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Limitations to the superposition principle: Superselection rules in
Limitations to the superposition principle: Superselection rules in

Linear optical controlled-NOT gate in the coincidence basis
Linear optical controlled-NOT gate in the coincidence basis

... given in Table IV. Using ␰ ⫽1 yields the perfectly matched case calculated previously 共see Table II兲. The error probability for Bell state discrimination is plotted in Fig. 4. For small mismatch the error is approximately equal to the percentage mismatch. Clearly, good Bell state discrimination will ...
270
270

institute of chemical technology
institute of chemical technology

LETTERS Generation of Fock states in a superconducting quantum circuit
LETTERS Generation of Fock states in a superconducting quantum circuit

Curriculum Vitae Irinel Chiorescu
Curriculum Vitae Irinel Chiorescu

PDF
PDF

... In this section we will construct a computational model, based on the lambda calculus, suitable for describing quantum computations. The language used will be an adaptation of the classical lambda calculus, extended with a set of quantum primitives. We will denote it by λi where the subscript stands ...
Josephson Effect for Photons in Two Weakly Linked Microcavities
Josephson Effect for Photons in Two Weakly Linked Microcavities

Fundamental aspects of quantum Brownian motion
Fundamental aspects of quantum Brownian motion

A Matrix Realignment Method for Recognizing Entanglement
A Matrix Realignment Method for Recognizing Entanglement

... We develop a very simple method to assess the inseparability of bipartite quantum systems, which is based on a realigned matrix constructed from the density matrix. It shows dramatic ability to identify many of the bounded entangled states discussed in the literature. Based on this criterion and the ...
Interference with correlated photons: Five quantum mechanics
Interference with correlated photons: Five quantum mechanics

Distinguishing mixed quantum states: Minimum
Distinguishing mixed quantum states: Minimum

A quantum model for the stock market
A quantum model for the stock market

29-sets-dictionaries
29-sets-dictionaries

Jensen3
Jensen3

Phys. Chem. Chem. Phys. 14, 9411-20
Phys. Chem. Chem. Phys. 14, 9411-20

Leftover Hashing Against Quantum Side Information
Leftover Hashing Against Quantum Side Information

Single Emitter Detection with Fluorescence and Extinction
Single Emitter Detection with Fluorescence and Extinction

Environment-Assisted Quantum Walks in Photosynthetic Energy
Environment-Assisted Quantum Walks in Photosynthetic Energy

Lecture 11 Identical particles
Lecture 11 Identical particles

... Quantum statistics: remarks Within non-relativistic quantum mechanics, correlation between spin and statistics can be seen as an empirical law. However, the spin-statistics relation emerges naturally from the unification of quantum mechanics and special relativity. The rule that fermions have half- ...
`To Be, To Be, What Does it Mean to Be?` : On Quantum
`To Be, To Be, What Does it Mean to Be?` : On Quantum

Three problems from quantum optics
Three problems from quantum optics

... transfer and protection against misuse. More specifically, quantum teleportation enables to transfer quantum information between stations where it cannot be be sent physically (i.e., that are not connected by a so-called quantum channel) [3, 5]. On the other hand, for protecting quantum information ...
Reprint  - Horizon Research Publishing
Reprint - Horizon Research Publishing

Strong-Disorder Fixed Point in the Dissipative Random Transverse-Field Ising Model
Strong-Disorder Fixed Point in the Dissipative Random Transverse-Field Ising Model

Molecule-Type Phases and Hund`s Rule in Vertically Coupled
Molecule-Type Phases and Hund`s Rule in Vertically Coupled

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Quantum key distribution



Quantum key distribution (QKD) uses quantum mechanics to guarantee secure communication. It enables two parties to produce a shared random secret key known only to them, which can then be used to encrypt and decrypt messages. It is often incorrectly called quantum cryptography, as it is the most well known example of the group of quantum cryptographic tasks.An important and unique property of quantum key distribution is the ability of the two communicating users to detect the presence of any third party trying to gain knowledge of the key. This results from a fundamental aspect of quantum mechanics: the process of measuring a quantum system in general disturbs the system. A third party trying to eavesdrop on the key must in some way measure it, thus introducing detectable anomalies. By using quantum superpositions or quantum entanglement and transmitting information in quantum states, a communication system can be implemented which detects eavesdropping. If the level of eavesdropping is below a certain threshold, a key can be produced that is guaranteed to be secure (i.e. the eavesdropper has no information about it), otherwise no secure key is possible and communication is aborted.The security of encryption that uses quantum key distribution relies on the foundations of quantum mechanics, in contrast to traditional public key cryptography which relies on the computational difficulty of certain mathematical functions, and cannot provide any indication of eavesdropping at any point in the communication process, or any mathematical proof as to the actual complexity of reversing the one-way functions used. QKD has provable security based on information theory, and forward secrecy.Quantum key distribution is only used to produce and distribute a key, not to transmit any message data. This key can then be used with any chosen encryption algorithm to encrypt (and decrypt) a message, which can then be transmitted over a standard communication channel. The algorithm most commonly associated with QKD is the one-time pad, as it is provably secure when used with a secret, random key. In real world situations, it is often also used with encryption using symmetric key algorithms like the Advanced Encryption Standard algorithm. In the case of QKD this comparison is based on the assumption of perfect single-photon sources and detectors, that cannot be easily implemented.
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