| Layered compounds containing transition metals usually exhibit flexible structures and special physical properties in electricity,magnetism and other aspects.In this dissertation,we focus on the synthesis and characterization of several layered compounds containing transition metal Fe or Co,with special attention to their magnetic and thermoelectric properties.In an effort to suppress the phase separation in AxFe2-ySe2 system,we synthesized three new layered compounds,studied their crystal structure and physical properties,and analyzed the hidden reasons behind the phenomena.In addition,we designed three novel layered compounds with intrinsic low lattice thermal conductivity,which shed light on searching for new thermoelectric materials.Finally,we studied certain layered compounds with complex Fe coordination environment,in order to further understand the relationship between the structure and physical properties.The main results of this thesis are summarized as follows:Firstly,three new layered compounds,namely,NaLiFeSe2 with a CaAl2Si2-type structure,and KLiFeSe2 and RbLi FeSe2 with a ThCr2Si2-type structure,are discovered through replacing half of the Fe in Ax Fe2-ySe2 with Li.The introduction of Li at Fe sites can successfully eliminate the Fe vacancy and avoid phase separation,resulting in a homogeneous structure and composition in these materials.Through comparing of the structures of AxFe2-ySe2 and ALi FeSe2,it can be seen that the substitution of Li at Fe site compresses the layer spacing and elongates A-Se bondlength in ThCr2Si2-type structure.Thus,the substitution of Li at Fe site in Nax Fe2-ySe2 would result in the elongation of Na-Se bondlength,leading to less overlap between Na and Se orbitals,which would destabilize the ThCr2Si2-type structure in NaLiFeSe2,while the CaAl2Si2-type structure would be stabilized with shorter Na-Se bondlength and more overlap between Na and Se.We speculate that Nax Fe2-ySe2 is at the border of ThCr2Si2-type structure and CaAl2Si2-type structure.Magnetic and resistivity measurements suggest an anisotropic spin-glass and narrow band-gap semiconductor ground state.The electrical conductivity behavior is well fitted by thermal activation model.The semiconducting behavior can be attributed to enhanced correlation effects.The discovery of these compounds would be instructive to further investigation of electronic correlations and magnetic structure in AxFe2-ySe2materials.Secondly,we designed and synthesized three novel layered compounds CsA’MSe2 with intrinsically low lattice thermal conductivities,namely,CsAgCoSe2,CsAgFeSe2 and Cs Li FeSe2,with a space group of Acmm(No.67).Their crystal structure can be regarded as a transformation of the ThCr2Si2-type structure with some atom arrangement ordering.Due to their complex layered structure,large atom weight,a low Debye temperature,as well as the disorder induced by the partial mix occupation,these compounds display low thermal conductivities.At room temperature,the lattice thermal conductivities of CsAgCoSe2,CsAgFeSe2 and Cs LiFeSe2,are 0.34 W m-1 K-1,0.27 W m-1 K-1 and 0.45 W m-1 K-1,respectively,opening up new avenues for exploring new thermoelectric materials.Compared with CsAgFeSe2 and Cs LiFeSe2,CsAgCoSe2 has a complex band structure,with a larger carrier effective mass,resulting in a higher Seebeck coefficient.The ZT value of CsAgCoSe2 reaches 0.57 at 875 K.Finally,we report that Fe3GeTe2 can form a wide solid solution by substitution of As for Ge,providing an opportunity to tune the magnetic and electronic properties in this 2D material.The crystal structure,physical properties and electronic structure of iron-deficient solid solution Fe3-yGe1-xAsxTe2(0≤x≤0.85)are studied.We found that the Curie temperature can substantially change from 177 K to 33 K and resistivity decreases by about 30%with the arsenic doping x from 0 to 0.85.First principles calculations demonstrate that the elongation of Fe(1)-Fe(1)dumb-bells along c axis,rather than the carrier doping,is essentially responsible for the decrease of Curie temperature.Our study reveals the magnetism manipulation can be realized via modification of bondlengths in 2D magnetic materials. |