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PDF (double-sided) - Physics Department, UCSB - University of ...

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Figure 3.4: Bloch Sphere – a) Bloch sphere: Quantum states in two-level systems<br />

can be depicted as vectors on a sphere. b) Rotations: Operations on the system are<br />

visualized as rotations <strong>of</strong> the state vector around an axis defined by the operation.<br />

c) Off-resonant rotations: If the qubit is driven <strong>of</strong>f resonance, the rotation vector<br />

points out <strong>of</strong> the X/Y-plane leading to rotations that can no longer cover great<br />

circles.<br />

the “Bloch Sphere” after Felix Bloch.<br />

The states | n 〉 and | m 〉 are placed at<br />

the poles <strong>of</strong> the sphere and any arbitrary superposition <strong>of</strong> the two is depicted by<br />

a vector pointing to the surface <strong>of</strong> the sphere, called the “Bloch Vector”. The<br />

spherical coordinates θ and ϕ that describe the direction <strong>of</strong> the Bloch Vector are<br />

related to the described state via:<br />

e iα | ψ 〉 = cos θ 2 | n 〉 + eiϕ sin θ 2 | m 〉 (3.37)<br />

In this picture, the qubit interaction described above corresponds to a rotation<br />

<strong>of</strong> the Bloch Vector around an axis pointing in the direction given by the prefactors<br />

<strong>of</strong> σ x , σ y , and σ z . The sum <strong>of</strong> the squares <strong>of</strong> the prefactors is related to the rotation<br />

angle. Since the I-part <strong>of</strong> the interaction only influences the overall phase factor<br />

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