Proton and carbon ion therapy by C-M Charlie Ma, Tony Lomax PDF

By C-M Charlie Ma, Tony Lomax

ISBN-10: 1439816077

ISBN-13: 9781439816073

"Preface: This ebook goals at offering a entire and useful consultant to proton and carbon ion treatment for a extensive diversity of team of workers in clinical physics and radiation remedy, together with scientific physicists, radiation oncologists, dosimetrists, therapists, clinical engineers, and trainees in those disciplines. The scope of this ebook comprises physics and radiobiology fundamentals of proton and ion beams, dosimetry methods Read more...

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Extra resources for Proton and carbon ion therapy

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8 Summary . . . . . . . . . . . . . . . 9 Context within the Particle Therapy Facility. . 26 References. . . . . . . . . . . . . . . . . 1 Introduction From 1895, when Roentgen discovered X-rays, to 1913, when Coolidge developed the vacuum X-ray tube, it has been shown that energetic particles can be useful for medical applications. 1 summarizes some of these applications, including the particles used and the energy range required. It is clear that there is a wide range of applications and, therefore, also a wide range of requirements for the particles that must be considered.

D) Insertable blocks with different thicknesses. (e) Rotatable Plexiglass curved wedge. (f) Adjustable multi­ wedge design. The beam is indicated at each degrader type. the beam diameter. , a stack of thin plates or a thinner wedge) is needed. 4c). A small fixed counterwedge is mounted close to the beam exit side of the degrader. The system is mounted in air. At PSI and in the Varian systems (van Goethem et al. 4f ) so that the travel distance between the maximum and the minimum energy setting is short.

The calculations have been performed with TURTLE. (U. Rohrer 2006b, PSI Graphic turtle framework based on a CERN-SLAC-FERMILAB version by K. L. 5%–±1%) can be accepted. 9 displays the influence of momentum spread on Bragg peaks for eye treatments, as well as for treatments of deep-seated tumors. 25% at the slits. 5%. 5 and 1% FWHM. ) where M is the magnification of the image of the beam size–defining collimator, radius rcol, x′ is the divergence of the beam behind the degrader, R12 is a coefficient representing a possible defocusing, D is the dispersion (in millimeters per percentage) at the dispersive focus, and σP /P is the relative width (in percentage) of the momentum distribution of the beam.

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Proton and carbon ion therapy by C-M Charlie Ma, Tony Lomax


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