The qubit is then in state v examples of qubits atomic

Info iconThis preview shows page 1. Sign up to view the full content.

View Full Document Right Arrow Icon
This is the end of the preview. Sign up to access the rest of the document.

Unformatted text preview: s on a tightly held piece of string. Two such individual levels can be isolated to configure the basis states for a qubit. 1.7. QUBITS 13 Figure 1.3: Energy level diagram of an atom. Ground state and first excited state correspond to qubit levels, |0￿ and |1￿, respectively. Photon Polarization Classically, a photon may be described as a traveling electromagnetic wave. This description can be fleshed out using Maxwell’s equations, but for our purposes we will focus simply on the fact that an electromagnetic wave has a polarization which describes the orientation of the electric field oscillations (see Fig. 1.4). So, for a given direction of photon motion, the photon’s polarization axis might lie anywhere in a 2-d plane perpendicular to that motion. It is thus natural to pick an orthonormal 2-d basis (such as ￿ and ￿ , or “vertical” and x y “horizontal”) to describe the polarization state (i.e. polarization direction) of a photon. In a quantum mechanical description, this 2-d nature of the photon polarization is represented by a qubit, where the amplitude of the overall polarization state in each basis vector is just the projection of the polarization in that direction. The polarization of a photon can be measured by using a polaroid film or a calcite crystal. A suitably oriented polaroid sheet transmits x-polarized photons and absorbs y-polarized photons. Thus a photon that is in a superposition |φ￿ = α |x￿ + β |y￿ is transmitted with probability |α|2 . If the photon now encounters another polariod sheet with the same orientation, then it is transmitted with probability 1. On the other hand, if the second polaroid sheet has its axes crossed at right angles to the first one, then if the photon is transmitted by the first polaroid, then it is definitely absorbed by the second sheet. This pair of polarized sheets at right angles thus blocks all the light. A somewhat counter-intuitive result is now obtained by interposing a third polariod sheet at a 45 degree angle between the first two. Now a photon that is transmitted by the first sheet makes it through the next two with probability 14 CHAPTER 1. INTRODUCTION 1/4. Figure 1.4: Using the polarization state of light as the qubit. Horizontal polarization corresponds to qubit state, |ˆ￿, while vertical polarization corresponds x to qubit state, |ˆ￿. y To see this first observe that any photon transmitted through the first filter is in the state, |0￿. The probability this photon is transmitted through the second filter is 1/2 since it is exactly the probability that a qubit in the state |0￿ ends up in the state |+￿ when measured in the |+￿ , |−￿ basis. We can repeat this reasoning for the third filter, except now we have a qubit in state |+￿ being measured in the |0￿ , |1￿-basis — the chance that the outcome is |0￿ is once again 1/2. Spins Like photon polarization, the spin of a (spin-1/2) particle is a two-state system, and can be d...
View Full Document

This document was uploaded on 09/22/2013.

Ask a homework question - tutors are online