Physics of Stereotactic Radiosurgery and Stereotactic Body Radiotherapy


Characteristic

Conventional RT

SRS/ SBRT

Prescription dose per fraction

≤3 Gy

≥5 Gy

Number of fractions

≥10

≤5

Dose distribution

Homogeneous (max PTV dose ≈105–110 %)

Heterogeneous (max PTV dose ≈110–200 %)a

Dose gradient outside PTV

Shallow slope

Steep slope

Prescription isodose line

≈90–95 %

≈50–95 %a

Target definition

Tumor might not have a sharp boundary

Well-delineated target

PTV margin

≈cm

≈mm


Modified from Linda Hong’s presentation (Benedict et al. 2010; Hong 2012)

aHeterogeneity of SRS /SBRT plans is highly dependent on the treatment technique used. The same applies to the prescription isodose line s




  • Patient setup and immobilization device s vary depending on body site, treatment platform, and the capability of the delivery system to detect and correct for changes in patient position during treatment.


  • The stereotactic coordinate system is provided either by an invasive fixation device (head frame ) or by the imaging system (frameless radiosurgery ).



    • SRS : Stereotactic head frame attached to the patient’s skull using pins (Khan 2003). Frameless system could include thermoplastic mask with reflective markers and vacuum-assisted mouthpieces.


    • SBRT : body frame s, body cast , and vacuum bags (Table 3.2).


      Table 3.2
      Reported accuracy of commercially available SBRT immobilization device s (Taylor et al. 2011)










































      Site

      System

      Reported accuracy (mm)

      Lung

      Elekta body frame

      1.8–5

      MI body fix

      2.5–3

      Leinbinger body frame

      2–4.4

      Liver

      Elekta body frame

      ≤4.4

      MI body fix

      ≤3.2

      Leinbinger body frame

      1.8–4.4

      Spine

      MI body fix

      ≈1

      Body cast

      ≈3

      Fiducial marker tracking

      2


  • Imaging techniques for SRS /SBRT treatment verification (Murphy et al. 2007; German et al. 2001; Broderick et al. 2007; Li et al. 2008; Jin et al. 2008): 2D MV electronic portal imaging (EPID) .



    • Orthogonal kV radiographs.


    • MV cone beam CT.


    • kV cone beam CT .


    • MV helical CT.


    • In-room diagnostic CT.


    • 4DCBCT.


    • Infrared imaging .


    • Radiofrequency tracking .


  • Management of respiratory motion for SBRT motion-encompassing techniques (4DCT—ITV delineation).



    • Abdominal compression—this method reduces the target excursion with breathing.


  • Breath-hold—radiation is delivered when the patient is holding the breath.


  • Gating —radiation is delivered only at a particular phase of respiration.


  • Dynamic target tracking—beams are re-targeted in real time to the continuously changing target position—advantages: no need for ITV expansion; no treatment interruptions; accounts for changes in target motion and respiratory pattern during treatment.




      SRS/SBRT Treatment Parameters



      • Target volumes: The concept of GTV , CTV , PTV , and ITV described in ICRU 50 and 62 for SRS also applies to SBRT planning (Medin et al. 2010; ICRU 1993). PTV margins depend on body site, treatment device, localization technique, and imaging frequency. Typical margins range from 2 to 5 mm for SBRT.


      • Dose conformity: the high-dose volume conforms tightly around the target.


      • Dose heterogeneity : hot spots located within the target are often considered not only acceptable, but also desirable. The prescription dose is typically 50–90 % of the maximum dose depending on the treatment delivery and treatment planning systems.


      • Dose gradient : the dose fall-off away from the target is steep. The volume of normal tissue receiving high doses of radiation is kept at a minimum. This is in comparison with other treatment techniques like 3D conformal.


      • Beam energy: 6 MV photons offer the best compromise between beam penetration and penumbra characteristics. Many techniques use unflattened beams .


      • Beam shaping: Radiation is collimated to a small field using heavy metal cones (circular field 4–60 mm diameters), multileaf collimator (MLCs), or microMLCs (2.5 mm leaves width). MLCs and micro MLCs are used to deliver treatments developed with conformal beams, intensity modulated fields, dynamic conformal arcs , or a combination of these (ICRU 1999).


      • Treatments are delivered via coplanar and non-coplanar beam arrangements.


      • Circular fields provide a sharper penumbra than microMLCs.


      • Beam geometry: multiple non-overlapping beams concentrically pointing to the target; 5–12 coplanar or non-coplanar beams; 1 or 2 coplanar or non-coplanar arcs; a continuously rotating fan beam; hundreds of non-coplanar pencil beams pointing to different parts of the target (non-isocentric beam arrangement) or to the same point (isocentric beam arrangement).


      Plan Optimization



      • Forward planning : the user manually adjusts beam arrangement, field shapes, and weights until the desirable dose distribution is achieved.


      • Inverse planning : the user specifies plan objectives for target and normal structures and a dose optimization algorithm calculates field shapes and weights based on the minimization of a mathematical cost function.


      Plan Classification



      • 3-Dimensional conformal radiation therapy (3D-CRT ): typically forward planned. It might be advantageous for moving targets, as the target is always in the open radiation field.


      • Intensity-modulated radiation therapy (IMRT ): typically inverse planned (although the field-in-field technique is forward planned).


      • Arc therapy (RapidArc , VMAT ).


      Dose Calculation Algorithms



      • Pencil beam algorithms using radiological path length corrections to account for tissue heterogeneities. Not accurate in conditions of electronic disequilibrium . In these cases, heterogeneity corrections explicitly accounting for the transport of secondary electrons must be employed. While the most accurate technique for dose calculation is Monte Carlo , convolution-superposition methods are sufficiently accurate in most clinical situations.


      • Calculation grid : should be less than 2 × 2 × 2 mm3.




      Treatment Platforms and Cross-Platform Comparisons






      • SRS /SBRT treatments can be performed using a variety of devices producing X rays, gamma rays or particle radiation (Tables 3.3 and 3.4) (Combs et al. 2012; Dieterich and Gibbs 2011; Soisson et al. 2006):


        Table 3.3
        Characteristics of various platforms for SRS /SBRT






































        Technology

        Delivery system

        Radiation

        Dose rate

        Beam shaping

        CyberKnife

        Compact linac mounted on a robotic arm

        6 MV unflattened photon beam

        Up to 1000 MU/min

        12 Interchangeable tungsten cones; variable aperture collimator; MLC (not yet clinically available)

        Tomotherapy

        Helical, CT-like gantry equipped with a linac waveguide

        6 MV unflattened photon beam

        ~850 cGy/min at isocenter

        Binary MLC (64 leaves, 0.625 cm wide)

        Gamma knife

        192 (Perfexion) or 201 (models B-4C) 60Co sources

        1.17 and 1.33 MeV gamma rays

        Initial source activity ~6000 Ci, dose-rate at focal point >3 Gy/min

        Tungsten barrel subdivided into 8 sectors (Perfexion) ; 4 interchangeable helmets (models B-4C)

        Linac-based systems

        Gantry-based linac rotating about the isocenter

        Multiphoton energies (6, 10, 15, 18 MV-flattened and unflattened) and electron energies

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        Sep 16, 2016 | Posted by in GENERAL RADIOLOGY | Comments Off on Physics of Stereotactic Radiosurgery and Stereotactic Body Radiotherapy

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