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X-ray imaging performance of scintillator-filled silicon pore arrays
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10.1118/1.2839441
/content/aapm/journal/medphys/35/3/10.1118/1.2839441
http://aip.metastore.ingenta.com/content/aapm/journal/medphys/35/3/10.1118/1.2839441

Figures

Image of FIG. 1.
FIG. 1.

Cross-sectional view of a pore array after electrochemical etching (tilt: ) before filling with CsI(Tl). The pitch is , the walls are , and the depth is about .

Image of FIG. 2.
FIG. 2.

Thickness maps for two samples (top No. 1, bottom No. 6). The inset in the bottom image gives the CsI thickness in . Note, that these maps are based on x-ray absorption measurements that do not resolve every single pore. The circular area defines the etched and CsI-filled region. The dimensions of the images are .

Image of FIG. 3.
FIG. 3.

Recalculated CsI thickness histograms for all samples (from maps as shown in Fig. 2). Note, that the thickness is derived from x-ray absorption measurements that do not resolve every single pore. The sample Nos. 1–4 show a similar mean value and width of the distribution.

Image of FIG. 4.
FIG. 4.

SEM image of a cross section from sample No. 3. The voids at the bottom of some columns appear to stem from the filling procedure rather than from the cross-section preparation. The polycrystalline nature of the solidified CsI is also visible.

Image of FIG. 5.
FIG. 5.

Schematic setup for x-ray measurements, not to scale.

Image of FIG. 6.
FIG. 6.

Sensitivity of three samples as histograms, normalized to their maximum values.

Image of FIG. 7.
FIG. 7.

Signal vs dose for sample No. 3 for two different beam qualities in a double logarithmic plot. The results for the slope are from a regression calculation.

Image of FIG. 8.
FIG. 8.

Experimental results of the MTF measurement with the edge method for three samples. For comparison the MTF of the aperture (sinc function) and the MTF of commercial columnar CsI, measured on the same sensor, is also shown.

Image of FIG. 9.
FIG. 9.

NPS of sample No. 3 vs spatial frequency, plotted for various dose levels and two different beam qualities. In addition, the dark NPS, i.e., without x ray, is shown.

Image of FIG. 10.
FIG. 10.

DQE vs spatial frequency for sample No. 1 for various applied doses and two different beam qualities ( and ).

Image of FIG. 11.
FIG. 11.

DQE vs spatial frequency for the best sample (No. 3).

Image of FIG. 12.
FIG. 12.

Comparison of the DQE of two pore array samples measured with beam quality at a dose of with the DQE of a commercial columnar CsI:Tl sheet at a dose of .

Image of FIG. 13.
FIG. 13.

DQE at a fixed spatial frequency (0.5 lp/mm) vs dose for sample Nos. 1, 2, and 3.

Image of FIG. 14.
FIG. 14.

X-ray images of line pair phantoms with 7.5 lp/mm (top) and 9 lp/mm (bottom). The black parts on the right and lower left are outside the scintillator-filled area. The black line in the center is caused by two adjacent defect columns of the sensor, which are not interpolated by the defect correction algorithm.

Image of FIG. 15.
FIG. 15.

X-ray image of the fingertip of an anatomical hand phantom. The black areas are outside of the scintillator-filled region.

Image of FIG. 16.
FIG. 16.

Combination of two x-ray images showing a joint in the little finger of an anatomical hand phantom.

Image of FIG. 17.
FIG. 17.

Light guiding efficiency and optical Swank factor as a function of mean scatter length calculated from simulation results for three different beam qualities.

Image of FIG. 18.
FIG. 18.

Top: x-ray absorption of sample No. 3 (, ), measured with a flat x-ray detector (not resolving each pore). Bottom: Corresponding gain map of the pore array in combination with the high-resolution optical CMOS sensor ( signal, signal). Hardly any correlation between the two images is seen.

Image of FIG. 19.
FIG. 19.

Top: x-ray absorption of sample No. 6 (, ). Bottom: Corresponding gain map ( signal, signal). Many of the black spots can be found in both images, representing low CsI filling and at the same time very low light output as indicated by the white ellipse.

Image of FIG. 20.
FIG. 20.

Theoretical contribution of pixel aperture, fluorescence and optical gap to the total MTF compared to the measurement results of sample No. 3.

Tables

Generic image for table
TABLE I.

Data on the beam qualities used for most of the measurements. is the thickness of Al placed in the beam. Together with the internal filtration an equivalent thickness of is achieved. is the number of quanta per area and dose as calculated by the simulation program.

Generic image for table
TABLE II.

Data on the three beam qualities that were explicitly verified for their defining half value layers. is the tube voltage for which the right HVL is reached experimentally.

Generic image for table
TABLE III.

Definition and numbers for the quantities used in Eq. (4). The absorption is dependent on the beam quality and is here shown for as example.

Generic image for table
TABLE IV.

Results for the light guiding efficiency of the three best samples.

Generic image for table
TABLE V.

DQE(0) for different samples and for two beam qualities with estimated errors. is the mean x-ray quantum energy corresponding to the used beam quality.

Generic image for table
TABLE VI.

DQE(0) for the best sample (No. 3) for different beam qualities.

Generic image for table
TABLE VII.

Factors contributing to the DQE. Theoretical and experimental results for the DQE(0) of three samples.

Generic image for table
TABLE VIII.

Theoretical and experimental results for one sample (No. 3) and three different beam qualities.

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/content/aapm/journal/medphys/35/3/10.1118/1.2839441
2008-02-20
2014-04-21
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: X-ray imaging performance of scintillator-filled silicon pore arrays
http://aip.metastore.ingenta.com/content/aapm/journal/medphys/35/3/10.1118/1.2839441
10.1118/1.2839441
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