• Nem Talált Eredményt

THE NUCLEATION AND GROWTH OF Fe UNDER INFLUENCE OF AN EXTERNAL MAGNETIC FIELD Jakub Adam Koza, Margitta Uhlemann, Annett Gebert, Ludwig Schultz

N/A
N/A
Protected

Academic year: 2022

Ossza meg "THE NUCLEATION AND GROWTH OF Fe UNDER INFLUENCE OF AN EXTERNAL MAGNETIC FIELD Jakub Adam Koza, Margitta Uhlemann, Annett Gebert, Ludwig Schultz"

Copied!
1
0
0

Teljes szövegt

(1)

THE NUCLEATION AND GROWTH OF Fe UNDER INFLUENCE OF AN EXTERNAL MAGNETIC FIELD

Jakub Adam Koza, Margitta Uhlemann, Annett Gebert, Ludwig Schultz

Leibniz Institute for Solid State and Materials Research IFW Dresden, P.O. Box 270116, D- 01171 Dresden, Germany

E-mail: j.koza@ifw-dresden.de

When thin films are deposited, the nucleation process will determine the physical properties of the film. Thus, the understanding of the earliest stages of a film growth and the influence of deposition parameters on it is of great importance for the process development and optimisation. It is known that a magnetic field applied during the deposition affects the process significantly [1-3].

The effect of an uniform magnetic field with a flux density up to 1T and different configurations relative to the electrode surface on the electrocrystallization of Fe was investigated. It was found, irrespective of the applied parameters, that the deposition proceeds through successive nucleation and growth steps. The first one related to 2D growth followed by a second nucleation and 3D diffusion controlled growth [3]. It was found by fitting of the Heerman-Tarallo model [4] to the experimental results, that the nucleation and growth at potentials of -1500 and -1550 mVMSE proceeds via a progressive mode, while at -1650 mVMSE it follows an almost instantaneous mode [3]. A strong influence of the parallel-to- electrode magnetic field on the nucleation processes was found for the progressive mode, which leads to the increase of the growth rate and as a consequence to retardation of the nucleation rate of the 3D step, i.e. a shift from progressive to instantaneous mode with a magnetic field [3]. This nucleation and growth mode change could be observed during the morphology evolution where in the parallel field more uniform gain size distribution was observed. No effect of a perpendicular-to-electrode magnetic field on the nucleation has been observed. But in this configuration a strong influence on the growth mode was observed [2].

The effects of a magnetic field on the nucleation and growth processes are discussed with respect to the magnetohydrodynamic effect (MHD) and confirmed by rotating disc electrode (RDE) experiments.

[1] A. Krause, C. Hamann, M. Uhlemann, A. Gebert, L. Schultz, J. Magn. Magn. Mater. 290- 291 (2005) 261

[2] J. Koza, M. Uhlemann, A. Gebert, L. Schultz, JOSSEC, 12 (2008) 181 [3] J.A. Koza, M. Uhlemann, A. Gebert, L. Schultz, Electrochim. Acta (2008), doi:10.1016/j.electacta.2008.06.011

[4] L. Heerman, A. Tarallo, J. Electroanal. Chem. 470 (1999) 70 [5] B. Scharifker, G. Hills, Electrochim. Acta 28 (1983) 879

Hivatkozások

KAPCSOLÓDÓ DOKUMENTUMOK

In this study, four native Trichoderma strains were examined for prevention of the rice sheath blight disease and promo- tion of plant growth and grain yields under paddy field

A correlation with a similar pattern was detected between gestational weight gain and the degree of growth restriction within the IUGR group: a more severe growth

Phase-field-crystal models applied to nucleation and pattern formation in metals As pointed out in reference [71], crystal nucleation can be handled in two different ways within

(i) the phase diagram of the 3D PFC/Swift–Hohenberg model; (ii) the height of the nucleation for homogeneous and heterogeneous nucleation; (iii) equilibrium shapes for the

We discuss a variety of phenomena, including homogeneous nucleation and competitive growth of crystalline particles having different crystal orientations, the kinetics

A phase field theory with model parameters evaluated from atomistic simulations/experiments is applied to predict the nucleation and growth rates of solid CO 2 hydrate in

The magnetic field at the position of the falling bead is the sum of the external field and the field due to induced magnetic momenta, which are represented by

Another external magnetic field perpendicular to the first disturbs the stationary state and the magnetic moments change their directions but continue their