Nanoscale X-ray imaging
By A. Sakdinawat, D. Attwood. 2009
668 citations recorded by the source corpus.
Subfields: Radiation, Structural Biology
View Paper: https://www.semanticscholar.org/paper/5ba5f29d59e64861a8ab5f95f29955738104ad77
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Radiation
- K. Nugent
- Richard L. Sandberg
- Changyong Song
- Henry N. Chapman
- M. Serdar
- S. Brisard
- Franz Pfeiffer
- Jianwei Miao
In Structural Biology
- Henry N. Chapman
- Richard L. Sandberg
- Changyong Song
- M. Serdar
- S. Brisard
- Franz Pfeiffer
- Jianwei Miao
- Paulo J. M. Monteiro
Citations in the corpus
- Coherent lensless X-ray imaging (2010, background): “Researchers at the Advanced Light Source in California, USA, have compared their image of a yeast cell with an image from a scanning transmission X-ray microscope (see ref”
- Coherent X-Ray Diffraction Imaging (2012, background): “The highest image resolution currently achievable by X-ray optics is around 10–15 nm [6], [7].”
- Multi-scale method of Nano(Micro)-CT study on microscopic pore structure of tight sandstone of Yanchang Formation, Ordos Basin (2013, neutral): “6 nm~1 mm;扫描电镜可观测不同尺度二维微孔形貌、 孔喉大小([2]),如利用场发射扫描电镜可获取孔径大于 5 nm的微孔二维平面图像,但对于孔喉的三维分布和孔 喉连通情况等信息无从获取([3])。要全面了解微观孔喉三 维空间分布特征,则主要依靠聚焦离子束技术与 X 射 线(CT)三维成像技术,前者利用离子束在亚微观尺 度对岩石不断剥蚀扫描获取一系列高分辨率二维图 像,最终将若干二维图像进行数值重构,获取岩石微 观结构的几何特征,如孔喉分布及其特殊形状([4-8])。但 聚焦离子束技术由于剥蚀岩石区域较小,属于微米级 别区域观察,并且花费时间较长,成本较高,且有损 扫描,难以广泛应用于孔”
- Multiscale X-ray tomography of cementitious materials: A review (2020, methodology): “Progress towards the development of Fresnel lenses capable of producing spatial resolution of a few nanometers [413] has been slow so the use of coherent lensless x-ray imaging, or Coherent Diffraction Imaging (CDI) becomes very attractive”
- X-ray ptychography (2017, background): “29 and contains the following steps: (1) ptychographic reconstruction of individual phase and amplitude projections; (2) phase-unwrapping and phaseramp removal; (3) registration alignment of projections to correct for experimental inaccuracies in positioning; (4) quantitative tomographic reconstruct”