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Basis Sets in Quantum Chemistry C. David Sherrill School of
Basis Sets in Quantum Chemistry C. David Sherrill School of

Mechanical Proof of the Second Law of Thermodynamics Based on
Mechanical Proof of the Second Law of Thermodynamics Based on

... This is also known as the Helmholtz Entropy (Campisi, 2005). Quantization of the Helmholtz Entropy is almost immediate. Indeed, using a colorful expression, I would say that Eq. (4) invites the reader to quantize. Using the semiclassical approximation of Bohr-Sommerfeld (Landau and Lifshitz, 1958) a ...
Document
Document

Rotation and phase-shift operations for a charge qubit in a double
Rotation and phase-shift operations for a charge qubit in a double

Singularity of the time-energy uncertainty in adiabatic perturbation
Singularity of the time-energy uncertainty in adiabatic perturbation

PDF
PDF

... it a better candidate for practical atom interferometry for rotation sensing. Furthermore, the CI may be used to realize novel configuration where the wavepackets may trace out multiple loops in a manner such that the rotational sensitivity would vanish, thus making it more versatile for other measu ...
Positronium: Review of symmetry, conserved quantities and decay
Positronium: Review of symmetry, conserved quantities and decay

Reflections on the deBroglie–Bohm Quantum Potential
Reflections on the deBroglie–Bohm Quantum Potential

... Theory came about (in part) from the abandonment of those previously held physical concepts and principles mentioned above. The state of a quantum system is represented in Orthodox Quantum Theory by a (state) vector in an abstract, mathematical space. The state vector is assumed to contain all possi ...
Superconducting Circuits and Quantum Computation—T. P. Orlando
Superconducting Circuits and Quantum Computation—T. P. Orlando

... Chapter 20. Superconducting Circuits and Quantum Computation Figure 1a shows a SEM image of the persistent current qubit (inner loop) and the measuring dc SQUID (outer) loop. A schematic of the qubit and the measuring circuit is shown in Figure 1b, where the Josephson junctions are denoted by x's. ...
Public-Key Cryptosystems Based on Hard Problems
Public-Key Cryptosystems Based on Hard Problems

NanoTrapS: Trapped nanoparticles for space experiments
NanoTrapS: Trapped nanoparticles for space experiments

An N-atom Collective State Atomic Interferometer with Ultra
An N-atom Collective State Atomic Interferometer with Ultra

The Quantum Perspective of Learing
The Quantum Perspective of Learing

majorization and quantum entanglement
majorization and quantum entanglement

Steady-state entanglement of two atoms created by classical driving
Steady-state entanglement of two atoms created by classical driving

... systems. It is well known that two-level atoms can be successfully used to model entangled states of qubits as well as realization of different quantum communication protocols. In fact, two-level atoms have been used for decades as the main tool for testing fundamentals of quantum mechanics 共see Ref ...
Measurability of Wilson loop operators
Measurability of Wilson loop operators

11th International Conference on Squeezed - icssur 2009
11th International Conference on Squeezed - icssur 2009

Ibrahim Aljubayri`s presentation on Secure Network Channel among
Ibrahim Aljubayri`s presentation on Secure Network Channel among

Optimum phase-shift estimation and the quantum description of the
Optimum phase-shift estimation and the quantum description of the

Good  Families  of  Quantum Low-Density
Good Families of Quantum Low-Density

A Bell Theorem Without Inequalities for Two
A Bell Theorem Without Inequalities for Two

Latched Detection of Excited States in an Isolated Double
Latched Detection of Excited States in an Isolated Double

Centre for Logic and Philosophy of Science
Centre for Logic and Philosophy of Science

85, 155302 (2012)
85, 155302 (2012)

Quantum and Classical Evolution of Chemical Reaction Wave Front
Quantum and Classical Evolution of Chemical Reaction Wave Front

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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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