首页> 外文会议>International symposium on System synthesis >Using spherically bent crystals for obtaining high-resolution,large-field, monochromatic X-ray backlighting imaging for wide range ofBragg angles
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Using spherically bent crystals for obtaining high-resolution,large-field, monochromatic X-ray backlighting imaging for wide range ofBragg angles

机译:使用球形弯曲的晶体来获得高分辨率,大范围,单色X射线背光成像,适用于宽范围的布拉格角

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Summary form only given, as follows. The new advantages ofwell-known combination of a laser-produced X-ray plasma source andspherically bent crystal for the soft X-ray region backlighting schemewere experimentally demonstrated and theoretically modelling byray-tracing package SHADOW. The X-ray source was produced by heatingradiation of Ti:sapphire laser (120 fs, 3-5 mJ, laser flux density 1013 W/cm2) or XeCl laser (1-1.3 J, 10 ns, laserflux density 1013 W/cm2) with repetition 10 Hz atdifferent solid targets (Mg, Fe, Ni, Dy, BaF2). X-ray sourcespot size on the target was well localised both spatially (~20 μm)and temporally (1 ps-10 ns, depend of used laser) and is spectrallytunable in a relatively wide range (6-19 Å). High qualitymonochromatic (δλ/λ~10-5-10-3)images with high spatial resolution (up to ~4 μm) and in a largefield of view (few mm) were obtained for different wavelengths using thesame spherically bent crystal. It was demonstrated at first time thatthe spherically bent crystals can be sufficiently used for obtaininghigh-resolution, large-field, monochromatic images in a wide range ofBragg angles (θ=40-90° ), thus spherically bent crystals areuniversal for very wide wavelength selection, what is very important formany applications. Obtained experimental results were independentlyconfirmed by ray-tracing modelling for different radius of crystalcurvatures, Bragg angles and linear magnification of images
机译:仅给出摘要表格,如下。的新优势 激光产生的X射线等离子体源与 球形弯曲晶体用于软X射线区域的背光方案 被实验证明和理论建模 光线跟踪包SHADOW。 X射线源是通过加热产生的 Ti:蓝宝石激光的辐射(120 fs,3-5 mJ,激光通量密度10 13 W / cm 2 )或XeCl激光(1-1.3 J,10 ns,激光 磁通密度10 13 W / cm 2 ),重复频率10 Hz 不同的固体靶(Mg,Fe,Ni,Dy,BaF 2 )。 X射线源 目标上的光斑大小在空间上都很好地定位(〜20μm) 和时间上(1 ps-10 ns,取决于所使用的激光),并且在光谱上 在相对较宽的范围(6-19Å)中可调。高质量 单色(δλ/λ〜10 -5 -10 -3 ) 具有高空间分辨率(最大〜4μm)和较大图像的图像 使用不同的波长获得不同波长的视场(几毫米)。 相同的球形弯曲晶体。第一次证明了 球形弯曲的晶体可以充分用于获得 宽范围的高分辨率,大视野,单色图像 布拉格角(θ= 40-90°),因此球形弯曲的晶体为 对于很宽的波长选择是通用的,对于 许多应用。获得的实验结果是独立的 通过射线追踪模型确定了不同半径的晶体 曲率,布拉格角和图像的线性放大

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