TY - JOUR
T1 - Quantum phase transitions in NbFe2 and Ca3Ru2O7
AU - Duncan, W. J.
AU - Welzel, O. P.
AU - Moroni-Klementowicz, D.
AU - Albrecht, C.
AU - Niklowitz, P. G.
AU - Grüner, D.
AU - Brando, M.
AU - Neubauer, A.
AU - Pfleiderer, C.
AU - Kikugawa, N.
AU - Mackenzie, A. P.
AU - Grosche, F. M.
PY - 2010/3
Y1 - 2010/3
N2 - We examine the low temperature states of two transition metal compounds: (i) NbFe2 is poised on the threshold of ferromagnetism and can be pushed into a spin-aligned state at low temperature by modifying the composition slightly. Stoichiometric NbFe2 has been reported as a rare example of lowtemperature spin density wave order in a d-metal system. We have used pressure, field and composition tuning to examine the phase diagram of NbFe2. Near the quantum critical point, we find distinct non-Fermi liquid forms of the resistivity and heat capacity, whereas we observe strong, hysteretic magnetoresistance effects deep in the ordered phase. (ii) Ca3Ru2O7 undergoes first a magnetic transition (TN = 56 K) and then a structural transition (TS = 48 K) on cooling. Most of the Fermi surface is gapped out at low temperature, leading to a very low carrier density and small Fermi surface pockets. Pressure suppresses both TN and TS and, for p>3.5 GPa, induces a third low temperature state, which is robust up to at least 7.5 GPa.
AB - We examine the low temperature states of two transition metal compounds: (i) NbFe2 is poised on the threshold of ferromagnetism and can be pushed into a spin-aligned state at low temperature by modifying the composition slightly. Stoichiometric NbFe2 has been reported as a rare example of lowtemperature spin density wave order in a d-metal system. We have used pressure, field and composition tuning to examine the phase diagram of NbFe2. Near the quantum critical point, we find distinct non-Fermi liquid forms of the resistivity and heat capacity, whereas we observe strong, hysteretic magnetoresistance effects deep in the ordered phase. (ii) Ca3Ru2O7 undergoes first a magnetic transition (TN = 56 K) and then a structural transition (TS = 48 K) on cooling. Most of the Fermi surface is gapped out at low temperature, leading to a very low carrier density and small Fermi surface pockets. Pressure suppresses both TN and TS and, for p>3.5 GPa, induces a third low temperature state, which is robust up to at least 7.5 GPa.
UR - http://www.scopus.com/inward/record.url?scp=77951997236&partnerID=8YFLogxK
U2 - 10.1002/pssb.200983079
DO - 10.1002/pssb.200983079
M3 - Article
AN - SCOPUS:77951997236
SN - 0370-1972
VL - 247
SP - 544
EP - 548
JO - Physica Status Solidi (B) Basic Research
JF - Physica Status Solidi (B) Basic Research
IS - 3
ER -