首页> 外文期刊>The European physical journal, B. Condensed matter physics >Optical investigation of the quasi two-dimensional monophosphate tungsten bronzes K_xP_4W_8O_(32) (x = 0 - 1.57)
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Optical investigation of the quasi two-dimensional monophosphate tungsten bronzes K_xP_4W_8O_(32) (x = 0 - 1.57)

机译:准二维单磷酸盐钨青铜K_xP_4W_8O_(32)的光学研究(x = 0-1.57)

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摘要

The potassium doped monophosphate tungsten bronzes K_xP_4W_8O_(32) are two-dimensional metals which show a metal-to-metal transition at a critical temperature which depends on the doping level. The metal-to-metal transition is accompanied by the formation of a commensurate charge density wave with wave vector (π/b, 0) which is independent of the doping level. Undoped P_4W_8O_(32), on the other hand, has two metal-to-metal transitions which are connected to the formation of incommensurate charge density waves. We measured the infrared reflectivity of the series K_xP_4W_8O_(32) (x = 0 - 1.57) in the spectral range from 100 to 10 000 cm~(-1) for room temperature and well below the critical temperature. Polarization-dependent infrared spectra find a two-dimensional behavior in the normal and the charge density wave state and show signatures of hybridization between one- and two-dimensional conduction bands. In undoped P_4W_8O_(32) the essentials of the charge density wave state can be understood from the nesting vectors of the calculated Fermi surface and two gaps are observed in the infrared spectra. The gap sizes are a factor of about 2.5 bigger than the predictions from mean-field theory in the weak-coupling limit which suggests medium- or strong electron-phonon coupling. For potassium doped K_xP_4W_8O_(32) one gap is observed in the charge density wave state. The energetics of the charge density formation may be dominated by the energy required for the lattice modulation.
机译:掺杂钾的单磷酸盐钨青铜K_xP_4W_8O_(32)是二维金属,其在取决于掺杂水平的临界温度下显示出金属到金属的转变。金属到金属的过渡伴随着相应的电荷密度波的形成,其波矢量(π/ b,0)与掺杂水平无关。另一方面,未掺杂的P_4W_8O_(32)具有两个金属到金属的跃迁,这两个跃迁与不相称的电荷密度波的形成有关。我们测量了K_xP_4W_8O_(32)系列的红外反射率(x = 0-1.57),其室温范围是100至10000 cm〜(-1),且远低于临界温度。偏振相关的红外光谱在法线和电荷密度波状态下发现二维行为,并显示一维和二维导带之间的杂交特征。在未掺杂的P_4W_8O_(32)中,可以从计算出的费米表面的嵌套向量中了解电荷密度波状态的本质,并在红外光谱中观察到两个间隙。在弱耦合极限中,间隙尺寸比平均场理论的预测大约2.5倍,这表明中等或强电子-声子耦合。对于钾掺杂的K_xP_4W_8O_(32),在电荷密度波状态下观察到一个间隙。电荷密度形成的高能可受晶格调制所需的能量支配。

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