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Origin of Giant Seebeck Coefficient for High Density 2DEGs Confined in the SrTiO_3/SrTi_(0.8)Nb_(0.2)O_3 Superlattices

机译:限制在SrTiO_3 / SrTi_(0.8)Nb_(0.2)O_3超晶格中的高密度2DEG的巨型塞贝克系数的起源

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We report two-dimensional Seebeck coefficients (|S|_(2D)) of [(SrTiO_3)_x/(SrTi_(0.8)Nb_(0.2)O_3)_y]_(20) (x = 1-50, y = 1-16) superlattices, which were grown on the (100)-face of insulating LaAlO_3 substrates, to clarify the origin of the giant |S|_(2D) values of the SrTiO_3 superlattices [H. Ohta et al., Nature Materials 6, 129 (2007)]. The |S|_(2D) values of the [(SrTiO_3)_(17)/(SrTi_(0.8)Nb_(0.2)O_3)_y]_(20) superlattices increased proportionally to y~(0.5), and reached 320 μV K~(-1) (y = 1), which is ~5 times larger than that of the SrTi_(0.8)Nb_(0.2)O_3 bulk (|S|_(3D) = 61 μV K~(-1)). The slope of the log |S|_(2D)-log y plots was -0.5, proving that the density of states in the ground state for SrTiO_3 increases inversely proportionally to y. Further, the |S|_(2D) value monotonically increases with x-value and is saturated when x-value > 16 (6.25 nm). We clarified that the critical barrier thickness for electron tunneling in [(SrTiO_3)_x)/(SrTi_(0.8)Nb_(0.2)O_3)_y]_z superlattice is 6.25 nm (16 unit cell layers of SrTiO_3).
机译:我们报告[(SrTiO_3)_x /(SrTi_(0.8)Nb_(0.2)O_3)_y] _(20)的二维塞贝克系数(| S | _(2D))(x = 1-50,y = 1 -16)在绝缘LaAlO_3衬底的(100)面上生长的超晶格,以阐明SrTiO_3超晶格的| S | _(2D)值的大起源[H. Ohta等人,Nature Materials 6,129(2007)]。 [(SrTiO_3)_(17)/(SrTi_(0.8)Nb_(0.2)O_3)_y] _(20)超晶格的| S | _(2D)值与y〜(0.5)成比例地增加,并达到320 μVK〜(-1)(y = 1),约为SrTi_(0.8)Nb_(0.2)O_3块的(〜| S | _(3D)= 61μVK〜(-1)的〜5倍。 )。 log | S | _(2D)-log y曲线的斜率是-0.5,证明SrTiO_3在基态下的态密度与y成反比。此外,| S | _(2D)值随x值单调增加,并且在x值> 16(6.25 nm)时达到饱和。我们阐明了[(SrTiO_3)_x)/(SrTi_(0.8)Nb_(0.2)O_3)_y] _z超晶格中电子隧穿的临界势垒厚度为6.25 nm(SrTiO_3的16个晶胞层)。

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