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<meta name="author" content="
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—
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Thomas Dehaeze
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" /><meta name="description" content="Tags Nano Active Stabilization System, Positioning Stations Reference (Holler {\it et al.}, 2012) Author(s) Holler, M., Raabe, J., Diaz, A., Guizar-Sicairos, M., Quitmann, C., Menzel, A., &amp; Bunk, O. Year 2012 Instrument similar to the NASS. Obtain position stability of 10nm (standard deviation).
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Figure 1: Schematic of the tomography setup
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Limited resolution due to instrumentation: The resolution of ptychographic tomography remains above 100nm due to instabilities and drifts of the scanning systems." />
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<h1 class="post-title">An instrument for 3d x-ray nano-imaging</h1>
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<dl>
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<dt>Tags</dt>
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<dd><a href="/zettels/nano_active_stabilization_system/">Nano Active Stabilization System</a>, <a href="/zettels/positioning_stations/">Positioning Stations</a></dd>
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<dt>Reference</dt>
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<dd><sup id="66ab0e7602a1dedda963d7da60533b0d"><a href="#holler12_instr_x_ray_nano_imagin" title="Holler, Raabe, Diaz, Guizar-Sicairos, , Quitmann, Menzel \& Bunk, An Instrument for 3d X-Ray Nano-Imaging, {Review of Scientific Instruments}, v(7), 073703 (2012).">(Holler {\it et al.}, 2012)</a></sup></dd>
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<dt>Author(s)</dt>
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<dd>Holler, M., Raabe, J., Diaz, A., Guizar-Sicairos, M., Quitmann, C., Menzel, A., & Bunk, O.</dd>
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<dt>Year</dt>
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<dd>2012</dd>
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</dl>
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<p>Instrument similar to the NASS.
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Obtain position stability of 10nm (standard deviation).</p>
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<p><a id="orgba4a339"></a></p>
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<figure>
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<img src="/ox-hugo/holler12_station.png"
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alt="Figure 1: Schematic of the tomography setup"/> <figcaption>
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<p>Figure 1: Schematic of the tomography setup</p>
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</figcaption>
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</figure>
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<ul>
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<li>
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<p><strong>Limited resolution due to instrumentation</strong>:
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The resolution of ptychographic tomography remains above 100nm due to instabilities and drifts of the scanning systems.</p>
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</li>
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<li>
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<p><strong>Need of a Metrology System</strong>:</p>
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<blockquote>
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<p>To achieve positioning accuracy and stability in the nanometer range, one cannot rely on the position encoders built into individual positioning stages.
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A precise exteroceptive measurement of the relative position of the optical elements with respect to the sample is mandatory.
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Thus, thermal drifts and parasitic motions can be measured and compensated for.</p>
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</blockquote>
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</li>
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<li>
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<p><strong>Interferometer System Concept</strong>:
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The sample is aligned with the X-ray with the XYZ piezo stage.
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As a result, the metrology sphere will be usually off center with respect to the rotation axis of the spindle.
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That implies that the laser will not propagate back to the interferometer at all rotation angles.
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A position sensitive detector (PSD) is used, it provides a measurement of the position of the sphere in the plane perpendicular to the laser.
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The interferometer is positionned on top of a translation stage. The PSD information is used to close the loop so that the interferometer follows the displacement of the metrology sphere.</p>
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</li>
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<li>
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<p><strong>Feedback Loop</strong>: Using the signals from the 2 interferometers, the loop is closed to compensate low frequency vibrations and thermal drifts.</p>
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</li>
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</ul>
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<h1 id="bibliography">Bibliography</h1>
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<p><a id="holler12_instr_x_ray_nano_imagin"></a>Holler, M., Raabe, J., Diaz, A., Guizar-Sicairos, M., Quitmann, C., Menzel, A., & Bunk, O., <em>An instrument for 3d x-ray nano-imaging</em>, Review of Scientific Instruments, <em>83(7)</em>, 073703 (2012). <a href="http://dx.doi.org/10.1063/1.4737624">http://dx.doi.org/10.1063/1.4737624</a> <a href="#66ab0e7602a1dedda963d7da60533b0d">↩</a></p>
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