共d兲to describe how these processes fit together with each
other and provide guidance on the clinical implementation of
IMRT.
Because of the emerging and rapidly changing nature of
IMRT, this document cannot be definitive or prescriptive.
Task group reports and Codes of Practice will eventually
emerge as the field matures. Our intention in this document
is to provide guidance during this introductory period. We
have tried to avoid being overly repetitive of other docu-
ments, such as the recent report of the IMRT Collaborative
Working Group 共CWG兲1and special issues of Medical
Dosimetry,2,3 with which readers should also be familiar. We
have also consulted with ASTRO representatives who are
developing recommendations for the clinical use of IMRT. It
should be recognized that the development of IMRT is still in
its infancy and is rapidly evolving. Therefore, many specific
statements made within this document are likely to be out-
dated as the new generation of planning and delivery systems
become available.
C. Organization of this document
After this introductory section, this presentation follows
with a description in Sec. II of delivery methods used for
IMRT and associated commissioning and QA. An under-
standing of delivery mechanisms is necessary to appreciate
some of the factors that impact IMRT treatment planning.
Section III on treatment planning follows. That section cov-
ers commissioning a planning system for dosimetric accu-
racy, which is inherently related to the delivery mechanism.
It also covers learning how to effectively use an inverse plan-
ning system. These two sections address objectives 共a兲-共c兲;
that is, they explain the differences from 3DCRT and provide
guidance on commissioning and QA of treatment planning
and delivery systems. Finally, in Sec. IV on clinical imple-
mentation we outline the issues that have to be addressed by
the physicist and other team members in order to bring IMRT
online, and so we address objective 共d兲.
II. DELIVERY SYSTEMS FOR IMRT
The difference between 3DCRT and IMRT with respect to
treatment delivery is implied in the phrase intensity modula-
tion. Three-dimensional conformal therapy uses blocks or
multileaf collimators 共MLCs兲to define fixed field bound-
aries. Modulators such as wedges or tissue compensators are
often employed to improve dose homogeneity within the tar-
get. IMRT extends the complexity of the intensity modula-
tion to achieve more complex dosimetric aims, such as cre-
ating dose distributions with concavities. Many methods of
achieving this modulation have been proposed and applied to
clinical practice. One class of techniques holds the beam
direction constant during irradiation and indexes the collima-
tor shape to a fraction of the total prescribed MU for that
direction, thus subjecting any given point in the patient to a
desired proportion of ‘‘open’’ and ‘‘blocked’’ beam. Another
technique uses fixed gantry angles and physical attenuators
to achieve the modulation. Yet another class of techniques
moves the gantry during the irradiation, indexing the colli-
mator shape and gantry angle to the delivered dose. Each
delivery technique has its own unique features that give rise
to different commissioning and QA considerations.
In this section we will emphasize those techniques that
have been implemented commercially using MLCs since
they are the most common and of widest interest to practic-
ing medical physicists. It provides guidance for commission-
ing and QA for these. Other techniques are described briefly.
Although IMRT planning and delivery are intimately re-
lated, in this section we suggest tests of the IMRT delivery
system using MLC control files that have been developed
independently from the IMRT planning system. In this fash-
ion, the causes of dose deviations can be isolated to the de-
livery or planning system.
In Secs. II A and II B we describe IMRT delivery systems
that use fixed gantry angles and MLCs. In Sec. II C we de-
scribe IMRT delivery systems that make use of fixed gantry
angles and physical attenuators. In Secs. II D and II E we
describe IMRT delivery systems that make use of gantry ro-
tations and MLC. In Sec. II F we provide background infor-
mation on the leaf sequencing algorithms that are used in the
segmental and dynamic IMRT techniques described in Secs.
II A and II B.
A. General issues of IMRT delivered with MLC
The CWG recommends the term segmental IMRT
共SMLC-IMRT兲when the collimator shape is constant during
irradiation and changes between irradiations. Synonymous
terms are step-and-shoot and stop-and-shoot. The gantry
does not move during irradiation. Each collimator shape thus
is a subfield 共or a segment兲. The desired intensity pattern is
obtained by the fractional weighted summation of the inten-
sity pattern from all subfields.
1. MLC leaf positional accuracy
In conventional 3DCRT, the MLC defines the outer aper-
ture of the beam shape. An uncertainty of 1 to 2 mm in leaf
location may be inconsequential to the output and, in gen-
eral, to clinical outcome, since the uncertainty is small com-
pared with the aperture size. Segmental IMRT builds up a
fluence pattern by adding together many segments, some of
which may be quite narrow. Several investigators have
shown that, for beam widths of 1 cm, uncertainties of a few
tenths of a millimeter in leaf position can cause dose uncer-
tainties of several percent.4,5 Furthermore, the beam edges
move to many locations within the treated area, so their lo-
cations must be known to high precision so that their contri-
butions sum accurately. For these reasons, the accuracy of
relative MLC leaf position must be maintained to a precision
of better than a millimeter. Conventional QA tests for static
MLCs are not sufficiently sensitive for this purpose.
A key point for IMRT is that the location of the radiation
field edge must be well established with respect to the nomi-
nal location of the MLC leaf end. For MLCs with rounded
leaf ends, there is an offset between the beam edge as defined
by the light field and that defined by the 50% decrement line
of the radiation field.6This is typically 0.4 to 1.1 mm de-
2091 Ezzell
et al.
: Clinical implementation of IMRT 2091
Medical Physics, Vol. 30, No. 8, August 2003