Heiss W.D. (ed.) Quantum dots.. a doorway to - tiera.ru
Heiss W.D. (ed.) Quantum dots.. a doorway to - tiera.ru
Heiss W.D. (ed.) Quantum dots.. a doorway to - tiera.ru
Create successful ePaper yourself
Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.
92 J.M. Elzerman et al.<br />
pulses <strong>to</strong> control the inter-dot coupling, in order <strong>to</strong> demonstrate superposition<br />
and entanglement of spin states.<br />
For such experiments, the QPC is an invaluable <strong>to</strong>ol. It allows us <strong>to</strong> probe a<br />
dot that is nearly isolat<strong>ed</strong> from the reservoirs, which is a regime not accessible<br />
<strong>to</strong> conventional transport experiments. Most importantly, it enables us <strong>to</strong><br />
study a single spin or charge, rather than measuring average properties of a<br />
large ensemble. The QPC charge and spin detec<strong>to</strong>r is therefore essential <strong>to</strong><br />
achieve the kind of single-particle control that is requir<strong>ed</strong> for creating a qubit –<br />
transport experiments are no longer necessary.<br />
The techniques we have develop<strong>ed</strong> are not only suitable for quantum computation.<br />
Now that the spin orientation of a single electroncan be measur<strong>ed</strong>,<br />
we can think of using the spin as a local probe <strong>to</strong> explore the semiconduc<strong>to</strong>r<br />
environment. For instance, measuring the spin relaxation time in various situations<br />
could reveal details of different mechanisms for spin-orbit coupling.<br />
We could vary the orientation of the magnetic field with respect <strong>to</strong> the crystal<br />
axes, or investigate the effect of static or time-varying electric fields. Once<br />
we can measure the electron spin resonance frequency, this would allow us <strong>to</strong><br />
study the polarization of the nuclear spin ensemble via the Overhauser effect.<br />
In all these cases, the fact that dot parameters such as the Zeeman splitting<br />
or the tunnel coupling <strong>to</strong> reservoirs can be controll<strong>ed</strong> in situ, makes a lateral<br />
quantum dot fill<strong>ed</strong> with a single spin a system of great versatility and<br />
fundamental importance.<br />
Acknowl<strong>ed</strong>gments<br />
We thank T. Fujisawa, T. Hayashi, T. Saku and Y. Hirayama for help with<br />
device fabrication, M. Blaauboer, D.P. DiVincenzo, H.A. Engel, C.J.P.M. Harmans,<br />
V. Golovach, D. Loss, R. Schoelkopf, K. Schwab and W.G. van der Wiel<br />
for helpful discussions, and B. van der Enden and R. Schouten for technical<br />
support. We acknowl<strong>ed</strong>ge financial support from the Specially Promot<strong>ed</strong><br />
Research Grant-in-Aid for Scientific Research from the Japanese Ministry<br />
of Education, Culture, Sports, Science and Technology, the DARPA-QUIST<br />
program (DAAD19-01-1-0659), the EU-RTN network on spintronics, and the<br />
Dutch Organisation for Fundamental Research on Matter (FOM).<br />
References<br />
1. M.A. Nielsen and I.L. Chuang, <strong>Quantum</strong> computation and quantum information,<br />
(Cambridge University Press, Cambridge, England, 2000). 25, 86<br />
2. D. Loss and D.P. DiVincenzo, Phys. Rev. A 57, 120 (1998). 25, 29, 30, 31, 48, 58, 59, 72, 82, 90<br />
3. R.P. Feynman, The Feynman Lectures on Physics, Vol. 3 (Addison Wesley,<br />
1970). 26, 27<br />
4. M. Riebe et al., Nature 429, 734 (2004). 26