Investigating the use of ionization chamber and solid-state detectors to evaluate kerma-area product meter accuracy under TG-125 geometry across variable field of views

IF 2.2 4区 医学 Q3 RADIOLOGY, NUCLEAR MEDICINE & MEDICAL IMAGING
Atsushi Fukuda, Pei-Jan Paul Lin
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However, it is unclear that external detectors could evaluate the KAP meter accuracy under the TG-125 geometry.</p>\n </section>\n \n <section>\n \n <h3> Purpose</h3>\n \n <p>This study investigated whether the reference air kerma rate (<span></span><math>\n <semantics>\n <msub>\n <mover>\n <mi>K</mi>\n <mo>̇</mo>\n </mover>\n <mrow>\n <mi>a</mi>\n <mo>,</mo>\n <mi>r</mi>\n </mrow>\n </msub>\n <annotation>${\\dot{K} _{a,r}}$</annotation>\n </semantics></math>) values of the KAP meter increase with increasing field of view (FOV) and whether an external ionization chamber and solid-state detector (SSD) could be used to evaluate KAP meter accuracy in TG-125 geometry.</p>\n </section>\n \n <section>\n \n <h3> Methods</h3>\n \n <p>An ionization chamber and three different SSDs (Radcal AGMS-DM+, Raysafe X2 R/F sensor, and RTI Dose Probe) were placed at the patient entrance reference point in a C-arm fluoroscopic system, and measurements were taken at FOV settings of 18, 25, 34, and 42 cm using both the TG-190 and TG-125 geometries. The <span></span><math>\n <semantics>\n <msub>\n <mover>\n <mi>K</mi>\n <mo>̇</mo>\n </mover>\n <mrow>\n <mi>a</mi>\n <mo>,</mo>\n <mi>r</mi>\n </mrow>\n </msub>\n <annotation>$\\dot{K} _{a,r}$</annotation>\n </semantics></math>, incident air kerma rate (<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mover>\n <mi>K</mi>\n <mo>̇</mo>\n </mover>\n <mrow>\n <mi>a</mi>\n <mo>,</mo>\n <mi>i</mi>\n </mrow>\n </msub>\n <mrow>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation>$\\dot{K} _{a,i})$</annotation>\n </semantics></math>, and entrance surface air kerma rate (<span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mover>\n <mi>K</mi>\n <mo>̇</mo>\n </mover>\n <mrow>\n <mi>a</mi>\n <mo>,</mo>\n <mi>e</mi>\n </mrow>\n </msub>\n <mrow>\n <mo>)</mo>\n </mrow>\n </mrow>\n <annotation>$\\dot{K} _{a,e})$</annotation>\n </semantics></math> values were recorded simultaneously and compared. The measurement data were used to calculate the backscatter factor.</p>\n </section>\n \n <section>\n \n <h3> Results</h3>\n \n <p>The <span></span><math>\n <semantics>\n <msub>\n <mover>\n <mi>K</mi>\n <mo>̇</mo>\n </mover>\n <mrow>\n <mi>a</mi>\n <mo>,</mo>\n <mi>r</mi>\n </mrow>\n </msub>\n <annotation>${\\dot{K} _{a,r}}$</annotation>\n </semantics></math> increased linearly with the relative X-ray output, and their slopes significantly increased with the FOV. The <span></span><math>\n <semantics>\n <msub>\n <mover>\n <mi>K</mi>\n <mo>̇</mo>\n </mover>\n <mrow>\n <mi>a</mi>\n <mo>,</mo>\n <mi>e</mi>\n </mrow>\n </msub>\n <annotation>${\\dot{K} _{a,e}}$</annotation>\n </semantics></math> values of the ionization chamber increased with the FOV; however, the <span></span><math>\n <semantics>\n <msub>\n <mover>\n <mi>K</mi>\n <mo>̇</mo>\n </mover>\n <mrow>\n <mi>a</mi>\n <mo>,</mo>\n <mi>i</mi>\n </mrow>\n </msub>\n <annotation>$\\dot{K} _{a,i}$</annotation>\n </semantics></math> values of the ionization chamber, <span></span><math>\n <semantics>\n <msub>\n <mover>\n <mi>K</mi>\n <mo>̇</mo>\n </mover>\n <mrow>\n <mi>a</mi>\n <mo>,</mo>\n <mi>i</mi>\n </mrow>\n </msub>\n <annotation>$\\dot{K} _{a,i}$</annotation>\n </semantics></math> and <span></span><math>\n <semantics>\n <msub>\n <mover>\n <mi>K</mi>\n <mo>̇</mo>\n </mover>\n <mrow>\n <mi>a</mi>\n <mo>,</mo>\n <mi>e</mi>\n </mrow>\n </msub>\n <annotation>$\\dot{K} _{a,e}$</annotation>\n </semantics></math> values of the SSDs were not dependent on the FOV and were nearly identical to each other. Although the backscatter factor for the KAP meter and ionization chamber increased with the FOV, the backscatter for the SSDs were close to unity in all FOVs and no significant difference was observed.</p>\n </section>\n \n <section>\n \n <h3> Conclusions</h3>\n \n <p>The results indicated that the <span></span><math>\n <semantics>\n <msub>\n <mover>\n <mi>K</mi>\n <mo>̇</mo>\n </mover>\n <mrow>\n <mi>a</mi>\n <mo>,</mo>\n <mi>r</mi>\n </mrow>\n </msub>\n <annotation>${\\dot{K} _{a,r}}$</annotation>\n </semantics></math> values of KAP meter were increased with the FOV. Furthermore, the SSDs could be utilized to evaluate the KAP meter accuracy in TG-125 geometry.</p>\n </section>\n </div>","PeriodicalId":14989,"journal":{"name":"Journal of Applied Clinical Medical Physics","volume":"26 10","pages":""},"PeriodicalIF":2.2000,"publicationDate":"2025-10-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://aapm.onlinelibrary.wiley.com/doi/epdf/10.1002/acm2.70281","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Applied Clinical Medical Physics","FirstCategoryId":"3","ListUrlMain":"https://aapm.onlinelibrary.wiley.com/doi/10.1002/acm2.70281","RegionNum":4,"RegionCategory":"医学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"RADIOLOGY, NUCLEAR MEDICINE & MEDICAL IMAGING","Score":null,"Total":0}
引用次数: 0

Abstract

Background

A kerma-area product (KAP) meter has been installed in a fluoroscopic system, and its accuracy has been evaluated in task group (TG)-190 geometry using an external detector. However, it is unclear that external detectors could evaluate the KAP meter accuracy under the TG-125 geometry.

Purpose

This study investigated whether the reference air kerma rate ( K ̇ a , r ${\dot{K} _{a,r}}$ ) values of the KAP meter increase with increasing field of view (FOV) and whether an external ionization chamber and solid-state detector (SSD) could be used to evaluate KAP meter accuracy in TG-125 geometry.

Methods

An ionization chamber and three different SSDs (Radcal AGMS-DM+, Raysafe X2 R/F sensor, and RTI Dose Probe) were placed at the patient entrance reference point in a C-arm fluoroscopic system, and measurements were taken at FOV settings of 18, 25, 34, and 42 cm using both the TG-190 and TG-125 geometries. The K ̇ a , r $\dot{K} _{a,r}$ , incident air kerma rate ( K ̇ a , i ) $\dot{K} _{a,i})$ , and entrance surface air kerma rate ( K ̇ a , e ) $\dot{K} _{a,e})$ values were recorded simultaneously and compared. The measurement data were used to calculate the backscatter factor.

Results

The K ̇ a , r ${\dot{K} _{a,r}}$ increased linearly with the relative X-ray output, and their slopes significantly increased with the FOV. The K ̇ a , e ${\dot{K} _{a,e}}$ values of the ionization chamber increased with the FOV; however, the K ̇ a , i $\dot{K} _{a,i}$ values of the ionization chamber, K ̇ a , i $\dot{K} _{a,i}$ and K ̇ a , e $\dot{K} _{a,e}$ values of the SSDs were not dependent on the FOV and were nearly identical to each other. Although the backscatter factor for the KAP meter and ionization chamber increased with the FOV, the backscatter for the SSDs were close to unity in all FOVs and no significant difference was observed.

Conclusions

The results indicated that the K ̇ a , r ${\dot{K} _{a,r}}$ values of KAP meter were increased with the FOV. Furthermore, the SSDs could be utilized to evaluate the KAP meter accuracy in TG-125 geometry.

Abstract Image

研究使用电离室和固态探测器在TG-125几何形状下跨可变视场评估克尔玛面积积计精度。
背景:克尔玛面积积(KAP)计已安装在荧光系统中,其准确性已在任务组(TG)-190几何使用外部检测器进行评估。然而,目前尚不清楚外部探测器能否评估TG-125几何结构下KAP仪表的精度。目的:研究KAP计的参考空气角率(K³a,r ${\dot{K} _{a,r}}$)值是否随视场(FOV)的增加而增加,以及是否可以使用外电离室和固态探测器(SSD)来评估TG-125几何形状下KAP计的精度。方法:将电离室和三个不同的ssd (Radcal AGMS-DM+, Raysafe X2 R/F传感器和RTI剂量探针)放置在c臂透视系统的患者入口参考点,并使用TG-190和TG-125几何形状在18、25、34和42 cm的视场设置下进行测量。同时记录K (a),r $\dot{K} _{a,r}$,入射空气流速(K (a,i)$ \dot{K} _{a,i})$和入口表面空气流速(K (a,e)$ \dot{K} _{a,e})$值并进行比较。利用测量数据计算后向散射系数。结果:K³a,r ${\dot{K} _{a,r}}$随相对x射线输出呈线性增加,斜率随视场显著增加。电离室的K³a,e ${\dot{K} _{a,e}}$值随着视场的增大而增大;然而,电离室的K (a),i $\dot{K} a,i}$值,ssd的K (a),i $\dot{K} a,i}$和K (a),e $\dot{K} a,e}$值不依赖于视场,彼此几乎相同。虽然KAP计和电离室的后向散射系数随视场的增大而增大,但ssd盘的后向散射系数在各视场内基本一致,无显著差异。结论:结果表明KAP仪的K (a),r ${\dot{K} _{a,r}}$值随视场的增大而增大。此外,ssd可用于评估TG-125几何形状的KAP仪表精度。
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来源期刊
CiteScore
3.60
自引率
19.00%
发文量
331
审稿时长
3 months
期刊介绍: Journal of Applied Clinical Medical Physics is an international Open Access publication dedicated to clinical medical physics. JACMP welcomes original contributions dealing with all aspects of medical physics from scientists working in the clinical medical physics around the world. JACMP accepts only online submission. JACMP will publish: -Original Contributions: Peer-reviewed, investigations that represent new and significant contributions to the field. Recommended word count: up to 7500. -Review Articles: Reviews of major areas or sub-areas in the field of clinical medical physics. These articles may be of any length and are peer reviewed. -Technical Notes: These should be no longer than 3000 words, including key references. -Letters to the Editor: Comments on papers published in JACMP or on any other matters of interest to clinical medical physics. These should not be more than 1250 (including the literature) and their publication is only based on the decision of the editor, who occasionally asks experts on the merit of the contents. -Book Reviews: The editorial office solicits Book Reviews. -Announcements of Forthcoming Meetings: The Editor may provide notice of forthcoming meetings, course offerings, and other events relevant to clinical medical physics. -Parallel Opposed Editorial: We welcome topics relevant to clinical practice and medical physics profession. The contents can be controversial debate or opposed aspects of an issue. One author argues for the position and the other against. Each side of the debate contains an opening statement up to 800 words, followed by a rebuttal up to 500 words. Readers interested in participating in this series should contact the moderator with a proposed title and a short description of the topic
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