Transmission bender for polarizing neutrons
Introduction
Nowadays, in many cases neutron beams are polarized using supermirrors. The angular interval which can be polarized by supermirrors is limited by their critical angle which is in the order of one degree. To polarize a beam with a width of several centimeter either a supermirror is needed with a length of several meter, as described in Ref. [1], or a system with parallel channels. These channels can be straight with the supermirrors at an angle to beam [2] or curved as in a bender. There are two types of benders. In one of them the neutrons fly in air and one spin component is reflected from supermirrors on bent glass walls [3], in the other one they fly in bent silicon wafers coated with supermirrors [4]. In the first set up the unwanted spin component is necessarily absorbed in the glass wall. The second set up allows to transmit both components which are distinguished by different angles and one spin state can be selected by putting a collimator behind the bender at the angle of the beam which should be used. In particular, the non deflected component can be chosen thus giving a polarizing device which polarizes a beam without changing the flight path of the neutrons.
Section snippets
Experimental set up
For the bender silicon wafers with the dimensions of 50 mm high, 54 mm long and 0.16 mm thick were coated on one side with FeCo–Si supermirrors with , where m denotes the ratio of the critical angle of the supermirror to the critical angle on natural nickel. One hundred and twenty five of these wafers were put into a holder which deflects the middle of this stack by one wafer thickness to close the direct line of sight. The supermirrors are subjected to a magnetic field of 1 kG.
The collimator
Results
Fig. 1 shows the rocking curve for the collimator normalized to the direct beam.
The FWHM is 0.37°. For a channel width of 0.2 mm this corresponds to an effective channel length of 31 mm.
The transmission reaches in the maximum 83.5%. According to the literature [5], the attenuation in the silicon amounts to 10%. The transmission of a beam which has a triangular angle distribution with a FWHM of 0.035° through a collimator which has a triangular transmission function with a FWHM of 0.37° is 96.8%.
Application
This very short polarizer system will be applied to deliver polarized neutrons with wavelengths above 4 Å to the entrance aperture of the magnetic focusing SANS spectrometers at C3-1-2-1 (NOP) and C3-2 (SANS-J) beam lines of JRR-3 in JAERI [8], [9]. It is necessary to deliver only one spin component to the focusing system because the other spin component is defocused in the magnet and hence produces background.
Conclusion
It was successfully shown that a solid state bender with polarizing coatings can be used as a polarizer working in transmission geometry. It was designed for wavelengths above 4 Å. For the wavelength of 4.7 Å a triangular transmission with a maximum of 54% of the spin down component and a mean flip ratio above 100 were reached over an angular range with a FWHM of 0.37°.
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