17,331 research outputs found
Translation termination depends on the sequential ribosomal entry of eRF1 and eRF3.
Translation termination requires eRF1 and eRF3 for polypeptide-and tRNA-release on stop codons. Additionally, Dbp5/DDX19 and Rli1/ABCE1 are required; however, their function in this process is currently unknown. Using a combination of in vivo and in vitro experiments, we show that they regulate a stepwise assembly of the termination complex. Rli1 and eRF3-GDP associate with the ribosome first. Subsequently, Dbp5-ATP delivers eRF1 to the stop codon and in this way prevents a premature access of eRF3. Dbp5 dissociates upon placing eRF1 through ATP-hydrolysis. This in turn enables eRF1 to contact eRF3, as the binding of Dbp5 and eRF3 to eRF1 is mutually exclusive. Defects in the Dbp5-guided eRF1 delivery lead to premature contact and premature dissociation of eRF1 and eRF3 from the ribosome and to subsequent stop codon readthrough. Thus, the stepwise Dbp5-controlled termination complex assembly is essential for regular translation termination events. Our data furthermore suggest a possible role of Dbp5/DDX19 in alternative translation termination events, such as during stress response or in developmental processes, which classifies the helicase as a potential drug target for nonsense suppression therapy to treat cancer and neurodegenerative diseases
Evolutional Entanglement in Nonequilibrium Processes
Entanglement in nonequilibrium systems is considered. A general definition
for entanglement measure is introduced, which can be applied for characterizing
the level of entanglement produced by arbitrary operators. Applying this
definition to reduced density matrices makes it possible to measure the
entanglement in nonequilibrium as well as in equilibrium statistical systems.
An example of a multimode Bose-Einstein condensate is discussed.Comment: 10 pages, Late
Enhanced spin accumulation at room temperature in graphene spin valves with amorphous carbon interfacial layers
We demonstrate a large enhancement of the spin accumulation in monolayer
graphene following electron-beam induced deposition of an amorphous carbon
layer at the ferromagnet-graphene interface. The enhancement is 10^4-fold when
graphene is deposited onto poly(methyl metacrylate) (PMMA) and exposed with
sufficient electron-beam dose to cross-link the PMMA, and 10^3-fold when
graphene is deposited directly onto SiO2 and exposed with identical dose. We
attribute the difference to a more efficient carbon deposition in the former
case due to an increase in the presence of compounds containing carbon, which
are released by the PMMA. The amorphous carbon interface can sustain very large
current densities without degrading, which leads to very large spin
accumulations exceeding 500 microeVs at room temperature
All-order evaluation of weak measurements: --- The cases of an operator which satisfies the property ---
Some exact formulae of the expectation values and probability densities in a
weak measurement for an operator which satisfies the property are derived. These formulae include all-order effects of the unitary
evolution due to the von-Neumann interaction. These are valid not only in the
weak measurement regime but also in the strong measurement regime and tell us
the connection between these two regime. Using these formulae, arguments of the
optimization of the signal amplification and the signal to noise ratio are
developed in two typical experimental setups.Comment: 17 pages, 10 figures (v1); Fig.3 and some typos are corrected (v2);
Comments and references are added and some typos are corrected (v3
Energy Loss from Reconnection with a Vortex Mesh
Experiments in superfluid 4He show that at low temperatures, energy
dissipation from moving vortices is many orders of magnitude larger than
expected from mutual friction. Here we investigate other mechanisms for energy
loss by a computational study of a vortex that moves through and reconnects
with a mesh of small vortices pinned to the container wall. We find that such
reconnections enhance energy loss from the moving vortex by a factor of up to
100 beyond that with no mesh. The enhancement occurs through two different
mechanisms, both involving the Kelvin oscillations generated along the vortex
by the reconnections. At relatively high temperatures the Kelvin waves increase
the vortex motion, leading to more energy loss through mutual friction. As the
temperature decreases, the vortex oscillations generate additional reconnection
events between the moving vortex and the wall, which decrease the energy of the
moving vortex by transfering portions of its length to the pinned mesh on the
wall.Comment: 9 pages, 10 figure
Probing of the Kondo peak by the impurity charge measurement
We consider the real-time dynamics of the Kondo system after the local probe
of the charge state of the magnetic impurity. Using the exactly solvable
infinite-degeneracy Anderson model we find explicitly the evolution of the
impurity charge after the measurement.Comment: 4 pages, 1 eps figure, revte
Electric dipole response of 208Pb from proton inelastic scattering: constraints on neutron skin thickness and symmetry energy
The electric dipole (E1) response of 208Pb has been precisely determined by
measuring Coulomb excitation induced by proton scattering at very forward
angles. The electric dipole polarizability, defined as inverse energy-weighted
sum rule of the E1 strength, has been extracted as 20.1+-0.6 fm^3. The data can
be used to constrain the neutron skin thickness of 208Pb to
0.168(+-0.009)_expt(+-0.013)_theo(+-0.021)_est fm, where the subscript "expt"
refers to the experimental uncertainty, "theor" to the theoretical confidence
band and "est" to the uncertainty associated with the estimation of the
symmetry energy at the saturation density. In addition, a constraint band has
been extracted in the plane of the symmetry energy (J) and its slope parameter
(L) at the saturation density.Comment: 6 pages, 8 figures, revised manuscript submitted to special volume of
Eur. Phys. J. A on symmetry energ
Direct measurement of general quantum states using weak measurement
Recent work [J.S. Lundeen et al. Nature, 474, 188 (2011)] directly measured
the wavefunction by weakly measuring a variable followed by a normal (i.e.
`strong') measurement of the complementary variable. We generalize this method
to mixed states by considering the weak measurement of various products of
these observables, thereby providing the density matrix an operational
definition in terms of a procedure for its direct measurement. The method only
requires measurements in two bases and can be performed `in situ', determining
the quantum state without destroying it.Comment: This is a later and very different version of arXiv:1110.0727v3
[quant-ph]. New content: a method to directly measure each element of the
density matrix, specific Hamiltonians to weakly measure the product of
non-commuting observables, and references to recent related wor
Statistical mechanics of scale-free networks at a critical point: Complexity without irreversibility?
Based on a rigorous extension of classical statistical mechanics to networks,
we study a specific microscopic network Hamiltonian. The form of this
Hamiltonian is derived from the assumption that individual nodes
increase/decrease their utility by linking to nodes with a higher/lower degree
than their own. We interpret utility as an equivalent to energy in physical
systems and discuss the temperature dependence of the emerging networks. We
observe the existence of a critical temperature where total energy
(utility) and network-architecture undergo radical changes. Along this
topological transition we obtain scale-free networks with complex hierarchical
topology. In contrast to models for scale-free networks introduced so far, the
scale-free nature emerges within equilibrium, with a clearly defined
microcanonical ensemble and the principle of detailed balance strictly
fulfilled. This provides clear evidence that 'complex' networks may arise
without irreversibility. The results presented here should find a wide variety
of applications in socio-economic statistical systems.Comment: 4 pages, 5 figure
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