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Point-contact-spectroscopy evidence of quasi-particle interactions in RNi2B2C (R=Ho, Y)

机译:RNi2B2C中准粒子相互作用的点接触光谱证据(R = Ho,Y)

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摘要

The point-contact (PC) d2V/dI2-spectra of HoNi2B2C and YNl2B2C reveal structure at applied voltages corresponding to the phonon frequencies. At about 4 meV a maximum is observed in the phonondensity of states by analogy to the soft-phonon structure in neutron scattering experiments for LuNi2B2C [P. Dervenagas et al., Phys. Rev. B52, R9839 (1995)]and YNl2B2C [H. Kawano et al., Czech. J. Phys. 46, S2-825 (1996), Phys. Rev. Lett.77, 4628 (1996)]. In the Ho compound the low-energy phonon peak is suppressed by an applied magnetic field in an anisotropic way, pointing to an interaction between the phonons and the magnetic systems. Surprisingly, in the nonmagnetic Y compound the 4-meV peak is also suppressed by a magnetic field. In the Ho-compound contacts which show the 〈quasi-thermal〉 behavior, the detailed magnetic-field and temperature dependences of PC spectra suggest that the magnetic order is destroyed due to the coupled phonon-magnon subsystem which is driven out of equilibrium by electrons that pass through the contact, by analogy with the nonequilibrium phonon-induced destruction of the superconducting state in point contacts [I. K. Yanson et al., JETP Lett. 45, 543 (1987)]. The PC electron-phonon interaction(EPI) spectral functions are reconstructed and the estimates for the λ-parameter yield the values of the order of 0.1. Comparison with PC EPI spectra of nonsuperconducting and nonmagnetic LaNi2B2C. [I. K. Yanson et al., Phys. Rev. Lett. 78, 935 (1997)], as well as the comparative study of PC EPI and Andreev-reflection spectra for various contacts with superconducting Ho and Y compounds suggest that the low-energy part of the electron-quasi-particle interaction spectral function is responsible for the Cooper pairing in these materials.
机译:HoNi2B2C和YNl2B2C的点接触(PC)d2V / dI2-光谱显示了在对应于声子频率的施加电压下的结构。类似于LuNi2B2C的中子散射实验中的软声子结构,在大约4 meV处观察到了最大的声子态密度。 Dervenagas et al。,Phys。 Rev.B52,R9839(1995)]和YN12B2C [H。 Kawano等,捷克。 J.物理46,S2-825(1996),物理学。 Rev.Lett.77,4628(1996)。在Ho化合物中,低能声子峰被各向异性施加的磁场抑制,表明声子与磁系统之间发生相互作用。令人惊讶地,在非磁性Y化合物中,4-meV峰也被磁场抑制。在表现出“准热”行为的Ho-化合物接触中,PC光谱的详细磁场和温度相关性表明,由于电子耦合驱使声子-磁振子子系统失衡,从而破坏了磁阶。类似于非平衡声子引起的点接触中超导状态的破坏,它们通过接触[I. K.Yanson等,JETP Lett。 45,543(1987)]。重构了PC电子-声子相互作用(EPI)的光谱函数,对λ参数的估计得出的值约为0.1。非超导和非磁性LaNi2B2C与PC EPI光谱的比较。 [一世。 K.Yanson等,《物理学报》牧师78,935(1997)],以及PC EPI和Andreev反射光谱与超导Ho和Y化合物的各种接触的比较研究表明,电子-准粒子相互作用谱函数的低能部分是负责任的这些材料中的库珀配对。

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