Very recently, first experimental evidence was published that the compressive thermal stress near the melt/solid interface makes a growing 300 mm diameter Czochralski Si crystal more vacancy-rich. The purpose of this letter is to explain these experimental results quantitatively by determining the dependence of the formation enthalpies of the vacancy and the self-interstitial on compressive plane stress using density functional theory based calculations. It is found that compressive plane stress gives a higher stress dependence of the so-called "Voronkov criterion" compared to the isotropic stress. In most of the central region of a growing crystal, the dominant component of the thermal stress near the melt/solid interface is compressive plane stress. The calculated plane stress dependence is in excellent agreement with the published experimental values and should be taken into account in the development of pulling processes for the mass-production of 450 mm diameter defect-free Si crystals.By evaluating the so-called "Voronkov criterion," 1 Nakamura et al. 2 very recently published clear experimental evidence that the compressive thermal stress near the melt/solid interface shifts the growing Czochralski Si crystal to more vacancy-rich. According to this criterion, a crystal that is pulled with the ratio (v/G) of the pulling speed v over the axial temperature gradient G at the melt/solid interface, larger than a critical value (v/G) crit , is vacancy (V) rich while when (v/G) is smaller than the critical value, the pulled crystal is self-interstitial (I) rich. They evaluated the boundaries of defect-free regions experimentally with changing the pulling speed v and calculated the temperature distributions with the global heat transfer model. 2 The "Voronkov criterion" (v/G) crit can be written as.,[1]C I , C I eq and C V , C V eq are the actual and the thermal equilibrium I and V concentrations, respectively. D I and D V are the I and V diffusivities, respectively. Q I and Q V are the reduced heats of transport of I and V, respectively, defined as the heat flux per unit flux of component atom in the absence of temperature gradient. T m is the melt temperature and k is the Boltzmann constant. E f I and E f V are the formation energy of I and V, respectively. One of the challenges to apply Eq. 1 in practice is the choice of intrinsic point defect formation and migration energies for zero stress. 4 Recent simulations at the atomic level, support the assumption that both I and V are incorporated in the crystal at the melt/solid interface with their thermal equilibrium concentrations at T m . 5 Before the recent experimental confirmation by Nakamura et al., 2 one of the authors, claimed in 2011 6 that one should take into account the impact of thermal stresses on the intrinsic point defect parameters and thus on the critical (v/G) crit . A detailed density functional theory (DFT) study followed to evaluate the pressure dependence of both the formation enthalpy (H f ) and the migration enthalpy (H m ) of the intrinsic ...