The spin-dependent electron transport has been studied in magnetic semiconductor waveguides (nanowires) in the helical magnetic field. We have shown that -apart from the known conductance dip located at the magnetic field equal to the helical-field amplitude B h -the additional conductance dips (with zero conductance) appear at magnetic field different from B h . This effect occuring in the non-adiabatic regime is explained as resulting from the resonant Landau-Zener transitions between the spin-splitted subbands.
PACS numbers: xxxThe experimental realization of an effective spintransistor remains a challenge facing spintronics since the pioneering concept proposed by Datta and Das. 1 According to the original idea the operation of the spin transistor is based on the gate-controlled spin-orbit interaction (SOI) of Rashba form. 2 The current of spin polarized electrons is injected from the ferromagnetic source into the conduction channel formed in a two-dimensional electron gas (2DEG) and is ballistically transported to the ferromagnetic drain. The state of the transistor depends on the electron spin orientation modulated via the Rashba SOI by the voltage applied to the gate attached close to the channel. The operation of spin transistor has been studied in many theoretical papers. 3-7 However, the experiments 8,9 indicate that the signals obtained in the up-to-date realized spin transistors based on the SOI are rather low, which results from the low efficiency of the spin injection from the ferromagnet into the semiconductor 10 and the spin relaxation. The SOI causes that the scattering processes affect the spin states of electrons, e.g., by the Elliott-Yafet or Dyakonov-Perel mechanism. 11 Although the spin relaxation is proposed to be suppressed by equating the Rashba and Dresselhaus term, 12,13 the concept of the non-ballistic spin transistor proposed by Schliemann et al. in Ref. 12 is still waiting for the experimental realizations.An alternative spin-transistor design, with the spin relaxation length as long as 50 µm, has been recently described byŽutić and Lee 14 and experimentally demonstrated by Betthausen et al. in Ref. 15. In this approach, the spin control is realized by combining the homogeneous and helical magnetic fields. The latter is generated by ferromagnetic stripes located above the conduction channel. The spin state of electrons flowing through the channel is protected against a possible decay by keeping the transport in the adiabatic regime. 16 The transistor action is driven by the diabatic Landau-Zener transitions 17,18 induced by the appropriate tuning of the homogeneous magnetic field. For these suitably chosen conditions the backscattering of spin polarized electrons appears, which gives raise to the large increase of the resistance, i.e., the transistor goes over into the 'off' state. In contrast to the SOI-based spin transistor, the proposed design is robust against the scattering processes. 19Motivated by the experiment, 15 we have performed the computer simulations of the spin-depend...