H. Nishiguchi , H. Danielsson , E. Hamada , Y. Hashimoto , M. Higashide , T. Nakabayashi , K. Oishi , K. Okabe , O. Osawa , M. Shoji , J. Suzuki , Z. Tsamalaidze , N. Tsverava , K. Ueno , A. Paulau , K. Watanabe
{"title":"全新极轻吸管管探测器,无纺布石墨织物","authors":"H. Nishiguchi , H. Danielsson , E. Hamada , Y. Hashimoto , M. Higashide , T. Nakabayashi , K. Oishi , K. Okabe , O. Osawa , M. Shoji , J. Suzuki , Z. Tsamalaidze , N. Tsverava , K. Ueno , A. Paulau , K. Watanabe","doi":"10.1016/j.nima.2025.170854","DOIUrl":null,"url":null,"abstract":"<div><div>The COMET experiment at J-PARC aims to search for a lepton-flavour violating process of muon to electron conversion, with a branching-ratio sensitivity of <span><math><mrow><mn>1</mn><msup><mrow><mn>0</mn></mrow><mrow><mo>−</mo><mn>17</mn></mrow></msup></mrow></math></span>. The expected signal of this process is monochromatic 105 MeV single electron. To distinguish such a low energy signal, a material budget of detector is essential since the detection accuracy is primarily limited by multiple scattering. To realise the required LOW material budget, a vacuum-compatible ultra-thin-wall straw tracker, <strong>20 µm-thick Mylar straw with 70 nm Al cathode</strong>, has been developed employing ultrasonic-welding technique. This was reported in VCI2016, and the detector performances such as detection efficiency and intrinsic spacial resolutions were reported in VCI2019. In parallel to 20 µm straw production, further thinner straw, <em>ie.</em> <strong>12 µm-thick</strong>, was developed for the COMET upgrade (COMET Phase-II). Details of R&D on 12 µm straw were reported in VCI2022.</div><div>In the process of developing the 12 µm straw, it became clear that it would be fundamentally difficult to make it any thinner using the current straw manufacturing method based on ultrasonic welding. Our R&D showed that the limit is around 10–12 µm. Then, the brand-new extremely light straw was developed with <strong>a nonwoven graphite-textile</strong>. This was enabled by a collaboration with the nano-tech textile science.</div><div>In this article, detailed R&D of the brand-new nonwoven graphite straw will be presented, in addition to the current status of straw-tube tracker construction for the COMET experiment.</div></div>","PeriodicalId":19359,"journal":{"name":"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment","volume":"1081 ","pages":"Article 170854"},"PeriodicalIF":1.4000,"publicationDate":"2025-07-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Brand-new extremely light straw-tube detector with a nonwoven graphite-textile\",\"authors\":\"H. Nishiguchi , H. Danielsson , E. Hamada , Y. Hashimoto , M. Higashide , T. Nakabayashi , K. Oishi , K. Okabe , O. Osawa , M. Shoji , J. Suzuki , Z. Tsamalaidze , N. Tsverava , K. Ueno , A. Paulau , K. Watanabe\",\"doi\":\"10.1016/j.nima.2025.170854\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><div>The COMET experiment at J-PARC aims to search for a lepton-flavour violating process of muon to electron conversion, with a branching-ratio sensitivity of <span><math><mrow><mn>1</mn><msup><mrow><mn>0</mn></mrow><mrow><mo>−</mo><mn>17</mn></mrow></msup></mrow></math></span>. The expected signal of this process is monochromatic 105 MeV single electron. To distinguish such a low energy signal, a material budget of detector is essential since the detection accuracy is primarily limited by multiple scattering. To realise the required LOW material budget, a vacuum-compatible ultra-thin-wall straw tracker, <strong>20 µm-thick Mylar straw with 70 nm Al cathode</strong>, has been developed employing ultrasonic-welding technique. This was reported in VCI2016, and the detector performances such as detection efficiency and intrinsic spacial resolutions were reported in VCI2019. In parallel to 20 µm straw production, further thinner straw, <em>ie.</em> <strong>12 µm-thick</strong>, was developed for the COMET upgrade (COMET Phase-II). Details of R&D on 12 µm straw were reported in VCI2022.</div><div>In the process of developing the 12 µm straw, it became clear that it would be fundamentally difficult to make it any thinner using the current straw manufacturing method based on ultrasonic welding. Our R&D showed that the limit is around 10–12 µm. Then, the brand-new extremely light straw was developed with <strong>a nonwoven graphite-textile</strong>. This was enabled by a collaboration with the nano-tech textile science.</div><div>In this article, detailed R&D of the brand-new nonwoven graphite straw will be presented, in addition to the current status of straw-tube tracker construction for the COMET experiment.</div></div>\",\"PeriodicalId\":19359,\"journal\":{\"name\":\"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment\",\"volume\":\"1081 \",\"pages\":\"Article 170854\"},\"PeriodicalIF\":1.4000,\"publicationDate\":\"2025-07-25\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://www.sciencedirect.com/science/article/pii/S0168900225006564\",\"RegionNum\":3,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"INSTRUMENTS & INSTRUMENTATION\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment","FirstCategoryId":"101","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0168900225006564","RegionNum":3,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"INSTRUMENTS & INSTRUMENTATION","Score":null,"Total":0}
Brand-new extremely light straw-tube detector with a nonwoven graphite-textile
The COMET experiment at J-PARC aims to search for a lepton-flavour violating process of muon to electron conversion, with a branching-ratio sensitivity of . The expected signal of this process is monochromatic 105 MeV single electron. To distinguish such a low energy signal, a material budget of detector is essential since the detection accuracy is primarily limited by multiple scattering. To realise the required LOW material budget, a vacuum-compatible ultra-thin-wall straw tracker, 20 µm-thick Mylar straw with 70 nm Al cathode, has been developed employing ultrasonic-welding technique. This was reported in VCI2016, and the detector performances such as detection efficiency and intrinsic spacial resolutions were reported in VCI2019. In parallel to 20 µm straw production, further thinner straw, ie.12 µm-thick, was developed for the COMET upgrade (COMET Phase-II). Details of R&D on 12 µm straw were reported in VCI2022.
In the process of developing the 12 µm straw, it became clear that it would be fundamentally difficult to make it any thinner using the current straw manufacturing method based on ultrasonic welding. Our R&D showed that the limit is around 10–12 µm. Then, the brand-new extremely light straw was developed with a nonwoven graphite-textile. This was enabled by a collaboration with the nano-tech textile science.
In this article, detailed R&D of the brand-new nonwoven graphite straw will be presented, in addition to the current status of straw-tube tracker construction for the COMET experiment.
期刊介绍:
Section A of Nuclear Instruments and Methods in Physics Research publishes papers on design, manufacturing and performance of scientific instruments with an emphasis on large scale facilities. This includes the development of particle accelerators, ion sources, beam transport systems and target arrangements as well as the use of secondary phenomena such as synchrotron radiation and free electron lasers. It also includes all types of instrumentation for the detection and spectrometry of radiations from high energy processes and nuclear decays, as well as instrumentation for experiments at nuclear reactors. Specialized electronics for nuclear and other types of spectrometry as well as computerization of measurements and control systems in this area also find their place in the A section.
Theoretical as well as experimental papers are accepted.