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Proton Therapy System PROBEAM ® Protons have potential advantages over photons for delivering higher radiation doses to the tumor while sparing the surrounding healthy tissue. Though protons are inherently capable of higher dose conformity and lower integral dose to the body, the method of proton beam delivery is an important consideration as well. Beam delivery methods Two proton beam delivery methods are available today: passive spreading, which includes single and dual scattering, and active spreading, which is commonly known as scanning. In passive spreading techniques, the proton beam is spread by placing scattering material in its path. A single scatterer broadens the beam sufficiently for the coverage of small fields. For larger fields, a second scatterer is needed to ensure a uniform dose profile. A combination of custom-made collimators and compensators conform the dose to the target volume. The spread out Bragg peak (SOBP) used for treatment is obtained by a set of range modulator wheels or ridge filters inside the gantry of the delivery system. (See Figure 1.) In scanning beam techniques, magnets deflect and steer the proton beam. Under computer control, the beam “paints” the treatment volume, voxel by voxel, in successive layers. The depth of penetration of the Bragg peak is adjusted by varying the energy of the beam before it enters the gantry. (See Figure 2.) PROTON BEAM THERAPY SCATTERING VERSUS SCANNING TREATMENT TECHNIQUES Figure 2: Scanning diagram Magnets Treatment volume Modulator wheels or ridge filters Scatterer Scatterer (contoured) Collimator Compensator Target Extra dose Patient Figure 1: Scattering diagram
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Page 1: PROTON BEAM THERAPY SCATTERING VERSUS … BEAM THERAPY SCATTERING VERSUS ... proton therapy using spot scanning. International Journal ... Not all features or products are available

Proton Therapy SystemPROBEAM®

Protons have potential advantages over photons for delivering higher radiation doses to the tumor while sparing the surrounding healthy tissue. Though protons are inherently capable of higher dose conformity and lower integral dose to the body, the method of proton beam delivery is an important consideration as well.

Beam delivery methodsTwo proton beam delivery methods are available today: passive spreading, which includes single and dual scattering, and active spreading, which is commonly known as scanning.

In passive spreading techniques, the proton beam is spread by placing scattering material in its path. A single scatterer broadens the beam sufficiently for the coverage of small fields.

For larger fields, a second scatterer is needed to ensure a uniform dose profile. A combination of custom-made collimators and compensators conform the dose to the target volume. The spread out Bragg peak (SOBP) used for treatment is obtained by a set of range modulator wheels or ridge filters inside the gantry of the delivery system. (See Figure 1.)

In scanning beam techniques, magnets deflect and steer the proton beam. Under computer control, the beam “paints” the treatment volume, voxel by voxel, in successive layers. The depth of penetration of the Bragg peak is adjusted by varying the energy of the beam before it enters the gantry. (See Figure 2.)

PROTON BEAM THERAPY SCATTERING VERSUS SCANNING TREATMENT TECHNIQUES

Figure 2: Scanning diagram

Magnets

Treatment volume

Modulator wheels or ridge filters

Scatterer

Scatterer (contoured)

Collimator Compensator

Target

Extra dose

Patient

Figure 1: Scattering diagram

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How do these two delivery methods compare in a clinical setting? Are there differences in the conformity of the treatment, or the integral dose to patients? What should centers consider when choosing a proton therapy system? The following table addresses these questions through a side-by-side comparison of scattering versus scanning to help clinicians determine the most appropriate treatment method.

SCATTERING SCANNING

Beam modifying devices

Dual scattering uses patient-specific beam-modifying devices to conform the dose to the treatment volume. These devices must be manufactured in-house or outsourced, increasing the cost of treatment. Treatment cannot begin until the devices are ready. The devices, which become radioactive from contact with the proton beam, must be stored for months, necessitating a rather large dedicated storage area. This requirement increases facility costs without contributing to revenue.

In most cases, scanning does not require any collimators, compensators, or other beam-modifying devices. A narrow mono-energetic beam paints the target volume in layers, steered by magnets. Varying the energy of the beam controls the depth of each layer.

Typically with scanning, there are no modifying devices to custom-make or store after treatment.

Secondary radiation

Dual scattering generates neutrons when the beam hits the scattering material or the beam-modifying devices. This secondary radiation increases the integral radiation dose to the patient. Any radiation that does not directly contribute to destroying cancer cells is undesirable.

Without scattering material, scanning naturally produces fewer neutrons and reduces the integral dose to the patient.

Low integral dose

Dual scattering may deposits some unnecessary dose in tissues proximal to the treatment volume. This occurs because the spread of the Bragg peak is constant across the treated depth. This may make it difficult to optimally cover the target volume while sparing the healthy tissue. Using multiple fields is not an ideal solution in these cases; switching the complex set of compensators and apertures required increases the treatment time. Figure 3 shows the hot areas of unwanted dose in a dual-scattering proton plan.

The smaller the treatment volume and the lower the integral dose, the better the patient is likely to tolerate treatment. Typically, proton therapy delivers lower doses to healthy tissue than external beam therapy with X rays, and scanning delivers lower dose than other proton delivery methods. Figure 4 shows a scanning proton plan for the same treatment volume as shown in Figure 3, without the extraneous radiation of the dual-scattering plan.

✪ Indicates advantage

Figure 3: Dual-scattering proton plan

Extra dose

Proton beam

Figure 4: Scanning proton plan

Proton beam

SCATTERING VERSUS SCANNING AT A GLANCE

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SCATTERING SCANNING

IMPT

With dual scattering, the ability to vary the dose distribution throughout the treatment volume is limited. Multiple fields can deposit dose from different directions. However, multiple fields require a complex set of compensators and apertures, and switching them adds to the treatment time.

Scanning makes IMPT possible. With scanning, dose distributions can be varied voxel by voxel. By varying the beam intensity or the speed of the scan, or both, dose is painted non-uniformly on a field-by-field basis to yield an overall uniform target dose. The scanning technique lets clinicians tailor treatments to improve dose conformity, reduce integral dose, or both.

Sensitivity to organ motion

Proton therapy poses the same challenges for accurate, repeatable patient positioning and setup as IMRT. In addition, bony structures moving in and out of the beam alter the range of the Bragg peak. The target volume and surrounding structures must be in their planned positions. This is true for all proton therapy techniques. However, scattering is more forgiving of tumor and organ motion because of the smearing effect of the broadened beam.

Patient positioning and immobilization are important in all conformal radiation treatments. However, the enhanced ability with proton scanning to paint dose more conformally, voxel by voxel, increases the risk of target misses due to organ motion. This risk can be mitigated by image-guidance techniques. Multiple re-paintings can also compensate for organ motion by effectively smearing out the dose.

Simplicity versus complexity

Dual scattering is less complex than scanning. There are fewer variables to consider in planning. The beam is shaped to the target volume by using apertures and compensators (bolus).

With scanning, clinicians have more flexibility to shape the beam. With this sophisticated capability comes increased complexity in planning, computation, and equipment.

Depth of proton penetration

When protons encounter scattering material and beam-modifying devices, they lose energy and, with it, penetrating power. For any given accelerator, scattering reduces the depth of the Bragg peak that can be obtained.

With scanning, there are no scatterers or beam-modifying devices in the way to reduce the energy of the proton beam. For any given accelerator, scanning penetrates deeper than scattering. The result: scanning can treat deeper seated tumors.

✪✪

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VARIAN PROTON THERAPY

Varian stakes its global reputation on giving patients and clinicians innovative treatment technology for fighting cancer. Our mission is to help save more lives, improve the quality of treatment, and provide solutions for treating a wide range of cancers. Proton therapy is one weapon in Varian’s advanced treatment arsenal, and we intend to drive its development forward as we have other modes of radiation treatment. Our pledge is this: when you want sophisticated, advanced treatments, you can turn to Varian.

ReferencesBlom M, Glimelius B, Lorin S, Medin J, Tilly N, Grusell E. Development of a scanning system for proton therapy in Uppsala. In: Proceedings of the 6th European Particle Accelerator Conference, Stockholm, Sweden. 1998: 2450-2451 http://accelconf.web.cern.ch/AccelConf/e98/PAPERS/WEP02C.PDF. Record created 2005-07-27, last modified 2006-12-03. Accessed: March 9, 2010.

Lomax A. TU-C-BRA-01: An Overview of Proton Therapy. Med. Phys. 2007; 34:6:2552-2552.

Pagnetti H, Bortfield T. Proton Therapy. In W. Schlegel, T. Bortfield, A-L. Grosu, eds. New Technologies in Radiation Oncology (Medical Radiology Series). Heidelberg: Springer Verlag; 2005: 345-365.

Pedroni E. Latest Developments In Proton Therapy. In: Proceedings of the 7th European Particle Accelerator Conference, Vienna, Austria. 2000, Vienna, Austria http://accelconf.web.cern.ch/AccelConf/e00/PAPERS/WEXF102.pdf Accessed: March 9, 2010.

Schneider U, Agosteo S, Pedroni E, Besserer J. Secondary neutron dose during proton therapy using spot scanning. International Journal of Radiation Oncology * Biology * Physics. 2002; 53:1:244-251.

Shinohara E, The Abramson Cancer Center of the University of Pennsylvania. Module 7: Treatment Volumes and Treatment Planning in Proton Therapy. Oncololink. http://www.oncolink.org/treatment/article.cfm?c=9&s=131&id=418 Last modified: March 18, 2009. Accessed: March 9, 2010.

Specifications subject to change without notice. Not all features or products are available in all markets.

Intended Use Summary The Varian ProBeam Proton Therapy System provides protons for precision radiotherapy of lesions, tumors, and conditions anywhere in the body where radiation treatment is indicated.

Safety Radiation treatments may cause side effects that can vary depending on the part of the body being treated. The most frequent ones are typically temporary and may include, but are not limited to, irritation to the respiratory, digestive, urinary or reproductive systems, fatigue, nausea, skin irritation, and hair loss. In some patients, they can be severe. Treatment sessions may vary in complexity and time. Radiation treatment is not appropriate for all cancers.

Particle Therapy Varian Particle Therapy GmbH

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© 2010, 2011, 2014 Varian Medical Systems, Inc. All rights reserved. Varian and Varian Medical Systems are trademarks of Varian Medical Systems, Inc. All other trademarks are the property of their respective owners.

RAD 10114C 09/2014

Proton Therapy SystemPROBEAM®


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