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(a) Attenuation coefficients of iodine, fibroglandular tissue, and adipose tissue in the energy range used in this study. (b) Diagram of laser‐Compton interaction. A well‐timed overlap of a laser pulse and an accelerated electron bunch will under Compton scattering to produce x‐rays in the direction of electron beam <t>propagation.</t> (c) Laser‐Compton intensity heat map with mean energy contours overlay. (d) Integrated laser‐Compton energy spectrum over different half‐angle collimations. More aggressive collimation blocks low energy photons at larger half‐angles resulting in decreasing energy bandwidth, but also causes lower overall flux.
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(a) Attenuation coefficients of iodine, fibroglandular tissue, and adipose tissue in the energy range used in this study. (b) Diagram of laser‐Compton interaction. A well‐timed overlap of a laser pulse and an accelerated electron bunch will under Compton scattering to produce x‐rays in the direction of electron beam <t>propagation.</t> (c) Laser‐Compton intensity heat map with mean energy contours overlay. (d) Integrated laser‐Compton energy spectrum over different half‐angle collimations. More aggressive collimation blocks low energy photons at larger half‐angles resulting in decreasing energy bandwidth, but also causes lower overall flux.
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(a) Attenuation coefficients of iodine, fibroglandular tissue, and adipose tissue in the energy range used in this study. (b) Diagram of laser‐Compton interaction. A well‐timed overlap of a laser pulse and an accelerated electron bunch will under Compton scattering to produce x‐rays in the direction of electron beam <t>propagation.</t> (c) Laser‐Compton intensity heat map with mean energy contours overlay. (d) Integrated laser‐Compton energy spectrum over different half‐angle collimations. More aggressive collimation blocks low energy photons at larger half‐angles resulting in decreasing energy bandwidth, but also causes lower overall flux.
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(a) Attenuation coefficients of iodine, fibroglandular tissue, and adipose tissue in the energy range used in this study. (b) Diagram of laser‐Compton interaction. A well‐timed overlap of a laser pulse and an accelerated electron bunch will under Compton scattering to produce x‐rays in the direction of electron beam <t>propagation.</t> (c) Laser‐Compton intensity heat map with mean energy contours overlay. (d) Integrated laser‐Compton energy spectrum over different half‐angle collimations. More aggressive collimation blocks low energy photons at larger half‐angles resulting in decreasing energy bandwidth, but also causes lower overall flux.
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(a) Attenuation coefficients of iodine, fibroglandular tissue, and adipose tissue in the energy range used in this study. (b) Diagram of laser‐Compton interaction. A well‐timed overlap of a laser pulse and an accelerated electron bunch will under Compton scattering to produce x‐rays in the direction of electron beam <t>propagation.</t> (c) Laser‐Compton intensity heat map with mean energy contours overlay. (d) Integrated laser‐Compton energy spectrum over different half‐angle collimations. More aggressive collimation blocks low energy photons at larger half‐angles resulting in decreasing energy bandwidth, but also causes lower overall flux.
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(a) Attenuation coefficients of iodine, fibroglandular tissue, and adipose tissue in the energy range used in this study. (b) Diagram of laser‐Compton interaction. A well‐timed overlap of a laser pulse and an accelerated electron bunch will under Compton scattering to produce x‐rays in the direction of electron beam <t>propagation.</t> (c) Laser‐Compton intensity heat map with mean energy contours overlay. (d) Integrated laser‐Compton energy spectrum over different half‐angle collimations. More aggressive collimation blocks low energy photons at larger half‐angles resulting in decreasing energy bandwidth, but also causes lower overall flux.
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(a) Attenuation coefficients of iodine, fibroglandular tissue, and adipose tissue in the energy range used in this study. (b) Diagram of laser‐Compton interaction. A well‐timed overlap of a laser pulse and an accelerated electron bunch will under Compton scattering to produce x‐rays in the direction of electron beam propagation. (c) Laser‐Compton intensity heat map with mean energy contours overlay. (d) Integrated laser‐Compton energy spectrum over different half‐angle collimations. More aggressive collimation blocks low energy photons at larger half‐angles resulting in decreasing energy bandwidth, but also causes lower overall flux.

Journal: Medical Physics

Article Title: Scanning K‐edge subtraction (SKES) imaging with laser‐compton x‐ray sources

doi: 10.1002/mp.17638

Figure Lengend Snippet: (a) Attenuation coefficients of iodine, fibroglandular tissue, and adipose tissue in the energy range used in this study. (b) Diagram of laser‐Compton interaction. A well‐timed overlap of a laser pulse and an accelerated electron bunch will under Compton scattering to produce x‐rays in the direction of electron beam propagation. (c) Laser‐Compton intensity heat map with mean energy contours overlay. (d) Integrated laser‐Compton energy spectrum over different half‐angle collimations. More aggressive collimation blocks low energy photons at larger half‐angles resulting in decreasing energy bandwidth, but also causes lower overall flux.

Article Snippet: The resulting angle‐correlated laser‐Compton x‐ray beam is propagated through digitally compressed breast phantoms containing iodine contrast‐enhanced inserts and then to a digital flat‐panel detector using a Matlab Monte Carlo propagation software.

Techniques: