Search results for "Exact solution"

showing 10 items of 77 documents

Three-body Coulomb interaction effects in the final state of thePb208(B8,Be7p)Pb208Coulomb breakup reaction

2005

The photodissociation reaction $^{8}\mathrm{B}+\ensuremath{\gamma}\ensuremath{\rightarrow}^{7}\mathrm{Be}+p$ is used to provide information on the astrophysical ${S}_{17}$ factor of the inverse radiative capture reaction, knowledge of which is crucial for an estimation of the high-energy neutrino flux from the sun. Since, at present, the Coulomb field of a fully stripped nucleus serves as the source of the photons, an adequate analysis requires a genuine three-body treatment of this reaction. Among the uncertainties still affecting present analyses, the possible modification of the dissociation cross section by the post-decay acceleration of the fragments $^{7}\mathrm{Be}$ and p in the targ…

PhysicsNuclear and High Energy PhysicsDipoleExact solutions in general relativityScatteringQuantum mechanicsCoulombInverseAtomic physicsMultipole expansionWave functionCharged particlePhysical Review C
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Three-Body Coulomb Final-State Interaction Effects in the Coulomb Breakup of Light Nuclei

2005

Coulomb breakup of a projectile in the Coulomb field of a fully stripped heavy nucleus is at present one of the most popular experimental methods to obtain information on reactions of interest in nuclear astrophysics. Its theoretical interpretation presents, however, considerable difficulties, due to the three-body nature and the infinite range of the Coulomb forces involved. Among the uncertainties affecting present analyses, the possible modification of the dissociation cross section by three-body Coulomb final-state interactions plays a major role. Various methods which have been proposed to deal with it are briefly reviewed. However, none of them is based on a consistent and mathematica…

PhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsProjectileGeneral Physics and AstronomyFOS: Physical sciencesAstronomy and AstrophysicsBreakup01 natural sciences3. Good healthNuclear Theory (nucl-th)Wave–particle dualityAmplitudeExact solutions in general relativityClassical mechanics0103 physical sciencesNuclear astrophysicsCoulomb010306 general physicsQuantum
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Tensor Network Annealing Algorithm for Two-Dimensional Thermal States

2019

Tensor network methods have become a powerful class of tools to capture strongly correlated matter, but methods to capture the experimentally ubiquitous family of models at finite temperature beyond one spatial dimension are largely lacking. We introduce a tensor network algorithm able to simulate thermal states of two-dimensional quantum lattice systems in the thermodynamic limit. The method develops instances of projected entangled pair states and projected entangled pair operators for this purpose. It is the key feature of this algorithm to resemble the cooling down of the system from an infinite temperature state until it reaches the desired finite-temperature regime. As a benchmark we …

PhysicsOptical latticeQuantum PhysicsStrongly Correlated Electrons (cond-mat.str-el)General Physics and AstronomyQuantum simulatortensor network methodsFOS: Physical sciences01 natural sciencesSquare latticequantum statistical mechanicsCondensed Matter - Strongly Correlated ElectronsExact solutions in general relativityquantum information0103 physical sciencesThermodynamic limit539strongly correlated systemsIsing modelQuantum information010306 general physicsQuantum statistical mechanicsQuantum Physics (quant-ph)Algorithmquantum simulationPhysical Review Letters
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Exact solutions for the mutual inductance of circular coils and elliptic coils

2012

An exact solution is presented for the mutual inductance between general noncoaxial thin circular and elliptic coils with parallel axes. The thin coil solution is given as an angular integral of an elliptic integral expression. In addition, for the coaxial case, an exact solution is given for the mutual inductance of a thick circular coil and a thick elliptic coil. The elliptic coil is such that the coil thickness is the same along both elliptic semi-axes. The thick coil solution is given as an integral of an expression involving Bessel and Struve functions. Extensive numerical results for sample geometries are given for both solutions, which are cross checked against each other in the limi…

PhysicsQuantitative Biology::BiomoleculesPhysics::Medical PhysicsMathematical analysisElectronic Optical and Magnetic MaterialsMagnetic fieldInductancesymbols.namesakeExact solutions in general relativityElectromagnetic coilStruve functionsymbolsElliptic integralElectrical and Electronic EngineeringCoaxialBessel functionIEEE Transactions on Magnetics
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Collision-model-based approach to non-Markovian quantum dynamics

2013

We present a theoretical framework to tackle quantum non-Markovian dynamics based on a microscopic collision model (CM), where the bath consists of a large collection of initially uncorrelated ancillas. Unlike standard memoryless CMs, we endow the bath with memory by introducing inter-ancillary collisions between next system-ancilla interactions. Our model interpolates between a fully Markovian dynamics and the continuous interaction of the system with a single ancilla, i.e., a strongly non-Markovian process. We show that in the continuos limit one can derive a general master equation, which while keeping such features is guaranteed to describe an unconditionally completely positive and tra…

PhysicsQuantum PhysicsQuantum decoherenceQuantum dynamicsMarkov processFOS: Physical sciencesAtomic and Molecular Physics and Opticssymbols.namesakeExact solutions in general relativityClassical mechanicsSPINNon-Markovian open quantum systems collision modelsMaster equationDissipative systemsymbolsStatistical physicsQuantum informationQuantum Physics (quant-ph)Quantum
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An Exact Riemann Solver for Multidimensional Special Relativistic Hydrodynamics

2001

We have generalised the exact solution of the Riemann problem in special relativistic hydrodynamics (Marti and Muller, 1994) for arbitrary tangential flow velocities. The solution is obtained by solving the jump conditions across shocks plus an ordinary differential equation arising from the self-similarity condition along rarefaction waves, in a similar way as in purely normal flow. This solution has been used to build up an exact Riemann solver implemented in a multidimensional relativistic (Godunov-type) hydro-code.

PhysicsRoe solverShock wavesymbols.namesakeRiemann problemExact solutions in general relativityOrdinary differential equationMathematical analysissymbolsJumpAstrophysicsRiemann's differential equationRiemann solver
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The exact solution of the Riemann problem with non-zero tangential velocities in relativistic hydrodynamics

2000

We have generalised the exact solution of the Riemann problem in special relativistic hydrodynamics for arbitrary tangential flow velocities. The solution is obtained by solving the jump conditions across shocks plus an ordinary differential equation arising from the self-similarity condition along rarefaction waves, in a similar way as in purely normal flow. The dependence of the solution on the tangential velocities is analysed, and the impact of this result on the development of multidimensional relativistic hydrodynamic codes (of Godunov type) is discussed.

PhysicsShock waveDifferential equationMechanical EngineeringMathematical analysisAstrophysics (astro-ph)Zero (complex analysis)Fluid Dynamics (physics.flu-dyn)FOS: Physical sciencesPhysics - Fluid DynamicsCondensed Matter PhysicsAstrophysicssymbols.namesakeExact solutions in general relativityRiemann problemFlow velocityMechanics of MaterialsOrdinary differential equationsymbolsJump
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Stopping a slow-light soliton: an exact solution

2005

We investigate propagation of a slow-light soliton in Λ-type media such as atomic vapours and Bose–Einstein condensates. We show that the group velocity of the soliton monotonically decreases with the intensity of the controlling laser field, which decays exponentially after the laser is switched off. The shock wave of the vanishing controlling field overtakes the slow soliton and stops it, while the optical information is recorded in the medium in the form of spatially localized polarization. In the strongly nonlinear regime we find an explicit exact solution describing the whole process.

PhysicsShock waveGeneral Physics and AstronomyStatistical and Nonlinear PhysicsPolarization (waves)Slow lightlaw.inventionDissipative solitonExact solutions in general relativitylawQuantum mechanicsQuantum electrodynamicsGroup velocitySolitonMathematical PhysicsBose–Einstein condensateJournal of Physics A: Mathematical and General
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XXZ-like phase in the F-AF anisotropic Heisenberg chain

2008

By means of the Density Matrix Renormalization Group technique, we have studied the region where $XXZ$-like behavior is most likely to emerge within the phase diagram of the F-AF anisotropic extended ($J-J'$) Heisenberg chain. We have analyzed, in great detail, the equal-time two-spin correlation functions, both in- and out-of- plane, as functions of the distance (and momentum). Then, we have extracted, through an accurate fitting procedure, the exponents of the asymptotic power-law decay of the spatial correlations. We have used the exact solution of $XXZ$ model ($J'=0$) to benchmark our results, which clearly show the expected agreement. A critical value of $J'$ has been found where the r…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Plane (geometry)Density matrix renormalization groupFOS: Physical sciencesCondensed Matter PhysicsCritical valueElectronic Optical and Magnetic MaterialsMomentumCondensed Matter - Strongly Correlated ElectronsExact solutions in general relativityExponentAnisotropyMathematical physicsPhase diagram
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Exact solution of the 1D Hubbard model with NN and NNN interactions in the narrow-band limit

2013

We present the exact solution, obtained by means of the Transfer Matrix (TM) method, of the 1D Hubbard model with nearest-neighbor (NN) and next-nearest-neighbor (NNN) Coulomb interactions in the atomic limit (t=0). The competition among the interactions ($U$, $V_1$, and $V_2$) generates a plethora of T=0 phases in the whole range of fillings. $U$, $V_1$, and $V_2$ are the intensities of the local, NN and NNN interactions, respectively. We report the T=0 phase diagram, in which the phases are classified according to the behavior of the principal correlation functions, and reconstruct a representative electronic configuration for each phase. In order to do that, we make an analytic limit $T\…

PhysicsStrongly Correlated Electrons (cond-mat.str-el)Statistical Mechanics (cond-mat.stat-mech)Hubbard modelFOS: Physical sciencesCondensed Matter PhysicsTransfer matrixElectronic Optical and Magnetic MaterialsCondensed Matter - Strongly Correlated ElectronsExact solutions in general relativityQuantum mechanicsCoulombLimit (mathematics)Electron configurationGround stateCondensed Matter - Statistical MechanicsPhase diagramThe European Physical Journal B
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