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Problem of attaining constant impurity concentration over ingot height

Michael A. Gonik 1
Michael A. Gonik
, 
Florin Baltaretu 2
Florin Baltaretu
1 Centre for Material Reseaches «Photon», Cheska Lipa Str., Aleksandrov, Vladimir Region 601655, Russia
2 Technical University of Civil Engineering of Bucharest, Lacul Tei Blvd, no. 122-124, Sector 2, Bucharest 510009, Romania
Published 1 June 2018
Communication , Volume 4, Issue 2, 41-51
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Gonik M. A., Baltaretu F. Problem of attaining constant impurity concentration over ingot height // Modern Electronic Materials. 2018. Vol. 4. No. 2. pp. 41-51.
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Gonik M. A., Baltaretu F. Problem of attaining constant impurity concentration over ingot height // Modern Electronic Materials. 2018. Vol. 4. No. 2. pp. 41-51.
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TY - JOUR
DO - 10.3897/j.moem.4.2.38536
UR - https://moem.colab.ws/publications/10.3897/j.moem.4.2.38536
TI - Problem of attaining constant impurity concentration over ingot height
T2 - Modern Electronic Materials
AU - Gonik, Michael A.
AU - Baltaretu, Florin
PY - 2018
DA - 2018/06/01
PB - НИТУ МИСИС
SP - 41-51
IS - 2
VL - 4
ER -
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@article{2018_Gonik,
author = {Michael A. Gonik and Florin Baltaretu},
title = {Problem of attaining constant impurity concentration over ingot height},
journal = {Modern Electronic Materials},
year = {2018},
volume = {4},
publisher = {НИТУ МИСИС},
month = {Jun},
url = {https://moem.colab.ws/publications/10.3897/j.moem.4.2.38536},
number = {2},
pages = {41--51},
doi = {10.3897/j.moem.4.2.38536}
}
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MLA
Gonik, Michael A., and Florin Baltaretu. “Problem of attaining constant impurity concentration over ingot height.” Modern Electronic Materials, vol. 4, no. 2, Jun. 2018, pp. 41-51. https://moem.colab.ws/publications/10.3897/j.moem.4.2.38536.
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Keywords

directional crystallization
germanium
impurity diffusion
mathematical simulation
multicrystalline silicon
submerged heater

Abstract

The possibility of growing crystals with homogeneous impurity distribution over crystal height has been demonstrated in a study of segregation during silicon and germanium growth from thin melt layers using the submerged heater method. Numeric simulation of 200 mm diam. antimony-doped germanium crystallization has shown that, beginning from a 40 mm melt layer thickness, the exact problem solution with convection allowance is identical to the unidimensional heat exchange problem solution in the central ingot part. The conditions under which convection can be ignored in mass transport calculation are more rigorous: the melt layer height must be within 20 mm. In this case Tiller’s ratio can be used for calculating the longitudinal impurity distribution for predominantly diffusion-controlled mass transport pattern. Analysis of the existing attempts to describe the experimental crystal growth results using the simplified formulae shows that they only yield acceptable results if the actual growth rate or change in melt layer thickness during crystallization are taken into account, e.g. as in the formula suggested by Marchenko et al. One can therefore analytically describe the longitudinal impurity distribution in the ingot, e.g. B and P distribution in silicon, and recommend the degree of additional doping of the melt zone under the heater so that to provide a constant impurity concentration over the ingot height. Homogeneous material can be obtained after residual layer solidification in the end portion of the ingot if the growth rate is controlled through varying the cooling rate.

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