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Effective aperture of X-ray compound refractive lenses

机译:X射线复合折射镜片的有效孔径

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摘要

A new definition of the effective aperture of the X-ray compound refractive lens (CRL) is proposed. Both linear (one-dimensional) and circular (two-dimensional) CRLs are considered. It is shown that for a strongly absorbing CRL the real aperture does not influence the focusing properties and the effective aperture is determined by absorption. However, there are three ways to determine the effective aperture in terms of transparent CRLs. In the papers by Kohn [(2002). JETP Lett.76, 600-603; (2003). J. Exp. Theor. Phys.97, 204-215; (2009). J. Surface Investig.3, 358-364; (2012). J. Synchrotron Rad.19, 84-92; Kohn et al. (2003). Opt. Commun.216, 247-260; (2003). J. Phys. IV Fr, 104, 217-220], the FWHM of the X-ray beam intensity just behind the CRL was used. In the papers by Lengeler et al. [(1999). J. Synchrotron Rad.6, 1153-1167; (1998). J.Appl. Phys.84, 5855-5861], the maximum intensity value at the focus was used. Numerically, these two definitions differ by 50%. The new definition is based on the integral intensity of the beam behind the CRL over the real aperture. The integral intensity is the most physical value and is independent of distance. The new definition gives a value that is greater than that of the Kohn definition by 6% and less than that of the Lengeler definition by 41%. A new approximation for the aperture function of a two-dimensional CRL is proposed which allows one to calculate the two-dimensional CRL through the one-dimensional CRL and to obtain an analytical solution for a complex system of many CRLs.
机译:提出了X射线复合折射镜(CRL)的有效孔的新定义。考虑线性(一维)和圆形(二维)CRL。结果表明,对于强烈吸收的CRL,实际孔径不会影响聚焦性能,并且通过吸收确定有效孔。然而,有三种方法可以在透明CRL方面确定有效孔径。在Kohn论文中[(2002)。 Jetp Lett.76,600-603; (2003)。 J. Exp。你。 Phys.97,204-215; (2009)。 J. Surface Investig.3,358-364; (2012)。 J. Synchrotron Rad.19,84-92; Kohn等人。 (2003)。选择。 216,247-260。 (2003)。 J. phys。 IV FR,104,217-220],使用CRL后面的X射线束强度的FWHM。在Lengeler等人的论文中。 [(1999)。 J. Synchrotron Rad.6,1153-1167; (1998)。 J.Appl。 Phys.84,5855-5861],使用重点的最大强度值。在数值上,这两个定义不同50%。新定义基于真实孔径上CRL后面的光束的积分强度。积分强度是最具物理值,并且与距离无关。新定义提供了一个值,该值大于Kohn定义的值6%,小于Lengeler定义的值为41%。提出了二维CRL的孔径函数的新近似,其允许人们通过一维CRL计算二维CRL,并获得许多CRL的复杂系统的分析解决方案。

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