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Improved quantum information motion control (Vol. 43 No. 5)

Sketch map of the double quantum dot (two horizontal lines) coupled with the nanomechanical resonator (rectangle).

A new model simulates closer control over the transport of information carrying electrons under specific external vibration conditions. The present article developes a new method for handling the effect of the interplay between vibrations and electrons on electronic transport, which could have implications for quantum computers due to improvements in the transport of discrete amounts of information, known as qubits, encoded in electrons.

The authors create an electron transport model to assess electrons’ current fluctuations based on a double quantum dot (DQD) subjected to quantized modes of vibration, also known as phonons, induced by a nanomechanical resonator. Unlike previous studies, this work imposes arbitrary strong coupling regimes between electrons and phonons.

They successfully control the excitations of the phonons without impacting the transport of quantum information. They decouple the electron-phonon interaction by inducing resonance frequency of phonons. When the energy excess between the two quantum dots of the DQD system is sufficient to create an integer number of phonons, electrons can reach resonance and tunnel from one quantum dot to the other.

As electron-phonon coupling becomes even stronger, the phenomenon of phonon scattering represses electron transport and confines them, suggesting that tuning the electron-phonon coupling, could make a good quantum switch to control the transport of information in quantum computers.

C. Wang, J. Ren, B. Li and Q-H. Chen, ‘Quantum transport of double quantum dots coupled to an oscillator in arbitrary strong coupling regime’, Eur. Phys. J. B (2012) 85, 110
[Abstract]

High intensity 6He beam production (Vol. 43 No. 5)

ISOLDE production unit equipped with a spallation neutron source along the target oven. Fast release of 6He anti-neutrino emitters, produced by a BeO target with the CERN’s proton beam.

Nuclear structures of short-lived radioisotopes are nowadays investigated in large scale facilities based on in-flight fragmentation or isotope separation online (ISOL) methods. The ISOL technique has been constantly extended at CERN-ISOLDE, where 1.4GeV protons are exploited by physicists to create radioisotopes in thick materials; these exotic nuclei are released and pumped online into an ion source, producing a secondary beam which is further selected in a magnetic mass spectrometer before post-acceleration.

Ten years ago a proposal to inject suitable ISOL beams into the CERN accelerator complex and to store these isotopes in a decay ring with straight sections was proposed for a ”Β-beam facility”; intense sources of pure electron neutrinos - emitted when such isotopes decay - are directed towards massive underground detectors for fundamental studies such as observation of neutrino flavour oscillations and CP violation.

Our paper reports on the experimental production of the anti-neutrino emitter 6He. We use a two-step reaction in which the proton beam interacts with a tungsten neutron spallation source. The emitted neutrons intercept a BeO target to produce 9Be(n,a)6He reactions. The neutron field was simulated by Monte-Carlo codes such as Fluka and experimentally measured. The large predicted 6He production rates were also experimentally verified. Fast 6He diffusion, driven by the selection of a suitable BeO material, could be demonstrated, leading to the highest 6He beam rates ever achieved at ISOLDE. These results provide a firm experimental confirmation that the Β-beam will be able to deliver enough anti-neutrino rates using a neutron spallation source similar to ISIS-RAL (UK). This work is now being completed by the experimental validation of the 18Ne neutrino source design.

T. Stora and 11 co-authors, ‘A high intensity 6He beam for the β-beam neutrino oscillation Facility’, EPL (2012) 98, 32001
[Abstract]

Translocation of polymers through lipid bilayers (Vol. 43 No. 5)

Snapshots of a polymer chain diffusing through the bilayer at the critical hydrophobicity. Strong perturbations of the lipid ordering can be observed during the adsorption/translocation event (middle).

Lipid bilayers emerge by self-organization of amphiphilic molecules and are the essential component of membranes of living cells. An important task of them is the selective exchange of substances between the cell and its environment. This becomes particularly interesting for delivering foreign molecules and RNA into the cell. In the classical view of cell biology static structures such as pores and channels formed by specific proteins control the translocation of molecules.

In this work we show that there exists a straightforward mechanism for translocation of polymers through lipid bilayers if the monomers of the chain show a certain balance of hydrophobic and hydrophilic strength. Using the bond fluctuation method with explicit solvent to simulate the self-organized lipid bilayer and the polymer chain we show that the chain is adsorbed by the bilayer at a critical hydrophobicity of the monomers. At this point all monomers have an intermediate degree of hydrophobicity, which is large enough to overcome the insertion barrier of the ordered lipids, but still small enough to avoid trapping in the core of the bilayer. In a narrow range around this critical hydrophobicity the chain can almost freely penetrate through the model membrane whose hydrophobic core becomes energetically transparent here. Our simulations also allow calculate the permeability of the membrane with respect to the solvent. We show that the permeability is strongly increased close to the critical hydrophobicity suggesting that here the perturbation of the membrane patch around the adsorbed chain is highest.

J-U. Sommer, M. Werner and V. A. Baulin, ‘Critical adsorption controls translocation of polymer chains through lipid bilayers and permeation of solvent’, EPL, (2012) 98, 18003
[Abstract]

The “inertia of heat” concept revisited (Vol. 43 No. 5)

What is the general relativistic version of the Navier-Stokes-Fourier dissipative hydrodynamics? Surprisingly, no satisfactory answer to this question is known today. Eckart's early solution [Eckart, Phys. Rev. (1940) 58, 919], is considered outdated on many grounds: the instability of its equilibrium states, ill-posed initial-value formulation, inconsistency with linear irreversible thermodynamics, etc. Although alternative theories have been proposed recently, none appears to have won the consensus.

This paper reconsiders the foundations of Eckart's theory, focusing on its main peculiarity and simultaneous difficulty: the “inertia of heat” term in the constitutive relation for the heat flux, which couples temperature to acceleration. In particular, it shows that this term arises only if one insists on defining the thermal diffusivity independently of the gravitational field. It is argued that this is not a physically sensible approach, because gravitational time dilation implies that the diffusivity actually varies in space. In a nutshell, where time runs faster, thermal diffusion also runs faster. It is proposed that this is the physical meaning of the “inertia of heat” concept, and that such an effect should be expected in any theory of dissipative hydrodynamics that is consistent with general relativity.

M. Smerlak, ‘On the inertia of heat’, Eur. Phys. J. Plus (2012) 127, 72
[Abstract]