论文标题
la $ _ {2-x} $ _ $ sr $ _x $ cuo $ _4 $ $ _4 $的两个组成部分共存
Coexistence of Two Components in Magnetic Excitations of La$_{2-x}$Sr$_x$CuO$_4$ ($x$ = 0.10 and 0.16)
论文作者
论文摘要
为了阐明la $ _ {2-x} $ sr $ _x $ cuo $ _4 $的旋转动力学,它与自由度相结合,跨越特征能量的旋转激发($ e _ {\ rm cross} $ $ \ $ \ sim $ 35-40 mee $ 35-40 $ $ $ $ x. 10.10 and $ x $ x = 10.10 000 x.10 x = 10.10 x = 10.10 x = 10.10 x.非弹性中子散射测量。基于高质量数据的两部分图片的分析阐明了能够在能量摩托车空间中与无间隙(c)激发的直立静态不相关(IC)激发的可能共存。随着能量传输的增加($ \hbarΩ$),IC组件削弱了$ e _ {\ rm cross} $的强度,而c组件在高-U \hbarΩ$区域中加强。分析结果表明,两个具有特定强度平衡的组件的叠加形成了沙漏形的兴奋。此外,每个组件强度的温度依赖性表现出不同的行为。变暖后,IC成分在伪空隙温度($ t $*)附近消失,而C组件在温度下稳健。这些结果表明,分别在IC和C激发的父母LA $ _2 $ _4 $ _4 $ _4 $ _4 $的静电性旋转性质和局部磁性中,类似于Op yba $ _2 $ _2 $ _2 $ _2 $ _3 $ _3 $ _3 $ o $ $ $ $ $ _ {6+δ} $ _2 $ _2 $ _2 $ - _2 $ - _}的旋转激发。温度。
To elucidate the spin dynamics of La$_{2-x}$Sr$_x$CuO$_4$, which couples with the charge degree of freedom, the spin excitations spanning the characteristic energy ($E_{\rm cross}$ $\sim$35-40 meV) are investigated for underdoped $x$ = 0.10 and optimally doped (OP) $x$ = 0.16 through inelastic neutron scattering measurements. Analysis based on a two-component picture of high-quality data clarified the possible coexistence of uprightly standing incommensurate (IC) excitations with gapless commensurate (C) excitations in the energy-momentum space. The IC component weakens the intensity toward $E_{\rm cross}$ with increasing energy transfer ($\hbarω$), whereas the C component strengthens at high-$\hbarω$ regions. The analysis results imply that the superposition of two components with a particular intensity balance forms an hourglass-shaped excitation in appearance. Furthermore, the temperature dependence of the intensity of each component exhibits different behaviors; the IC component disappears near the pseudo-gap temperature ($T$*) upon warming, whereas the C component is robust against temperature. These results suggest the itinerant electron spin nature and the localized magnetism of the parent La$_2$CuO$_4$ in IC and C excitations, respectively, similar to the spin excitations in the OP YBa$_2$Cu$_3$O$_{6+δ}$ and HgBa$_2$CuO$_{4+δ}$ with higher superconducting-transition temperatures.