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December, 3 rd 2007 Philippe LABOUCHERE Annika BEHRENS. Quantum Cryptography. Introduction Photon sources Quantum Secret Sharing. Introduction Photon sources Quantum Secret Sharing. How to measure information (1). Claude E. Shannon 1948 Information entropy Mutual information. [bits].
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December, 3rd 2007 Philippe LABOUCHERE Annika BEHRENS Quantum Cryptography
Introduction • Photon sources • Quantum Secret Sharing
Introduction • Photon sources • Quantum Secret Sharing
How to measure information (1) • Claude E. Shannon 1948 • Information entropy • Mutual information [bits]
How to measure information (2) • Relation between H and I • Mutual information between 2 parties
The BB84 protocol: principle • 2 conjugate basis • Information encoded in photon’s polarization → ’0’ ≡ —& / → ’1’ ≡ | & \ • Quantum & classical channels used for key exchange Charles H. Bennett Gilles Brassard
From random bits to a sifted key Quantum transmission Public discussion
The no-cloning theorem • Dieks, Wootters, Žurek 1982 ”It is forbidden to create identical copies of an arbitrary unknown quantum state.” • Quantum operations : unitary & linear transformations on the state of a quantum system
Introduction • Photon sources • Quantum Secret Sharing
Sources of photons • Thermal light • Coherent light • Squeezed light Average photon number of photons in a mode Number of photons
Faint-laser pulses • <n> = μ~ 0.1 photon / pulse • Photon-number splitting attack! • Dark counts of detectors vs high pulse rate & weaker pulses Detection yield Transmission efficiency ! Tradeoff
Entangled photon pairs • Spontaneous Parametric Down Conversion • Idler photon acts as trigger for signal photon • Very inefficient
Single-photon sources • Intercept/resend attack => error rate < dark count rate ! • Condition for security: • Drawback : dark counts & afterpulses Detection yield Transmission efficiency
Practical limits of QC • Realization of signal • Stability under the influence of the environment (transportation) - Birefringence - Polarization dispersion - Scattering • Need of efficient sources & detectors (measurements)
Bite rate as function of distance after error correction and privacy amplification Pulse rate = 10 MHz μ = 0.1 (faint laser pulses) Losses:@ 800nm : 2dB / km @ 1300 nm: 0.35dB / km @ 1550 nm: 0.25 dB /km
Introduction • Photon sources • Quantum Secret Sharing
QSS (2) • N-qubit GHZ source • Define