FeSi and alpha-FeSi2 single crystals were prepared by the Czochraiski
technique. beta-FeSi2 and alpha-FeSi2 single crystals were prepared by
chemical vapour transport. FeSi single crystals 18 cm(3) in size and
alpha-FeSi2 single crystals of a few cubic centimetres were obtained.
beta-FeSi2 decomposes peritectically above 970 degrees C, therefore on
ly needle-like crystals, each about 10 mm long, were grown from the va
pour. The temperature dependence of the resistivity was measured from
4.2 K up to room temperature. alpha-FeSi2 shows a weak temperature dep
endence of resistivity. The activation energy of FeSi, calculated from
In p=f(1/T) is equal to 58.2 meV. the Hall coefficient and resistivit
y of beta-FeSi2 single crystals was measured between 30 and 300 K. The
as-grown, not intentionally doped beta-FeSi2 crystals exhibit n-type
conductivity, while Cr and Al doped crystals show p-type conductivity.
The Hall coefficient of n-type samples depends on the magnetic field;
therefore, the transport properties of beta-FeSi2 were explained taki
ng into account two types of carrier, heavy and light. At low temperat
ure (32 K) heavy electrons show a mobility of mu(n) = 48 cm(2) V-1 s(-
1). An impurity band and an additional deep acceptor level are observe
d in p-type crystals. The activation energies of the shallow acceptor
level and deep acceptor level are equal to 55 meV and 100 meV respecti
vely. The mobility of holes mu(p) in p-type crystals reaches a maximum
of 1200 cm(2) V-1 s(-1) at 67 K. Magnetization and magnetic susceptib
ility measurements in the temperature range 4-320 K show a small posit
ive value of susceptibility and nonlinear magnetization for beta-FeSi2
but no ferromagnetic phase was detected. alpha-FeSi2 crystals show li
near magnetization and susceptibility similar to beta-FeSi2. Magnetiza
tion of FeSi is linear but the susceptibility passes through a minimum
at about 150-200 K.