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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

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