The Intelligent Investor by Benjamin Graham, Jason Zweig, Warren E. Buffett

By Benjamin Graham, Jason Zweig, Warren E. Buffett

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10) (11) Equation (8) is a quadratic field gradient whose coefficient is varied in the zdirection. The center position of the quadratic field can be moved to an arbitrary position (x ), as shown in Eq. (6), by simultaneous application of the scanning field written as Eq. (9). Equation (10) is a field gradient in the z-direction under the presence of a field offset of b0y , and Eq. (11) is a field gradient in the y-direction whose coefficient increments by α in the z-direction. The field gradient of Eq. (9) can be rewritten as Gy y + Gyz yz, thus Eq.

Simply ignoring the cone angle and analyzing the longitudinal sampling engendered by helical scans is not sound since the effect of the cone angle on aliasing is significant even for four-slice scanners, as discussed above. One potential approach to characterizing sampling in conebeam CT is to make use of Fourier crosstalk analysis,77 –79 a generalized, object-independent form of aliasing analysis in which one quantifies the transmission of Fourier components through an imaging system as well as the ability to distinguish different Fourier components from the measured data.

25 (1998) 550–560. 26. S. Schaller, T. Flohr, K. Klingenbeck, J. Krause, T. Fuchs and W. Kalender, Spiral interpolation algorithms for multi-slice spiral CT part I: Theory, IEEE Trans. Med. Imag. 19 (2000) 822–834. 27. P. J. La Rivi`ere and X. Pan, Interlaced interpolation weighting functions for multislice helical CT, Optical Engineering 42 (2003) 3461–3470. 28. P. E. Danielsson, P. Edholm and M. Seger, Towards exact 3D-reconstruction for helical cone-beam scanning of long objects. A new detector arrangement and a new completeness condition, in Proceedings of the 1997 International Meeting on Fully Three-Dimensional Image Reconstruction in Radiology and Nuclear Medicine (D.

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