{"title":"一个中子电视摄像机探测器。","authors":"U W Arndt, D J Gilmore","doi":"","DOIUrl":null,"url":null,"abstract":"<p><p>The system under development has a large counting rate capability; this is extremely important where the total background count exceeds the total counts in the signals of interest. Its spatial resolution is of the order of one mm, which is perfectly adequate for neutron work, while the screen size of 400 mm is reasonable. The main limitation of the system is its limited counting efficiency, and this is directly attributable to the optical self-absorption of the neutron phosphor. Any newly developed transparent phosphor with the same light output would immediately change the situation. The success of the electronics hardware in reducing random noise is demonstrated in Figure 3, which shows in the bottom trace the live video output when the input to the system is a grey-scale test chart. The top trace is the output after the image has been digitally integrated. Figures 4 and 5 show the monitor outputs of the see articles x-ray system with a \"still\" diffraction pattern of a crystal of GPD (glyceraldehyde-3-phosphate dehydrogenase). Figure 4 is a photograph of the \"live\" video display, and Figure 5 is the digitally summed image. All coherent noise in the system, i.e., all noise synchronized with the TV scans has to be kept lower than the first bit threshold. However, this requirement can be relaxed when dealing with diffraction patterns, such as those from single crystals, for which a local background is subtracted from the pattern.</p>","PeriodicalId":75624,"journal":{"name":"Brookhaven symposia in biology","volume":" 27","pages":"VIII16-VIII23"},"PeriodicalIF":0.0000,"publicationDate":"1976-05-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A neutron television camera detector.\",\"authors\":\"U W Arndt, D J Gilmore\",\"doi\":\"\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>The system under development has a large counting rate capability; this is extremely important where the total background count exceeds the total counts in the signals of interest. Its spatial resolution is of the order of one mm, which is perfectly adequate for neutron work, while the screen size of 400 mm is reasonable. The main limitation of the system is its limited counting efficiency, and this is directly attributable to the optical self-absorption of the neutron phosphor. Any newly developed transparent phosphor with the same light output would immediately change the situation. The success of the electronics hardware in reducing random noise is demonstrated in Figure 3, which shows in the bottom trace the live video output when the input to the system is a grey-scale test chart. The top trace is the output after the image has been digitally integrated. Figures 4 and 5 show the monitor outputs of the see articles x-ray system with a \\\"still\\\" diffraction pattern of a crystal of GPD (glyceraldehyde-3-phosphate dehydrogenase). Figure 4 is a photograph of the \\\"live\\\" video display, and Figure 5 is the digitally summed image. All coherent noise in the system, i.e., all noise synchronized with the TV scans has to be kept lower than the first bit threshold. However, this requirement can be relaxed when dealing with diffraction patterns, such as those from single crystals, for which a local background is subtracted from the pattern.</p>\",\"PeriodicalId\":75624,\"journal\":{\"name\":\"Brookhaven symposia in biology\",\"volume\":\" 27\",\"pages\":\"VIII16-VIII23\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1976-05-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Brookhaven symposia in biology\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Brookhaven symposia in biology","FirstCategoryId":"1085","ListUrlMain":"","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The system under development has a large counting rate capability; this is extremely important where the total background count exceeds the total counts in the signals of interest. Its spatial resolution is of the order of one mm, which is perfectly adequate for neutron work, while the screen size of 400 mm is reasonable. The main limitation of the system is its limited counting efficiency, and this is directly attributable to the optical self-absorption of the neutron phosphor. Any newly developed transparent phosphor with the same light output would immediately change the situation. The success of the electronics hardware in reducing random noise is demonstrated in Figure 3, which shows in the bottom trace the live video output when the input to the system is a grey-scale test chart. The top trace is the output after the image has been digitally integrated. Figures 4 and 5 show the monitor outputs of the see articles x-ray system with a "still" diffraction pattern of a crystal of GPD (glyceraldehyde-3-phosphate dehydrogenase). Figure 4 is a photograph of the "live" video display, and Figure 5 is the digitally summed image. All coherent noise in the system, i.e., all noise synchronized with the TV scans has to be kept lower than the first bit threshold. However, this requirement can be relaxed when dealing with diffraction patterns, such as those from single crystals, for which a local background is subtracted from the pattern.