Reliabilität der Hornhautrückflächen-Topographie für das Scanning-Slit-System Orbscan II und die rotierende Scheimpflugkamera Pentacam

2006 ◽  
Vol 223 (S 1) ◽  
Author(s):  
MS Reuland ◽  
AJ Reuland ◽  
TM Rabsilber ◽  
IJ Limberger ◽  
GU Auffarth
Keyword(s):  
2005 ◽  
Vol 31 (3) ◽  
pp. 636-639 ◽  
Author(s):  
Nicolás Charles ◽  
Martin Charles ◽  
Oscar J. Croxatto ◽  
Daniel E. Charles ◽  
Diego Wertheimer

Cornea ◽  
2006 ◽  
Vol 25 (10) ◽  
pp. 1158-1161 ◽  
Author(s):  
Arthur C K Cheng ◽  
Emily Tang ◽  
Shaheeda Mohamed ◽  
Dennis S C Lam
Keyword(s):  

2018 ◽  
Vol 2018 ◽  
pp. 1-5
Author(s):  
Zheren Xia ◽  
Chengmin Lin ◽  
Xueping Huang ◽  
Jinglu Ying ◽  
Mingguang Shi ◽  
...  

Objective. To calculate the Q values from the human anterior corneal surface with the tangential radius of curvature and analyze its distribution characteristics in different age and refractive status groups. Methods. Tangential power maps of the anterior cornea from Orbscan II were acquired for 201 subjects’ right eyes. They were divided into groups of adults and children and then divided further into subgroups according to the refraction status. The Q values of each semimeridian were calculated by the tangential radius with a linear regression equation. The Q value distribution in both the nasal cornea and temporal cornea were analyzed. Results. The mean temporal Q values of the emmetropia group of adults and all children’s groups were significantly different from the mean nasal Q value. The mean nasal corneal Q values were more negative in children. The adult group showed differences only in the low myopia group. The mean Q value of the nasal cornea among different refractive groups of children was significantly different, and so was the temporal cornea between the adult myopia and emmetropia group. Conclusion. The method using the tangential radius of curvature combined with linear regression to obtain anterior surface Q values for both adults and children was stable and reliable. When we analyzed the anterior corneal Q value, area division was necessary.


2008 ◽  
Vol 24 (8) ◽  
pp. 807-810 ◽  
Author(s):  
Arthur C. K. Cheng ◽  
Srinivas K. Rao ◽  
Thomas Ho ◽  
Silvania Lau ◽  
Dennis S. C. Lam

2010 ◽  
Vol 27 (7) ◽  
pp. 502-508 ◽  
Author(s):  
Farid Karimian ◽  
Sepehr Feizi ◽  
Azadeh Doozandeh ◽  
Amir Faramarzi ◽  
Mehdi Yaseri

2005 ◽  
Vol 21 (3) ◽  
pp. 294-296 ◽  
Author(s):  
Arthur C K Cheng ◽  
Dennis S C Lam
Keyword(s):  

1970 ◽  
Vol 14 ◽  
pp. 38-56
Author(s):  
E. M. Proctor ◽  
T. C. Furnas ◽  
W. F. Loranger

AbstractThe efficiency and effectiveness of diffracted beam x-ray monochromators used in powder diffractometry have been described in so many ways that much confusion exists regarding their true performance. Although significant improvements in signal to noise ratios are readily achievable, and they offer a solution to the sample fluorescence problem, it is not without sacrifice to total intensity or achievable resolution or both. This paper discusses and describes a series of comparisons between filtered direct beam, LiF and graphite monochromators.These comparisons include the considerations necessary for the appropriate selection of diffracted beam slit system, the effect of vertical divergence as a function of two theta for singly bent crystals, the effects of a non-uniformity of contribution over the length of the crystal, and the geometry necessary for the singly bent and doubly bent crystals. The total intensity and the resolution of LiF and graphite are discussed, in particular, it is noted that the performance of monochromators with randomly oriented samples is quite different than their performance with samples showing preferred orientation or grain effects.A new diffracted beam monochromator based on the Rowland focusing geometry is described.


1974 ◽  
Vol 52 (17) ◽  
pp. 1716-1722
Author(s):  
C. Berger ◽  
A. Adnot ◽  
J.-D. Carette

A method to calculate the transmission properties of a slit–slit system in electronic optics is described. It includes the following steps: calculation of the electric field between the electrodes, calculation of the electron trajectories point by point as a function of the initial conditions, and finally counting of the electrons which reach the second slit. Calculated and measured values of the transmission efficiency for usual geometrical dimensions of this system are presented.


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