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
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26 J.M. Elzerman et al.<br />
combining fast QPC charge detection with “spin-<strong>to</strong>-charge conversion”. This<br />
fully electrical technique <strong>to</strong> read out a spin qubit is then us<strong>ed</strong> <strong>to</strong> determine<br />
the relaxation time of the single spin, giving a value of 0.85 ms at a magnetic<br />
field of 8 Tesla.<br />
Finally, Sect. 6 puts the results in perspective, arriving at a realistic path<br />
<strong>to</strong>wards the experimental demonstration of single- and two-qubit gates and<br />
the creation of entanglement of spins in quantum dot systems.<br />
1 Introduction<br />
This section gives a brief introduction in<strong>to</strong> quantum computing, continuing<br />
with a description of semiconduc<strong>to</strong>r quantum <strong>dots</strong> that covers their fabrication<br />
as well as their electronic behavior. We also describe our experimental setup<br />
for performing low-temperature transport experiments <strong>to</strong> probe such quantum<br />
<strong>dots</strong>.<br />
1.1 <strong>Quantum</strong> Computing<br />
More than three quarters of a century after its birth, quantum mechanics remains<br />
in many ways a peculiar theory [3]. It describes many physical effects<br />
and properties with great accuracy, but uses unfamiliar concepts like superposition,<br />
entanglement and projection, that seem <strong>to</strong> have no relation with the<br />
everyday world around us. The interpretation of these concepts can still cause<br />
controversy.<br />
The inherent strangeness of quantum mechanics already emerges in the<br />
simplest case: a quantum two-level system. Unlike a classical two-level system,<br />
which is always either in state 0 or in state 1, a quantum two-level system can<br />
just as well be in a superposition of states |0〉 and |1〉. It is, in some sense, in<br />
both states at the same time.<br />
Even more exotic states can occur when two such quantum two-level systems<br />
interact: the two systems can become entangl<strong>ed</strong>. Evenifweknowthe<br />
complete state of the system as a whole, for example (|01〉−|10〉)/ √ 2, which<br />
tells us all there is <strong>to</strong> know about it, we cannot know the state of the two<br />
subsystems individually. In fact, the subsystems do not even have a definite<br />
state! Due <strong>to</strong> this strong connection between the two systems, a measurement<br />
made on one influences the state of the other, even though it may be arbitrarily<br />
far away. Such spooky non-local correlations enable effects like “quantum<br />
teleportation” [4, 5].<br />
Finally, the concept of measurement in quantum mechanics is rather special.<br />
The evolution of an isolat<strong>ed</strong> quantum system is deterministic, as it is<br />
govern<strong>ed</strong> by a first order differential equation – the Schrödinger equation.<br />
However, coupling the quantum system <strong>to</strong> a measurement apparatus forces<br />
it in<strong>to</strong> one of the possible measurement eigenstates in an apparently nondeterministic<br />
way: the particular measurement outcome is random, only the