{"title":"Enhanced bulk-etch-rate of gamma irradiated PADC detector expressed by the radiation chemical yield of hydroxyl group","authors":"Reo Yamada , Atsushi Kimoto , Hayato Seiichi , Shunto Sadamitsu , Daisuke Kohinata , Masato Kanasaki , Tamon Kusumoto , Hisashi Kitamura , Satoshi Kodaira , Sachiko Tojo , Tomoya Yamauchi","doi":"10.1016/j.radmeas.2025.107584","DOIUrl":null,"url":null,"abstract":"<div><div>Enhanced bulk-etch-rate of PADC (polyallyl diglycol carbonate) detectors exposed to gamma rays has been found to be described well as an exponential function of the product of the radiation chemical yield of hydroxyl group (<em>G</em><sub><em>OH</em></sub>) and the adsorbed dose (<em>D</em>) at different dose-rates between 0.41 and 8.14 Gy/s. The examined absorbed doses were ranging from 30 to 100 kGy, comparable with the local dose in proton tracks. By matching the bulk-etch-rates and the <em>G</em><sub><em>OH</em></sub> values obtained under identical conditions on dose-rate, the following equation was derived for the relative bulk-etch-rate, <em>V</em><sub><em>irra</em></sub>/<em>V</em><sub><em>b</em></sub> = exp(<em>y</em>・<em>G</em><sub><em>OH</em></sub>・<em>D</em>), where, <em>V</em><sub><em>irra</em></sub> and <em>V</em><sub><em>b</em></sub> denote the bulk-etch-rates after and before gamma irradiations, respectively, and <em>y</em> is an experimentally obtained constant in a unit of kg/mol, with a value of <em>y</em> = 5.98. In this relation, significant dose-rate dependence is explained as the dose-rate dependence of the <em>G</em><sub><em>OH</em></sub> value. This means that the radiation damage that increases the bulk-etch-rate is the hydroxyl group itself, and <em>y</em> appears as a constant specific to PADC which relates the damage to bulk-etch-rate. Here, <em>y</em> is termed the “etching coefficient \".</div></div>","PeriodicalId":21055,"journal":{"name":"Radiation Measurements","volume":"191 ","pages":"Article 107584"},"PeriodicalIF":1.8000,"publicationDate":"2026-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Radiation Measurements","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S1350448725002136","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"2025/12/3 0:00:00","PubModel":"Epub","JCR":"Q2","JCRName":"NUCLEAR SCIENCE & TECHNOLOGY","Score":null,"Total":0}
引用次数: 0
Abstract
Enhanced bulk-etch-rate of PADC (polyallyl diglycol carbonate) detectors exposed to gamma rays has been found to be described well as an exponential function of the product of the radiation chemical yield of hydroxyl group (GOH) and the adsorbed dose (D) at different dose-rates between 0.41 and 8.14 Gy/s. The examined absorbed doses were ranging from 30 to 100 kGy, comparable with the local dose in proton tracks. By matching the bulk-etch-rates and the GOH values obtained under identical conditions on dose-rate, the following equation was derived for the relative bulk-etch-rate, Virra/Vb = exp(y・GOH・D), where, Virra and Vb denote the bulk-etch-rates after and before gamma irradiations, respectively, and y is an experimentally obtained constant in a unit of kg/mol, with a value of y = 5.98. In this relation, significant dose-rate dependence is explained as the dose-rate dependence of the GOH value. This means that the radiation damage that increases the bulk-etch-rate is the hydroxyl group itself, and y appears as a constant specific to PADC which relates the damage to bulk-etch-rate. Here, y is termed the “etching coefficient ".
期刊介绍:
The journal seeks to publish papers that present advances in the following areas: spontaneous and stimulated luminescence (including scintillating materials, thermoluminescence, and optically stimulated luminescence); electron spin resonance of natural and synthetic materials; the physics, design and performance of radiation measurements (including computational modelling such as electronic transport simulations); the novel basic aspects of radiation measurement in medical physics. Studies of energy-transfer phenomena, track physics and microdosimetry are also of interest to the journal.
Applications relevant to the journal, particularly where they present novel detection techniques, novel analytical approaches or novel materials, include: personal dosimetry (including dosimetric quantities, active/electronic and passive monitoring techniques for photon, neutron and charged-particle exposures); environmental dosimetry (including methodological advances and predictive models related to radon, but generally excluding local survey results of radon where the main aim is to establish the radiation risk to populations); cosmic and high-energy radiation measurements (including dosimetry, space radiation effects, and single event upsets); dosimetry-based archaeological and Quaternary dating; dosimetry-based approaches to thermochronometry; accident and retrospective dosimetry (including activation detectors), and dosimetry and measurements related to medical applications.