TY - JOUR
T1 - Susceptibility of dilutely doped CrFe alloys
AU - Fishman, R. S.
AU - Galkin, V. Yu
AU - Ortiz, W. A.
PY - 1998/7/20
Y1 - 1998/7/20
N2 - For low dopant concentrations, Fe is the only impurity atom which exhibits Pauli paramagnetism below the Néel temperature TN of a Cr host. A series of measurements on Cr1-xFex and (Cr-2.7%Fe)1-xVx alloys reveal that the magnetization M is sensitive to the amplitude of the spin-density wave (SDW) below TN. The Fe moment also depends on the period of the SDW and is about 6% larger in the incommensurate than in the commensurate SDW state. Surprisingly, the differential susceptibility dM/dH peaks at the field Hp, which is about 5 kOe for low temperatures and small V concentrations. While Hp increases with the temperature, it decreases with the V and Fe concentrations. These observations may be explained by making the radical assumption that the rigidity of the Fe moment is broken by its interaction with the SDW. Whereas part of the Fe moment is bound to the SDW by the nesting free energy, the remainder experiences a weak effective field exerted by the surrounding SDW and by the ferromagnetically coupled, nearest-neighbour pairs of Fe atoms. The peak in dM/dH occurs when the external field H overcomes the antiferromagnetic field experienced by the single Fe atoms. This model explains the temperature and doping dependence of Hp, as well as the difference between the Fe moments in the commensurate and incommensurate SDW hosts.
AB - For low dopant concentrations, Fe is the only impurity atom which exhibits Pauli paramagnetism below the Néel temperature TN of a Cr host. A series of measurements on Cr1-xFex and (Cr-2.7%Fe)1-xVx alloys reveal that the magnetization M is sensitive to the amplitude of the spin-density wave (SDW) below TN. The Fe moment also depends on the period of the SDW and is about 6% larger in the incommensurate than in the commensurate SDW state. Surprisingly, the differential susceptibility dM/dH peaks at the field Hp, which is about 5 kOe for low temperatures and small V concentrations. While Hp increases with the temperature, it decreases with the V and Fe concentrations. These observations may be explained by making the radical assumption that the rigidity of the Fe moment is broken by its interaction with the SDW. Whereas part of the Fe moment is bound to the SDW by the nesting free energy, the remainder experiences a weak effective field exerted by the surrounding SDW and by the ferromagnetically coupled, nearest-neighbour pairs of Fe atoms. The peak in dM/dH occurs when the external field H overcomes the antiferromagnetic field experienced by the single Fe atoms. This model explains the temperature and doping dependence of Hp, as well as the difference between the Fe moments in the commensurate and incommensurate SDW hosts.
UR - http://www.scopus.com/inward/record.url?scp=11544305939&partnerID=8YFLogxK
U2 - 10.1088/0953-8984/10/28/015
DO - 10.1088/0953-8984/10/28/015
M3 - Article
AN - SCOPUS:11544305939
SN - 0953-8984
VL - 10
SP - 6347
EP - 6366
JO - Journal of Physics Condensed Matter
JF - Journal of Physics Condensed Matter
IS - 28
ER -