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 in | Medical physics (Lancaster) Vol. 39; no. 2; pp. 671 - 675 |
|---|---|
| Main Authors | , , |
| Format | Journal Article |
| Language | English |
| Published |
United States
American Association of Physicists in Medicine
01.02.2012
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| Subjects | |
| Online Access | Get full text |
| ISSN | 0094-2405 2473-4209 |
| DOI | 10.1118/1.3675405 |
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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 |
| Author_xml | – sequence: 1 givenname: Minoru surname: Tajiri fullname: Tajiri, Minoru email: m_tajiri@nirs.go.jp organization: Research Center Hospital for Charged Particle Therapy, National Institute of Radiological Sciences, 4-9-1, Anagawa, Inage-ku, Chiba 263-8555, Japan – sequence: 2 givenname: Yuji surname: Tokiya fullname: Tokiya, Yuji organization: International University of Health and Welfare, 1-4-3, Mita, Minato-ku, Tokyo 108-8329, Japan – sequence: 3 givenname: Kazuhiro surname: Watanabe fullname: Watanabe, Kazuhiro organization: Research Center Hospital for Charged Particle Therapy, National Institute of Radiological Sciences, 4-9-1, Anagawa, Inage-ku, Chiba 263-8555, Japan |
| BackLink | https://www.ncbi.nlm.nih.gov/pubmed/22320776$$D View this record in MEDLINE/PubMed https://www.osti.gov/biblio/22098754$$D View this record in Osti.gov |
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| Keywords | output variation rectangular field monitor-backscatter effect equivalent square field in-air output ratio |
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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 |
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