Recent studies of n-type semiconductors have demonstrated spin-coherent tra
nsport over macroscopic distances(1), with spin-coherence times exceeding 1
00 ns(2,3); such materials are therefore potentially useful building blocks
for spin-polarized electronics ('spintronics'). Spin injection into a semi
conductor (a necessary step for spin electronics(4)) has proved difficult(5
,6); the only successful approach involves classical injection of spins fro
m magnetic semiconductors(7,8). Other work has shown that optical excitatio
n can provide a short (<500 ps) non-equilibrium burst of coherent spin tran
sfer across a GaAs/ZnSe interface, but less than 10% of the total spin cros
ses into the ZnSe layer, leaving long-lived spins trapped in the GaAs layer
(ref. 9). Here we report a 'persistent' spin-conduction mode in biased sem
iconductor heterostructures, in which the sourcing of coherent spin transfe
r lasts at least 1-2 orders of magnitude longer than in unbiased structures
. We use time-resolved Kerr spectroscopy to distinguish several parallel ch
annels of interlayer spin-coherent injection. The relative increase in spin
-coherent injection is up to 500% in the biased structures, and up to 4,000
% when p-n junctions are used to impose a built-in bias. These experiments
reveal promising opportunities for multifunctional spin electronic devices
(such as spin transistors that combine memory and logic functions), in whic
h the amplitude and phase of the net spin current are controlled by either
electrical or magnetic fields.