Evidence map›Paper›PMID 39733431›Full record

ArticleAsian Pacific journal of cancer prevention : APJCP2024

Dosimetric Evaluation of Different Algorithms on Heterogeneous Slab Phantom Using CMS XiO and MONACO Treatment Planning System for 4MV, 6MV and 15MV Beam Energy: An Institutional Study.

Ajay Katake, Lalit Kumar, Balbir Singh, Nijun Mishra, Pradeep Gurjar, Rajesh Vashistha, Deepak Basandrai

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Article in Asian Pacific journal of cancer prevention : APJCP, 2024. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Not yet cited in PubMed.

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5 · Who and what money

Authors and funding

7 authors.

Ajay KatakeDepartment of Physics, Lovely Professional University, Phagwara, India.
Lalit KumarDepartment of Radiation Oncology, Max Super speciality Hospital, Saket, India.ORCID 0000-0001-7753-253X
Balbir SinghDepartment of Radiation Oncology, SLBSGMC & H, Nerchowk, Mandi, India.ORCID 0000-0003-1818-5851
Nijun MishraDepartment of Radiation Oncology, GCRI-BCCRI, Bhavnagar, India.
Pradeep GurjarDepartment of Radiation Oncology, Max Super Speciality Hospital, Bathinda, India.
Rajesh VashisthaDepartment of Radiation Oncology, Max Super Speciality Hospital, Bathinda, India.ORCID 0000-0001-6898-2440
Deepak BasandraiDepartment of Physics, Lovely Professional University, Phagwara, India.ORCID 0000-0001-5762-4648

Funding

No grant is acknowledged in the PubMed record.

6 · The paper itself

Abstract

aimTo study the dosimetric behavior of dose computational algorithms in inhomogeneous medium using CMS XiO and MONACO treatment planning system (TPS) for 4 megavoltage (MV), 6 MV and 15 MV photon beam energies. MATERIAL AND

methodsStyrofoam blocks of thickness 1.90 cm, 3.8 cm and 5.70 cm was used to introduce inhomogeneity in a slab phantom. Wipro GE computed tomography (CT) scanner was used to scan the phantom. Doses were computed on the central axis of the beam using convolution (C), superposition (S), fast superposition (FS), collapsed cone convolution (CCC) and monte carlo (MC) algorithms for field geometries of 5x5 cm2 and 10x10 cm2 for above said photon beam energies, respectively. An Ion chamber (IC) of 0.6 cc volume was used for the dose measurements. The deviation between measured and TPS computed doses were recorded.

resultsThe PDD (Percentage depth dose) data obtained from the TPS (calculated data) and LINAC (measured data) was used for comparison based on different algorithms in order to calculate the percentage of maximum deviation (PMD). The PMD in MC algorithm were calculated for field sizes of 5x5 cm2 and 10x10 cm2 are found to be in ranging from 0.73% to -4.49% for 4MV,  1.62% to -2.42% for 6MV and 4.53% to -1.47%  for 15 MV for 1.90 cm air gap, 2.21% to -3.75% for 4MV, 3.87% to -2.88% for 6 MV and 4.87% to -3.46%  for 15 MV for 3.80 cm air gap, 2.77% to -4.66% for 4MV, 3.87% to -2.86% for 6 MV and 5.66% to -4.92% for 15 MV for 5.70cm air gap which is less as compared to CCC, C, FS, and S algorithms.

conclusionThe comparison of C, S, FS, CCC and MC algorithms demonstrated that MC having better agreement with IC measurements. In conclusion, MC is a superior option for dose computation, particularly in the presence of low-density heterogeneities.

Indexed as

AlgorithmsMonte Carlo MethodPhantoms, ImagingRadiotherapy DosageRadiotherapy Planning, Computer-AssistedHumansParticle AcceleratorsPhotonsRadiometryRadiotherapy, Intensity-ModulatedTomography, X-Ray ComputedAir gapKeywords:- Monte Carlophantom and heterogeneity

Identifiers

PMID39733431
PMCPMC12008326

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Read under generation 80e0d062 · epoch 390. Bibliography from PubMed, PubMed Central and OpenAlex; grants from NIH RePORTER; trial links from ClinicalTrials.gov; estimates, votes and beliefs from the OpenQuestion graph.