what’s next after imrt and vmat ? - digital linac therapy...

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1 @01-258_via99-011_hepatoma_onscreen Director of Radiation Physics Division Department of Radiation Oncology & MIPS Stanford University School of Medicine Lei Xing , Ph.D. & Jacob Haimson Professor What’s next after IMRT and VMAT ? - Digital LINAC - Beam level imaging & imaging of RT beams - Station parameter optimized radiation therapy (SPORT ) - New QA tools for emerging RT technologies Ruijiang Li, Karl Bush, Benjamin Fahimian, Dimitre Hristov, Victor Yu, Bin Han, Gary Luxton National Cancer Institute & Varian Medical Systems

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Page 1: What’s next after IMRT and VMAT ? - Digital LINAC therapy ...amos3.aapm.org/abstracts/pdf/90-25503-334462-103365.pdf · •What’s next after IMRT and VMAT ? - Digital LINAC -

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Director of Radiation Physics Division

Department of Radiation Oncology & MIPS

Stanford University School of Medicine

Lei Xing , Ph.D. & Jacob Haimson Professor

• What’s next after IMRT and VMAT ?

- Digital LINAC

- Beam level imaging & imaging of RT beams

- Station parameter optimized radiation

therapy (SPORT )

- New QA tools for emerging RT technologies

Ruijiang Li, Karl Bush, Benjamin

Fahimian, Dimitre Hristov, Victor Yu,

Bin Han, Gary Luxton

National Cancer Institute &

Varian Medical Systems

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TrueBeam™ STx at Stanford

One of the first three TrueBeam LINACs - installed in 2009, Commissioning & acceptance test: July 2010, First SBRT

patient: Sept. 2010

Versa - Elekta

Stanford University

School of Medicine

Gated RapidArc Treatment Delivery

• During treatment, acquire

kV images at the

beginning of beam on for

every breathing cycle.

• For each image,

– Detect fiducials

– Estimate 3D positions

– Compare fiducials with

software “markers”

Beam-Level Imaging: Verification of

Geometric Accuracy

Ruijiang Li et al, Stanford

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Infrared reflective

markers

Infrared camera

Real-time Image Guidance for Gated RT

TrueBeam STx & SBRT at Stanford

High geometric accuracy (~1 mm)

HDMLC –for small lesions

Fast delivery – 1400/2400 MU/Min for 6/10 MV FFF photons

Motion management – onboard kV imaging during dose delivery

Programmable station-by-station

(node-by-node) delivery

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Intensity Modulation

IMRT

VMAT

SPORT

3D CRT

R. Li & L. Xing, Bridging the Gap between IMRT and VMAT: Dense Angularly Sampled and

Sparse Intensity Modulated Radiation Therapy (DASSIM-RT), Med Phys. 38, 4912-19, 2011.

VMAT Tomorrow:

Simultaneous

couch/collimator/gantry

motion

• Determination and optimization of non-

isocentric non-collisional trajectories

• RT will be delivered station by station, instead of

field by field.

-An intensity modulated field consists of a number

of stations at the same gantry angle (i.e., segments).

-An arc consists of a large number of stations at

different gantry angle.

• SPORT planning –depending on the specific

delivery scheme!

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SPORT: Non-isocentric Treatment

R. Li, K. Horst, L. Xing, K. Bush, IJROBP, 2013.

SPORT: Non-isocentric Treatment

R. Li, K. Horst, L. Xing, K. Bush, IJROBP, 2013.

SPORT: Non-isocentric Treatment

R. Li, K. Horst, L. Xing, K. Bush, IJROBP, 2013.

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SPORT: Non-isocentric Treatment

R. Li, K. Horst, L. Xing, K. Bush, IJROBP, 2013.

Non-isocentric Tx Bush and Li

R. Li, K. Horst, L. Xing, K. Bush, IJROBP, 2013.

Non-isocentric Trteatment

R. Li, K. Horst, L. Xing, K. Bush, IJROBP, 2013.

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TrueBeam developer mode

• Custom beam data in xml

Method I: Segmentally boosted VMAT – adding a

few segments in certain directions and optimize the

RapidArc plan together with the added segments.

Improved dose distribution with a single arc.

Method II: Differentially boosted VMAT – adding a

few apertures to certain angular regions and optimize

the system. An adaptive optimization algorithm has

been developed for this purpose.

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Field Setup

• Single full arc VMAT

• Boosted partial arcs

– 3 arcs in this HN case

– each ~30 deg

• Treatment planning

– VMAT optimization

Comparison with single-arc

VMAT

Triangle: 1-arc VMAT

Square: Segmented boost

Comparison with double-arc VMAT

Triangle: 2-arc VMAT

Square: Segmented boost

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Iso-dose distributions (20% and above)

2-arc VMAT Segmented boost

Iso-dose distributions (45% and above)

2-arc VMAT Segmented boost

Treatment delivery

• Delivered in a single-arc

– Each of the 3 partial arcs

is converted into 2 static

sub-fields.

– 1 continuous arc with 6

static beams inserted

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Delivery summary

• Rx: 200 cGy times 35 fractions

MU Control

Points

Gantry span

(deg) Delivery time

1-ARC VMAT 276 178 360 1 min

2-ARC VMAT 520 376 720 2 min

Segmented boost 331 376 450 1 min 55 sec

Intensity Modulation

IMRT

VMAT

SPORT

3D CRT

R. Li & L. Xing, Bridging the Gap between IMRT and VMAT: Dense Angularly Sampled and

Sparse Intensity Modulated Radiation Therapy (DASSIM-RT), Med Phys. 38, 4912-19, 2011.

L Zhu & L. Xing, Med Phys, 2009

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Compressed Sensing-Based Inverse Planning Framework

Quality Assurance of SPORT

V. Yu, B. Fahimian, L. Xing & D. Hristov, Med Phys, in press, 2014

Quality Assurance of SPORT

V. Yu, B. Fahimian, L. Xing & D. Hristov, Med Phys, in press, 2014

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Quality Assurance of SPORT

V. Yu, B. Fahimian, L. Xing & D. Hristov, Med Phys, in press, 2014

Quality Assurance of SPORT

V. Yu, B. Fahimian, L. Xing & D. Hristov, Med Phys, in press, 2014

Quality Assurance of SPORT

V. Yu, B. Fahimian, L. Xing & D. Hristov, Med Phys, in press, 2014

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Re-constituted

DICOM RP file

MUi

MUi-1

MUi+1

• gantry angle

• leaf positions

• delivered MUs

Delivery

Parameters:

System’s Logfiles

Varian TrueBeam System

Dosimetric Evaluation

Treatment

Planning

System

Gated-VMAT

Dose Reconstruction

Treatment Phase of 4D

pCT or

Pre-treatment 4D CBCT

Actual Parameters at Control Points

in-house

program

Dose Reconstruction Technique

TrueBeam Gated RapidArc – original plan, reconstructed dose

distribution and PTW Measurement

Gated VMAT delivery

with 3 sec respiration

period

Non-gated VMAT delivery

(Reference)

Gamma passing

rate = 99.4%

J. Qian, G. Luxton, L. Xing, 2010

Planned and Reconstructed Dose Profile Comparison

R L

A

P

R-L profile A-P profile

Qian J, Lee L, Liu W, Fu K, Luxton, G, Le Q, and Xing L, Cone

beam CT-based dose reconstruction for modulated arc therapy,

Physics in Medicine and Biology, 2010.

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Dose Distribution Comparison

plan reconstruction

Reconstructio

n

Plan PTV DVH

Comparison

Position #1: same as the plan

Position #3: L R: 3 mm; A P: 5mm; S I: 5 mm

Positioning errors intentionally introduced

Position #2: L R: 0 mm; A P: -2 mm; S I: 2 mm

Positioning Errors and Dose Delivered to PTV

plan reconstruction

Case 1: Dose Distribution

pCT

CBCT3 CBCT2 CBCT1

•Lee L, Le Q, Xing L: Retrospective IMRT dose reconstruction based on cone-beam CT and MLC log-

file. International Journal of Radiation Oncology, Biology and Physics, 70: 634-644, 2008.

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0

20

40

60

80

100

0 40 80 120 160 200 240

Case 1: DVHs

Brainstem

PT

V

pCT

CBCT3

CBCT1

CBCT2

DVH comparison of the intended and delivered plans

Dose (cGy)

Rela

tive v

olu

me (

%)

Data

2

Local

Computer

Python script

Worker 1

Worker 2

Worker N

Processor

Memory

.bcast(

…)

SSH

EGS

Master Node

Cloud-Computing

based Monte Carlo

infrastructure

K. Bush, H. Wang, G. Pratx, L Xing

X Chen, K Bush, A Zhang & L Xing, Med Phys Lett, submitted , 2014

Comparison between MC, Acuros, and AAA.

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MU verification for VMAT

MU verification for VMAT

MU verification for VMAT

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• unflattened beam

• high dose rate

• small sized fields in (SBRT)

Routine SBRT QA – High efficiency

– High dose resolution

– Ease of use

EPID-based absolute dosimetry for

digital linac

Bin Han, E. Mok, G. Luxton, L. Xing, ASTRO, 2013

EPID Response Core

• Monte Carlo dose distribution kernel,

Optical spread kernel, Total EPID response

kernel

1.0E-08

1.0E-07

1.0E-06

1.0E-05

1.0E-04

1.0E-03

1.0E-02

1.0E-01

1.0E+00

-20 -10 0 10 20

Rela

tive d

ose

Radial distance from center (cm)

Pencil beam dose distribution in EPID

6XFF

F

10XF

FF

1.0E-08

1.0E-07

1.0E-06

1.0E-05

1.0E-04

1.0E-03

1.0E-02

1.0E-01

1.0E+00

0 0.1 0.2 0.3 0.4

Rela

tive a

mp

litu

de

Radial distance from center (cm)

Optical spread kernel

Exp(-45 x r)

1.0E-07

1.0E-06

1.0E-05

1.0E-04

1.0E-03

1.0E-02

1.0E-01

1.0E+00

-20 -10 0 10 20

Rela

tive A

mp

litu

de

Radial distance from center (cm)

EPID Response Kernel

6XFFF

10XFFF

Bin Han, E. Mok, G. Luxton, L. Xing, AAPM, 20102

0

0.1

0.2

0.3

0.4

0.5

0.6

-100 -50 0 50 100

Dose

(cG

y)

Off-axis position (mm)

TPS

EPID

PTW729

Bin Han, E. Mok, G. Luxton, L. Xing, 20102

EPID-based absolute dosimetry

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Result: EPID dosimetry for

SBRT pt QA

• Gamma results: 3mm/3%: 99.9% 2mm/3%: 98.5% 2mm/2%: 92.8% 1mm/3%: 63.0%

6XFFF EPID vs. TPS verification plan

Isodose line LR profile TG profile

2%, 2mm γ histogram 2%, 2mm γ distribution

SUMMARY

• Features available in new generation of

LINACs facilitate RT workflow and

improve the efficiency & accuracy.

• Mechanical accuracy & imaging.

• SPORT.

• New QA tools are urgently needed.