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Yield Enhancement by Defect Control

In the following, typical tasks in the field of optimi2ation of Bridgman-type crystal-growth processes are presented where both, thermal modeling and experimental analysis, contribute. [Pg.158]

The control of the shape of the solid/liquid interface during the whole growth process is, in general, and not only for Bridgman-type crystal-growth processes, of great importance for several reasons  [Pg.158]

From Eq. (5.6) the crystal grower can estimate, for a given growth rate R, which temperature gradients in the melt and in the crystal have to be adjusted in order to grow a crystal with a flat interface, that means AQ = 0. But, Eq. (5.6) gives no information on which heater temperatures have to be chosen in order to achieve these temperature gradients and thus a flat solid/Uquid interface. [Pg.158]

For this purpose, the inverse modeling approach described in Section 5.2 allows the crystal grower in a very comfortable way to obtain the required information. By inverse modeling the heater temperature-time profiles can be optimized in order [Pg.158]

The optimization of the thermal conditions in Bridgman-type crystal growth of GaAs and InP with respect to low thermal stress conditions by using numerical simulation results mainly in a reduction of the dominant type of dislocations, the so-called 60°-dislocations with curved line vectors [49]. In Table 5.4 typical dislocation densities reported for different crystals grown by Bridgman-type growth techniques are summarized. [Pg.159]


See other pages where Yield Enhancement by Defect Control is mentioned: [Pg.158]    [Pg.159]    [Pg.161]    [Pg.163]    [Pg.165]    [Pg.167]    [Pg.158]    [Pg.159]    [Pg.161]    [Pg.163]    [Pg.165]    [Pg.167]    [Pg.497]    [Pg.65]    [Pg.129]    [Pg.130]    [Pg.193]    [Pg.425]    [Pg.200]    [Pg.332]    [Pg.516]    [Pg.89]    [Pg.95]    [Pg.126]    [Pg.144]   


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