By Lajos Diosi

This brief and concise primer takes the vantage element of theoretical physics and the solidarity of physics. It units out to strip the burgeoning box of quantum details technological know-how to its fundamentals via linking it to common ideas in physics. an intensive lecture instead of a entire textbook, this quantity relies on classes brought over numerous years to complex undergraduate and starting graduate scholars, yet basically it addresses an individual with a operating wisdom of uncomplicated quantum physics. Readers will locate those lectures a so much sufficient access aspect for theoretical reports during this box.

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Extra info for A Short Course In Quantum Information Theory An Approach From Theoretical Physics

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We shall see in Sect. 4 of the next Chapter that such transition probabilities can be chosen as a measure of likeness — the fidelity — between two states in general. 3 The unknown qubit, Alice and Bob Because of the irreversibility of q-measurements an unknown q-state represents an issue much different from that of an unknown classical state. For various purposes in the forthcoming Chapters, we need the precise notion of the unknown qubit. Interestingly, there is no theoretical standard for the totally unknown mixed q-states but for the subset of the pure states.

The notion of qubit is best realized in the computational basis. We introduce the computational basis vectors |0 and |1 : |x x| = Iˆ , {|x ; x = 0, 1} , x |x = δx x . 1) x=0,1 Also the primitive binary q-physical quantity x ˆ is defined in the computational basis: x |x x| = |1 1| . 2) x=0,1 This is the (singular) 2 × 2 hermitian matrix of the qubit, as q-physical quantity. Its eigenvalues are 0 and 1. Often the q-state, rather than x ˆ, is called the qubit. The generic pure state is a superposition of the basis vectors: c0 |0 + c1 |1 ≡ cx |x ; |c0 |2 + |c1 |2 = 1 .

H ≡ H⊗n . 51) ρˆ ⊗ ρˆ ⊗ . . 52) The collective state reads: while the state vector of a pure collective state is: |ψ ⊗ |ψ ⊗ . . |ψ ≡ |ψ ⊗n . 53) If Aˆ is a q-physical quantity of the elementary subsystem then, in a natural way, one can introduce its arithmetic mean, over the n subsystems, as a collective q-physical quantity: Aˆ ⊗ Iˆ⊗(n−1) + Iˆ ⊗ Aˆ ⊗ Iˆ⊗(n−2) + · · · + Iˆ⊗(n−1) ⊗ Aˆ . 54) Collective q-physical quantities are not necessarily of such simple form. Their measurement is the collective q-measurement.

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