683 research outputs found
Shot Noise of Spin-Decohering Transport in Spin-Orbit Coupled Nanostructures
We generalize the scattering theory of quantum shot noise to include the full
spin-density matrix of electrons injected from a spin-filtering or
ferromagnetic electrode into a quantum-coherent nanostructure governed by
various spin-dependent interactions. This formalism yields the spin-resolved
shot noise power for different experimental measurement setups--with
ferromagnetic source and ferromagnetic or normal drain electrodes--whose
evaluation for the diffusive multichannel quantum wires with the Rashba (SO)
spin-orbit coupling shows how spin decoherence and dephasing lead to
substantial enhancement of charge current fluctuations (characterized by Fano
factors ). However, these processes and the corresponding shot noise
increase are suppressed in narrow wires, so that charge transport experiments
measuring the Fano factor in a
ferromagnet/SO-coupled-wire/paramagnet setup also quantify the degree of
phase-coherence of transported spin--we predict a one-to-one correspondence
between the magnitude of the spin polarization vector and .Comment: 8 pages, 3 figure; enhanced with 2 new figure
Charge qubits and limitations of electrostatic quantum gates
We investigate the characteristics of purely electrostatic interactions with
external gates in constructing full single qubit manipulations. The quantum bit
is naturally encoded in the spatial wave function of the electron system.
Single-electron{transistor arrays based on quantum dots or insulating
interfaces typically allow for electrostatic controls where the inter-island
tunneling is considered constant, e.g. determined by the thickness of an
insulating layer. A representative array of 3x3 quantum dots with two mobile
electrons is analyzed using a Hubbard Hamiltonian and a capacitance matrix
formalism. Our study shows that it is easy to realize the first quantum gate
for single qubit operations, but that a second quantum gate only comes at the
cost of compromising the low-energy two-level system needed to encode the
qubit. We use perturbative arguments and the Feshbach formalism to show that
the compromising of the two-level system is a rather general feature for
electrostatically interacting qubits and is not just related to the specific
details of the system chosen. We show further that full implementation requires
tunable tunneling or external magnetic fields.Comment: 7 pages, 5 figures, submitted to PR
Photon-mediated qubit interactions in one-dimensional discrete and continuous models
In this work we study numerically and analytically the interaction of two qubits in a one-dimensionalwaveguide, as mediated by the photons that propagate through the guide. We develop strategies to assert the Markovianity of the problem, the effective qubit-qubit interactions, and their individual and collective spontaneous emission. We prove the existence of collective Lamb shifts that affect the qubit-qubit interactions and the dependency of coherent and incoherent interactions on the qubit separation. We also develop the scattering theory associated with these models and prove single-photon spectroscopy does probe the renormalized resonances of the singleand multiqubit models, in sharp contrast to earlier toy models in which individual and collective Lamb shifts cancel
Decoherence by a spin thermal bath: Role of the spin-spin interactions and initial state of the bath
We study the decoherence of two coupled spins that interact with a spin-bath
environment. It is shown that the connectivity and the coupling strength
between the spins in the environment are of crucial importance for the
decoherence of the central system. For the anisotropic spin-bath, changing the
connectivity or coupling strenghts changes the decoherence of the central
system from Gaussian to exponential decay law. The initial state of the
environment is shown to affect the decoherence process in a qualitatively
significant manner.Comment: submitted to PR
Photons uncertainty solves Einstein-Podolsky-Rosen paradox
Einstein, Podolsky and Rosen (EPR) pointed out that the quantum-mechanical
description of "physical reality" implied an unphysical, instantaneous action
between distant measurements. To avoid such an action at a distance, EPR
concluded that Quantum Mechanics had to be incomplete. However, its extensions
involving additional "hidden variables", allowing for the recovery of
determinism and locality, have been disproved experimentally (Bell's theorem).
Here, I present an opposite solution of the paradox based on the greater
indeterminism of the modern Quantum Field Theory (QFT) description of Particle
Physics, that prevents the preparation of any state having a definite number of
particles. The resulting uncertainty in photons radiation has interesting
consequences in Quantum Information Theory (e.g. cryptography and
teleportation). Moreover, since it allows for less elements of EPR physical
reality than the old non-relativistic Quantum Mechanics, QFT satisfies the EPR
condition of completeness without the need of hidden variables. The residual
physical reality does never violate locality, thus the unique objective proof
of "quantum nonlocality" is removed in an interpretation-independent way. On
the other hand, the supposed nonlocality of the EPR correlations turns out to
be a problem of the interpretation of the theory. If we do not rely on hidden
variables or new physics beyond QFT, the unique viable interpretation is a
minimal statistical one, that preserves locality and Lorentz symmetry.Comment: Published version, with updated referenc
Non-adiabatic effects in long-pulse mixed-field orientation of a linear polar molecule
We present a theoretical study of the impact of an electrostatic field
combined with non-resonant linearly polarized laser pulses on the rotational
dynamics of linear molecules. Within the rigid rotor approximation, we solve
the time-dependent Schr\"odinger equation for several field configurations.
Using the OCS molecule as prototype, the field-dressed dynamics is analyzed in
detail for experimentally accessible static field strengths and laser pulses.
Results for directional cosines are presented and compared to the predictions
of the adiabatic theory. We demonstrate that for prototypical field
configuration used in current mixed-field orientation experiments, the
molecular field dynamics is, in general, non-adiabatic, being mandatory a
time-dependent description of these systems. We investigate several field
regimes identifying the sources of non-adiabatic effects, and provide the field
parameters under which the adiabatic dynamics would be achieved.Comment: 16 pages, 16 figures. Submitted to Physical Review
Rabi lattice models with discrete gauge symmetry: Phase diagram and implementation in trapped-ion quantum simulators
We study a spin-boson chain that exhibits a local Z2 symmetry. We investigate the quantum phase diagram of the model by means of perturbation theory, mean-field theory, and the density matrix renormalization group method. Our calculations show the existence of a first-order phase transition in the region where the boson quantum dynamics is slow compared to the spin-spin interactions. Our model can be implemented with trapped-ion quantum simulators, leading to a realization of minimal models showing local gauge invariance and first-order phase transitions
Classical and Quantum Fluctuation Theorems for Heat Exchange
The statistics of heat exchange between two classical or quantum finite
systems initially prepared at different temperatures are shown to obey a
fluctuation theorem.Comment: 4 pages, 1 included figure, to appear in Phys Rev Let
Optical Aharonov-Bohm Effect on Wigner Molecules in Type-II Semiconductor Quantum Dots
We theoretically examine the magnetoluminescence from a trion and a biexciton
in a type-II semiconductor quantum dot, in which holes are confined inside the
quantum dot and electrons are in a ring-shaped region surrounding the quantum
dot. First, we show that two electrons in the trion and biexciton are strongly
correlated to each other, forming a Wigner molecule: Since the relative motion
of electrons is frozen, they behave as a composite particle whose mass and
charge are twice those of a single electron. As a result, the energy of the
trion and biexciton oscillates as a function of magnetic field with half the
period of the single-electron Aharonov-Bohm oscillation. Next, we evaluate the
photoluminescence. Both the peak position and peak height change
discontinuously at the transition of the many-body ground state, implying a
possible observation of the Wigner molecule by the optical experiment.Comment: 10 pages, 10 figures, accepted for publication in Phys. Rev.
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