首页> 外文期刊>Bulletin of materials science >Mathematical model of Boltzmann’s sigmoidal equation applicable to the set-up of the RF-magnetron co-sputtering in thin films deposition of Ba$_x$Sr$_{1?x}$TiO$_3$
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Mathematical model of Boltzmann’s sigmoidal equation applicable to the set-up of the RF-magnetron co-sputtering in thin films deposition of Ba$_x$Sr$_{1?x}$TiO$_3$

机译:玻尔兹曼S形方程的数学模型适用于薄膜沉积Ba $ _x $ Sr $ _ {1?x} $ TiO $ _3 $的射频磁控共溅射的建立

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In this work, we present the stoichiometric behaviour of Ba$^{2+}$ and Sr$^{2+}$ when they are deposited to make asolid solution of barium strontium titanate. Bax Sr$_{1?x}$ TiO$_3$ (BST) thin films of nanometric order on a quartz substrate were obtained by means of in-situ RF-magnetron co-sputtering at 495$^{circ}$C temperature, applying a total power of 120 W divided into intervals of 15 W that was distributed between two magnetron sputtering cathodes containing targets of BaTiO$_3$ and SrTiO$_3$, as follows: 0–120, 15–105, 30–90, 45–75, 60–60, 75–45, 90–30, 105–15 and 120–0 W. Boltzmann’s sigmoidalmodified equation (Boltzmann’s profile) is proposed to explain the behaviour and the deposition ratio Ba/Sr of the BSTas a function of the RF-magnetron power. The Boltzmann’s profile proposal shows concordance with experimental data ofdeposits of BST on substrates of nichrome under the same experimental conditions, showing differences in the ratio Ba/Srof the BST due to the influence of the substrate.
机译:在这项工作中,我们介绍了Ba $ ^ {2 +} $和Sr $ ^ {2 +} $沉积成钛酸钡锶固体溶液时的化学计量行为。通过在495 $ ^ { circ} $ C的原位RF-磁控管共溅射获得了石英衬底上纳米级Bax Sr $ _ {{1?x} $ TiO $ _3 $(BST)薄膜。温度,施加总功率120 W,分为15 W的间隔,该功率分布在两个包含BaTiO $ _3 $和SrTiO $ _3 $靶的磁控溅射阴极之间,如下:0–120、15–105、30–90 ,45–75、60–60、75–45、90–30、105–15和120-0W。提出了Boltzmann的S型修正方程(Boltzmann轮廓)来解释BST的行为和沉积率Ba / Sr。射频磁控管电源的功能。玻尔兹曼的轮廓提议与在相同实验条件下镍铬合金衬底上的BST沉积物的实验数据一致,表明由于衬底的影响,Ba / Srof BST的比率存在差异。

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