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Unformatted text preview: vector spaces, is also endowed with an inner product. And an inner product is a way of taking two states (vectors in the Hilbert space) and getting a number out. For instance, define ￿ |ψ ￿ = ak | k ￿ , k where the kets |k ￿ form a basis, so are orthogonal. If we instead write this state as a column vector, a0 a1 |ψ ￿ = . . . a N −1 Then the inner product of |ψ ￿ with itself is a0 a1 ￿ ￿ ￿ ψ , ψ ￿ = a∗ a∗ · · · a∗ 1 · . 0 1 N . . a N −1 N −1 N −1 ￿ ￿∗ ak ak = | ak | 2 = k=0 k=0 The complex conjugation step is important so that when we take the inner product of a vector with itself we get a real number which we can associate 10 CHAPTER 1. INTRODUCTION with a length. Dirac noticed that there could be an easier way to write this by defining an object, called a “bra,” that is the conjugate-transpose of a ket, ￿ψ | = |ψ ￿† = ￿ k a∗ ￿ k | . k This object acts on a ket to give a number, as long as we remember the rule, ￿j | |k ￿ ≡ ￿j |k ￿ = δjk Now we can write the inner product of |ψ ￿ with itself as ￿ψ |ψ ￿ = = ￿ j ￿ j,k = ￿ ￿ a∗ ￿ j | j a∗ ak ￿ j | k ￿ j ￿ k ak | k ￿ ￿ a∗ ak δjk j j,k = ￿ k | ak | 2 Now we can use the same tools to write the inner product of any two states, |ψ ￿ and |φ￿, where ￿ |φ￿ = bk | k ￿ . k Their inner product is, ￿ψ |φ￿ = ￿ j,k a ∗ bk ￿ j | k ￿ = j ￿ a ∗ bk k k Notice that there is no reason for the inner product of two states to be real (unless they are the same state), and that ￿ψ |φ￿ = ￿φ|ψ ￿∗ ∈ C In this way, a bra vector may be considered as a “functional.” We feed it a ket, and it spits out a complex number. 1.6. THE MEASUREMENT PRINCIPLE 11 The Dual Space We mentioned above that a bra vector is a functional on the Hilbert space. In fact, the set of all bra vectors forms what is known as the dual space. This space is the set of all linear functionals that can act on the Hilbert space. 1.6 The Measurement Principle ￿ −1 This linear superposition |ψ ￿ = k=0 αj |j ￿ is part of the private world of the j electron. Access to the information describing this state is severely limited — in particular, we cannot actually measure the complex amplitudes αj . This is not just a practical limitation; it is enshrined in the measurement postulate of quantum physics. A measurement on this k state system yields one of at most k possible outcomes: i.e. an integer between 0 and k − 1. Measuring |ψ ￿ in the standard basis yields j with probability |αj | 2 . One important aspect of the measurement process is that it alters the state of the quantum system: the effect of the measurement is that the new state is exactly the outcome of the measurement. I.e., if the outcome of the measurement is j , then following the measurement, the qubit is in state |j ￿. This implies that you cannot collect any additional information about the amplitudes αj by repeating...
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This document was uploaded on 09/22/2013.

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