Correction method for in-air output ratio for output variations occurring with changes in backscattered radiation

Purpose: The in-air output ratio (Sc) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known that Sc obtained using an equivalent square field formula differs slightly from the measured Sc. Though several correction methods have been suggested...

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Published inMedical physics (Lancaster) Vol. 39; no. 2; pp. 671 - 675
Main Authors Tajiri, Minoru, Tokiya, Yuji, Watanabe, Kazuhiro
Format Journal Article
LanguageEnglish
Published United States American Association of Physicists in Medicine 01.02.2012
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ISSN0094-2405
2473-4209
DOI10.1118/1.3675405

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Abstract Purpose: The in-air output ratio (Sc) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known that Sc obtained using an equivalent square field formula differs slightly from the measured Sc. Though several correction methods have been suggested for the monitor-backscatter effect, the authors propose a more simple correction method for a rectangular field. Methods: For rectangular fields and equivalent square fields, the authors assumed that the output variation was the product of six output variations for each backscattering area at the top of the collimator jaws, and the correction factor was the ratio of the output variation for a rectangular field to the output variation for an equivalent square field. The output variation was measured by using a telescope measurement. Results: The differences between the measured and corrected Sc ranged from −0.20% to 0.28% for symmetric rectangular fields by applying the correction factor to Sc obtained using an equivalent square field formula. This correction method is also available for asymmetric rectangular fields. Conclusions: The authors propose a method to correct Sc obtained using an equivalent square field formula, and a method to obtain the output variation for a field defined by collimator jaws.
AbstractList Purpose: The in-air output ratio (Sc) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known that Sc obtained using an equivalent square field formula differs slightly from the measured Sc. Though several correction methods have been suggested for the monitor-backscatter effect, the authors propose a more simple correction method for a rectangular field. Methods: For rectangular fields and equivalent square fields, the authors assumed that the output variation was the product of six output variations for each backscattering area at the top of the collimator jaws, and the correction factor was the ratio of the output variation for a rectangular field to the output variation for an equivalent square field. The output variation was measured by using a telescope measurement. Results: The differences between the measured and corrected Sc ranged from −0.20% to 0.28% for symmetric rectangular fields by applying the correction factor to Sc obtained using an equivalent square field formula. This correction method is also available for asymmetric rectangular fields. Conclusions: The authors propose a method to correct Sc obtained using an equivalent square field formula, and a method to obtain the output variation for a field defined by collimator jaws.
Purpose: The in-air output ratio (S{sub c}) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known that S{sub c} obtained using an equivalent square field formula differs slightly from the measured S{sub c}. Though several correction methods have been suggested for the monitor-backscatter effect, the authors propose a more simple correction method for a rectangular field. Methods: For rectangular fields and equivalent square fields, the authors assumed that the output variation was the product of six output variations for each backscattering area at the top of the collimator jaws, and the correction factor was the ratio of the output variation for a rectangular field to the output variation for an equivalent square field. The output variation was measured by using a telescope measurement. Results: The differences between the measured and corrected S{sub c} ranged from -0.20% to 0.28% for symmetric rectangular fields by applying the correction factor to S{sub c} obtained using an equivalent square field formula. This correction method is also available for asymmetric rectangular fields. Conclusions: The authors propose a method to correct S{sub c} obtained using an equivalent square field formula, and a method to obtain the output variation for a field defined by collimator jaws.
Purpose: The in-air output ratio (S c ) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known that S c obtained using an equivalent square field formula differs slightly from the measured S c . Though several correction methods have been suggested for the monitor-backscatter effect, the authors propose a more simple correction method for a rectangular field. Methods: For rectangular fields and equivalent square fields, the authors assumed that the output variation was the product of six output variations for each backscattering area at the top of the collimator jaws, and the correction factor was the ratio of the output variation for a rectangular field to the output variation for an equivalent square field. The output variation was measured by using a telescope measurement. Results: The differences between the measured and corrected S c ranged from −0.20% to 0.28% for symmetric rectangular fields by applying the correction factor to S c obtained using an equivalent square field formula. This correction method is also available for asymmetric rectangular fields. Conclusions: The authors propose a method to correct S c obtained using an equivalent square field formula, and a method to obtain the output variation for a field defined by collimator jaws.
The in-air output ratio (S(c)) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known that S(c) obtained using an equivalent square field formula differs slightly from the measured S(c). Though several correction methods have been suggested for the monitor-backscatter effect, the authors propose a more simple correction method for a rectangular field.PURPOSEThe in-air output ratio (S(c)) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known that S(c) obtained using an equivalent square field formula differs slightly from the measured S(c). Though several correction methods have been suggested for the monitor-backscatter effect, the authors propose a more simple correction method for a rectangular field.For rectangular fields and equivalent square fields, the authors assumed that the output variation was the product of six output variations for each backscattering area at the top of the collimator jaws, and the correction factor was the ratio of the output variation for a rectangular field to the output variation for an equivalent square field. The output variation was measured by using a telescope measurement.METHODSFor rectangular fields and equivalent square fields, the authors assumed that the output variation was the product of six output variations for each backscattering area at the top of the collimator jaws, and the correction factor was the ratio of the output variation for a rectangular field to the output variation for an equivalent square field. The output variation was measured by using a telescope measurement.The differences between the measured and corrected S(c) ranged from -0.20% to 0.28% for symmetric rectangular fields by applying the correction factor to S(c) obtained using an equivalent square field formula. This correction method is also available for asymmetric rectangular fields.RESULTSThe differences between the measured and corrected S(c) ranged from -0.20% to 0.28% for symmetric rectangular fields by applying the correction factor to S(c) obtained using an equivalent square field formula. This correction method is also available for asymmetric rectangular fields.The authors propose a method to correct S(c) obtained using an equivalent square field formula, and a method to obtain the output variation for a field defined by collimator jaws.CONCLUSIONSThe authors propose a method to correct S(c) obtained using an equivalent square field formula, and a method to obtain the output variation for a field defined by collimator jaws.
The in-air output ratio (S(c)) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known that S(c) obtained using an equivalent square field formula differs slightly from the measured S(c). Though several correction methods have been suggested for the monitor-backscatter effect, the authors propose a more simple correction method for a rectangular field. For rectangular fields and equivalent square fields, the authors assumed that the output variation was the product of six output variations for each backscattering area at the top of the collimator jaws, and the correction factor was the ratio of the output variation for a rectangular field to the output variation for an equivalent square field. The output variation was measured by using a telescope measurement. The differences between the measured and corrected S(c) ranged from -0.20% to 0.28% for symmetric rectangular fields by applying the correction factor to S(c) obtained using an equivalent square field formula. This correction method is also available for asymmetric rectangular fields. The authors propose a method to correct S(c) obtained using an equivalent square field formula, and a method to obtain the output variation for a field defined by collimator jaws.
Author Tokiya, Yuji
Watanabe, Kazuhiro
Tajiri, Minoru
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Issue 2
Keywords output variation
rectangular field
monitor-backscatter effect
equivalent square field
in-air output ratio
Language English
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Snippet Purpose: The in-air output ratio (Sc) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known that Sc...
Purpose: The in-air output ratio (S c ) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known that S...
Purpose: The in‐air output ratio (Sc) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well‐known that Sc...
The in-air output ratio (S(c)) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known that S(c)...
Purpose: The in-air output ratio (S{sub c}) for a rectangular field is usually obtained using an equivalent square field formula. However, it is well-known...
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SubjectTerms Air
ASYMMETRY
backscatter
BACKSCATTERING
COLLIMATORS
Computer Simulation
Conformal radiation treatment
CORRECTIONS
equivalent square field
Field size
in-air output ratio
Ionization chambers
Lead
Linear accelerators
Models, Theoretical
monitor-backscatter effect
output variation
Photons
Polynomials
radiation therapy
RADIOLOGY AND NUCLEAR MEDICINE
Radiometry - methods
RADIOTHERAPY
Radiotherapy, Computer-Assisted - methods
Radiotherapy, Conformal - methods
rectangular field
Scattering, Radiation
SYMMETRY
Telescopes
X‐ray scattering
X‐rays
Title Correction method for in-air output ratio for output variations occurring with changes in backscattered radiation
URI http://dx.doi.org/10.1118/1.3675405
https://onlinelibrary.wiley.com/doi/abs/10.1118%2F1.3675405
https://www.ncbi.nlm.nih.gov/pubmed/22320776
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