NdCu2 shows a complex magnetic phase diagram below its Neel temperature of
T-N = 6.5 K and for magnetic fields applied in the easy b direction. This c
omplicated behavior is expected to be due to Ruderman-Kittel-Kasuya-Yoshida
interaction of the 4f shells of the Nd ions in the presence of crystal fie
ld splitting. In order to obtain deeper insight into the mechanism leading
to such different magnetic phases we started to study the spin wave spectra
in a NdCu2 single crystal. In zero field as well as in fields applied in t
he easy b direction of magnetization, a pronounced minimum in the excitatio
n spectrum has been observed and it forms an energy gap. The position of th
is spin wave gap does not coincide with any magnetic ordering wave vector i
n NdCu2, indicating anisotropic magnetic coupling. The temperature and fiel
d dependence of the spin wave gap have been studied. The position of the ga
p remains constant at q(gap) = (0.35, 0, 0), whereas the character of the e
xcitations changes with temperature and the value of the energy gap changes
with the magnetic field. Applying a field of 10 T in the hard c direction
of magnetization changes the position of the minimum to q(gap) = (0.6, 0, 0
) and gives proof of magnetic anisotropy. (C) 1999 American Institute of Ph
ysics. [S0021-8979(99)40808-4].