2017
DOI: 10.1088/1361-6560/aa642c
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An analysis of beam parameters on proton-acoustic waves through an analytic approach

Abstract: It has been reported that acoustic waves are generated when a high-energy pulsed proton beam is deposited in a small volume within tissue. One possible application of proton-induced acoustics is to get real-time feedback for intra-treatment adjustments by monitoring such acoustic waves. A high spatial resolution in ultrasound imaging may reduce proton range uncertainty. Thus, it is crucial to understand the dependence of the acoustic waves on the proton beam characteristics. In this manuscript, firstly, an ana… Show more

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Cited by 16 publications
(18 citation statements)
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“…PGs are high energy gamma rays created by inelastic interactions between incident proton and target nuclei. PGs are emitted with decay time less than 1 ps and a broad energy spectrum (1)(2)(3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15). This approach faces two main challenges: (a) low detection efficiency due to the high energy of gamma rays; and (b) discrimination of PG signals from background noise originating from secondary neutrons.…”
Section: Introductionmentioning
confidence: 99%
“…PGs are high energy gamma rays created by inelastic interactions between incident proton and target nuclei. PGs are emitted with decay time less than 1 ps and a broad energy spectrum (1)(2)(3)(4)(5)(6)(7)(8)(9)(10)(11)(12)(13)(14)(15). This approach faces two main challenges: (a) low detection efficiency due to the high energy of gamma rays; and (b) discrimination of PG signals from background noise originating from secondary neutrons.…”
Section: Introductionmentioning
confidence: 99%
“…In this study, we assume that the proton beam is injected in a short period of time ( σ p = 30–500 ns), which is within the output range of fast-extraction synchrotron, fixed-field alternating gradient, dielectric wall and laser-driven accelerators 19 . Figure 2(a,b) show the transferred energy distributions on the z-x plane without and with the gold marker, respectively.…”
Section: Resultsmentioning
confidence: 99%
“…The width of beam pulse σ p was varied from 30 to 500 ns. To obtain a clear signal, the pulse width was chosen in the < μs range 18,19 , which fulfils the confinement conditions. Moreover, Z m was varied from 16 to 38 mm, which corresponds to a residual range of 15 mm and −7 mm for 60-MeV protons, respectively; the marker was therefore positioned at both pre- and post-Bragg peak regions in the tests.…”
Section: Methodsmentioning
confidence: 99%
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“…Note that the amplitude and temporal behavior of the resulting pressure field not only depend on the amplitude but also on the spatial distribution and temporal profile of the dose distribution. [8] To image the dose distribution, a set of 900 point receivers is homogeneous distributed in the plane z = 0. An example of a synthetically measured A-scan is displayed in Fig.…”
Section: Resultsmentioning
confidence: 99%