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Section 7.5 Quantum Mechanics and the Atom
Section 7.5 Quantum Mechanics and the Atom

... Atomic Spectroscopy and the Bohr Model The Bohr Model • So basically what we need is a new kind of physics to explain the behavior of the atom. • This process had already begun with the breaking down of the barrier between light as a wave and matter as a particle. • Einstein showed that light behave ...
Brief history of the atom
Brief history of the atom

Embracing the quantum limit in silicon computing
Embracing the quantum limit in silicon computing

Affine computation and affine automaton
Affine computation and affine automaton

Effective Quantum Spin Systems with Trapped Ions
Effective Quantum Spin Systems with Trapped Ions

arXiv:1504.04012v1 [cond-mat.quant
arXiv:1504.04012v1 [cond-mat.quant

Part 3: Lattice: Quantum to Ising to RG
Part 3: Lattice: Quantum to Ising to RG

Quantum digital spiral imaging
Quantum digital spiral imaging

... We employ the experimental set-up shown in Figure 2 to demonstrate the non-local decomposition of non-integer phase vortices. A collimated 355-nm beam pumps a 5-mm long b-barium borate (BBO) crystal, where a degenerate 710 nm signal and idler photons are produced in pairs via type-I collinear SPDC a ...
Paper
Paper

... quantum system cannot be said to exist if they have not being measured. Whether a given property of a given physical system in a given state may be asserted, denied, or regarded as meaningless, depends on the measuring context; the observer determines the physical facts being observed. An entire “ph ...
Chapter 3 Foundations II: Measurement and Evolution 3.1
Chapter 3 Foundations II: Measurement and Evolution 3.1

... We would like to examine the properties of the generalized measurements that can be realized on system A by performing orthogonal measurements on a larger system that contains A. But first we will briefly consider how (orthogonal) measurements of an arbitrary observable can be achieved in principle, ...
Nature physics
Nature physics

... with a fixed particle number per site (see Fig. 6b). Therefore, the system cannot be described by a giant coherent matter wave, and for very strong interactions, no interference pattern can be observed upon releasing the particles from the lattice. Instead, perfect correlations in the particle numbe ...
Many Worlds? An Introduction - General Guide To Personal and
Many Worlds? An Introduction - General Guide To Personal and

... microscopic system itself, but our knowledge of it, or the information we have available of it (perhaps ‘ideal’ or ‘maximal’ knowledge or information). No wonder modelling the apparatus in the wavefunction is no solution: that only shifts the problem further back, ultimately to ‘the observer’ and to ...
Transition form factor of the hydrogen Rydberg atom
Transition form factor of the hydrogen Rydberg atom

field concepts and the emergence of a holistic
field concepts and the emergence of a holistic

E4. Free Fall
E4. Free Fall

How Quantum Theory Helps us Explain
How Quantum Theory Helps us Explain

... Notice the key role representation plays here: feature Y of the model corresponds to X by representing it. Hughes even calls his accompanying version of the so-called semantic conception of scientific theories the representational account. A Newtonian model aids understanding by allowing us to think ...
Section 7.5 Quantum Mechanics and the Atom
Section 7.5 Quantum Mechanics and the Atom

... Atomic Spectroscopy and the Bohr Model The Bohr Model • So basically what we need is a new kind of physics to explain the behavior of the atom. • This process had already begun with the breaking down of the barrier between light as a wave and matter as a particle. • Einstein showed that light behave ...
Revista Mexicana de Física . Darboux-deformed barriers
Revista Mexicana de Física . Darboux-deformed barriers

... functions) and are associated with poles of the S-matrix in the 4th quadrant of the complex ²-plane [7, 8]. The fact that ΨG diverges at large distances is usually stressed to motivate the study of the rigged Hilbert space [9], the mathematical structure of which lies on the spectral theorem of Dira ...
Information Theory and Machine Learning
Information Theory and Machine Learning

arXiv:1302.5365v1 [quant-ph] 21 Feb 2013
arXiv:1302.5365v1 [quant-ph] 21 Feb 2013

Print this article
Print this article

... opposite states (for example, 1 and 0) would accomplish calculations that would be impossible to achieve by processing information through digital bits, which rest on the need to choose 1 over 0, or vice versa. Computer scientists theorize that the superior performance of a quantum computer over a c ...
Tailoring Optical Nonlinearities via the Purcell Effect
Tailoring Optical Nonlinearities via the Purcell Effect

... temperatures [22]. Equation (8) implies that substantial enhancement of the Kerr coefficient occurs in that regime. At a temperature of about 200 K, nr 0:1rad [22]. Although experimental measurements for phase are unavailable to the authors, the presence of a substantial phonon bath at that tem ...
Energy-time entanglement, elements of reality, and local realism Linköping University Post Print
Energy-time entanglement, elements of reality, and local realism Linköping University Post Print

Initial Conditions from Inflation
Initial Conditions from Inflation

Multi-party Quantum Computation Adam Smith
Multi-party Quantum Computation Adam Smith

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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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