Mathematical Physics of BlackBody Radiation
... equations of Calculus, crowned by Maxwell’s equations for electromagnetics formulated in 1865 by the British physicist Clerk Maxwell. The collapse resulted from a couple of scientific paradoxes, which appeared unsolvable using classical physics, both connected to light as electromagnetic waves descr ...
... equations of Calculus, crowned by Maxwell’s equations for electromagnetics formulated in 1865 by the British physicist Clerk Maxwell. The collapse resulted from a couple of scientific paradoxes, which appeared unsolvable using classical physics, both connected to light as electromagnetic waves descr ...
Atomic Hong–Ou–Mandel experiment - HAL-IOGS
... A pair of entangled particles is described by a state vector that cannot be factored as a product of two state vectors associated with each particle. Although entanglement does not require that the two particles be identical2 , it arises naturally in systems of indistinguishable particles due to th ...
... A pair of entangled particles is described by a state vector that cannot be factored as a product of two state vectors associated with each particle. Although entanglement does not require that the two particles be identical2 , it arises naturally in systems of indistinguishable particles due to th ...
QUANTUM ESTIMATION FOR QUANTUM TECHNOLOGY 1
... transformations, e.g. bilinear coupling.13 Local QET has been applied to the estimation of quantum phase14 and to estimation problems with open quantum systems and non unitary processes15 : to finite dimensional systems,16 to optimally estimate the noise parameter of depolarizing17 or amplitude-damp ...
... transformations, e.g. bilinear coupling.13 Local QET has been applied to the estimation of quantum phase14 and to estimation problems with open quantum systems and non unitary processes15 : to finite dimensional systems,16 to optimally estimate the noise parameter of depolarizing17 or amplitude-damp ...
Crystallization of strongly interacting photons in a nonlinear optical fiber
... The 2kF oscillations are a direct manifestation of ‘fermionization’ of bosons. The Friedel oscillations represent more than simple antibunching in that they indicate real crystal correlations. In particular, we cannot predict the position of an individual photon, but, knowing the position of one, ot ...
... The 2kF oscillations are a direct manifestation of ‘fermionization’ of bosons. The Friedel oscillations represent more than simple antibunching in that they indicate real crystal correlations. In particular, we cannot predict the position of an individual photon, but, knowing the position of one, ot ...
here.
... 1901 Blackbody radiation: Planck’s and Einstein’s quantum hypothesis (interpreted by Einstein as a packet of light) 1905 Einstein’s explanation of photoelectric effect via photon 1911 Rutherford discovery of heavy small positively charged nucleus via α(He 42 ) scattering 1913 Bohr model of the atom ...
... 1901 Blackbody radiation: Planck’s and Einstein’s quantum hypothesis (interpreted by Einstein as a packet of light) 1905 Einstein’s explanation of photoelectric effect via photon 1911 Rutherford discovery of heavy small positively charged nucleus via α(He 42 ) scattering 1913 Bohr model of the atom ...
The Spectrum of the Hydrogen Atom
... • Paul Dirac did a lot of work in quantum mechanics and relativity, and proposed an equation of motion for an electron, taking into consideration relativistic effects. • Albert Einstein did a lot of work in order to explain the photoelectric effect, but did not like the path the new quantum mechanic ...
... • Paul Dirac did a lot of work in quantum mechanics and relativity, and proposed an equation of motion for an electron, taking into consideration relativistic effects. • Albert Einstein did a lot of work in order to explain the photoelectric effect, but did not like the path the new quantum mechanic ...
High performance quantum computing
... ries information related to the quantum algorithm being run on the client side. As the photon stream transmitted to the client is the 3D topological lattice generated by the mainframe, interrogation of the quantum channel is unnecessary as the state transmitted is globally known. Additionally, the o ...
... ries information related to the quantum algorithm being run on the client side. As the photon stream transmitted to the client is the 3D topological lattice generated by the mainframe, interrogation of the quantum channel is unnecessary as the state transmitted is globally known. Additionally, the o ...
Lecture 6
... The next step involves Hadamard gate . First, we need to find out what Hadamard gate does to a qubit. The matrix for the Hadamard gate is ...
... The next step involves Hadamard gate . First, we need to find out what Hadamard gate does to a qubit. The matrix for the Hadamard gate is ...
Stochastic simulations of conditional states of partially observed
... into two separate environments, only one of which is accessible to our detectors. Such partially observed systems cannot be described by a stochastic Schrödinger equation (SSE) [6, 7, 8], but rather requires a more general form of a quantum trajectory that has been called a stochastic master equati ...
... into two separate environments, only one of which is accessible to our detectors. Such partially observed systems cannot be described by a stochastic Schrödinger equation (SSE) [6, 7, 8], but rather requires a more general form of a quantum trajectory that has been called a stochastic master equati ...
Quantum discord and remote state preparation
... is a resource for remote state preparation (RSP). The result was obtained considering a broad class of two-qubit states. For this family of states, it was proven that the RSP fidelity F is equal to the square of a geometric version of discord [16], providing an operational meaning for this quantity. ...
... is a resource for remote state preparation (RSP). The result was obtained considering a broad class of two-qubit states. For this family of states, it was proven that the RSP fidelity F is equal to the square of a geometric version of discord [16], providing an operational meaning for this quantity. ...
Advanced Quantum Mechanics - Pieter Kok
... choice for additional material. It has everything up to many-body quantum mechanics. 2. Quantum Information and Quantum Computation, by Nielsen and Chuang, Cambridge University Press (2000). This is the current standard work on quantum information theory. It has a comprehensive introduction to quant ...
... choice for additional material. It has everything up to many-body quantum mechanics. 2. Quantum Information and Quantum Computation, by Nielsen and Chuang, Cambridge University Press (2000). This is the current standard work on quantum information theory. It has a comprehensive introduction to quant ...
Universidad de Cantabria ON LIGHT SCATTERING BY NANOPARTICLES WITH CONVENTIONAL AND NON-CONVENTIONAL
... with an abrupt minimum (dark zone) in the backward direction. However, as the observer approaches the particle’s surface, the backward intensity becomes higher and even comparable to the one in the forward direction. This evolution is analyzed, in more detail, in Figure 5.4. In this figure, we plot ...
... with an abrupt minimum (dark zone) in the backward direction. However, as the observer approaches the particle’s surface, the backward intensity becomes higher and even comparable to the one in the forward direction. This evolution is analyzed, in more detail, in Figure 5.4. In this figure, we plot ...
1 simultaneous polarization squeezing of all three stokes
... relation but the individual fluctuations can be reduced and this gives the well known concept of squeezing. In classical optics the polarization state of light beam can be visualized as direction of a Stokes vector in Poincare sphere and is determined by the four Stokes parameters [1,2] S0 , S1 , S ...
... relation but the individual fluctuations can be reduced and this gives the well known concept of squeezing. In classical optics the polarization state of light beam can be visualized as direction of a Stokes vector in Poincare sphere and is determined by the four Stokes parameters [1,2] S0 , S1 , S ...
Paper
... condensates spread out with a very narrow momentum distribution when released from the atom trap @1,2#. The coherence properties of the Bose-Einstein condensate have been directly addressed only in very recent experiments @3,4#. It is the purpose of this Brief Report to discuss various aspects of co ...
... condensates spread out with a very narrow momentum distribution when released from the atom trap @1,2#. The coherence properties of the Bose-Einstein condensate have been directly addressed only in very recent experiments @3,4#. It is the purpose of this Brief Report to discuss various aspects of co ...
Opening up three quantum boxes causes classically undetectable
... superpose a physical ball under three separate boxes, real-space separation is not essential to the three-box argument. Alice and Bob can bet on any physical property of a system for which MR assigns mutually exclusive outcomes; for instance, a classical gyroscope revolving about one of three possi ...
... superpose a physical ball under three separate boxes, real-space separation is not essential to the three-box argument. Alice and Bob can bet on any physical property of a system for which MR assigns mutually exclusive outcomes; for instance, a classical gyroscope revolving about one of three possi ...
Bohr–Einstein debates
The Bohr–Einstein debates were a series of public disputes about quantum mechanics between Albert Einstein and Niels Bohr. Their debates are remembered because of their importance to the philosophy of science. An account of the debates was written by Bohr in an article titled ""Discussions with Einsteinon Epistemological Problems in Atomic Physics"". Despite their differences of opinion regarding quantum mechanics, Bohr and Einstein had a mutual admiration that was to last the rest of their lives.The debates represent one of the highest points of scientific research in the first half of the twentieth century because it called attention to an element of quantum theory, quantum non-locality, which is absolutely central to our modern understanding of the physical world. The consensus view of professional physicists has been that Bohr proved victorious, and definitively established the fundamental probabilistic character of quantum measurement.