5,899 research outputs found
Integrating all-optical switching with spintronics
All-optical switching (AOS) of magnetic materials describes the reversal of
the magnetization using short (femtosecond) laser pulses, and has been observed
in a variety of materials. In the past decade it received extensive attention
due to its high potential for fast and energy-efficient data writing in future
spintronic memory applications. Unfortunately, the AOS mechanism in the
ferromagnetic multilayers commonly used in spintronics needs multiple pulses
for the magnetization reversal, losing its speed and energy efficiency. Here,
we experimentally demonstrate `on-the-fly' single-pulse AOS in combination with
spin Hall effect (SHE) driven motion of magnetic domains in Pt/Co/Gd
synthetic-ferrimagnetic racetracks. Moreover, using field-driven-SHE-assisted
domain wall (DW) motion measurements, both the SHE efficiency in the racetrack
is determined and the chirality of the optically written DW's is verified. Our
experiments demonstrate that Pt/Co/Gd racetracks facilitate both single-pulse
AOS as well as efficient SHE induced domain wall motion, which might ultimately
pave the way towards integrated photonic memory devices
Absorption and generation of femtosecond laser-pulse excited spin currents in non-collinear magnetic bilayers
Spin currents can be generated on an ultrafast timescale by excitation of a
ferromagnetic (FM) thin film with a femtosecond laser-pulse. Recently, it has
been demonstrated that these ultrafast spin currents can transport angular
momentum to neighbouring FM layers, being able to change both the magnitude and
orientation of the magnetization in the adjacent layer. In this work, both the
generation and absorption of these optically excited spin currents are
investigated. This is done using non-collinear magnetic bilayers, i.e. two FM
layers separated by a conductive spacer. Spin currents are generated in a Co/Ni
multilayer with out-of-plane (OOP) anisotropy, and absorbed by a Co layer with
an in-plane (IP) anisotropy. This behaviour is confirmed by careful analysis of
the laser-pulse induced magnetization dynamics, whereafter it is demonstrated
that the transverse spin current is absorbed very locally near the injection
interface of the IP layer (90% within the first approx. 2 nm). Moreover, it
will also be shown that this local absorption results in the excitation of THz
standing spin waves within the IP layer. The dispersion measured for these high
frequency spin waves shows a discrepancy with respect to the theoretical
predictions, for which a first explanation involving intermixed interface
regions is proposed. Lastly, the spin current generation is investigated using
different number of repeats for the Co/Ni multilayer, which proves to be of
great relevance for identifying the optical spin current generation mechanism
Multi-Centered Invariants, Plethysm and Grassmannians
Motivated by multi-centered black hole solutions of Maxwell-Einstein theories
of (super)gravity in D=4 space-time dimensions, we develop some general
methods, that can be used to determine all homogeneous invariant polynomials on
the irreducible (SL_h(p,R) x G4)-representation (p,R), where p denotes the
number of centers, and SL_h(p,R) is the "horizontal" symmetry of the system,
acting upon the indices labelling the centers. The black hole electric and
magnetic charges sit in the symplectic representation R of the generalized
electric-magnetic (U-)duality group G4. We start with an algebraic approach
based on classical invariant theory, using Schur polynomials and the Cauchy
formula. Then, we perform a geometric analysis, involving Grassmannians,
Pluecker coordinates, and exploiting Bott's Theorem. We focus on non-degenerate
groups G4 "of type E7" relevant for (super)gravities whose (vector multiplets')
scalar manifold is a symmetric space. In the triality-symmetric stu model of
N=2 supergravity, we explicitly construct a basis for the 10 linearly
independent degree-12 invariant polynomials of 3-centered black holes.Comment: 1+29 pages, 6 Table
Delayed kinetics of poliovirus RNA synthesis in a human cell line with reduced levels of hnRNP C proteins.
The hnRNP C heterotetramer [(C1(3))C2] binds RNA polymerase II transcripts in the nucleus, along with other proteins of the core hnRNP complex, and plays an important role in mRNA biogenesis and transport. Infection of HeLa cells with poliovirus causes hnRNP C to re-localize from the nucleus, where it is normally retained during interphase, to the cytoplasm. We have proposed that in the cytoplasm, the protein isoforms of hnRNP C participate in the recognition of viral specific RNAs by the poliovirus replication proteins and/or in the assembly of membrane-bound RNA replication complexes. In SK-OV-3 cells, which express reduced levels of hnRNP C compared to HeLa cells or 293 cells, the kinetics of poliovirus replication are delayed. hnRNP C is also re-localized from the nucleus to the cytoplasm in SK-OV-3 cells infected with poliovirus. Increased expression of hnRNP C in SK-OV-3 cells by transient transfection increases the rate of virus production and overall yield over that seen in mock-transfected cells. We propose that hnRNP C interacts with poliovirus RNA and replication proteins to increase the efficiency of viral genomic RNA synthesis
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