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Electronic structure and its contribution to the thermoelectric power of Ca/sub 3/Co/sub 4/O/sub 9/ and Na/sub x/CoO/sub 2/ layered cobalt oxides

机译:Ca / sub 3 / Co / sub 4 / O / sub 9 /和Na / sub x / CoO / sub 2 /层状氧化钴的电子结构及其对热电势的贡献

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Angle resolved photoemission spectroscopy (ARPES) with synchrotron radiation as an incident photon source was performed on the two different layered cobalt oxides, Ca/sub 3/Co/sub 4/O/sub 9/ and Na/sub 0.6/CoO/sub 2/. The energy-momentum dispersion was clearly observed in ARPES spectra, indicating the presence of extended and coherent Bloch states, and consequently the Boltzmann-type electrical conduction. The electronic structure near the Fermi level (E/sub F/) in Ca/sub 3/Co/sub 4/O/sub 9/ was assigned not to be those from the Ca/sub 2/CoO/sub 3/ rock-salt layers but consisting of the a/sub 1g/ and e'/sub g/ bands from the CoO/sub 2/ layers in the same manner as in Na/sub 0.6/CoO/sub 2/. The topology of the measured band was essentially the same with the calculated ones, but the energy width of the bands was greatly reduced to less than 60% of the calculated ones in both compounds most likely due to strong electron-correlation. The bilayer-splitting of the a/sub 1g/ and e'/sub g/ bands was observed for Na/sub 0.6/CoO/sub 2/ in sharp contrast with its absence in Ca/sub 3/Co/sub 4/O/sub 9/. This difference is caused by the difference in nature of the interstitial layers; thin disordered Na layer in Na/sub 0.6/CoO/sub 2/ and thick insulating Ca/sub 2/CoO/sub 3/ rock-salt layer in Ca/sub 3/Co/sub 4/O/sub 9/. Making full use of the measured electronic structure, we succeeded in qualitatively accounting for mechanism of the coexistence of a metallic electrical conduction with a large thermoelectric power.
机译:在两种不同的层状钴氧化物Ca / sub 3 / Co / sub 4 / O / sub 9 /和Na / sub 0.6 / CoO / sub 2上进行了以同步加速器辐射为入射光子源的角度分辨光发射光谱(ARPES) /。在ARPES光谱中清楚地观察到了能量动量色散,表明存在扩展和相干的布洛赫状态,并因此形成了玻耳兹曼型电导率。 Ca / sub 3 / Co / sub 4 / O / sub 9 /中接近费米能级(E / sub F /)的电子结构被指定为不来自Ca / sub 2 / CoO / sub 3 / rock-盐层,但以与Na / sub 0.6 / CoO / sub 2 /中相同的方式由来自CoO / sub 2 /层的a / sub 1g /和e'/ sub g /条带组成。测量的能带的拓扑结构与计算的能带基本相同,但是在两种化合物中,能带的能量宽度都大大减小到小于计算的能带的60%,这很可能是由于强的电子相关性所致。 Na / sub 0.6 / CoO / sub 2 /观察到a / sub 1g /和e'/ sub g /带的双层分裂,与Ca / sub 3 / Co / sub 4 / O中不存在的形成鲜明对比/ sub 9 /。这种差异是由间隙层的性质差异引起的。 Na / sub 0.6 / CoO / sub 2 /中的薄无序Na层和Ca / sub 3 / Co / sub 4 / O / sub 9 /中的厚绝缘Ca / sub 2 / CoO / sub 3 /岩盐层。充分利用测得的电子结构,我们成功地定性地解释了金属导电与大热电并存的机理。

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