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    <title>Satyajit Ghosh | Theragnostic Imaging</title>
    <link>https://www.theragnostics.no/en/author/satyajit-ghosh/</link>
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    <description>Satyajit Ghosh</description>
    <generator>Hugo Blox Builder (https://hugoblox.com)</generator><language>en-us</language><lastBuildDate>Wed, 13 Nov 2024 00:00:00 +0000</lastBuildDate>
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      <title>Satyajit Ghosh</title>
      <link>https://www.theragnostics.no/en/author/satyajit-ghosh/</link>
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      <title>Twisted clustered pinhole collimation for improved high-energy preclinical SPECT/PET</title>
      <link>https://www.theragnostics.no/en/publications/cosmi-2024-twisted/</link>
      <pubDate>Wed, 13 Nov 2024 00:00:00 +0000</pubDate>
      <guid>https://www.theragnostics.no/en/publications/cosmi-2024-twisted/</guid>
      <description>&lt;hr&gt;
&lt;p&gt;&lt;em&gt;Objective.&lt;em&gt;Advanced pinhole collimation geometries optimized for preclinical high-energy&lt;/em&gt;ɣ&lt;/em&gt;imaging facilitate applications such as&lt;em&gt;ɑ&lt;/em&gt;and&lt;em&gt;ß&lt;/em&gt;emitter imaging, simultaneous multi-isotope PET and PET/SPECT, and positron range-free PET. These geometries replace each pinhole with a group of clustered pinholes (CPs) featuring smaller individual pinhole opening angles (POAs), enabling sub-mm resolution imaging up to ∼1 MeV. Further narrowing POAs while retaining field-of-view (FOV) may enhance high-energy imaging but faces geometrical constraints. Here, we detail how the novel twisted CPs (TCPs) address this challenge.*Approach.*We compared TCP and CP collimator sensitivity at equal system resolution (SR) and SR at matched sensitivity by tuning pinhole diameters for&lt;sup&gt;18&lt;/sup&gt;F (511 keV) and&lt;sup&gt;89&lt;/sup&gt;Zr (909 keV). Additionally, simulated Derenzo phantoms at low activity (LA: 12 MBq ml&lt;sup&gt;-1&lt;/sup&gt;) and high activity (HA: 190 MBq ml&lt;sup&gt;-1&lt;/sup&gt;) levels, along with uniformity images, were compared to assess image resolution and uniformity.*Main results.*At equal SR, TCP increased average central FOV sensitivity by 15.6% for&lt;sup&gt;18&lt;/sup&gt;F and 29.4% for&lt;sup&gt;89&lt;/sup&gt;Zr compared to CP. Image resolution was comparable, except for&lt;sup&gt;89&lt;/sup&gt;Zr at LA, where TCP resolved 0.80 mm diameter rods compared to 0.90 mm for CP. Image uniformity was equivalent for&lt;sup&gt;18&lt;/sup&gt;F, while for&lt;sup&gt;89&lt;/sup&gt;Zr TCP granted a 10.4% improvement. For collimators with matched sensitivity, TCP improved SR by 6.6% for&lt;sup&gt;18&lt;/sup&gt;F and 17.7% for&lt;sup&gt;89&lt;/sup&gt;Zr while also enhancing image resolution; for&lt;sup&gt;18&lt;/sup&gt;F, rods distinguished were 0.65 mm (CP) and 0.60 mm (TCP) for HA, and 0.70 mm (CP and TCP) for LA. For&lt;sup&gt;89&lt;/sup&gt;Zr, image resolutions were 0.75 mm (CP) and 0.65 mm (TCP) for HA, and 0.90 mm (CP) and 0.80 mm (TCP) for LA. Image uniformity with TCP decreased by 18.3% for&lt;sup&gt;18&lt;/sup&gt;F but improved by 20.1% for&lt;sup&gt;89&lt;/sup&gt;Zr.&lt;em&gt;Significance.&lt;em&gt;This study suggests that the TCP design has potential to improve high-energy&lt;/em&gt;ɣ&lt;/em&gt;imaging.&lt;/p&gt;
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