{"title":"高分辨率成像中的相干软x射线","authors":"M. Howells, J. Kirz","doi":"10.1063/1.34649","DOIUrl":null,"url":null,"abstract":"To illustrate the coherence problems in X-ray imaging we shall examine\n - scanning X-ray microscopy\n - holography, and\n - soft X-ray diffraction\n as illustrative examples. We show that only X-rays from within the emittance xx'yy' < (2.44λ)2 have the necessary spatial coherence to yield diffraction- limited images. The degree of temporal coherence required depends on the nature of the imaging system, and the size of the specimen. In conventional X-ray systems, spatial coherence is generated by collimation, while temporal coherence is achieved with monochromators. In these systems, then, one filters out a minute coherent fraction of an intense incoherent beam. Aside from the inefficiency of the procedure, there is a practical limitation of the temporal coherence length of about 103λ that one can generate this way in the soft X-ray regime.","PeriodicalId":436319,"journal":{"name":"Topical Meeting on Free Electron Generation of Extreme Ultraviolet Coherent Radiation","volume":"94 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2008-06-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"7","resultStr":"{\"title\":\"Coherent Soft X-Rays in High Resolution Imaging\",\"authors\":\"M. Howells, J. Kirz\",\"doi\":\"10.1063/1.34649\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"To illustrate the coherence problems in X-ray imaging we shall examine\\n - scanning X-ray microscopy\\n - holography, and\\n - soft X-ray diffraction\\n as illustrative examples. We show that only X-rays from within the emittance xx'yy' < (2.44λ)2 have the necessary spatial coherence to yield diffraction- limited images. The degree of temporal coherence required depends on the nature of the imaging system, and the size of the specimen. In conventional X-ray systems, spatial coherence is generated by collimation, while temporal coherence is achieved with monochromators. In these systems, then, one filters out a minute coherent fraction of an intense incoherent beam. Aside from the inefficiency of the procedure, there is a practical limitation of the temporal coherence length of about 103λ that one can generate this way in the soft X-ray regime.\",\"PeriodicalId\":436319,\"journal\":{\"name\":\"Topical Meeting on Free Electron Generation of Extreme Ultraviolet Coherent Radiation\",\"volume\":\"94 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2008-06-05\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"7\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Topical Meeting on Free Electron Generation of Extreme Ultraviolet Coherent Radiation\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1063/1.34649\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Topical Meeting on Free Electron Generation of Extreme Ultraviolet Coherent Radiation","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.34649","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
To illustrate the coherence problems in X-ray imaging we shall examine
- scanning X-ray microscopy
- holography, and
- soft X-ray diffraction
as illustrative examples. We show that only X-rays from within the emittance xx'yy' < (2.44λ)2 have the necessary spatial coherence to yield diffraction- limited images. The degree of temporal coherence required depends on the nature of the imaging system, and the size of the specimen. In conventional X-ray systems, spatial coherence is generated by collimation, while temporal coherence is achieved with monochromators. In these systems, then, one filters out a minute coherent fraction of an intense incoherent beam. Aside from the inefficiency of the procedure, there is a practical limitation of the temporal coherence length of about 103λ that one can generate this way in the soft X-ray regime.