Fourier transform based, which works best on large number of not much curved and not closed fringes , like in image 7. More on this in Wiki:

 http://starryridge.com/mediawiki-1.9.1/index.php?title=Main_Page

SEPARATION OF TEST STAND ASTIGMATISM

Zernike coefficients for astigmatism obtained from Bath interferometry 
contain astigmatism on the glass, stand induced astigmatism and
Bath interferometer induced instrumental astigmatism.
method to separate them was suggested by Dale Eason and is known
as derotation method.
 
I will here describe variation of this method as I am using it with PSI-Bath
interferometer. I have already posted first results on two small mirrors
one of 83 mm diameter f/5,  1:3.3 thickness to diameter ratio,  and another
one  115 mm diameter f/4.5, 1:6.2 ratio.
The mirrors are small  and thick and tested with optical axis vertical so not
much stand deformation was expected.
 
In the meantime  another mirror was obtained, 200 mm, f/4,  1: 8 ratio and
the method was tested on this one.
 
Mirror was resting on Plop designed 6 point cell. 4 rotations were used.
0, 45, 90 and 135 degrees (approximately, exact values are not required
by the method). Since angular part of astigmatism polynomials  is sin(2 theta)
and cos( 2 theta), astigmatism from rotations was oriented 0, 90, 180 and
270 degrees.
 
For each rotation 10 interferograms phase shifted by 72  degrees, were made.
By using Stephens running method and Michaels 5 phase cycle PSI analysis
program, it was possible to make 6 cycles from 10 shifted interferograms.
So I have 6 results for each rotation (24 in total).
 
Analysis program provided Z4 (x-ast) and Z5 (y-ast) components which were
plotted y-ast  versus x-ast . Resulting plot is here, and in my Photos folder of
Interferometry group. interferometry@yahoogroups.com
Photos, Vladimir Galogaza.
 
>How did you determine this uncertainty of +- .003 waves?

 
I have made 6 interferometric measurements for each of four rotations.
That brings total of 24 pairs of Zernike astigmatism coefficients.
Fitting circle to measurements points is kind of averaging and circle
center is averaged results for all 24 points.
Circle radius is averaged mirror astigmatism. Distance from circle
center to each of measurement points is individual result.
The error is maximal deviation of all individual results from mean value
of all individual results.
Michael Peck told me that modified rotation method can also determine higher
order astigmatism . I have tried it with previous measurements and quality of
data was low enough to spoil such determination.
With my latest measurements, secondary astigmatism determination could
be estimated while  tertiary failed,  as demonstrated in the following three graphs.
(If the graphs are stripped in archives they can be found in my Photos album
Interferometry@yahoogroups.). This is one more demonstration of the superiority of the PSBI  (Phase Shift Bath Interferometry)  data quality (IMO).

Minimizing the Bath interferometer

 
light path through the glued assembly
Interferogram with this interferometer
Interferogram with this interferometer
Bath interferometer 6
Bath interferometer 5
Bath interferometer 4
Bath interferometer 3
Bath interferometer 2
Bath interferometer 1

Bath interferometer is very small. To further reduce its size to essentials, I have eliminated holders for lens and folding flat by gluing them to the beam splitter cube. Cube is 15 mm on side, the diverging lens is plano convex, 9 mm diameter (cut on one side), 21mm focal length. Folding flat is right angle prism, 6mm.Laser for the interferograms was green diode laser pointer. Interferogram pictures are from hand-held  DSLR camera (1/800 sec).Beam separation for this unit is 6 mm.

Intensity regulation of the green solid state laser

Intensity of the green diode laser can be changed by variable serial resistor in power supply. The graph shows dependence of laser intensity on serial resistance. This laser has power stabilization cirsuit which has not prevented intensity controll . Power stabilization action is visible when input voltage is close to nominal value (3 V for this usnit) by leveling off  the curve for small resistance.