# Evolution of the bulk properties, structure, magnetic order, and   superconductivity with Ni doping in CaFe2-xNixAs2

**Authors:** Neeraj Kumar, Songxue Chi, Ying Chen, Gaurav Rana, A. K. Nigam, A., Thamizhavel, William Ratcliff II, S. K. Dhar, and Jeffrey W. Lynn

arXiv: 0908.2255 · 2009-10-29

## TL;DR

This study investigates how Ni doping affects the structural, magnetic, and superconducting properties of CaFe2-xNixAs2, revealing a transition from magnetic order to superconductivity with increasing Ni content.

## Contribution

It provides a detailed experimental characterization of the evolution of phase transitions, magnetic order, and superconductivity in CaFe2-xNixAs2 as a function of Ni doping.

## Key findings

- Superconductivity appears at x ≈ 0.053 with T_C ≈ 15 K.
- Magnetic order diminishes and disappears at higher doping levels.
- Structural transitions are suppressed and the structure remains tetragonal in the superconducting phase.

## Abstract

Magnetization, susceptibility, specific heat, resistivity, neutron and x-ray diffraction have been used to characterize the properties of single crystalline CaFe2-xNixAs2 as a function of Ni doping for x varying from 0 to 0.1. The combined first-order structural and magnetic phase transitions occur together in the undoped system at 172 K, with a small decrease in the area of the a-b plane along with an abrupt increase in the length of the c-axis in the orthorhombic phase. With increasing x the ordered moment and transition temperature decrease, but the transition remains sharp at modest doping while the area of the a-b plane quickly decreases and then saturates. Warming and cooling data in the resistivity and neutron diffraction indicate hysteresis of ~2 K. At larger doping the transition is more rounded, and decreases to zero for x=0.06. The susceptibility is anisotropic for all values of x. Electrical resistivity for x = 0.053 and 0.06 shows a superconducting transition with an onset of nearly 15 K which is further corroborated by substantial diamagnetic susceptibility. For the fully superconducting sample there is no long range magnetic order and the structure remains tetragonal at all temperature, but there is an anomalous increase in the area of the a-b plane in going to low T. Heat capacity data show that the density of states at the Fermi level increases for x > 0.053 as inferred from the value of Sommerfeld coefficient. The regime of superconductivity is quite restrictive, with a maximum TC of 15 K and an upper critical field Hc2=14 T. Superconductivity disappears in the overdoped region.

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Source: https://tomesphere.com/paper/0908.2255