High-Speed X-Ray Projection Microscopy at Beamline 9D of the Pohang Light Source-II

2020 ◽  
Vol 77 (9) ◽  
pp. 802-805
Author(s):  
Kyungjin Park ◽  
Seob-Gu Kim ◽  
Ye Ji Lee ◽  
Jae-Hong Lim ◽  
Jong Hyun Kim
2007 ◽  
Vol 51 (4) ◽  
pp. 1256 ◽  
Author(s):  
Guk Bae Kim ◽  
Sang Joon Lee ◽  
Jin Pyung Lee ◽  
Jong Hyun Kim ◽  
Suk Sang Chang ◽  
...  

2010 ◽  
Vol 81 (2) ◽  
pp. 026103 ◽  
Author(s):  
Ik-Jae Lee ◽  
Chung-Jong Yu ◽  
Young-Duck Yun ◽  
Chae-Soon Lee ◽  
In Deuk Seo ◽  
...  

2018 ◽  
Vol 25 (3) ◽  
pp. 878-884 ◽  
Author(s):  
Hyun-Joon Shin ◽  
Namdong Kim ◽  
Hee-Seob Kim ◽  
Wol-Woo Lee ◽  
Chae-Soon Lee ◽  
...  

A scanning transmission X-ray microscope is operational at the 10A beamline at the Pohang Light Source. The 10A beamline provides soft X-rays in the photon energy range 100–2000 eV using an elliptically polarized undulator. The practically usable photon energy range of the scanning transmission X-ray microscopy (STXM) setup is from ∼150 to ∼1600 eV. With a zone plate of 25 nm outermost zone width, the diffraction-limited space resolution, ∼30 nm, is achieved in the photon energy range up to ∼850 eV. In transmission mode for thin samples, STXM provides the element, chemical state and magnetic moment specific distributions, based on absorption spectroscopy. A soft X-ray fluorescence measurement setup has been implemented in order to provide the elemental distribution of thicker samples as well as chemical state information with a space resolution of ∼50 nm. A ptychography setup has been implemented in order to improve the space resolution down to 10 nm. Hardware setups and application activities of the STXM are presented.


2021 ◽  
Vol 28 (2) ◽  
pp. 602-608
Author(s):  
Jae-Hee Jeong ◽  
Cheolsoo Eo ◽  
Hyo-Yun Kim ◽  
Jin-Hong Kim ◽  
Chae-Soon Lee ◽  
...  

BL-5C is an in-vacuum undulator beamline dedicated to macromolecular crystallography (MX) at the 3 GeV Pohang Light Source II in Korea. The beamline delivers X-ray beams with a focal spot size of 200 µm × 40 µm (FWHM, H × V) over the energy range 6.5–16.5 keV. The measured flux is 7 × 1011 photons s−1 at 12.659 keV through an aperture size of 50 µm. The experimental station is newly equipped with the photon-counting detector EIGER 9M, the multi-axis micro-diffractometer MD2, and a robotic sample changer with a high-capacity dewar. These instruments enable the operation of this beamline as an automated MX beamline specialized in X-ray fragment screening. This beamline can collect more than 400 data sets a day without human intervention, and a difference map can be automatically calculated by using the data processing pipeline for ligand or fragment identification.


1993 ◽  
Vol 32 (34) ◽  
pp. 6934 ◽  
Author(s):  
Steven J. Haney ◽  
Kurt W. Berger ◽  
Glenn D. Kubiak ◽  
Paul D. Rockett ◽  
John Hunter

2013 ◽  
Vol 21 (1) ◽  
pp. 264-267 ◽  
Author(s):  
Chung-Jong Yu ◽  
Hae Cheol Lee ◽  
Chan Kim ◽  
Wonsuk Cha ◽  
Jerome Carnis ◽  
...  

The coherent X-ray scattering beamline at the 9C port of the upgraded Pohang Light Source (PLS-II) at Pohang Accelerator Laboratory in Korea is introduced. This beamline provides X-rays of 5–20 keV, and targets coherent X-ray experiments such as coherent diffraction imaging and X-ray photon correlation spectroscopy. The main parameters of the beamline are summarized, and some preliminary experimental results are described.


2002 ◽  
Vol 09 (01) ◽  
pp. 497-501 ◽  
Author(s):  
M. K. LEE ◽  
H. J. SHIN ◽  
G. B. KIM ◽  
C. K. HONG ◽  
O. H. KIM ◽  
...  

Scanning photoelectron microscopy (SPEM) was used to investigate a semiconductor sensor chip and Cu patterns embedded in Si substrate. It was found that the line shift in X-ray photoelectron spectroscopy (XPS) caused by local charges on the passivated surface is proportional to the distance between the surface and the conducting layer of the sensor chip. By using the line shift in XPS, inner-layered microstructure of the sensor chip could be imaged without destroying the sample. The result for the Cu patterns indicates that the surface of Cu patterns is more contaminated with carbon in the air than the surface of the Si pattern.


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