| Literature DB >> 25493507 |
Prema Rassiah-Szegedi1, Martin Szegedi, Vikren Sarkar, Seth Streitmatter, Y Jessica Huang, Hui Zhao, Bill Salter.
Abstract
The purpose of this work is to investigate if the change in plan quality with the finer leaf resolution and lower leakage of the 160 MLC would be dosimetrically significant for head and neck intensity-modulated radiation therapy (IMRT) treat- ment plans. The 160 MLC consisting of 80 leaves of 0.5 cm on each bank, a leaf span of 20 cm, and leakage of less than 0.37% without additional backup jaws was compared against the 120 Millennium MLC with 60 leaves of 0.5 and 1.0 cm, a leaf span of 14.5 cm, and leakage of 2.0%. CT image sets of 16 patients previously treated for stage III and IV head and neck carcinomas were replanned on Prowess 5.0 and Eclipse 11.0 using the 160 MLC and the 120 MLC. IMRT constraints for both sets of 6 MV plans were identical and based on RTOG 0522. Dose-volume histograms (DVHs), minimum dose, mean dose, maximum dose, and dose to 1 cc to the organ at risks (OAR) and the planning target volume, as recommended by QUANTEC 2010, were compared. Both collimators were able to achieve the target dose to the PTVs. The dose to the organs at risk (brainstem, spinal cord, parotids, and larynx) were 1%-12% (i.e., 0.5-8 Gy for a 70 Gy prescription) lower with the 160 MLC compared to the 120 MLC, depending on the proximity of the organ to the target. The large field HN plans generated with the 160 MLC were dosimetrically advantageous for critical structures, especially those located further away from the central axis, without compromising the target volume.Entities:
Mesh:
Year: 2014 PMID: 25493507 PMCID: PMC5711108 DOI: 10.1120/jacmp.v15i6.4770
Source DB: PubMed Journal: J Appl Clin Med Phys ISSN: 1526-9914 Impact factor: 2.102
A comparative list of some of the characteristics of the two MLCs. Both the 160 MLC and the 120 MLC are in clinical use in our department.
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| Source collimator distance | 460 mm | 535 mm |
| Patient clearance | 430 mm | 334 mm |
| Leaf resolution | 5 mm leaf entire 40 cm field | 5 mm central 40 leaves and 10 mm remaining outer leaf |
| Leaf End | S‐shaped | C‐shaped |
| Leaf height | 95 mm | 55 mm |
| Penumbra (80 ‐ 20%) | 3.6 mm | 3.2 mm |
| Leakage and transmission | 0.37% | 2.00% |
| Inter‐digitization | Yes | Yes |
| Method to avoid a direct ray in between leaves | Tilted alternating pattern of upper and lower leaf | tongue and groove |
| Max Leaf Speed |
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| Leaf Span | 200 mm | 145 mm |
| Step and shoot IMRT | Yes | Yes |
| Dynamic IMRT | No | Yes |
The agreement between measured and calculated dose for two IMRT plans with the Prowess planning system.
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| Plan#1 | Ion chamber deviation / % (measured ‐ calculated) | 1.4 |
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| Gamma index (3%/mm) | 92.5 | 92.7 | |
| Plan#2 | Ion chamber deviation / % (measured ‐ calculated) |
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| Gamma index (3%/mm) | 94.5 | 93.3 | |
Difference (dose 120 MLC ‐ dose 160 MLC) maximum, mean, and dose in brainstem between the two collimators.
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| Average Difference/Gy (Range) | 2.0 | 0.6 | 1.4 | 2.6 | 1.3 | 1.8 |
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| (0.2 ‐3.8) | (0.1–4.4) | |
| p‐value | 0.04 | 0.03 | 0.04 | 0.04 | 0.01 | 0.02 |
Difference (dose 120 MLC ‐ dose 160 MLC) in maximum and for spinal cord dose between the two collimators.
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| Average Difference/Gy (Range) | 1.6 | 1.7 | 1.5 | 1.2 |
| (0.0–8.3) | (0.5– 6.6) | (0.5–5.6) | (0.5–5.5) | |
| p‐value | 0.01 | 0.01 | 0.04 | 0.02 |
Difference (dose 120 MLC ‐ dose 160 MLC) in mean dose in the left parotid, right parotid, and larynx between the two collimators.
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| Average Difference/Gy (Range) | 0.7 | 1.1 | 1.7 | 1.7 | 1.3 | 1.8 |
| (0.4–3.1) | (0.2–3.9) | (0.4–4.1) | (0.7–6.9) | (0.5–5.0) | (0.2–5.2) | |
| p‐value | 0.01 | 0.1 | 0.01 | 0.01 | 0.01 | 0.02 |
Figure 1Typical DVH for plans calculated with the 160 MLC and 120 MLC.
Figure 2The left (a) and right (b) panels show the comparative dose distribution for the 160 MLC and 120 MLC, respectively. Note the dose sparing on the larynx and spinal cord with the 160 MLC.
Figure 3A typical fluence map for the 160 MLC (a) and 120 MLC (b) for the same patient at 180° beam angle.