Interfractional anatomic variation
in patients treated with
respiration-gated radiotherapy
Ellen Yorke,1 Kenneth E. Rosenzweig,2 Raquel Wagman,2 and Gikas S. Mageras1
Department of Medical Physics1, Department of Radiation Oncology,2 Memorial Sloan Kettering Cancer Center, 1275 York Avenue, New York City, New York 10021 U.S.A.
yorkee@mskcc.orgReceived 23 August 2004; accepted 15 December 2004
As quality assurance for respiration-gated treatments using the Varian RPMT system, we monitor interfractional diaphragm variation throughout treatment using extra anterior-posterior (AP) portal images. We measure the superior-inferior (SI) distance between one or more bony landmarks and the ipsilateral diaphragm dome in each such radiograph and calculate its difference, D, from the corresponding distance in a planning CT scan digitally reconstructed radiograph (DRR). For each patient, the mean of D represents the systematic diaphragm displacement, and the standard deviation of D represents random diaphragm variations and is a measure of interfractional gating reproducibility. We present results for 31 sequential patients (21 lung, 10 liver tumors), each with at least 8 such portal images. For all patients, the gate included end-exhale. The patient-specific duty cycle ranged from 30% to 60%. All patients received customized audio prompting for simulation and treatment, and 14 patients also received visual prompting. Respiration-synchronized fluoroscopic movies taken at a conventional simulator revealed patient-specific diaphragm excursions from 1.0 cm to 5.0 cm and diaphragm excursion within the gate from 0.5 cm to 1.0 cm, demonstrating a significant reduction of intra-fractional diaphragm (and by inference tumor) motion by respiratory gating. One standard deviation of the systematic displacement (the mean of D) was 0.63 cm and 0.48 cm for the lung and liver patient groups, respectively. The average ±1 SD of the random displacements (i.e., the average of the standard deviations of D) was 0.42 ± 0.11 cm and 0.50 ± 0.19 for the two groups, respectively. The similar magnitude of the systematic and random displacements suggests that both derive from a common distribution of interfractional variations. Combining visual with audio prompting did not significantly improve performance, as judged by D. Guided by these portal images, field changes were made during the course of treatment for 6 patients (1 lung, 5 liver).
PACS numbers: 87.53.-j, 87.53.Oq
Key words: gating, respiration, radiotherapy
I. INTRODUCTION
Respiratory motion of thoracic and abdominal tumors
can exceed 2 cm, which compromises the accuracy of three-dimensional
conformal radiation therapy at these sites. For current surveys of
thoracic tumor motion studies, see Langen and Jones,(1) Mechalakos et al.,(2) and references therein. To prevent
underdosing of a target that undergoes respiratory motion during
simulation and treatment, an extra safety margin is included in the
planning target volume (PTV). However, this includes excess normal
tissue, which causes increased risk to normal tissues and/or a
reduction in prescription
dose.
Respiratory gating is a
technique for limiting the adverse effects of this motion by
acquiring planning images and delivering therapy beams only during a
selected portion of the breathing cycle (the gate), which is
determined by the signal from a breathing monitor. Ideally, when the
monitor signal is within the gate, the tumor and normal anatomy are
in the same position (within user-specified tolerances) at
simulation and for all treatments. A variety of breathing monitors
have been suggested and used.(3-9) One
such is the Varian RPMT system (Real-time Position Management,
Varian Medical Systems, Palo Alto, CA), which has been the subject
of several reports.(10-17) The RPM
system monitors respiratory motion using the motion of markers on
the patient's surface. A key assumption underlying this method is
that reproducible marker motion implies reproducible tumor motion.
Ideally, this would be verified by direct observation of the tumor,
but if the tumor is poorly visualized on portal images, the
diaphragm is often used as a clearly visible surrogate. The motion
of liver tumors in the superior-inferior (SI) direction is reported
to correlate well with diaphragm motion.(18) Good correlation between diaphragm and
lung tumor motion has also been observed in some patients,(19) but the more complicated motion of lung
tumors makes further, patient-specific study desirable.(20)
In
fluoroscopic studies, we observed good correlation of marker and
diaphragm motion and good intra-fractional reproducibility of the SI
location of the apex of the diaphragm(11) with RPM gating. However,
intra-fractional reproducibility does not necessarily imply
reproducibility over 4 to 8 weeks of treatment, since respiratory
patterns and internal anatomy can change due to comorbid conditions,
therapy response, disease progression, or breathing changes as the
patient adapts to the treatment routine. For the first 8 patients
treated with RPM gating at our institution, the mean displacement of
the diaphragm on localization films taken at treatment differed from
the value at simulation by more than 0.4 cm for 4 patients.(12) Subsequently, as quality assurance of
all RPM-gated treatments in our department, we acquire gated
anterior-posterior (AP) portal images 1 to 3 times per week
throughout the course of treatment and measure the SI distance
between isocenter and the dome of the ipsilateral diaphragm,
corrected for SI setup error. Below, we report on the
interfractional variations in a larger and later group of 31
sequential patients treated with RPM gating.
II. METHODS
A. RPM system
In
the RPM gating system, a pair of infrared reflective markers rigidly
mounted in a plastic block is placed on the patient's chest. The
motion of these markers is monitored by a CCD camera with an
attached infrared illuminator. The camera output goes to a PC
running the RPM software. After a "tracking" algorithm establishes
the period and amplitude of the marker motion, the motion is
"recorded" and displayed as a graph (the marker motion trace) on the
PC monitor. In this study, we used amplitude gating, where the user
sets amplitude thresholds that define the range of marker positions
within the gate. At a conventional simulator, fluoroscopic movies
can be taken in synchrony with the marker motion, saved, and played
back to observe anatomical motion within any chosen gate. At a
CT-simulator, a signal from the RPM system triggers slice
acquisition in axial mode when the motion enters the gate. For
treatment, a signal from the PC to the gun grid enables the beam
only when the motion is within the
gate.
The RPM data from the
planning CT is the reference session for treatment. To encourage
regular breathing, customized voice instruction is produced by
adjusting pause lengths in a recorded phrase, "breathe in (pause1),
breathe out (pause2)," to a rhythm that is comfortable for the
patient. To implement visual prompting, which has been suggested to
further improve breathing regularity,(17,19) an amplitude typical of the marker
excursion at simulation is chosen. This is displayed as a
cross-hatched region in the marker motion trace and as a solid
rectangle in a simpler display for the patient. This amplitude and
the audio instructions are saved in the reference session and
provide breathing constancy cues for the patient and the therapists
at treatment. In our clinic, the patient views the visual prompt on
a couch-mounted monitor (Fig. 1(b)) and is trained to make the bar
touch the top of the blue rectangle at end-inhale and the bottom at
end-exhale. The therapist sees the full display on the PC and can
supervise breathing regularity. A typical PC screen is shown in Fig.
1(a).
FIG. 1. The RPM screen and visual feedback hardware. (a) The RPM v1.5 PC screen for amplitude-gated treatment or simulation at end-inhale. The treatment beam would be on when the marker motion trace is between the two horizontal lines labeled “Gate Region.” (b) The small LCD monitor mounted on the couch, on which the patient can view the visual prompt |
||
B. Simulation and treatment planning
We analyzed the portal images for 31 sequential
patients treated with RPM respiratory gating. This study has been
approved by our Institutional Review Board. There were 21 nonsmall
cell lung cancer patients, 9 patients with liver cancer (primary or
metastases) and one with a rhab-domyosarcoma near the liver. All
were outpatients, treated with curative or long-term palliative
intent. The average lung patient age was 67.6 years (range 54 to 83
years), with 11 males and 10 females. The average liver patient age
was 55 years (range 17 to 80 years), with 6 males and 4 females. A
graticule tray projecting a 2-cm square grid at isocenter was used
for all films, and a similar grid was overlaid on the digitally
reconstructed radiographs (DRRs) to facilitate absolute distance
measurements and locate
isocenter.
Before simulation, each
patient was immobilized supine, with arms above the head, in a
custom foam cradle (Alpha Cradle Molds, Akron, OH). The marker block
was between umbilicus and xiphoid, at a location where its motion
amplitude was at least 0.5 cm. All patients were trained to follow
the customized voice instruction described above, and 16 were
trained and simulated with the addition of visual prompting. Because
patients breath more deeply when following voice instruction,(11) they were encouraged to "breath
normally" and to not hyperventilate. The same marker block location
and breathing instructions were used for CT simulation and
treatment. At an RPM-equipped simulator (Ximatron, Varian Medical
Systems, Palo Alto, CA), anterior fluoroscopic movies of the
ipsilateral diaphragm (estimated skin exposure 2.5 R for a 45-s
movie) were acquired for 27 of the patients. If the tumor was
visible, its motion amplitude was also noted. For all patients, the
gate interval for acquisition of the planning CT images and
treatment included end-exhale. The gate width was based on the
fluoroscopic movies and the motion trace so that the duty cycle
(percent of breathing cycle within the gate) was at least 25%. Gated
AP simulator films or computed radiographs (Kodak RT3000, Rochester,
NY) were acquired at the isocenter set by the radiation
oncologist.
Planning CT images were
acquired on an RPM-equipped PQ 5000 (Philips Marconi Medical
Systems, Cleveland, OH). Slice separation and thickness were 5 mm
for 28 patients and decreased to 3 mm for the most recent 3
patients. Patients who participated in an imaging study also
received a respiration-triggered scan at end-inspiration(21) or a respiration-correlated CT
scan.(22-25) For all patients,
high-contrast DRRs of the treatment fields and an orthogonal pair
were generated as well as a "soft tissue" AP and/or PA DRR (same
mass attenuation coefficient for all tissues). These resemble
megavoltage portal images and are reference images for the diaphragm
position during gated treatment. The treatment fields were selected
by the planner and did not have to include AP or PA beams. A
volumetric, patient-specific CTV to PTV margin of 1 cm to 1.5 cm for
lung patients(26) and 1 cm for the
liver patients(21) was used for
planning, but this could be increased partway through treatment
depending on observed interfraction variability.
C. Diaphragm radiographs
All patients were treated with RPM gating on a
Varian 2100-EX LINAC. The therapists gave extra instruction to
patients who had difficulty with regular breathing and reported
persistent problems to a physician or physicist. All portal imaging
was gated and used 6-MV photons. In addition to the weekly treatment
field portal images, extra open AP or PA radiographs showing the
ipsilateral diaphragm, isocenter, and spine (hereafter called
"diaphragm films") were acquired. Four monitor units (MU) were used
per extra film to restrict the imaging dose (our double-exposure
treatment field films are 6 to 8 MU). For the first two weeks of
treatment, we requested diaphragm films for at least 5 sessions. If
no problems were encountered, the frequency of these films was
reduced to twice per week in weeks 3 and 4 and weekly thereafter.
Most diaphragm imaging used film or computed radiography because
electronic portal imaging with RPM versions 1.3 to 1.5 requires
physics assistance. However, electronic imaging was done for lung
patients LU-13 (5 days), LU-14 (1 day), and LU-15 (3 days). Each
electronic portal imaging device (EPID) session used a total of 4 MU
but provided 3 to 5 diaphragm
images.
For each diaphragm film, we
visually chose as an origin a prominent vertebral feature that was
also visible on the DRR or the gated AP simulator film. It was
sometimes necessary to use different features for different
diaphragm films because a feature visible on one diaphragm film was
obscured on another. The most prominent bony landmarks are also
different from patient to patient. The only requirement for a
reference feature was that it not move with respiration and be
clearly identifiable on both the reference image and the diaphragm
film. The DRRs and diaphragm films were digitized into an in-house
image review program. Measurements were done with the aid of an
electronic ruler and the graticule. We determined the shift required
to make the SI distance from isocenter to this feature the same as
in the reference DRR and/or simulator film. We defined dp as the SI distance between the ipsilateral
diaphragm apex and the shifted isocenter and calculated the
difference between dp and the
isocenter-diaphragm distance, dref, in the reference image. We defined
D as
(1a) |
(1b) |
D is positive if the diaphragm is inferior relative to the DRR for both the lung patients (isocenter superior to diaphragm) and the liver patients (isocenter inferior to diaphragm); D is negative for a superior diaphragm displacement. Ideally, D is not affected by setup error and depends only on the interfractional performance of gating. However, because small vertebral features are blurred by partial volume effects in the DRR and are often indistinct on thoracic port films, we did not attempt to correct setup errors less than 3 mm. Figure 2 illustrates the determination of D.
FIG. 2. The determination of D. D is found by comparing the distance of isocenter to diaphragm on an AP DRR from the planning scan with the distance of isocenter to diaphragm on an AP or PA portal image. Correction for setup error on the portal image is made by finding the distance from isocenter to a vertebral landmark visible on both images. |
||
Both D and the "raw" isocenter-diaphragm distance supply information on the adequacy of the PTV. If a large systematic or film-to-film variation of D was seen in the first 2 to 3 weeks, the case was discussed and sometimes replanned with a larger PTV. At the end of treatment, Dpt, the mean value of D, and Spt, the standard deviation of D, were calculated for each patient. Dpt represents the systematic change in diaphragm position compared to simulation. Spt is determined by random positional variation of the diaphragm and is a measure of interfraction gating reproducibility.
III. RESULTS
All patients had between 8 and 16 diaphragm films. Approximately 20% of these had SI setup error exceeding 3 mm. The average value of D over all the patients was -0.12 cm with the standard error in the mean of ±0.1 cm. The average of the standard deviations (Spt's) over all patients was 0.45 cm with standard error in the mean of ±0.03 cm. Breathing periods ranged from 4 s to 6 s, and duty cycles ranged from 27% to 55%; breathing traces of patients with large duty cycles were characterized by a long, flat exhale plateau. Tables 1 and 2 summarize the data for the individual lung and liver patients, respectively.
TABLE 1. Summary for lung cancer patients. Positive Dpt means portal image diaphragm is inferior to DRR (more like“inhale” than simulation). Spt is the SD of D for an individual patient. The estimated error in Dpt is Spt/ |
| a Fluoro movie connection to breathing trace corrupted; breathing trace for fluoro qualitatively different from CT
and treatment. b Offered visual prompting but declined |
TABLE 2. Summary for liver cancer patients. Positive Dpt means portal image diaphragm is inferior to DRR (more like“inhale” than simulation). Spt is the SD of D for an individual patient. The estimated error in Dpt is Spt/ |
A. Lung cancer patients
Fluoroscopic movies
were available for 19 of the 21 lung cancer patients, and
breathing-synchronized movies could be reconstructed for 17 lung
patients. For 2 patients, the motion trace recorded along with the
movie was atypical in that it differed greatly from the trace at CT
and treatment. Without gating, the end-exhale to end-inhale
ipsilateral diaphragm excursion estimated from the movies ranged
from 1 cm to 5 cm, and gating reduced it to a mean of 0.6 cm (0.4 cm
to 1 cm). These differences were statistically significant (p < 10-3, two-sided
t-test).
For each lung
patient, the systematic deviation of the ipsilateral diaphragm
position relative to simulation (Dpt) and the random film-to-film variation
(Spt) are listed in Table 1 and
plotted in Fig. 3. Averaging over the lung patients, the average ±1
SD of Dpt was -0.13 ± 0.63 cm
(range 1.41 cm superior to 1.04 cm inferior), and the average ±1 SD
of Spt was 0.42 ± 0.11 cm (range
0.17 to 0.58 cm). For 16 patients, Dpt was 0.5 cm or less, indicating that their
average diaphragm position was within 0.5 cm of simulation. The
other 5 patients (5_LU, 8_LU, 13_LU, 14_LU, and 17_LU) had
systematic deviations from simulation exceeding 1 cm, although, as
judged by the PC display, they were regular breathers with no
notable change in marker motion relative to simulation. Patients
13_LU and 14_LU also had visual prompting throughout treatment.
Patient 17_LU (also 18_LU) found visual prompting confusing, and it
was discontinued early in treatment. Although the gate was centered
approximately at end-exhale, for 4 patients (5_LU, 8_LU, 14_LU, and
17_LU) the systematic diaphragm shift was superior (Dpt < 0) by more than 1 cm, suggesting a
more pronounced exhale at treatment than at simulation. Five
patients (2_LU, 4_LU, 6_LU, 11_LU, and 19_LU) had small systematic
difference from simulation (|Dpt|
< 0.2 cm), but three of these (4_LU, 6_LU, and 19_LU) had
larger than average film-to-film variations. For an individual
patient, the distribution of Ds did not visually appear to be
Gaussian, as shown in Figs. 4(a) and 4(b). Thus, as a second measure
of diaphragm variability, Table 1 also lists the percent of each
patient's diaphragm films with D within 0.5 cm of
Dpt. This was all films for 4
patients and all but one film for 11 patients. Patient 5_LU was
noted to have a large Spt (0.48
cm) but had D within 0.5 cm of Dpt for 11 of the 12 films; S pt was dominated by a single film. This
patient also had a large systematic difference from simulation, but
the diaphragm position was consistent with one exception.
|
||
|
||
Repeat EPID images
for patients 13_LU and 14_LU demonstrated the good intra-fraction
variability that has been reported previously,(12) with a maximum intra-fraction diaphragm
variation of 0.3 cm for 13_LU and 0.5 cm for 14_LU. Patient 15_LU
had three EPID imaging sessions. For two sessions, the maximum
intra-session variation was 0.3 cm. In the third session, 4 of 5
images had diaphragm positions within 0.5 cm of each other, but the
largest difference in this session was 0.9 cm due to one
outlier.
The PTV and beam apertures
for 5_LU were increased. To do this, we assumed that the gross tumor
volume (GTV) would shift rigidly in the SI direction by the same
amount as the diaphragm and enlarged the PTV to cover both the
planning and the shifted GTVs. The apertures were enlarged to cover
the new PTV in beam's-eye view. We enlarged apertures rather than
shift the isocenter with fixed apertures because we could not
predict diaphragm displacements later in the course of treatment,
and we did not want to make repeated field changes. Because
estimated normal tissue toxicity (lung and cord) was small for this
patient, we did not change the prescription dose. Patients 8_LU and
13_LU had tumors that were visible on the portal images and were
seen to be well within the field so no field changes were made. In
addition, no field changes were made for 14_LU and 17_LU.
B. Liver cancer patients
There were fluoroscopic movies for 8 of the 10
liver patients. Their free-breathing diaphragm excursion ranged from
1 cm to 4 cm, and gating reduced it to an average of 0.7 cm (range
0.4 cm to 1 cm), a statistically significant reduction (p < 10-3). The difference in diaphragm
excursion between the lung cancer and liver cancer patients was not
statistically
significant.
Dpt ranged from 0.79 cm superior to 0.78 cm
inferior of simulation. Averaging over the liver patients,D ±
1 SD was -0.08 cm ± 0.48 cm, and the average ±1 SD of Spt was 0.50 ± 0.19 cm. Although the gate was
around end-exhale, 3 patients (6_Li, 7_Li, and 8_Li) had systematic
diaphragm shifts superior of simulation. For 7 patients, Dpt was within 0.5 cm of
simulation, but 3 of these had large film-to-film variation as
indicated by S pt and the fact
that more than 30% of their films had D over 0.5 cm different
from Dpt. Spt ranged from 0.14 cm to 0.84 cm, and for
only one patient (7_Li) was D within 0.5 cm of Dpt for all the films. Although this patient
had a large systematic deviation from simulation, the value of
D was consistent over the course of treatment. The difference
between Dpt and Spt for the liver and lung patients is not
statistically significant.
The
liver cancer patients' results are tabulated in Table 2, and Dpt and Spt are plotted in Fig. 5. The target volume of
patient 3_Li crossed midline, so the displacements of both
diaphragms are included. Field and treatment plan changes based on
the diaphragm films were made during treatment for five patients:
2_Li, 3_Li, 4_Li, 7_Li, and 8_Li. As described for patient 5_LU, we
created new plans with enlarged PTVs and apertures. However, except
for patient 7_Li, we also decreased the total prescription dose to
respect liver tolerance.
FIG. 5. The mean and standard deviation of D (Dpt and Spt) for the liver cancer patients. Note that there are two sets of bars for patient 3, for whom both right and left diaphragms were monitored. |
||
C. Visual prompting
The average ±1 SD of Dpt over the 14 patients who had both audio and visual prompting throughout treatment was -0.02 ± 0.6 cm, and over those with audio prompting only, it was -0.19 ± 0.56 cm. The two patients who declined visual prompting are included in the audio-only group. The average ±1 SD of Spt over the patients with both types of prompting was 0.42 ± 0.12 cm and over those with audio prompting only, was 0.47 ± 0.16 cm. These differences were not statistically significant (two-sided t-test).
D. Clinical feasibility
The time to acquire and evaluate diaphragm films is not excessive, amounting to less than 5 min per film if only isocenter-to-diaphragm distance is examined. A film adds less than a minute to the patient's in-room time. The raw change in isocenter-to-diaphragm distance relative to simulation (no correction for setup error) can be rapidly determined by visual inspection aided by the grid. Determining setup error relative to bony landmarks can be time-consuming, depending on port film and DRR quality, but radiation oncologists can efficiently judge whether the setup error is clinically acceptable. In this study, setup error was examined with particular care in order to separate the interfractional performance of the RPM system from setup error. For purely clinical purposes, the raw isocenter-diaphragm distance gives sufficient information providing that setup error is within the physician's tolerance. The most time-consuming part of the process is discussing and replanning patients. However, we feel this is necessary to evaluate and, if possible, correct systematic errors introduced by respiratory gating based on an external marker. Extra time required for gated simulation and treatment(14,17) is an accepted cost of respiratory gating and is beyond the scope of this study of interfractional changes.
IV. DISCUSSION
Previous studies of respiratory gating with the RPM
system demonstrated good intra-fraction reproducibility of the
positions of diaphragm(12) and other
thoracic organs(21) as indicated by
repeat images during a single session. However, the goal of
respiratory gating is to reproduce tumor and normal tissue positions
from simulation throughout the course of treatment. Our observations
were qualitatively similar to those of Ford et al.(12) for the first 8 RPM-gated patients (4
liver, 4 lung) at our institution. They found that the absolute
value of Dpt exceeded 0.5 cm for 1
patient and exceeded 0.4 cm for 4, and that the average of
Spt over the 8 patients was 0.28
cm. For one patient with gate centered around end-exhale,
Dpt was systematically superior of
simulation by 0.6 cm. Because these results were obtained early in
our clinical gating experience, they might have been adversely
affected by inexperience or positively affected by strict physics
oversight. For the patients in the current study, gating was
integrated into the clinical process, and diaphragm filming
continued for the entire course of treatment. In this study, we
found that the absolute value of Dpt exceeded 0.4 cm for 10 of 31 patients, and
the mean diaphragm position was systematically superior of its
simulation position by 0.5 cm or more for 6
patients.
We observed a variety of
patient-specific patterns of diaphragm variability, as shown in Fig.
6, a chronological plot of D over the course of treatment for
4 patients. The preferred behavior, shown by patient 3_LU, is a
small systematic deviation and a small interfraction variation.
However, some patients have a large systematic deviation from
simulation with a small interfraction variation, as shown by patient
8_LU. There are also cases (patient 6_LU) with a large interfraction
variability where superior and inferior displacements approximately
cancel, resulting in a small systematic displacement. The most
difficult cases (patient 8_Li) have both large interfraction
variability and large systematic displacement.
FIG. 6. Chronological variation of D over the course of treatment for four patients. These show four qualitatively different types of variation in diaphragm position. |
||
Because there were
almost four times more patients in this study than in the study
reported in Ref. 12, we could more confidently examine the
population distribution of D. The systematic and random
deviations of D for the lung and liver patients are of
similar magnitude. One interpretation of this observation is that
there is a distribution of possible diaphragm positions that governs
both simulation and treatment. Simulation is a single sample from
the distribution, and each treatment is another sample. This
distribution need not be normal. The four behaviors shown in Fig. 6
would follow from such a model.
Our
expectation that the diaphragm films and the DRRs image
approximately the same part of the breathing cycle for breathing
periods (4 s to 6 s) and duty cycles (27% to 55%) characteristic of
our patients is based on two estimates. First, the average of D over the entire patient set is close to zero (-0.12 cm),
indicating that little or no systematic bias is introduced by
comparing diaphragm positions on the DRRs and the diaphragm films.
Second, the diaphragm spends similar time in the gate for the CT and
portal images. Slice acquisition on the PQ500 starts 330 ms after
the breathing trace enters the gate and takes 1 s. For a 5-s
breathing period and a 33% duty cycle, 1.7 s is spent in the gate,
and the slice is acquired approximately equally about the center of
the gate interval. For port films, the beam turns on when the trace
enters the gate. At the port-film mode dose rate of 100 MU/min, a 4
MU diaphragm film takes about 2.4 s (1.4 gate intervals), so the
film certainly includes the end-exhale position of the diaphragm
apex. For both film and DRRs, the apex density depends on how
quickly it moves through end-exhale, an effect that may bias both
film and DRR toward an estimated position inferior to true
end-exhale.
We used customized
voice instruction for all patients for two main reasons, as
described in Ref. 11. First, it substantially reduces the fraction
of treatment time that the beam is held off due to irregular
breathing. Second, it reduces cycle-to-cycle variation in the marker
position at end expiration, thus reducing the likelihood of waveform
drift with respect to the gating thresholds. Thus, it helps the
patient breath regularly throughout the course of treatment.
Although total breathing amplitude is increased, in Ref. 11 we found
that the diaphragm excursion within the gate is not adversely
affected by the larger amplitude but rather is comparable or
slightly reduced compared to the uninstructed
case.
We could not identify a
priori patients with significant interfraction diaphragm
variability. All the patients were able to tolerate the longer
simulation and approximately 5 min longer treatment time and were
willing and able to follow voice prompting. Patient 4_Li developed
ascites during treatment, a medical reason for a superior diaphragm
shift, and the stomach contents of 2_Li may have differed between
simulation and treatments. Otherwise, we saw no distinction between
patients with large and small interfraction changes. Large
systematic or random changes in D were of particular concern
for the liver patients because they were selected for gating to
reduce PTV margins. As a result of the diaphragm films, the PTVs and
field sizes were increased for 5 liver cancer patients and 1 lung
cancer patient.
In the future,
respiration-correlated CT (RCCT) imaging(22-25,27,28) of the GTV and diaphragm will
be helpful. RCCT acquires CT images for breathing phases covering
the whole breathing cycle and shows GTV displacement and deformation
and the GTV's relation to the diaphragm. If contrast is used to
visualize liver tumors, precise timing of the RCCT study relative to
the contrast administration is crucial. This may be possible with
the multislice scanner/cine method described by Pan et al.,(24) which acquires 1 cm of data (four
2.5-mm slices) per breathing cycle (~5 s). While end-exhale images
could be used for planning, the envelope of the GTVs at all
breathing phases within the gate would determine an intra-fractional
margin for motion within the gate. The population distribution of
diaphragm displacements acquired from the diaphragm films of
previous patients together with the relationship between diaphragm
and GTV from the patient's RCCT scan would determine a
patient-specific initial margin for interfractional variability. The
PTV would include further margin for setup error. After
approximately five daily diaphragm films (one week), the
interfraction margin could be changed on the basis of the observed
diaphragm displacements. For a nondeforming GTV and a large
systematic diaphragm shift with small random variation, an isocenter
shift might be sufficient. For patients with small interfraction
variability, margin reduction might be possible. Surveillance of
interfraction variability would continue at reduced frequency,
determined in part by imaging dose, to identify large diaphragm
variability later in the course of treatment. Currently, we cut back
to 1 or 2 per week. If we could conveniently use the EPID, the
imaging dose could be reduced to 1 MU per diaphragm "film."
Anticipating this capability, we are investigating the applicability
of alternative monitoring and correction strategies.(29)
RCCT
will not solve all interfractional variation problems. If Dpt is outside the range of
diaphragm displacements in the RCCT session, as for the 7 patients
whose diaphragms at treatment were significantly superior to their
end-exhale position at simulation, the GTV displacement would have
to be extrapolated from the RCCT images. For some patients, the
relationship between diaphragm and GTV displacements may change over
the course of treatment. And in general, it would be preferable to
image the tumor rather than the diaphragm surrogate. Developing the
ability to do this conveniently, at weekly or more frequent
intervals over the course of treatment, is a subject of active
research.(4,30-39)
V. CONCLUSION
Interfractional reproducibility of internal thoracic anatomy, as indicated by the diaphragm, is not assured by respiratory gating based on the motion of an external marker. Radiographic surveillance of gating patients throughout their course of treatment is needed to monitor interfractional variability.
ACKNOWLEDGMENTS
Supported in part by grant #PO1-CA-59017 from the National Cancer Institute, National Institutes of Health. We also acknowledge a research agreement with Varian Medical Systems.
REFERENCES
- Langen KM, Jones DTL. Organ motion and its management. Int J Radiat Oncol Biol Phys. 2001;50:265-278.
- Mechalakos J, Yorke E, Mageras G, et al. Dosimetric effect of respiratory motion in external beam radiotherapy of the lung. Radiother Oncol. 2004;71:191-200.
- Tada T, Minakuchi K, Fujioka T, et al. Lung cancer: Intermittent irradiation synchronized with respiratory motion-Results of a pilot study. Radiology. 1998;207:779-783.
- Shirato H, Shimizu S, Kunieda T, et al. Physical aspects of a real-time tumor-tracking system for gated radio-therapy. Int J Radiat Oncol Biol Phys. 2000;48:1187-1195.
- Kubo HD, Hill BC. Respiration gated radiotherapy treatment: A technical study. Phys Med Biol. 1996;41:83-91.
- Kubo H, Len P, Minohara S, Mostafavi H. Breathing-synchronized radiotherapy program at the University of California Davis Cancer Center. Med Phys. 2000;27:346-353.
- Ohara K, Okumura T, Akisada M, et al. Irradiation synchronized with respiration gate. Int J Radiat Oncol Biol Phys. 1989;17:853-857.
- Okumara T, Tsuji H, Hayakawa Y. Respirationgated irradiation system for proton radiotherapy. In: North Western Medical Physics Dept., Christie Hospital, Manchester, editors. Proceedings of the 11th international conference on the use of computers in radiation therapy; 1994, pp. 358-359.
- Zhang T, Keller H, O'Brien MJ, Mackie TR, Paliwal B. Application of the spirometer in respiratory gated radio-therapy. Med Phys. 2003;30:3165-3171.
- Ramsey CR, Cordrey IL, Oliver AL. A comparison of beam characteristics for gated and nongated clinical x-ray beams. Med Phys. 1999;26:2086-2091.
- Mageras GS, Yorke E, Rosenzweig K, et al. Fluoroscopic evaluation of diaphragmatic motion reduction with a respiratory gated radiotherapy system. J Appl Clin Med Phys. 2001;2:191-200.
- Ford E, Mageras GS, Yorke E, Rosenzweig KE, Wagman R, Ling CC. Evaluation of respiratory movement during gated radiotherapy using film and electronic portal imaging. Int J Radiat Oncol Biol Phys. 2002;52:522-531.
- Vedam SS, Kini VR, Keall PJ, Ramakrishnan V, Mostafavi H, Mohan R. Quantifying the predictability of diaphragm motion during respiration with a noninvasive external marker. Med Phys. 2003;30:505-513.
- Mageras GS, Yorke E. Deep inspiration breath hold and respiratory gating strategies for reducing organ motion in radiation treatment. Semin Radiat Oncol. 2004;14:65-75.
- Vedam SS, Keall PJ, Kini VR, Mohan R. Determining parameters for respiration-gated radiotherapy. Med Phys. 2002;28:2139-2146.
- Kini VR, Vedam SS, Keall PJ, Arthur DW, Mohan R. A dynamic non-invasive technique for predicting organ motion in respiratory-gated radiotherapy of the chest. Int J Radiat Oncol Biol Phys. 2001;51:25-26.
- Kini VR, Vedam SS, Keall PJ, Patil S, Chen C, Mohan R. Patient training in respiratory-gated radiotherapy. Med Dosim. 2003;28:7-11.
- Balter JM, Dawson LA, Kazanjian S, et al. Determination of ventilatory liver movement via radiographic evaluation of diaphragm position. Int J Radiat Oncol Biol Phys. 2001;51:267-270.
- Mah D, Hanley J, Rosenzweig K, et al. Technical aspects of the deep inspiration breath hold technique in the treatment of thoracic cancer. Int J Radiat Oncol Biol Phys. 2000;48:1175-1185.
- Stevens CW, Munder RF, Forster KM, et al. Respiratory-driven lung tumor motion is independent of tumor size, tumor location, and pulmonary function. Int J Radiat Oncol Biol Phys. 2001;51:62-68.
- Wagman R, Yorke E, Giraud P, Mageras GS, Minsky B, Rosenzweig KE. Reproducibility of organ position with respiratory gating for liver tumors: Use in dose escalation. Int J Radiat Oncol Biol Phys. 2003;55:659-668.
- Ford EC, Mageras GS, Yorke E, Ling CC. Respiration-correlated spiral CT: A method of measuring respiratory-induced anatomic motion for radiation treatment planning. Med Phys. 2003;30:88-97.
- Vedam SS, Keall PJ, Kini VR, Mostafavi H, Shukla HP, Mohan R. Acquiring a four-dimensional computed tomography dataset using an external respiratory signal. Phys Med Biol. 2003;48:45-62.
- Pan T, Lee TY, Rietzel E, Chen GT. 4D-CT imaging of a volume influenced by respiratory motion on multi-slice CT. Med Phys. 2004;31:333-340.
- Mageras G, Pevsner A, Yorke E, et al. Measurement of lung tumor motion using respiration-correlated CT. Int J Radiat Oncol Biol Phys. 2004; 60(3):933-941.
- Rosenzweig KE, Hanley J, Mah D, et al. The deep inspiration breath hold technique in the treatment of inoperable non-small cell lung cancer. Int J Radiat Oncol Biol Phys. 2000;48:81-87.
- Rietzel E, Chen GT, Doppke KP, Pan T, Choi NC, Willett CG. 4D computed tomography for treatment planning. Int J Radiat Oncol Biol Phys. 2003; 57(2 Suppl):S232-S233.
- Low DA, Nystrom M, Kalinin E, et al. A method for the reconstruction of four-dimensional synchronized CT scans acquired during free breathing. Med Phys. 2003;30:1254-1263.
- Brame R, Mageras G, Lovelock DM, Hua C, Zelefsky MJ, Ling C. A Bayesian approach to management of setup error and organ motion using offline monitoring and correction (abstract). Med Phys. 2003;30:1473.
- Balter JM, Brock KK, Litzenberg DW, et al. Daily targeting of intrahepatic tumors for radiotherapy. Int J Radiat Oncol Biol Phys. 2002;52:266-271.
- Erridge SC, Seppenwoolde Y, Muller SH, et al. Portal imaging to assess set-up errors, tumor motion and tumor shrinkage during conformal radiotherapy of non-small cell lung cancer. Radiother Oncol. 2003;66:75-85.
- Ford EC, Chang J, Mueller K, et al. Cone-beam CT with megavoltage beams and an amorphous silicon electronic portal imaging device: Potential for verification of radiotherapy of lung cancer. Med Phys. 2002;29:2913-2924.
- Jaffray DA, Siewerdsen JH, Wong JW, Martinez AA. Flat-panel cone-beam computed tomography for image-guided radiation therapy. Int J Radiat Oncol Biol Phys. 2002;53:1337-1349.
- Litzenberg D, Dawson LA, Sandler H, et al. Daily prostate targeting using implanted radiopaque markers. Int J Radiat Oncol Biol Phys. 2002;52:699-703.
- Mackie TR, Kapatoes J, Ruchala L, et al. Image guidance for precise conformal radiotherapy. Int J Radiat Oncol Biol Phys. 2003;56:89-105.
- Ozhasoglu C, Murphy MJ. Issues in respiratory motion compensation during external-beam radiotherapy. Int J Radiat Oncol Biol Phys. 2002;52:1389-1399.
- Rodebaugh RF, Crownover RL, Weinhous MS, et al. The accuracy of tracking lung tumors with the cyberknife. Int J Radiat Oncol Biol Phys. 2001;51:24-25.
- Shimizu S, Shirato H, Ogura S, et al. Detection of lung tumor movement in real-time tumor-tracking radio-therapy. Int J Radiat Oncol Biol Phys. 2001;51:304-310.
- Shirato H, Harada T, Harabayashi T, et al. Feasibility of insertion/implantation of 2.0-mm-diameter gold internal fiducial markers for precise setup and real-time tumor tracking in radiotherapy. Int J Radiat Oncol Biol Phys. 2003;56:240-247.
© 2005 Am. Coll. Med. Phys.