ENTANGLED SYSTEMS AUDRETSCH FILETYPE PDF

Entangled Systems: New Directions In Quantum Physics. Quantum Physics Who Already Know The Fundamentals, Audretsch’s “Entangled . File Type: PDF . as every virtual system must be booted up. It is suggested that If two quantum particles are “entangled”, what happens to one instantly affects the other, even if . creation could be simply when the system was booted up. . travels faster than light but one entangled quantum entity instantly affects the other anywhere.

Author: Tura Neshakar
Country: Latvia
Language: English (Spanish)
Genre: Finance
Published (Last): 17 March 2006
Pages: 252
PDF File Size: 12.1 Mb
ePub File Size: 5.34 Mb
ISBN: 591-9-52949-237-8
Downloads: 89296
Price: Free* [*Free Regsitration Required]
Uploader: Tojin

However, the qubits in the two models have different decoherence The parameters are the same as in Fig. The decoherence and relaxation of the qubit in SIB model Using the numerical path integral method we investigate the decoherence and relaxation of qubits in spin-boson SB and spin-intermediate harmonic oscillator IHO -bath SIB models.

The cases that the environment baths with low and medium frequencies are investigated.

Entangled Systems: New Directions in Quantum Physics | Physics & Astronomy | Subjects | Wiley

It is shown that the qubits in SB and SIB models have the same decoherence and relaxation as the baths with low frequencies. However, the qubits in the two models have different decoherence and relaxation as the baths with medium frequencies. Here, we suppose the oscillation frequencies of the Using the numerical path filethpe method we investigate the decoherence and relaxation of qubits coupled to an Ohmic bath directly and via an intermediate harmonic oscillator IHO.

When we choose suitable parameters the qubits in the two models may have almost same decoherence and relaxation times. However, the decoherence and relaxation times of the qubit in the qubit -IHO-bath model can be modulated through changing the coupling coefficients of the qubit -IHO and IHO-bath and the oscillation frequency of the IHO.

The net magnetic flux threading An additional magnetic flux threading A part of the flux -qubit larger loop is projected A part of the flux- qubit larger loop is projected In this paper a macroscopic quantum oscillator is proposed, which consists of a flux- qubit in the form of a cantilever.

The net magnetic flux threading through the flux- qubit sstems the mechanical degrees of freedom of the cantilever are naturally coupled. The coupling between the cantilever and the magnetic flux is controlled through an fileype magnetic field.

The ground state of the flux- qubit -cantilever turns out to be an entangled quantum state, where the cantilever deflection and the magnetic flux are the entangled degrees of freedom. A variant, which is a special case of the flux- qubit -cantilever without a Josephson junction, is audretscu discussed. Starting in the ground state We show that for a qubit coupled to one oscillatorLandau—Zener LZ sweep of a qubit coupled to two oscillators. A qubit may undergo Landau—Zener transitions due to its coupling to one sysyems several quantum harmonic oscillators.

  INTRODUCING SOCIOLINGUISTICS MESTHRIE PDF

Entangled Systems: New Directions in Quantum Physics – Free eBooks Download

We show that for a qubit coupled to one oscillatorLandau—Zener transitions can be used for single-photon generation and for the controllable creation of qubit — oscillator entanglement, with state-of-the-art circuit QED as a promising realization. Moreover, for a qubit coupled to two cavities, we show that Landau—Zener sweeps of the qubit are well suited for the audretscj creation of entangled cavity states, in particular symmetric Bell states, with the qubit filerype as the entanglement mediator.

At the heart of our proposals lies the calculation of the exact Landau—Zener transition probability for the qubitby summing all orders of the corresponding series in time-dependent perturbation theory.

This transition probability emerges to be independent of the oscillator frequenciesboth inside and outside the regime where a rotating-wave approximation is valid. We propose a method for characterising the energy level structure of a solid state qubit by monitoring the noise level in its environment. We consider a model persistent current qubit in a lossy reservoir and demonstrate that the noise in a classical bias field is a sensitive function of the applied field.

In both cases, the experimental data Black bars denote Cooper pair boxes. Each qubit is based on a Cooper pair box connected to a reservoir In both cases, the experimental data open We have analyzed and measured the quantum coherent dynamics of a circuit containing two-coupled superconducting charge qubits.

Each qubit is based on a Cooper pair box connected to a reservoir electrode through a Josephson junction. Two qubits are coupled electrostatically by a small island overlapping both Cooper pair boxes.

Quantum state manipulation of the qubit circuit is done by applying non-adiabatic voltage pulses to the common audretach.

We read out each qubit by means of probe electrodes connected to Cooper pair boxes through high-Ohmic tunnel junctions. With such a setup, the measured pulse-induced probe currents are proportional to the probability for each qubit to have an extra Cooper pair after the manipulation.

As expected from theory and observed experimentally, the measured pulse-induced current in each probe has two frequency components whose position on the frequency axis can be externally controlled. Our simulations flietype that in the absence of decoherence and with a rectangular pulse shape, the system remains entangled most of the time reaching maximally entangled states at certain instances. We discuss an experimental proposal on quantum feedback control of a double-dot qubitwhich seems to be within audretcsh reach of the present-day technology.

  EDDA IN PROSA ITALIANO PDF

Similar to the earlier proposal, the feedback loop is used to maintain the coherent oscillations in the qubit for an arbitrary long dystems however, this is done in a significantly simpler way. The main idea is to use the quadrature components of the noisy detector current to monitor approximately the phase of qubit oscillations.

The correlated oscillation is shown Fipetype couple the Rabi oscillation in a double quantum dot DQD with the quantum tunneling in filetpe DQD by Coulomb interaction between the neighboring dots. The correlated oscillation is shown clearly in the tunneling current. And then, a single optical signal fiiletype a gang control of two electrons.

This result encourages superior design of two- qubit quantum gates based on correlated DQDs. The accumulation of information The scheme is based We present a new scheme to detect and visualize oscillations of a single quantum system in real time. The scheme is based upon a sequence of very weak generalized measurements, distinguished by their low disturbance and low information gain. Accumulating the information from the single measurements by means of an appropriate Bayesian estimator, the actual oscillations can be monitored nevertheless with high accuracy and low disturbance.

For this purpose only the minimum and the maximum expected oscillation frequency need to be known.

The accumulation of information is based on a general derivation of the optimal estimator of the expectation value of a Hermitian audretsdh for a sequence of measurements. At any time it takes into account all the preceding measurement results. It is almost zero in the time interval The frequency of the beats Quantum computing requires a set of universal quantum gates.

Entangled Systems: New Directions in Quantum Physics

It flips the state of the target qubit conditioned on the state of entangldd control qubit. We investigated the possibility of implementing a CNOT logic gate using magnetically coupled impurity spins of diamond, namely systeme electron spin-1 carried by the nitrogen-vacancy color center and the electron spin carried by a nearby nitrogen atom in substitutional position P1 center.

It is shown that a 96ns gate time with a high-fidelity can be realized by means of pulsed electron spin resonance spectroscopy. Filters Reset Filter Results. Klee, Thomas Konrad Date: Image 5 Tabular Data.