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The Structure of the Catalytic Domain of a Plant Cellulose Synthase and Its Assembly into Dimers
Olek, Anna T.,Rayon, Catherine,Makowski, Lee,Kim, Hyung Rae,Ciesielski, Peter,Badger, John,Paul, Lake N.,Ghosh, Subhangi,Kihara, Daisuke,Crowley, Michael,Himmel, Michael E.,Bolin, Jeffrey T.,Carpita, American Society of Plant Biologists 2014 The Plant cell Vol.26 No.7
<P>Small-angle x-ray scattering gives a glimpse at the solution structure of the catalytic domains of plant cellulose synthase and their dimerization. Dimerization through the plant-specific sequences of the catalytic domain provides important clues for how Zn-finger domains couple these fundamental scaffold units into large, multimeric synthase complexes.</P>
Arkadiusz Kuś,Wojciech Krauze,Piotr L. Makowski,Małgorzata Kujawińska 한국전자통신연구원 2019 ETRI Journal Vol.41 No.1
In this paper, we demonstrate the current concepts in holographic tomography (HT) realized within limited angular range with illumination scanning. The presented solutions are based on the work performed at Warsaw University of Technology in Poland and put in context with the state of the art in HT. Along with the theoretical framework for HT, the optimum reconstruction process and data visualization are described in detail. The paper is concluded with the description of hardware configuration and the visualization of tomographic reconstruction, which is calculated using a provided processing path.
Control of plasma profiles in DIII-D discharges
Gohil, P,Evans, T E,Ferron, J R,Moyer, R A,Petty, C C,Burrell, K H,Casper, T A,Garofalo, A M,Hyatt, A W,Jayakumar, R J,Kessel, C,Kim, J Y,La Haye, R J,Lohr, J,Luce, T C,Makowski, M A,Mazon, D,Menard, Published jointly by The Institute of Physics and 2006 Plasma physics and controlled fusion Vol.48 No.a5
<P>Active control of plasma profiles is an essential requirement for operating within plasma stability limits, for steady-state operation and for optimization of the plasma performance. In DIII-D, plasma profiles have been actively controlled using various actuators in the following manner: (a) real time closed loop control of the <I>q</I> profile evolution using electron cyclotron heating and neutral beam injection as actuators; (b) active control of the density and pressure profiles in quiescent H-mode and quiescent double barrier plasmas using electron cyclotron current drive (ECCD) and pellet injection; (c) active control of the edge profiles to suppress edge localized modes using resonant magnetic perturbation with toroidal mode number <I>n</I> = 3, (d) real time control of the current density profile to suppress neoclassical tearing modes using localized deposition of co-ECCD.</P>