Lean, informalized

Nielsen & Chuang · Chapter 8, Quantum noise and quantum operations · p. 386

Exercise 8.29 - What three noise channels of a qubit do to the identity operator

Depolarizing and phase damping are unital, amplitude damping is not.

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The Exercise

A quantum operation ℰ\mathcal{E} on a qubit is unital if it maps the identity operator to itself, ℰ(I)=I\mathcal{E}(I) = I. A unital operation leaves the maximally mixed state I/2I/2 where it is. The exercise asks to show that two of the standard noise channels on a qubit, the depolarizing channel and the phase damping channel, are unital, and that the amplitude damping channel is not.

A Qubit

The library states the three facts together, for a qubit with a fixed computational basis. Let HH be the state space of the qubit and |0⟩|0\rangle, |1⟩|1\rangle its computational basis, with |0⟩|0\rangle the ground state and |1⟩|1\rangle the excited state. For ii in {0,1}\{0,1\}, the projector PiP_i onto the basis vector |i⟩|i\rangle is the rank one operator |i⟩⟨i||i\rangle\langle i| on HH.✦ The lowering operator σ−\sigma_- of the qubit is the operator |0⟩⟨1||0\rangle\langle 1| on HH.✦

Three Noise Channels

The amplitude damping channel ℰAD\mathcal{E}_{AD} with damping probability γ\gamma is the quantum operation that sends a linear operator ρ\rho on HH to ℰAD(ρ)=E0ρE0†+E1ρE1†,\mathcal{E}_{AD}(\rho) = E_0 \rho E_0^\dagger + E_1 \rho E_1^\dagger ,(1) where the dagger denotes the adjoint and the operation elements E0E_0 and E1E_1 are the operators on HH E0=P0+1−γP1,E1=γσ−.E_0 = P_0 + \sqrt{1-\gamma}\, P_1 , \qquad E_1 = \sqrt{\gamma}\, \sigma_- .(2)✦ The element E1E_1 describes the loss of one quantum of energy.

The phase damping channel ℰPD\mathcal{E}_{PD} with parameter λ\lambda is the quantum operation that sends a linear operator ρ\rho on HH to ℰPD(ρ)=F0ρF0†+F1ρF1†,F0=P0+1−λP1,F1=λP1,\mathcal{E}_{PD}(\rho) = F_0 \rho F_0^\dagger + F_1 \rho F_1^\dagger , \qquad F_0 = P_0 + \sqrt{1-\lambda}\, P_1 , \quad F_1 = \sqrt{\lambda}\, P_1 ,(3)✦ with operation elements F0F_0 and F1F_1.

The Pauli matrices XX, YY and ZZ are the two by two complex matrices X=(0110),Y=(0−ii0),Z=(100−1).X = \begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix} , \qquad Y = \begin{pmatrix} 0 & -i \\ i & 0 \end{pmatrix} , \qquad Z = \begin{pmatrix} 1 & 0 \\ 0 & -1 \end{pmatrix} .(4) The depolarizing channel ℰdep\mathcal{E}_{\mathrm{dep}} with parameter pp is the map on two by two complex matrices ρ\rho given by ℰdep(ρ)=(1−3p4)ρ+p4(XρX+YρY+ZρZ).\mathcal{E}_{\mathrm{dep}}(\rho) = \Bigl(1 - \frac{3p}{4}\Bigr) \rho + \frac{p}{4} \bigl( X \rho X + Y \rho Y + Z \rho Z \bigr) .(5)✦

The Claim

Theorem 1. For every real pp, the depolarizing channel maps the two by two identity matrix II to itself, ℰdep(I)=I.\mathcal{E}_{\mathrm{dep}}(I) = I .(6)✦ For every λ\lambda with 0≤λ≤10 \le \lambda \le 1, the phase damping channel maps the identity operator II on the state space HH of the qubit to itself, ℰPD(I)=I.\mathcal{E}_{PD}(I) = I .(7)✦ For every damping probability γ\gamma with 0<γ≤10 < \gamma \le 1, the amplitude damping channel does not, ℰAD(I)≠I.\mathcal{E}_{AD}(I) \neq I .(8)✦

What Is Checked

The claim is stated over the three channels (1), (3) and (5).