113.8 ± 5.3) and the fi rst latewood vessels were observed around 5 June 2008 (DOY 156.5 ± 7.7). Latewood formation continued until 29 September 2008 (DOY 273.9 ± 10.5) when the terminal cells of the newly formed xylem ring were fully lignifi ed. In 2009, the main phases of wood formation generally

the vessel wall. This increase in the number of spins affected by deoxyhemoglobin is a form of amplification. When the susceptibility-induced local field differences exist within an imaging voxel, there is a resultant distribution of shifts in water resonance frequencies. In the gradient-echo method, a phase

pRB, the product of the retinoblastoma tumor suppressor gene, operates in the midst of the cell cycle clock appara-tus. Its main role is to act as a signal transducer connecting the cell cycle clock with the transcriptional machinery. In this role, pRB allows the clock to control the expression

[1] The separation of the solar cycle in the modulation of the galactic cosmic ray intensity into the four main phases (the minimum, ascending, maximum, and descending) is considered. We substantiate advantages of such classification, choose as its initial point one of the known classifications

Abstract. By the method of Artificial Neural Networks (ANN) the connection of magnetic disturbances in auroral region and mid and low latitude magnetic disturbances at the main phase of a geomagnetic storm is investigated. The search of nonlinear correlations between indices of auroral electrojets

Abstract: Synthesis of several recent structural studies in the Pyrenees points to a syntec-tonic emplacement of granitic plutons, more or less early during the D2 main phase of the Hercynian orogenesis. A dextral E-W component ofsimple shear is demonstrated forD2, which was previously considered

This is the author’s version of a work that was submitted/accepted for publication in the following source:

Abstract Based on the empirical electron theory (EET) of solids and molecules, the valence-electron structures (VESs) of the main phases in Ti(C, N)-based cermets were calculated, and the relationship between the VES and properties was determined. The results indicated that the hardness

: (1) determine node--anchor distances, (2) compute node positions, and (3) optionally refine the positions through an iterative procedure. We present a detailed analysis comparing the various alternatives for each phase, as well as a head-to-head comparison of the complete algorithms. The main

The Kuramoto model describes a large population of coupled limit-cycle oscillators whose natural frequencies are drawn from some prescribed distribution. If the coupling strength exceeds a certain threshold, the system exhibits a phase transition: some of the oscillators spontaneously synchronize