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Deutsche Tagung f ¨ur Forschung mit ... - SNI-Portal

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Methoden und Instrumentierung Poster: Mi., 14:00–16:30 M-P81<br />

A double monochromator device for the CONRAD imaging instrument at<br />

HMI Berlin<br />

Markus Strobl 1,2 , Nicolay Kardjilov 1 , André Hilger 1 , Wolfgang<br />

Treimer 1,2 , Ingo Manke 1<br />

1 Hahn Meitner Institut, Glienickerstr. 100, 14109 Berlin – 2 TFH Berlin, Luxemburger<br />

Str. 10, 13353 Berlin<br />

Besides the disadvantage of lower flux densities, imaging with monochromatic radiation,<br />

in our case neutrons, offers a number of advantages especially in the case of<br />

various energies available. Avoiding beam hardening effects allows more sensitive and<br />

accurate quantitative measurements and in the latter case energy selective and energy<br />

dispersive techniques can be applied opening new fields of application. Here we want<br />

to introduce the first neutron double monochromator device for that purpose installed<br />

at the imaging beam line CONRAD. CONRAD is the new cold neutron radiography<br />

and tomography instrument at the Hahn Meitner Institute in Berlin which recently<br />

started operation as a part of the Berlin Neutron Scattering Centre (BENSC). It includes<br />

two measurement positions of which the first one directly at the end of the NL1b<br />

neutron guide was used to install a flexible monochromator device as an additionally<br />

available insert. While the CONRAD instrument uses in standard operation the full<br />

cold spectrum of the lower part of the guide, a first PCG(002) monochromator with<br />

a mosaic spread of app. 2 degrees is placed in the upper beam part deflecting neutrons<br />

downwards. The initial lower beam part is blocked by a shutter and on a linear<br />

manipulation table behind it the second corresponding graphite crystal is installed.<br />

Hence, while both crystals can be rotated to chosen Bagg angles, the second one can<br />

be positioned along the original beam direction in order to reflect the monochromatic<br />

beam from the first crystal into the initial beam path of the CONRAD instrument.<br />

This construction enables to choose a monochromatic beam with wavelengths between<br />

0.25 nm and 0.65 nm for high resolution imaging at the second measurement position<br />

of CONRAD app. 5 m downstream. First measurements and results concerning operational<br />

parameters, tests of methods ranging from energy selective radiography to stress<br />

mapping, first quantitative analyses and application perspectives will be presented.

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