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Sajeev Surendran et al Int. Journal of Engineering Research and Applications www.ijera.com
ISSN : 2248-9622, Vol. 4, Issue 5( Version 6), May 2014, pp.134-137
www.ijera.com 134 | P a g e
Dynamic MLC-QA Based On Portal Dosimetry
Sajeev Surendran1, 2
, Durga Prasada Rao2
, Jayesh kunnanchath1
, Swapna Lilly
Cyriac1
1
Kims Pinnacle cancer care and research center, Trivandrum, Kerala, India.
2
Department of Nuclear Physics, Andhra University, vizag, Andhrapradesh, India.
Abstract
Purpose: Intensity modulated radiotherapy using dynamic delivery method requires accurate verification of
MLC, its position and speed of motion. These parameter have major impact on dose delivery on patients. For
quality assurance (QA) procedure requires more time consumed in a radiotherapy department. The main purpose
of this study was to investigate the potential use of amorphous silicon based EPID portal dosimetry for dMLC
QA
Methods and Materials: A varian Clinac_iX with On Board Imager (OBI) and Rapid Arc facility ( VMAT)
equipped with 120 leaf Millennium MLC and with Amorphous Silicon Based EPID (aSi-1000, varian) mounted
on a Exact Robotic Arm is used. The dMLC QA consists of different dynamic MLC pattern provided by varian
for checking positional accuracy, MLC gap, Leaf speed and complex dynamic field.
Results and Discussion: Various dMLC tests were done using portal dosimetry. All results are within the
tolerance limit. Picket fence test shows that leaf position errors of upto 0.2mm can be detected which are within
the tolerance limit. Complex dynamic field were exposed to EPID, which shows the leaf speed and are within
the tolerance limit.
Conclusion: dMLC QA test takes no longer than 5 minute in the linac room with EPID. So we can considerably
reduce the time for dMLC QA procedures in a busy department and these tests can be include as a daily QA
programme.
I. 1.Introduction
IMRT treatments are generally delivered using linear
accelerators equipped with MLC’s. During the
treatment, the MLC leaves move over the area of
interest instead of defining the outer boundaries [1].
The gap between leaf pairs is variable and can also be
small, so the gap width must be carefully controlled.
For dynamic MLC treatment (dMLC), the leaf speed
accuracy is very important.
Leaf positioning is after assessed by imaging a series
of MLC defined opening (or dose strips) along an
opposing leaf pair track, designed overlap or to about
or to have a 1 mm gap between them [2]. Images of
these dose strips may be acquired by an EPID.
Differences from the expected positions can be
visualised with a threshold of 0.5 mm at isocenter [3-
6]. The assessment can be quantified using scans
across the images, by positioning the leaf edges using
an EPID [7-11].
The total time spending for QA procedures is always
an issue for a busy department. By considering this,
EPID based portal dosimetry is very helpful for daily
dMLC QA test for saving time by comparing other
QA modalities such as ionization chamber, film
dosimetry or detector array system. EPID provides
images with high spatial resolution, fast, directly
stored in the system, no need of separate system and
easy analysing tools.
The purpose of this study is (1) to investigate the use
of EPID for detecting small errors in dynamic MLC
QA and (2) the potential use of EPID for routine
daily QA procedures and thus to save time.
II. 2. Materials and methods
In this study, a varian Clinac_iX with OBI and Rapid
Arc equipped with an 120 leaf Millennium MLC has
been used. This MLC consists of two carriages of 60
leaves each, with leaf width 0.5 cm at isocenter for
20 X 20 cm field size and 1 cm width for remaining
leaves. The leaves can be travel upto 14.5 cm
maximum relative to the carriage. During IMRT
delivery only leaves are moving and carriages are
fixed. The maximum leaf speed is 2.5 cm/S. For
IMRT treatments photons of 6 MV with a dose rate
of 400 MU/Min are used.
Amorphous silicon based EPID is attached to the
exact arm of clinac_iX. aSi-1000 (varian medical
systems) calibrated for hardware and dosimetric
purpose for different energies and various dose rates.
The active area of EPID consists in a matrix 1024 X
768 for 40 X 30 cm2
at source to detector distance
(SDD) of 100 cm with 30fps having resolution 0.39
mm. The result analysis done in portal dosimetry
Eclipse version 10 software. For the measurement we
used 100 cm SDD and 400 MU/Min for preventing
saturation problems and for better resolution. The
RESEARCH ARTICLE OPEN ACCESS
Sajeev Surendran et al Int. Journal of Engineering Research and Applications www.ijera.com
ISSN : 2248-9622, Vol. 4, Issue 5( Version 6), May 2014, pp.134-137
www.ijera.com 135 | P a g e
dosimetric characteristics of aSi based EPID’s have
been widely discussed in literature [12-16].
The following dMLC QA plans are provided by
varian, and the QA procedures are explained below.
2.1. Picket Fence: This test is to verify leaf positions
and carriage movement accuracy and calibrations
[17]. The picket fence test comprises eight
consecutive movements of a 5cm wise rectangular
field. We can examine of the match lines between the
5 cm wide fields to detect a 0.5mm displacement in
leaf positioning.
Figure-1: Picket fence test
2.2. Synchronized segmented strips: The
segmented strips test to verify the accuracy and
calibration of the leaf position and carriage
movement when some adjacent leaf pairs are closed
during beam delivery [17]. This test detects possible
effects of inter leaf friction on leaf positioning and
the ability of the leaves interdigitate. There are six
consecutive movements of a 4 X 24 Cm2
rectangular
field is divided into a series of horizontal strips. The
leaves between the 4cm wide field on the EPID
image to detect a 0.5mm displacement in the leaf
positioning.
Figure-2: Synchronized segmented strips
2.3. Non synchronized segmented strips: This test
is to verify leaf position accuracy and calibration and
detect possible effects of interleaf friction in case of
non synchronized leaf motion.
Figure-3: Non synchronized segmented strips.
2.4 X wedges: X-wedge test to verify the accuracy
and calibration of the leaves in producing an X-
wedged field. Two leaf sequence files produce the X
wedged field and the inverted X wedged field
respectively. The intensity pattern of both fields
complements each other so that the total exposure is
of uniform intensity everywhere inside the field.
Figure-4: X wedges
2.5. Y wedges: This test is similar to X wedge except
that the wedged field is oriented in the Y direction.
Figure-5: y wedges
2.6. Pyramids: Pyramids test to verify the accuracy
and calibration of the leaves in producing complex
pyramid fields. Two leaf sequences files produce the
Sajeev Surendran et al Int. Journal of Engineering Research and Applications www.ijera.com
ISSN : 2248-9622, Vol. 4, Issue 5( Version 6), May 2014, pp.134-137
www.ijera.com 136 | P a g e
pyramid and inverted pyramid fields. Super position
of the two fields creates a rectangular field with
uniform intensity everywhere inside the field.
Figure-6: Pyramids
2.7. Complex field A: This test is to verify the
accuracy and calibration of the leaves and to evaluate
the ability of dMLC to produce complex intensity
modulated patterns. We can evaluate how well the
system produces complex intensity pattern by
examining the field boundaries and symmetries.
Figure-7: Complex field A
2.8. Complex field B: This test is to verify the
accuracy and calibration of leaves, and to evaluate
the ability of dMLC to produce complex intensity
modulated patterns.
Figure-8: Complex field B
2.9. Continuous strips: This test is to verify the
stability and calibrations of leaf positioning, stability
of leaf speed, possible effects of interleaf friction,
and possible effects of finite acceleration and
deceleration of the leaves as they move from one
segment to the next.
Figure-9: Continuous strips
III. Results and Discussion
In the following, results of the implemented tests are
presented.
3.1. Picket fence: The match lines between 5cm
wide field should be straight and approximately equal
in intensity. In the figure, each match line includes a
1mm gap. The match line appears at -15.0 ± 0.1cm, -
10.0 ± 0.1 cm, - 5.0 ± 0.1cm, 0.0 ± 0.1cm, 5.0 ±
0.1cm, 10.0 ± 0.1cm and 15.0 ± 0.1cm from the
centre of the field.
All the match lines falls within 0.5 mm, the QA test
indicates that the MLC is operating properly.
3.2. Synchronized segmented strips: The match
lines between 4 cm wide fields should be straight and
approximately equal in intensity. The match lines
appeared at -12.0 ± 0.1cm, - 8.0 ± 0.1cm - 4.0 ±
0.1cm, 0 ± 0.1cm, 4.0 ± 0.1cm, 8.0 ± 0.1cm and 12.0
± 0.1cm from the centre of the field.
Intensity of all exposed strips are uniform, and the
non exposed strips are clear without exposure. The
results thus obtained, clearly indicate that dMLC is
operating properly.
3.3. Non synchronized segmented strips: The
match line between 2cm wide field segments appears
straight and approximately equal in intensity. The
match line segments appear at – 4.0 ± 0.1cm, – 2.0 ±
0.1cm, 2.0 ± 0.1cm and 4.0 ± 0.1cm from the centre
of the field. The match lines are within 0.5 mm, so
the QA test indicates that the dMLC is operating
properly.
3.4. X wedges: For the first image, the match lines
between the 2 cm wide field segments are straight.
The match lines appear at – 4.0 ± 0.1cm, – 2.0 ±
0.1cm, 0 ± 0.1cm, 2.0 ± 0.1cm and 4.0 ± 0.1cm from
the centre of the field. The results are within the
tolerance limit, QA test indicates that the dMLC is
operating properly. On the second image, the
intensity of each line segment are uniform and shows
no areas of irregular under exposure or over
exposure.
Sajeev Surendran et al Int. Journal of Engineering Research and Applications www.ijera.com
ISSN : 2248-9622, Vol. 4, Issue 5( Version 6), May 2014, pp.134-137
www.ijera.com 137 | P a g e
3.5. Y wedges: For the first image, the match lines
between 2 cm wide field segments are straight and
coincide with the interface between the adjacent
leaves. The match line segments appear at – 4.0 ±
0.1cm, – 2.0 ± 0.1cm, 0 ± 0.1cm, 2.0 ± 0.1cm and 4.0
± 0.1cm are from the centre of the field. The intensity
is uniform everywhere on the combined image.
3.6. Pyramids: For the first image, the match lines
between the squares with different intensity levels are
straight. The match lines are appear at – 4.0 ± 0.1cm,
– 3.0 ± 0.1cm – 2.0 ± 0.1cm, – 1.0 ± 0.1cm 0 ±
0.1cm, 1.0 ± 0.1cm, 2.0 ± 0.1cm, 3.0 ± 0.1cm and 4.0
± 0.1cm from the centre of the field. The intensity of
each line segment are uniform on the combined
image.
3.7. Complex field A: The field boundaries and
match lines between different segments are straight.
3.8. Complex field B: The field boundaries and the
match lines between different intensity segments are
straight.
3.9. Continuous strips: The intensities of all the
exposed match lines are uniform, and the non
exposed vertical strips are clear without exposure.
The match lines are straight.
IV. Conclusion
Because of the high efficiency and
resolution of EPID, we can reliable on EPID portal
dosimetry and can be reduce the time for complex
QA procedure compared with other QA modalities.
Any complex dynamic fields can be test with EPID
very fast and accurately.
We can do complete dMLC QA with EPID
and a lot of time can be saved and thus we can ensure
the information about position, speed of MLC and
confidentially can go on with dynamic MLC
treatments.
References
[1] Sasso T, Chui CS, Ling CC. Physical and
dosimetric aspects of a multileaf collimation
system used in the dynamic mode for
implementing intensity modulated
radiotherapy. Med Phys 1998;30:1919e27.
[2] Van Elmpt W, McDermott L, Nijsten S,
Wendling M, Lambin P, Mijnheer B. A
literature review of electronic portal imaging
for radiotherapy dosimetry. Radiother Oncol
2008;88: 289e309.
[3] Van Elmpt W, Ezzel GA. EPID dosimetry
must soon become an essential component of
IMRT quality assurance. Med Phys
2009;36:4325e7.
[4] Van Zijveld M, Dirkx ML, de Boer HC,
Heijmen BJ. Dosimetric pre-treatment
verification of IMRT using an EPID; clinical
experience. Radiother Oncol 2006;81:168e75.
[5] Van Elmpt W, Nijsten S, Petit S, Mijnheer B,
Lambin P, Dekker A. 3D in vivo dosimetry
using megavoltage cone-beam CT and EPID
dosimetry. Int J Radiat Oncol Biol Phys
2009;73: 1580e7.
[6] Lee C, Menk F, Cadman P, Greer B. A simple
approach to using an amorphous silicon EPID
to verify IMRT planar dose maps. Med Phys
2009;36:984e92.
[7] Yang Y, Lei Xing. Quantitative measurement
of MLC leaf displacements using an electronic
portal image device. Phys Med Biol
2004;49:1521e33.
[8] Mamalui-Hunter M, Li H, Low DA. MLC
quality assurance using EPID: a fitting
technique with subpixel precision. Med Phys
2008;35:2347e55.
[9] Parent L, Seco J, Evans PM, Dance DR,
Fielding A. Evaluation of two methods of
predicting MLC leaf positions using EPID
measurements. Med Phys 2006;33:3174e82.
[10] Chang J, Obcemea CH, Sillanpaa J,
Mechalakos J, Burman CM. Use of EPID for
leaf position accuracy QA of dynamic multi-
leaf collimator (DMLC) treatment. Med Phys
2004;31: 2091e6.
[11] Beck JA, Budgell GJ, Roberts DA, Evans PM.
Electron beam quality control using an
amorphous silicon EPID. Med Phys
2009;36:1859e66.
[12] Van Esch A, Depuydt T, Huyskens DP. The
use of an aSi-based EPID for routine absolute
dosimetric pre-treatment verification of
dynamic IMRT fields. Radiother Oncol
2004;71: 223e34.
[13] Greer PB, Popescu CC. Dosimetric properties
of an amorphous silicon electronic portal
imaging device for verification of dynamic
intensity modulated radiation therapy. Med
Phys 2003;30:1618e27.
[14] McCurdy BM, Luchka K, Pistorius S.
Dosimetric investigation and PD image
prediction using an amorphous silicon
electronic portal imaging device. Med Phys
2001;28:911e24.
[15] Louwe RJ, McDermott LN, Sonke JJ,
Tielenburg R, Wendling M, van Herk MB, et
al. The long-term stability of amorphous
silicon flat panel imaging devices for
dosimetry purposes. Med Phys
2004;31:2989e95.
[16] Greer PB. Off-axis dose response characteristics
of an amorphous silicon electronic portal
imaging device. Med Phys 2007; 34:3815e24.
[17] Chui CS, Spirou SV, LoSasso T. Testing of
dynamic multileaf collimation. Med Phys
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Y04506134137

  • 1. Sajeev Surendran et al Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 5( Version 6), May 2014, pp.134-137 www.ijera.com 134 | P a g e Dynamic MLC-QA Based On Portal Dosimetry Sajeev Surendran1, 2 , Durga Prasada Rao2 , Jayesh kunnanchath1 , Swapna Lilly Cyriac1 1 Kims Pinnacle cancer care and research center, Trivandrum, Kerala, India. 2 Department of Nuclear Physics, Andhra University, vizag, Andhrapradesh, India. Abstract Purpose: Intensity modulated radiotherapy using dynamic delivery method requires accurate verification of MLC, its position and speed of motion. These parameter have major impact on dose delivery on patients. For quality assurance (QA) procedure requires more time consumed in a radiotherapy department. The main purpose of this study was to investigate the potential use of amorphous silicon based EPID portal dosimetry for dMLC QA Methods and Materials: A varian Clinac_iX with On Board Imager (OBI) and Rapid Arc facility ( VMAT) equipped with 120 leaf Millennium MLC and with Amorphous Silicon Based EPID (aSi-1000, varian) mounted on a Exact Robotic Arm is used. The dMLC QA consists of different dynamic MLC pattern provided by varian for checking positional accuracy, MLC gap, Leaf speed and complex dynamic field. Results and Discussion: Various dMLC tests were done using portal dosimetry. All results are within the tolerance limit. Picket fence test shows that leaf position errors of upto 0.2mm can be detected which are within the tolerance limit. Complex dynamic field were exposed to EPID, which shows the leaf speed and are within the tolerance limit. Conclusion: dMLC QA test takes no longer than 5 minute in the linac room with EPID. So we can considerably reduce the time for dMLC QA procedures in a busy department and these tests can be include as a daily QA programme. I. 1.Introduction IMRT treatments are generally delivered using linear accelerators equipped with MLC’s. During the treatment, the MLC leaves move over the area of interest instead of defining the outer boundaries [1]. The gap between leaf pairs is variable and can also be small, so the gap width must be carefully controlled. For dynamic MLC treatment (dMLC), the leaf speed accuracy is very important. Leaf positioning is after assessed by imaging a series of MLC defined opening (or dose strips) along an opposing leaf pair track, designed overlap or to about or to have a 1 mm gap between them [2]. Images of these dose strips may be acquired by an EPID. Differences from the expected positions can be visualised with a threshold of 0.5 mm at isocenter [3- 6]. The assessment can be quantified using scans across the images, by positioning the leaf edges using an EPID [7-11]. The total time spending for QA procedures is always an issue for a busy department. By considering this, EPID based portal dosimetry is very helpful for daily dMLC QA test for saving time by comparing other QA modalities such as ionization chamber, film dosimetry or detector array system. EPID provides images with high spatial resolution, fast, directly stored in the system, no need of separate system and easy analysing tools. The purpose of this study is (1) to investigate the use of EPID for detecting small errors in dynamic MLC QA and (2) the potential use of EPID for routine daily QA procedures and thus to save time. II. 2. Materials and methods In this study, a varian Clinac_iX with OBI and Rapid Arc equipped with an 120 leaf Millennium MLC has been used. This MLC consists of two carriages of 60 leaves each, with leaf width 0.5 cm at isocenter for 20 X 20 cm field size and 1 cm width for remaining leaves. The leaves can be travel upto 14.5 cm maximum relative to the carriage. During IMRT delivery only leaves are moving and carriages are fixed. The maximum leaf speed is 2.5 cm/S. For IMRT treatments photons of 6 MV with a dose rate of 400 MU/Min are used. Amorphous silicon based EPID is attached to the exact arm of clinac_iX. aSi-1000 (varian medical systems) calibrated for hardware and dosimetric purpose for different energies and various dose rates. The active area of EPID consists in a matrix 1024 X 768 for 40 X 30 cm2 at source to detector distance (SDD) of 100 cm with 30fps having resolution 0.39 mm. The result analysis done in portal dosimetry Eclipse version 10 software. For the measurement we used 100 cm SDD and 400 MU/Min for preventing saturation problems and for better resolution. The RESEARCH ARTICLE OPEN ACCESS
  • 2. Sajeev Surendran et al Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 5( Version 6), May 2014, pp.134-137 www.ijera.com 135 | P a g e dosimetric characteristics of aSi based EPID’s have been widely discussed in literature [12-16]. The following dMLC QA plans are provided by varian, and the QA procedures are explained below. 2.1. Picket Fence: This test is to verify leaf positions and carriage movement accuracy and calibrations [17]. The picket fence test comprises eight consecutive movements of a 5cm wise rectangular field. We can examine of the match lines between the 5 cm wide fields to detect a 0.5mm displacement in leaf positioning. Figure-1: Picket fence test 2.2. Synchronized segmented strips: The segmented strips test to verify the accuracy and calibration of the leaf position and carriage movement when some adjacent leaf pairs are closed during beam delivery [17]. This test detects possible effects of inter leaf friction on leaf positioning and the ability of the leaves interdigitate. There are six consecutive movements of a 4 X 24 Cm2 rectangular field is divided into a series of horizontal strips. The leaves between the 4cm wide field on the EPID image to detect a 0.5mm displacement in the leaf positioning. Figure-2: Synchronized segmented strips 2.3. Non synchronized segmented strips: This test is to verify leaf position accuracy and calibration and detect possible effects of interleaf friction in case of non synchronized leaf motion. Figure-3: Non synchronized segmented strips. 2.4 X wedges: X-wedge test to verify the accuracy and calibration of the leaves in producing an X- wedged field. Two leaf sequence files produce the X wedged field and the inverted X wedged field respectively. The intensity pattern of both fields complements each other so that the total exposure is of uniform intensity everywhere inside the field. Figure-4: X wedges 2.5. Y wedges: This test is similar to X wedge except that the wedged field is oriented in the Y direction. Figure-5: y wedges 2.6. Pyramids: Pyramids test to verify the accuracy and calibration of the leaves in producing complex pyramid fields. Two leaf sequences files produce the
  • 3. Sajeev Surendran et al Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 5( Version 6), May 2014, pp.134-137 www.ijera.com 136 | P a g e pyramid and inverted pyramid fields. Super position of the two fields creates a rectangular field with uniform intensity everywhere inside the field. Figure-6: Pyramids 2.7. Complex field A: This test is to verify the accuracy and calibration of the leaves and to evaluate the ability of dMLC to produce complex intensity modulated patterns. We can evaluate how well the system produces complex intensity pattern by examining the field boundaries and symmetries. Figure-7: Complex field A 2.8. Complex field B: This test is to verify the accuracy and calibration of leaves, and to evaluate the ability of dMLC to produce complex intensity modulated patterns. Figure-8: Complex field B 2.9. Continuous strips: This test is to verify the stability and calibrations of leaf positioning, stability of leaf speed, possible effects of interleaf friction, and possible effects of finite acceleration and deceleration of the leaves as they move from one segment to the next. Figure-9: Continuous strips III. Results and Discussion In the following, results of the implemented tests are presented. 3.1. Picket fence: The match lines between 5cm wide field should be straight and approximately equal in intensity. In the figure, each match line includes a 1mm gap. The match line appears at -15.0 ± 0.1cm, - 10.0 ± 0.1 cm, - 5.0 ± 0.1cm, 0.0 ± 0.1cm, 5.0 ± 0.1cm, 10.0 ± 0.1cm and 15.0 ± 0.1cm from the centre of the field. All the match lines falls within 0.5 mm, the QA test indicates that the MLC is operating properly. 3.2. Synchronized segmented strips: The match lines between 4 cm wide fields should be straight and approximately equal in intensity. The match lines appeared at -12.0 ± 0.1cm, - 8.0 ± 0.1cm - 4.0 ± 0.1cm, 0 ± 0.1cm, 4.0 ± 0.1cm, 8.0 ± 0.1cm and 12.0 ± 0.1cm from the centre of the field. Intensity of all exposed strips are uniform, and the non exposed strips are clear without exposure. The results thus obtained, clearly indicate that dMLC is operating properly. 3.3. Non synchronized segmented strips: The match line between 2cm wide field segments appears straight and approximately equal in intensity. The match line segments appear at – 4.0 ± 0.1cm, – 2.0 ± 0.1cm, 2.0 ± 0.1cm and 4.0 ± 0.1cm from the centre of the field. The match lines are within 0.5 mm, so the QA test indicates that the dMLC is operating properly. 3.4. X wedges: For the first image, the match lines between the 2 cm wide field segments are straight. The match lines appear at – 4.0 ± 0.1cm, – 2.0 ± 0.1cm, 0 ± 0.1cm, 2.0 ± 0.1cm and 4.0 ± 0.1cm from the centre of the field. The results are within the tolerance limit, QA test indicates that the dMLC is operating properly. On the second image, the intensity of each line segment are uniform and shows no areas of irregular under exposure or over exposure.
  • 4. Sajeev Surendran et al Int. Journal of Engineering Research and Applications www.ijera.com ISSN : 2248-9622, Vol. 4, Issue 5( Version 6), May 2014, pp.134-137 www.ijera.com 137 | P a g e 3.5. Y wedges: For the first image, the match lines between 2 cm wide field segments are straight and coincide with the interface between the adjacent leaves. The match line segments appear at – 4.0 ± 0.1cm, – 2.0 ± 0.1cm, 0 ± 0.1cm, 2.0 ± 0.1cm and 4.0 ± 0.1cm are from the centre of the field. The intensity is uniform everywhere on the combined image. 3.6. Pyramids: For the first image, the match lines between the squares with different intensity levels are straight. The match lines are appear at – 4.0 ± 0.1cm, – 3.0 ± 0.1cm – 2.0 ± 0.1cm, – 1.0 ± 0.1cm 0 ± 0.1cm, 1.0 ± 0.1cm, 2.0 ± 0.1cm, 3.0 ± 0.1cm and 4.0 ± 0.1cm from the centre of the field. The intensity of each line segment are uniform on the combined image. 3.7. Complex field A: The field boundaries and match lines between different segments are straight. 3.8. Complex field B: The field boundaries and the match lines between different intensity segments are straight. 3.9. Continuous strips: The intensities of all the exposed match lines are uniform, and the non exposed vertical strips are clear without exposure. The match lines are straight. IV. Conclusion Because of the high efficiency and resolution of EPID, we can reliable on EPID portal dosimetry and can be reduce the time for complex QA procedure compared with other QA modalities. Any complex dynamic fields can be test with EPID very fast and accurately. We can do complete dMLC QA with EPID and a lot of time can be saved and thus we can ensure the information about position, speed of MLC and confidentially can go on with dynamic MLC treatments. References [1] Sasso T, Chui CS, Ling CC. Physical and dosimetric aspects of a multileaf collimation system used in the dynamic mode for implementing intensity modulated radiotherapy. Med Phys 1998;30:1919e27. [2] Van Elmpt W, McDermott L, Nijsten S, Wendling M, Lambin P, Mijnheer B. A literature review of electronic portal imaging for radiotherapy dosimetry. Radiother Oncol 2008;88: 289e309. [3] Van Elmpt W, Ezzel GA. EPID dosimetry must soon become an essential component of IMRT quality assurance. Med Phys 2009;36:4325e7. [4] Van Zijveld M, Dirkx ML, de Boer HC, Heijmen BJ. Dosimetric pre-treatment verification of IMRT using an EPID; clinical experience. Radiother Oncol 2006;81:168e75. [5] Van Elmpt W, Nijsten S, Petit S, Mijnheer B, Lambin P, Dekker A. 3D in vivo dosimetry using megavoltage cone-beam CT and EPID dosimetry. Int J Radiat Oncol Biol Phys 2009;73: 1580e7. [6] Lee C, Menk F, Cadman P, Greer B. A simple approach to using an amorphous silicon EPID to verify IMRT planar dose maps. Med Phys 2009;36:984e92. [7] Yang Y, Lei Xing. Quantitative measurement of MLC leaf displacements using an electronic portal image device. Phys Med Biol 2004;49:1521e33. [8] Mamalui-Hunter M, Li H, Low DA. MLC quality assurance using EPID: a fitting technique with subpixel precision. Med Phys 2008;35:2347e55. [9] Parent L, Seco J, Evans PM, Dance DR, Fielding A. Evaluation of two methods of predicting MLC leaf positions using EPID measurements. Med Phys 2006;33:3174e82. [10] Chang J, Obcemea CH, Sillanpaa J, Mechalakos J, Burman CM. Use of EPID for leaf position accuracy QA of dynamic multi- leaf collimator (DMLC) treatment. Med Phys 2004;31: 2091e6. [11] Beck JA, Budgell GJ, Roberts DA, Evans PM. Electron beam quality control using an amorphous silicon EPID. Med Phys 2009;36:1859e66. [12] Van Esch A, Depuydt T, Huyskens DP. The use of an aSi-based EPID for routine absolute dosimetric pre-treatment verification of dynamic IMRT fields. Radiother Oncol 2004;71: 223e34. [13] Greer PB, Popescu CC. Dosimetric properties of an amorphous silicon electronic portal imaging device for verification of dynamic intensity modulated radiation therapy. Med Phys 2003;30:1618e27. [14] McCurdy BM, Luchka K, Pistorius S. Dosimetric investigation and PD image prediction using an amorphous silicon electronic portal imaging device. Med Phys 2001;28:911e24. [15] Louwe RJ, McDermott LN, Sonke JJ, Tielenburg R, Wendling M, van Herk MB, et al. The long-term stability of amorphous silicon flat panel imaging devices for dosimetry purposes. Med Phys 2004;31:2989e95. [16] Greer PB. Off-axis dose response characteristics of an amorphous silicon electronic portal imaging device. Med Phys 2007; 34:3815e24. [17] Chui CS, Spirou SV, LoSasso T. Testing of dynamic multileaf collimation. Med Phys 1996;23:635e41.