* Corresponding author. Tel.: #49-892891-4661; fax: #49- 892895-4661. E-mail address: pyka@physik.tu-muenchen.de (N.M. Pyka). Physica B 292 (2000) 191}193 The momentum space distribution of the low-energy magnetic response in Nd Ce CuO at T)0.1 K and up to 5.7 T N.M. Pyka*, M. Loewenhaupt, A. Metz, W. Schmidt Technical University Munich, ZBE FRM-II, D-85747 Garching, Germany Institut fu ( r Angewandte Physik (IAPD), TU-Dresden, D-01062 Dresden, Germany Institut fu ( r Festko ( rperforschung, FZ-Ju ( lich, D-52425 Ju ( lich, Germany Institut Laue-Langevin, F-38042 Grenoble, France Received 25 February 2000 Abstract The momentum space distribution of the magnetic response of Nd spins in a single crystal of Nd Ce CuO has been measured with inelastic neutron scattering as a function of an applied magnetic "eld along [0 1 0]. The observed q-widths along [1 0 0] and [0 0 1] of the tetragonal lattice are rather large in the low-"eld region up to 2 T, which corresponds to the heavy-fermion phase. A drastic decrease in q-width occurs to higher "elds. The q-width of the magnetic response at (0 0 2) along the [1 0 0] direction changes by a factor two, while in the [0 0 1] direction and around (0 0 3) the decrease is 30% to 40%. Nevertheless, all observed q-widths remain signi"cantly broadened up to 5.7 T. 2000 Elsevier Science B.V. All rights reserved. Keywords: Heavy fermions; Magnetic correlations; Short-range order In pure Nd CuO low-energy spin waves with E(1 meV are observed, which are due to transi- tions within the ground state of Nd [1]. Replac- ing Nd ions by Ce shifts these excitations to lower energies, mainly due to a reduction of the Cu-staggered "eld acting on the Nd spins [2]. With increasing Ce doping the Nd spin waves lose the long-range correlation and a broad inelastic mag- netic response is observed [3,4]. In addition, at high doping, x'0.1 in Nd Ce CuO , heavy- fermion behavior was observed [5,6], which is caused by a hybridization of Nd-4f electrons with Cu-3d band electrons and can be detected with neutron scattering as Q-independent quasielastic scattering [7]. At a Ce doping of x"0.15 this quasielastic scattering is removed by the applica- tion of a magnetic "eld of 2 T [8]. For "elds above 3.7 T, a partially aligned phase of Nd spins is for- med [9] and in the following this is referred to as the high-"eld phase. On a x"0.15 single crystal, the same as used in the present experiment, two branches of magnetic excitations have been ob- served in the c-direction [7], starting at the - points (0 0 2) and (0 0 3) at 0.13 and 0.24 meV energy transfer. In this paper, we present the magnetic "eld dependence of the momentum space distribution of the inelastic magnetic response of Nd spins in Nd Ce CuO around (0 0 2) and (0 0 3). 0921-4526/00/$ - see front matter 2000 Elsevier Science B.V. All rights reserved. PII: S 0 9 2 1 - 4 5 2 6 ( 0 0 ) 0 0 4 7 8 - 6