  Previous studies have demonstrated spin-orbit torque (SOT) switching of Mn3Sn
where the spin polarization lies in the kagome plane (configuration I).
However, the critical current density ($ J_{crit}$) is unrealistically large ($
J_{crit}$=$ 10^{14}$ A/$ m^2$) and independent on the external field ($
H_{ext}$). The stabilized magnetic state also depends on the initial state.
These features conflict with the ferromagnet (FM) switching scheme as claimed
in those studies, and thus call for other explanations. Alternatively, the
system with the spin polarization perpendicular to the kagome plane
(configuration II) is more like the FM based system since the spin polarization
is orthogonal to all magnetic moments. In this work, we show SOT switching of
Mn3Sn in configuration II. Similar to the FM, Jcrit and Hext are in the order
of $ 10^{10}$ A/$ m^2$ and hundreds of Oersted, respectively. The switching
result is also independent of the initial state. Interestingly, the unique spin
structure of Mn3Sn also leads to distinct features from FM systems. We
demonstrate that Jcrit increases linearly with Hext, and extrapolation gives
ultralow $ J_{crit}$ for the field-free switching system. In addition, the
switching polarity is opposite to the FM. We also provide the switching phase
diagram as a guideline for experimental demonstration. Our work provides
comprehensive understanding for the switching mechanism in both configurations.
The switching protocol proposed in this work is more advantageous in realistic
spintronic applications. We also clearly reveal the fundamental difference
between FM and noncollinear antiferromagnetic switching.
