ABSTRACT - DRUM - University of Maryland
ABSTRACT - DRUM - University of Maryland
ABSTRACT - DRUM - University of Maryland
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Chapter 5<br />
Topological Protection <strong>of</strong> Majorana-Based Qubits<br />
In this chapter we investigate the effect <strong>of</strong> finite-temperature thermal fluctuations<br />
on three key aspects <strong>of</strong> topological quantum computation: quantum coherence<br />
<strong>of</strong> the topological qubits, topologically-protected quantum gates and the read-out<br />
<strong>of</strong> qubits. Since the information is encoded in non-local degrees <strong>of</strong> freedom <strong>of</strong> the<br />
ground state many-body wavefunction, it is important to keep the system close to<br />
the ground state. However, any systems realized in the laboratory are operated at<br />
a finite temperature T > 0. To prevent uncontrollable thermal excitations, it is<br />
generally accepted that T has to be way below the bulk excitation gap. However,<br />
complications appear when there exist various types <strong>of</strong> single-particle excitations<br />
with different magnitudes <strong>of</strong> gaps which can change the occupation <strong>of</strong> the nonlocal<br />
fermionic modes. Note that throughout the chapter we assume that Majorana<br />
fermions are sufficiently far away from each other and neglect exponentially small<br />
energy splitting due to inter-vortex tunneling. The effect <strong>of</strong> these processes on topological<br />
quantum computing has been discussed elsewhere [91, 106]. Another trivial<br />
effect not considered in this work is a situation where the fermion parity conservation<br />
is explicitly broken by the Majorana mode being in direct contact with a<br />
bath <strong>of</strong> fermions (electrons and holes) where obviously the Majorana will decay into<br />
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