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Yue Yan Prof. Bhudatt Paliwal 10/24/2014

Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

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Page 1: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Yue YanProf. Bhudatt Paliwal 10/24/2014

Page 2: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Background Motivation Preliminary studies

• Clinical comparison• Monte-Carlo (MC) simulation• Measurement test

Conclusion Questions and answers

2

Page 3: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Flattening filter (FF) has been applied as an essential part of Linac

system over decades.

The development of modern RT makes the FF no longer an

indispensable part of Linac system.

The potential clinical application of the FFF bremsstrahlung photon

beams generated by modern Linacs is becoming much more

apparent[1-12].

However, limitations still exist for the FFF beam.

3

Page 4: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Pros of FFF• Greatly increased dose rate (approx. 2-4 times compared with the

flattened beam)[2-5,9].

• Large decrease of external scatter from the gantry head[6].

• Greatly reduced neutron contamination for high energy photon beams[7].

• Reduced uncertainty in dose calculation due to scatter from the FF[8]. Cons of FFF

• High dose rate of the FFF beam is more likely to lead to unacceptable

dose deviation caused by intrafraction patient motion during treatment

delivery[1].

• Soft spectrum of the FFF beam tends to increase the internal patient

scatter to peripheral organs[9-12].

4

Page 5: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Internal patient scatter is the predominate factor

contributing to peripheral organ dose[12].

External head scatter and dose leakage from the gantry

head also contribute smaller amounts to peripheral

organ dose.

5

Page 6: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

The hypothesis: Dose to OARs can be further reduced by attenuating the soft

photons in the FFF beam spectrum.

6

FFF Beam Flattened BeamLow head scatter High head scatter from the flattening filter

Soft spectrum Hard spectrum

High dose rate Low dose rate

Increased internal scatter due to soft photons Increased internal scatter due to dose normalization

Lower tail dose in the beam profile Higher tail dose in the beam profile

SPECTER

In general, lower mean dose to the OARs In general, higher mean dose to the OARs

Page 7: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Adjusting both the beam spectra and the profile to yield a more hardened SPECTER beam could reduce the internal patient scatter and reduce the dose to OARs for the FFF beam.

7

Page 8: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Clinical comparison (cont…):• Treatment plans study summary:

8

Category Beam ModalityDelivery

TechniqueTreatment Schedule OARs

Head and Neck

6 MV and 10 MVFlattened beam &

FFF Beam

Static IMRT&

VMAT

60 Gy/30 frac. (2 pts.)30 Gy/15 frac. (1 pt.)70 Gy/28 frac. (1 pt.)

spinal cord, brainstem,

brain, larynx, pharynx, parotid

Lung45 Gy/30 frac. (1 pt.)66 Gy/33 frac. (2 pts.)60 Gy/30 frac. (1 pt.)

lungs, spinal cord, heart,

larynx, thyroid, esophagus

Prostate 70 Gy/28 frac. (3 pts.)78 Gy/39 frac. (1 pt.)

rectum, bladder, hips

Breast(RTOG 1005)[13]

Static IMRT50 Gy/25 frac.

12 Gy/6 frac. (1 pt.) (sequential boost)

lungs, heart, thyroid, skin

Page 9: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Clinical comparison (cont…):• Normalization: 95% @95% to exclude lower-

mean-dose effect to the target of the FFF beam compared with the

flattened beam.

• TrueBeam (Varian, CA) system was commissioned on Eclipse®

(Varian, Palo Alto, Medical Systems) TPS workstation.

• Anisotropic Analytical Algorithm (AAA) was used to calculate the

dose.

• Treatment parameters (e.g. field size, arc number, beam angle)

were kept to be identical to exclude differences from these factors.

• Clinical objectives were used to simulate clinical application.

9

Page 10: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Clinical comparison (cont…): head and neck (case 7):o Dashed line: FFF beam; solid line: flattened beam

10

VMAT Plans

IMRT Plans

Page 11: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Clinical comparison (cont…):

11

Dose and NTCP Ratios(FFF/flattened) for Head and Neck Cancer CasesVMAT

6 MV 10 MV

Organs' name Mean dose ratio

Max dose ratio

Mean BED ratio NTCP ratio Mean dose

ratioMax dose

ratioMean BED

ratio NTCP ratio

Larynx 0.98±0.02 0.99±0.02 0.97±0.02 0.84±0.20 0.97±0.04 1.00±0.01 0.97±0.05 0.87±0.19R parotid 0.94±0.03 0.96±0.02 0.93±0.03 0.31±0.20 0.91±0.04 0.96±0.05 0.91±0.04 0.24±0.27

R submandibular 0.97±0.02 0.98±0.00 0.96±0.02 0.64±0.03 0.92±0.04 0.96±0.04 0.91±0.04 0.28±0.14L cochlea 0.97±0.04 0.98±0.04 0.97±0.05 0.71±0.48 0.94±0.06 0.95±0.06 0.93±0.07 0.43±0.40

IMRT

6 MV 10 MV

Organs’ name Mean dose ratio

Max dose ratio

Mean BED ratio NTCP ratio Mean dose

ratioMax dose

ratioMean BED

ratio NTCP ratio

Larynx 1.02±0.02 1.02±0.01 1.03±0.02 1.57±0.39 1.02±0.01 1.02±0.01 1.02±0.01 1.42±0.25R parotid 1.00±0.02 1.01±0.01 1.00±0.02 0.95±0.47 0.99±0.04 1.00±0.02 0.99±0.04 0.89±0.72

R submandibular 1.00±0.04 1.00±0.01 1.00±0.05 1.21±0.75 1.04±0.02 1.02±0.02 1.05±0.02 1.74±0.15L cochlea 0.98±0.03 1.00±0.07 0.98±0.04 1.32±1.29 1.00±0.03 1.02±0.08 1.00±0.05 2.18±2.25

Page 12: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Clinical comparison (cont…):

12

MU for Head and Neck Cancer CasesEnergy 6 MV 10 MV

Delivery Method VMAT IMRT VMAT IMRT

Beam Modality Flattened FFF Flattened FFF Flattened FFF Flattened FFF

Total MUs

Case 5 559 640 2117 3072 545 674 2001 3633

Case 7 812 959 1726 2647 780 1011 1655 3128

Case 8 605 757 965 1292 581 801 883 1380

Case 10 390 459 916 1323 373 483 873 1773

Case 24 389 430 803 1254 370 427 768 1758MU Ratio

(FFF/Flattened) 1.17±0.05 1.47±0.09 1.27±0.08 1.92±0.27

Page 13: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Clinical comparison (cont…):• Summary and discussion:

The differences between the FFF beam and the flattened beam are more

obvious in VMAT plans compared with the static IMRT plans.

Maximum dose rates may not be achievable for the FFF beam plans in

general due to MLC speed limitation.

In certain clinical cases with large field sizes (~16 20 ), the FFF

beam tends to provide higher dose to OARs compared with the flattened

beam in the static IMRT plans.

The FFF beam plans uses higher MU to provide the same target

coverage compare with the flatted beam plans.

In general, FFF beam provides lower mean dose to OARs compared with

the flattened beam.

13

Page 14: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Monte-Carlo study:• Detailed geometry information is necessary to accurately simulate

the TrueBeamTM system (Varian, CA).

• Varian provided the IAEA (International Atomic Energy

Agency)phase space data above the jaws inside the gantry head.

14(http://sudentas.com/tag/truebeam) (TrueBeam Monte Carlo Data Package, Varian Medical System)

Page 15: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Monte-Carlo study (cont…):• VirtuaLinac web interface based on Amazon Web Services (AWS) system enables

us to consider the geometry of the jaws inside the gantry head[17,18].

• Based on the new IAEA phase space data, BEAMnrc MC software package was

used to simulate the TrueBeam system.

15

Page 16: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Monte-Carlo Study (cont…):• Excellent agreements were obtained between the MC simulation

and the standard measurement data.

16

10

Page 17: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Monte-Carlo study (cont…):• Dose profile normalization: 6 MV beams

17

Page 18: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Monte-Carlo study (cont…):• Dose normalization: 6 MV and 10 MV beams

18

6 MV

Page 19: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Monte-Carlo study (cont…):• A soft-spectrum-filter (SPECTER) is proposed to attenuate the soft

photons in the FFF spectrum.

• The low density of the SEPCTER in the central axis (filled with air)

enables us to keep the high dose rate of the FFF beam.

19

Page 20: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Monte-Carlo study (cont…):• Different designs of the SPECTER: (gantry head z=58 cm.)

20

21 cm18.3 cm

15.4 cm

12.5 cm

9.6 cm

6.7 cm

21 cm

18.3 cm

15.4 cm

12.5 cm

9.6 cm

6.7 cm

18.3 cm

15.4 cm

12.5 cm

9.6 cm

6.7 cm

18.3 cm

15.4 cm

12.5 cm

9.6 cm

6.7 cm

Page 21: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Monte-Carlo study (cont…): • Steps to calculate the internal scatter[12,19]:

.

• Boundary of the central region was slightly larger than the field

size.

21

Page 22: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Monte-Carlo study (cont…): beam fluence

22

All MC simulations after this slice were based on the lead circularcross section SPECTER.

Page 23: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Monte-Carlo study (cont…):• The SPECTER beam reduced the total dose and the internal scatter compared

with the FFF beam.

23

25 25 , 10 40 40 , 10

Page 24: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Measurement results:• Two SPECTERs were made using lead and tin.

• Cross sections were square.

• The heights were chosen to be 6 for lead and 1.5 for tin.

24

Page 25: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Measurement results (cont…):• Lead SPECTER provides better dose reduction effect compared

with tin, due to higher attenuation of the soft photons of lead.

25

Field sizes from left to right: 3 3, 5 5, 10 10, 15 15,20 20, 25 25 . 10 . Solid line: FFF beam,dashed lines with and without dots: SPECTER beamswith square cross section. Dashed line without dots: leadSPECTER; dashed line with dots: tin SPECTER.

Measurement Results

Field size is chosen to be 25 25 . Solid line: FFF beam,dashed lines with and without dots: SPECTER beamswith square cross section. Dashed line without dots: leadSPECTER; dashed line with dots: tin SPECTER.

Page 26: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Measurement results (cont…):• However, the MC simulation did not agree with the measurement

data in the tail region.

• It can be explained by the over-responding of the Profiler(Sun

Nuclear, Melbourne, FL)[21].

26

Page 27: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

Conclusion:• The SPECTER beam has potential to reduce the internal scatter

and improve the dose sparing effect to OARs.

• The low density in the central axis of SPECTER provides high

dose rate compared with the flattened beam.

• Attenuating the soft photons in the FFF beam spectrum may not

lead to prolonged treatment time compared with the FFF beam due

to the speed limitation of the MLCs.

• Geometry and material are important for the design of the

SPECTER.

27

Page 28: Yue Yan Prof. Bhudatt Paliwal - AAPM Chapterchapter.aapm.org/nccaapm/z_meetings/2014-10-23_and... · 23.10.2014  · Pros of FFF • Greatly increased dose rate (approx. 2-4 times

1. Ong CL, Dahele M, Slotman BJ and Verbakel FFAR. (2013) Dosimetric Impact of the Interplay Effect During Stereotactic Lung Radiation Therapy Delivery Using Flattening Filter-Free Beams and Volumetric Modulated Arc Therapy. Int J Radiat Oncol Biol Phys 86(4): 743-748.

2. Huang YF, Siochi RA, Bayouth JE. (2012) Dosimetric properties of a beam quality-matched 6 MV unflattened photon beam. J Appl Clin Med Phys 13(4):71-81.

3. Vassiliev ON, Titt U, Kry SF, Pönisch F, Gillin MT and Mohan R. (2006) Monte Carlo study of photon fields from a flattening filter-free clinical accelerator. Med Phys 33(4):820-827.

4. Reggiori G, Mancosu P, Castiglioni S, Alongi F, Pellegrini C, Lobefalo F, Catalano M, Fogliata A, Arcangeli S, Navarria P, Cozzi L and Scorsetti M. (2012) Can volumetric modulated arc therapy with flattening filter free beams play a role in stereotactic body radiotherapy for liver lesions? A volume-based analysis. Med Phys 39(2):1112-1118.

5. Titt U, Vassiliev ON, Pönisch F, Dong L, Liu H and Mohan R. (2006) A flattening filter free photon treatment concept evaluation with Monte Carlo. Med Phys 33(6):1595-1602.

6. Cashmore J, Ramtohul M and Ford D. (2011) Lowering whole-body radiation doses in pediatric intensity-modulated radiotherapy through the use of unflattened photon beams. Int J Radiat Oncol BiolPhys 80(4):1220-1227.

7. Kry SF, Titt U, Pönisch F, Vassiliev ON, Salehpour M, Gillin M, Mohan R. (2007) Reduced neutron production through use of a flattening-filter-free accelerator. Int J Radiat Oncol Biol Phys 68(4):1260-4.

8. Georg D, Knöös T and McClean B. (2011) Current status and future perspective of flattening filter free photon beams. Med Phys 38(3):1280-1293.

9. Kry SF, Vassiliev ON and Mohan R. (2010) Out-of-field photon dose following removal of the flattening filter from a medical accelerator. Phys Med Biol 55 2155-2166.

10. Kragl G, Baier F, Lutz S, Albrich D, Dalaryd M, Kroupa B, Wiezorek T, Knöös T, Georg D. (2011) Flattening filter free beams in SBRT and IMRT: Dosimetric assessment of peripheral doses. Z Med Phys21 91-101.

11. Wang YN, Khan MK, Ting JY, Easterling SB. (2012) Surface dose investigation of the flattening filter-free photon beams. Int J Radiation Oncol Biol Phys 83(2):e281-e285.

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12. Chofor N, Harder D, Willborn KC and Poppe B. (2012) Internal scatter, the unavoidable major component of the peripheral dose in photon-beam radiotherapy. Phys Med Biol 57 1733-1743.

13. Vicini FA, Freedman GM, White JR, Arthur DW, Haylard M, Taghian A, Hayman J, Rosenstein B, Bentzen SM, Li XA, Bleicher RJ and Winter K. A Phase III trial of accelerated whole breast irradiation with hypofractionation plus concurrent boost versus standard whole breast irradiation plus sequential boost for early-stage breast cancer RTOG 1005 (unpublished).

14. Dhabaan A, Elder E, Schreibmann E, Crocker I, Curran WJ, Oyesiku NM, Shu H-K, Fox T. (2010) Dosimetricperformance of the new high-definition multileaf collimator for intracranial stereotactic radiosurgery. J Appl ClinMed Phy 11(3):197-211.

15. Zhang GG, Ku L, Dilling TJ, Stevens CW, Zhang RR, Li WQ and Feygelman V. (2011) Volumetric modulated arc planning for lung stereotactic body radiotherapy using conventional and unflattened photon beams: a dosimetric comparison with 3D technique. Radiat Oncol 6:152.

16. Gay HA, Niemierko A. (2007) A free program for calculating EUD-based NTCP and TCP in external beam radiotherapy. Phys Medica 23:115-125.

17. J. F. Fowler. (1989) The linear-quadratic formula and progress in fractionated radiotherapy The British journal of radiology 62:679-694.

18. Constantin M, Perl J, LoSasso T, Salop A, Whittum D, Narula A, Svatos M and Keall PJ. (2011) Modeling the TrueBeam linac using a CAD to Geant4 geometry implementation: Dose and IAEA-compliant phase space calculations. Med Phys 38(7):4018-4024.

19. Constantin M, Constantin D E, Keall P J, Narula A, Svatos M, and Perl J. (2010) Linking computer-aided design (CAD) to Geant4-based Monte Carlo simulations for precise implementation of complex treatment head geometries, Phys Med Biol 55 N211-20.

20. Chofor N, Harder D, Willborn K, Rühmann, A and Poppe B. (2011) Low-energy photons in high-energy photon fields – Monte Carlo generated spectra and a new descriptive parameter. Z Med Phys 21 183-197.

21. Sun Nuclear Cooperation, Diodes versus Ion Chambers. 22. Agostinelli S et al. (2003) Geant4—a simulation toolkit. Nucl Instrum Methods Phys Res A 506 250-

303; see also http:// http://geant4.cern.ch/geant4/.

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