Judge each claim by whether the stated device's noise allows it

PHYSICS · Multi-part · Fermi University Physics · Quantum Information & Technology · Physical realizations and quantum technologies · Physical realizations and quantum technologies

Quantum Information and Technology, Ch Quantum metrology and sensing

Problem

Judge each claim by whether the stated device's noise allows it. Idealisations: for the computing claim, gate errors act independently and identically on every gate, with no correlations; for the sensing claim, atoms dephase independently at the stated rate. ((a)) Computing. A team runs Shor's algorithm on 5050 physical qubits with no error correction, each two-qubit gate having average infidelity r=5×10−3r=5\times10^{-3}, and claims it can factor a 20482048-bit RSA modulus because Shor's algorithm needs only O(L3)O(L^3) gates, here about L3≈8.6×109L^3\approx8.6\times10^9 gates for L=2048L=2048. Estimate the probability that every gate in such a circuit succeeds, and say whether the claim survives. ((b)) Key distribution. A team runs BB84 over 200 km200\,\mathrm{km} of fibre attenuating at 0.2 dB/km0.2\,\mathrm{dB/km}, sending weak coherent pulses with mean photon number μ=1\mu=1 and no decoy states, and claims the resulting key is "secure against any eavesdropper permitted by quantum mechanics." Give the fibre transmission in decibels and as a fraction, and say what standard attack this claim ignores and why it matters at this loss. ((c)) Sensing. A team prepares N=104N=10^4 atoms, each with independent dephasing time T2=1 sT_2=1\,\mathrm{s}, either as independent atoms or as one NN-atom GHZ state, averages for T=1000 s\mathcal{T}=1000\,\mathrm{s}, and optimises the free-precession time for each scheme, then claims "entanglement gives us a hundredfold better frequency sensitivity." Using Δωopt=2e/(NTT2)\Delta\omega_{\rm opt}=\sqrt{2e/(N\mathcal{T}T_2)}, valid for both optimised schemes, evaluate the claim.

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