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Resistively-detected
NMR
NMR (Nuc=
lear
Magnetic Resonance) is widely used to chemical, medical and physical studie=
s. In
spite of its excellent performance, however, NMR application to semiconduct=
or
systems, which play essential roles in recent electronics and cutting edge
solid-state physics, is limited due to the low sensitivity of conventional =
NMR.
Conventional NMR based on induction-detection requires multiple layers (100,
for example) of quantum wells to achieve a sufficient signal-to-noise ratio=
and
is not suitable for the analysis of semiconductor layer- and nano-structure=
s.
In fundamental studies of high mobility heterostructures, we studied the
interactions between electrons and nuclear spins at n=3D2/3 by
using quantum wells having full gate controllability [For example, <=
span
lang=3DEN-US style=3D'mso-bidi-font-size:10.5pt;font-family:"Times New Roma=
n"'>K.
Hashimoto, K. Muraki, T. Saku, and Y. Hirayama, Phys. Rev. Lett. 88, 176601
(2002)], and we confirmed
dynamic nuclear spin polarization induced by a current flow. Nuclear spin
polarization was detected as enhanced resistance, which is proportional to =
the
magnetization, Mz, of nuclear spins. Resistance can be measured for a
single layer and even for a nanostructure, so we can extend the powerful
feature of NMR to studies of semiconductor systems. The following figures
illustrate examples how we can get an NMR spectrum and nuclear spin relaxat=
ion
time (T1) by using a novel resistance detection technique=
. It
should be stressed that we need special states at<=
span
lang=3DEN-US style=3D'mso-bidi-font-size:10.5pt;font-family:Symbol;mso-fare=
ast-font-family:
"MS Gothic"'>n=3D2/3 f=
or
dynamic nuclear polarization, but we can apply these measurements for any
states we want to estimate.
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