A quarter wave plate made of a 16 mu m thin silicon single crystal was
inserted in front of a double crystal monochromator which was used as
linear polarimeter for Bragg angles close to 45 degrees. This allowed
us to demonstrate that, at 2.836 keV, the circular polarisation rate
P-3 of the helical undulator Helios-I was greater than or equal to 97%
. At higher energies, we used a more conventional optical configuratio
n which included again the double crystal monochromator, a diamond qua
rter-wave plate and a linear polarimeter consisting of a kapton foil s
cattering at 90 degrees. Fairly reasonable circular polarisation rates
were then measured at 7 keV with the second (P-3 greater than or equa
l to 0.88) and third harmonics (P-3 greater than or equal to 0.84) of
the helical undulator Helios-II. On changing the phase of the helical
undulator we also measured reasonably good linear polarisation rates (
P-2 greater than or equal to 0.94) with the polarisation vector inclin
ed at 45 degrees with respect to the vertical axis. The results obtain
ed with Helios-II call nevertheless for further investigation of possi
ble sources of depolarisation.