论文标题
通过磁化,热容量,电阻率和NMR测量结果研究的巡回G型抗fiferromagnet SRCR2AS2
Itinerant G-type antiferromagnet SrCr2As2 studied by magnetization, heat capacity, electrical resistivity, and NMR measurements
论文作者
论文摘要
巡回抗铁磁(AFM)Srcr $ _2 $ AS $ _2 $的物理特性,以身体为中心的四方THCR $ _2 $ _2 $ si $ _2 $结构以单晶和多晶的形式通过电阻$ρ$ $ρ$ $ c _ $ c _ $ c $ c $ c {$ p pys $ c} $ c}以单晶和多晶的形式进行了调查磁化$ m $ versus施加的磁场$ h $等化液测量值以及$^{75} $ as和$^{53} $^{53} $ cr核磁共振(NMR)的测量值$ t $ t $ = 1.6---900 k。 $ t _ {\ rm n} $ = 615(15)k已确定,与先前的中子划分测量值一致。通过观察$^{53} $ cr nmr频谱在$ h $ = 0中的观察显示,从$χ(t)$测量中观察到单晶srcr $ _2 $ as $ _2 $ as $ _2 $,在两个不同的磁场方向$ h | ab $ h || $ h | $ h | $ h | $ h | G型AFM状态中的轴。金属状态直接证明了$ρ$,$ c _ {\ rm p} $和NMR测量值,以及Fermi Energy $ {\ cal D}(e_ {\ rm f})在AFM状态中的状态$ {\ cal D}(e_ {\ rm f})$估计为7.53 Statation/Ev f.u。对于两个旋转方向,几乎是裸露的$ {\ cal d}(e _ {\ rm f})$从第一原理计算估算的,这表明在AFM状态下,导电携带者质量增加了两个因子。 $ {\ cal d}(e _ {\ rm f})$被发现至少低于100 k,并且独立于$ h $。 $ρ(t)$发现在$ t _ {\ rm n} $上方显示$ t $ - 线性行为,并在$ t _ {\ rm n} $下方展示正曲率,在观察到磁性订购时自旋disordersorder散射的大量损失。
The physical properties of itinerant antiferromagnetic (AFM) SrCr$_2$As$_2$ with body-centered tetragonal ThCr$_2$Si$_2$ structure were investigated in single crystalline and polycrystalline forms by electrical resistivity $ρ$, heat capacity $C_{\rm p}$, magnetic susceptibility $χ$ versus temperature~$T$ and magnetization $M$ versus applied magnetic field $H$ isotherm measurements as well as $^{75}$As and $^{53}$Cr nuclear magnetic resonance (NMR) measurements in the wide temperature range $T$ = 1.6--900 K. From the $χ(T)$ and $^{75}$As NMR measurements, the G-type AFM state below $T_{\rm N}$ = 615(15) K has been determined, consistent with the previous neutron-diffraction measurements. Direct evidence of magnetic ordering of the Cr spins was shown by the observation of the $^{53}$Cr NMR spectrum under $H$ = 0. From the $χ(T)$ measurements on single-crystal SrCr$_2$As$_2$ under the two different magnetic field directions $H||ab$ and $H||c$ in the AFM state, the Cr ordered moments are shown to align along the $c$ axis in the G-type AFM state. The metallic state is directly evidenced by the $ρ$, $C_{\rm p}$, and NMR measurements, and the density of states at the Fermi energy ${\cal D}(E_{\rm F})$ in the AFM state is estimated to be 7.53 states/eV f.u. for both spin directions which is almost twice the bare ${\cal D}(E_{\rm F})$ estimated from first-principles calculations, suggesting an enhancement of the conduction-carrier mass by a factor of two in the AFM state. The ${\cal D}(E_{\rm F})$ is found to be nearly constant below at least 100 K and is independent of $H$. The $ρ(T)$ is found to show $T$-linear behavior above $T_{\rm N}$ and exhibits positive curvature below $T_{\rm N}$ where significant loss of spin-disorder scattering upon magnetic ordering is observed.