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By Campana F.
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Extra resources for 4-folds with numerically effective tangent bundles and second Betti numbers greater than one
Two X-ray images were taken of the gel phantom in the uncompressed state at 90◦ relative to each other (see Fig. 2). These images were used to calculate the 3D location of the metal beads inside the gel phantom. 22 V. Rajagopal et al. Fig. 2 The uncompressed gel phantom. Left: Custom-built teflon mould used to create gel phantom. 5% of original thickness, similar to clinical mammography compression loads) were then applied to the phantom (using acrylic plates), during which it was X-ray imaged (see Fig.
Fig. 4 (a) Left: velocity waveform of CCA from the 1D model; right: measurement from an ultrasonic scanner; (b) left: pressure waveform of subclavian artery from the 1D model; right: pressure waveform of subclavian artery after Mills et al.  we consider that the overall simulation result is within the acceptable physiological range of in vivo ultrasonic measurement. , in [6,7,10]. The measurement methods in these literature include non-invasive transcranial Doppler ultrasound  and validated computational fluid dynamics (CFD) analysis [6,7].
Third row right: The 3D locations of the two identified microcalcifications (black) are tracked to the uncompressed state and superimposed on the MR image set (bottom row) 3 Mapping Microcalcifications Between 2D Mammograms and 3D MRI Fig. 6 (continued) 27 28 V. Rajagopal et al. One of the main features that sets this modelling apart from previous studies is the fact that very few kinematic constraints were required to solve the compression problems because the problem was solved with contact mechanics theory.
4-folds with numerically effective tangent bundles and second Betti numbers greater than one by Campana F.