Evidence map›Paper›PMID 38558430›Full record

ArticleMedical physics2024

A four-grating interferometer for x-ray multi-contrast imaging.

Houxun Miao, James C Williams, Daniel Josell

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Article in Medical physics, 2024. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Not yet cited in PubMed.

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5 · Who and what money

Authors and funding

3 authors.

Houxun MiaoGeneral Optics, LLC, Zionsville, Indiana, USA.
James C WilliamsDepartment of Anatomy, Cell Biology & Physiology, Indiana University School of Medicine, Indianapolis, Indiana, USA.
Daniel JosellMaterials Science and Engineering Division, National Institute of Standards and Technology, Gaithersburg, Maryland, USA.

Funding

The Structural Basis of Kidney Stone FragilityR01DK059933 · NIDDK · INDIANA UNIV-PURDUE UNIV AT INDIANAPOLIS · PI WILLIAMS, JAMES C · 2004 to 2011
$2.4M
SkyScan 1172 High-resolution desk-top micro-CT systemS10RR023710 · NCRR · INDIANA UNIV-PURDUE UNIV AT INDIANAPOLIS · PI WILLIAMS, JAMES C · 2007 to 2007
$297k
NCRR NIH HHS S10 RR023710NIDDK NIH HHS R01 DK059933
6 · The paper itself

Abstract

backgroundX-ray multi-contrast imaging with gratings provides a practical method to detect differential phase and dark-field contrast images in addition to the x-ray absorption image traditionally obtained in laboratory or hospital environments. Systems have been developed for preclinical applications in areas including breast imaging, lung imaging, rheumatoid arthritis hand imaging and kidney stone imaging. PURPOSE: Prevailing x-ray interferometers for multi-contrast imaging include Talbot-Lau interferometers and universal moiré effect-based phase-grating interferometers. Talbot-Lau interferometers suffer from conflict between high interferometer sensitivity and large field of view (FOV) of the object being imaged. A small period analyzer grating is necessary to simultaneously achieve high sensitivity and large FOV within a compact imaging system but is technically challenging to produce for high x-ray energies. Phase-grating interferometers suffer from an intrinsic fringe period ranging from a few micrometers to several hundred micrometers that can hardly be resolved by large area flat panel x-ray detectors. The purpose of this work is to introduce a four-grating x-ray interferometer that simultaneously allows high sensitivity and large FOV, without the need for a small period analyzer grating.

methodsThe four-grating interferometer consists of a source grating placed downstream of and close to the x-ray source, a pair of phase gratings separated by a fixed distance placed downstream of the source grating, and an analyzer grating placed upstream of and close to the x-ray detector. The object to be imaged is placed upstream of and close to the phase-grating pair. The distance between the source grating and the phase-grating pair is designed to be far larger than that between the phase-grating pair and the analyzer grating to promote simultaneously high sensitivity and large FOV. The method was evaluated by constructing a four-grating interferometer with an 8 µm period source grating, a pair of phase gratings of 2.4 µm period, and an 8 µm period analyzer grating.

resultsThe fringe visibility of the four-grating interferometer was measured to be ≈24% at 40 kV and ≈18% at 50 kV x-ray tube operating voltage. A quartz bead of 6 mm diameter was imaged to compare the theoretical and experimental phase contrast signal with good agreement. Kidney stone specimens were imaged to demonstrate the potential of such a system for classification of kidney stones.

conclusionsThe proposed four-grating interferometer geometry enables a compact x-ray multi-contrast imaging system with simultaneously high sensitivity and large FOV. Relaxation of the requirement for a small period analyzer grating makes it particularly suitable for high x-ray energy applications such as abdomen and chest imaging.

Indexed as

InterferometryEquipment DesignX-Raysx‐ray gratingsx‐ray interferometerx‐ray multi‐contrast imaging

Identifiers

PMID38558430
PMCPMC11261508

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