Doubly curved crystals direct x-rays

SPIE Newsroom ◽  
2003 ◽  
Author(s):  
Zewu Chen
2020 ◽  
Vol 9 (3) ◽  
pp. 806
Author(s):  
Gilbert Manuel Schwarz ◽  
Lukas Zak ◽  
Lena Hirtler ◽  
Gerald Eliot Wozasek

Intramedullary lengthening, in cases of extensive humeral shortening, offers the advantages of preventing external-fixator-associated problems. The humeral cavity, as the main parameter in nailing, however, has been neglected in recent literature. It was hypothesized that available implants might be too large and therefore increase the risk of intraoperative fractures. The aim of this cross-sectional study was to describe the humeral canal and how it might affect the choice of implant and the surgical approach. Thirty humeri (15 female, 15 male) from clinical patients and anatomical specimens were studied. Specifically, the medullary cavity width (MCW), cortical thickness (CoT), and the course of the medullary canal were examined. The smallest MCW diameters were found at the distal third of the humeral shaft with mean diameters of 10.15 ± 1.96 mm. CoTs of female humeri were significantly smaller than those of male humeri (p < 0.001). The mean angles of the pro- and recurvatum were 4.01 ± 1.68° and 10.03 ± 2.25°, and the mean valgus bending was 3.37 ± 1.58°. Before implanting a straight lengthening nail into a doubly curved humerus, X-rays and, in selected cases, CT-scans should be performed. The unique size and course of the humeral canal favors an antegrade approach in cases of intramedullary lengthening.


Author(s):  
D. B. Wittry ◽  
W. Z. Chang ◽  
T. W. Barbee

X-ray diffractors having doubly curved crystal planes can have a high collection efficiency for radiation from a point source and can provide point-to-point focusing of monochromatic x rays as shown by some of the authors. These kinds of diffractors can be used to form x-ray microprobes that can give lower detection limits than electron microprobes or to make wavelength dispersive spectrometers with better signal and signal/background ratio than conventional ones employing the Johann or Johansson geometry. However, fabrication of diffractors of the desired geometry by the use of bent crystals has been difficult. In this paper, we explore the use of oriented polycrystalline films to fabricate doubly curved diffractors for x rays of short wavelength.Oriented polycrystalline films (OPF) have been of interest for many applications, e.g., magnetic recording media, non-linear optical device components, inexpensive large-area substrates for semiconductor device fabrication, etc. These films consist of small monocrystalline grains that have a high degree of preferential orientation of one crystallographic axis relative to the substrate surface.


2002 ◽  
Vol 17 (2) ◽  
pp. 99-103 ◽  
Author(s):  
Zewu Chen ◽  
Walter M. Gibson

Doubly curved crystal (DCC) X-ray optics provide an enabling technology for new portable, remote, and in situ applications of monochromatic X-rays for composition and structure analysis of amorphous, polycrystalline, and crystalline solids. Femtogram sensitivity for surface contamination, parts-per-billion (ppb) impurity levels for solids, and composition, structure and uniformity of thin films with compact, low power (20–50 W) source optic combinations are possible.


2012 ◽  
Vol 45 (5) ◽  
pp. 890-901 ◽  
Author(s):  
Sayyed Jalal Pestehe ◽  
Golamreza Askari Germi

The X-ray optics of singly and doubly curved crystals are studied using a vector procedure and rotation matrices and general relations for the angular deviation from the Bragg angle over the crystal surface with a source aligned or misaligned on the Rowland circle. Hence, the effective scattering area, collection solid angle and diffracted X-ray intensity profile on the crystal surface are derived. The effective areas and the diffracted X-ray intensity profiles on the crystal surface for both aligned and misaligned source cases are plotted and compared. It is argued that the introduced point-focusing crystal configuration confirms the radii that have been obtained previously by a trial and error method by optimizing the crystal collection solid angle.


1995 ◽  
Vol 77 (5) ◽  
pp. 1843-1848 ◽  
Author(s):  
F. N. Chukhovskii ◽  
W. Z. Chang ◽  
E. Förster

2007 ◽  
Vol 22 (2) ◽  
pp. 188-188
Author(s):  
Z. W. Chen ◽  
F. Wei ◽  
B. Beumer ◽  
D. Li ◽  
W. M. Gibson

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