1,479 research outputs found
All-optical control of ferromagnetic thin films and nanostructures
The interplay of light and magnetism has been a topic of interest since the
original observations of Faraday and Kerr where magnetic materials affect the
light polarization. While these effects have historically been exploited to use
light as a probe of magnetic materials there is increasing research on using
polarized light to alter or manipulate magnetism. For instance deterministic
magnetic switching without any applied magnetic fields using laser pulses of
the circular polarized light has been observed for specific ferrimagnetic
materials. Here we demonstrate, for the first time, optical control of
ferromagnetic materials ranging from magnetic thin films to multilayers and
even granular films being explored for ultra-high-density magnetic recording.
Our finding shows that optical control of magnetic materials is a much more
general phenomenon than previously assumed. These results challenge the current
theoretical understanding and will have a major impact on data memory and
storage industries via the integration of optical control of ferromagnetic
bits.Comment: 21 pages, 11 figure
Fast spin exchange between two distant quantum dots
The Heisenberg exchange interaction between neighboring quantum dots allows
precise voltage control over spin dynamics, due to the ability to precisely
control the overlap of orbital wavefunctions by gate electrodes. This allows
the study of fundamental electronic phenomena and finds applications in quantum
information processing. Although spin-based quantum circuits based on
short-range exchange interactions are possible, the development of scalable,
longer-range coupling schemes constitutes a critical challenge within the
spin-qubit community. Approaches based on capacitative coupling and
cavity-mediated interactions effectively couple spin qubits to the charge
degree of freedom, making them susceptible to electrically-induced decoherence.
The alternative is to extend the range of the Heisenberg exchange interaction
by means of a quantum mediator. Here, we show that a multielectron quantum dot
with 50-100 electrons serves as an excellent mediator, preserving speed and
coherence of the resulting spin-spin coupling while providing several
functionalities that are of practical importance. These include speed (mediated
two-qubit rates up to several gigahertz), distance (of order of a micrometer),
voltage control, possibility of sweet spot operation (reducing susceptibility
to charge noise), and reversal of the interaction sign (useful for dynamical
decoupling from noise).Comment: 6 pages including 4 figures, plus 8 supplementary pages including 5
supplementary figure
Strain dependence of bonding and hybridization across the metal-insulator transition of VO2
Soft x-ray spectroscopy is used to investigate the strain dependence of the
metal-insulator transition of VO2. Changes in the strength of the V 3d - O 2p
hybridization are observed across the transition, and are linked to the
structural distortion. Furthermore, although the V-V dimerization is
well-described by dynamical mean-field theory, the V-O hybridization is found
to have an unexpectedly strong dependence on strain that is not predicted by
band theory, emphasizing the relevance of the O ion to the physics of VO2
Study of deuterium plasma interaction with a tungsten target within RPI-IBIS facility
The paper presents results of experimental research on the interaction of a pulsed plasma-ion stream with a tungsten (W) target. The pulsed deuterium plasma was produced within the RPI-IBIS (Multi-Rod Plasma Injector) facility at IPJ in Swierk. Measurements were carried out by means of optical spectroscopy and corpuscular diagnostic techniques. Structural changes in the irradiated targets were investigated with a SEM. Before experiments with the W-target there were determined operational conditions, when clean deuterium plasma streams can be generated. For that purpose a so-called βslow or PID (Plasma Ion Deposition) modeβ of the RPI-IBIS operation was chosen. Particular attention was paid to the identification of spectral lines from WI and WII species. The obtained results, i.e. optical spectra and other characteristics have demonstrated applicability of the RPI-IBIS facility for research on the interaction of plasma streams with W-targets, e.g. those constituting some internal parts of fusion facilities.ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½ΠΎ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΈ Π΅ΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΠΈΡ
Π΄ΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½Ρ ΠΏΠΎ Π²Π·Π°ΡΠΌΠΎΠ΄ΡΡ ΡΠΌΠΏΡΠ»ΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠ»Π°Π·ΠΌΠΎΠ²ΠΎ-ΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΠΎΡΠΎΠΊΡ Π· Π²ΠΎΠ»ΡΡΡΠ°ΠΌΠΎΠ²ΠΎΡ ΠΌΡΡΠ΅Π½Π½Ρ. ΠΠΌΠΏΡΠ»ΡΡΠ½Ρ Π΄Π΅ΠΉΡΠ΅ΡΡΡΠ²Ρ ΠΏΠΎΡΠΎΠΊΠΈ ΠΏΠ»Π°Π·ΠΌΠΈ Π³Π΅Π½Π΅ΡΡΠ²Π°Π»ΠΈΡΡ Π² Π‘ΠΠ-ΠΠΠΠ‘ (ΡΡΠ΅ΡΠΆΠ½Π΅Π²ΠΈΠΉ ΠΏΠ»Π°Π·ΠΌΠΎΠ²ΠΈΠΉ ΡΠ½ΠΆΠ΅ΠΊΡΠΎΡ), ΡΠΊΠΈΠΉ Π·Π½Π°Ρ
ΠΎΠ΄ΠΈΡΡΡΡ Π² ΠΠ―Π Ρ Π¨Π²Π΅ΡΠΊΡ. ΠΠΈΠΌΡΡΠΈ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈΡΡ Π·Π° Π΄ΠΎΠΏΠΎΠΌΠΎΠ³ΠΎΡ ΠΎΠΏΡΠΈΡΠ½ΠΎΡ ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΡΡ ΡΠ° ΠΊΠΎΡΠΏΡΡΠΊΡΠ»ΡΡΠ½ΠΎΡ Π΄ΡΠ°Π³Π½ΠΎΡΡΠΈΠΊΠΈ. Π‘ΡΡΡΠΊΡΡΡΠ½Ρ Π·ΠΌΡΠ½ΠΈ ΠΎΠ±Π»ΡΡΠ°ΡΠΌΠΎΡ ΠΌΡΡΠ΅Π½Ρ Π΄ΠΎΡΠ»ΡΠ΄ΠΆΡΠ²Π°Π»ΠΈΡΡ Π·Π° Π΄ΠΎΠΏΠΎΠΌΠΎΠ³ΠΎΡ SEM. ΠΠ΅ΡΠ΅Π΄ Π΅ΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°ΠΌΠΈ Π· Π²ΠΎΠ»ΡΡΡΠ°ΠΌΠΎΠ²ΠΎΡ ΠΌΡΡΠ΅Π½Π½Ρ Π²ΠΈΠ·Π½Π°ΡΠ°Π»ΠΈΡΡ ΡΠΎΠ±ΠΎΡΡ ΡΠΌΠΎΠ²ΠΈ, ΠΊΠΎΠ»ΠΈ Π³Π΅Π½Π΅ΡΡΠ²Π°Π»ΠΈΡΡ ΡΠΈΡΡΡ Π΄Π΅ΠΉΡΠ΅ΡΡΡΠ²Ρ ΠΏΠ»Π°Π·ΠΌΠΎΠ²Ρ ΠΏΠΎΡΠΎΠΊΠΈ. ΠΡΠ² Π²ΠΈΠ±ΡΠ°Π½ΠΈΠΉ ΡΠ°ΠΊ Π·Π²Π°Π½ΠΈΠΉ ΡΠ΅ΠΆΠΈΠΌ βΠΏΠΎΠ²ΡΠ»ΡΠ½ΠΈΠΉ Π°Π±ΠΎ PID-ΠΌΠΎΠ΄ΠΈβ (ΠΏΠ»Π°Π·ΠΌΠΎΠ²ΠΎΠ³ΠΎ ΡΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΎΡΠ°Π΄ΠΆΠ΅Π½Π½Ρ). Π§Π°ΡΡΠΈΡΠ½Π° ΡΠ²Π°Π³Π° ΠΏΡΠΈΠ΄ΡΠ»ΡΠ»Π°ΡΡ ΡΠ΄Π΅Π½ΡΠΈΡΡΠΊΠ°ΡΡΡ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΠΈΡ
Π»ΡΠ½ΡΠΉ WI ΡΠ° WII. ΠΡΡΠΈΠΌΠ°Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠΈ, ΠΎΠΏΡΠΈΡΠ½Ρ ΡΠΏΠ΅ΠΊΡΡΠΈ ΡΠ° ΡΠ½ΡΡ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ, ΠΏΡΠΎΠ΄Π΅ΠΌΠΎΠ½ΡΡΡΡΠ²Π°Π»ΠΈ ΠΌΠΎΠΆΠ»ΠΈΠ²ΡΡΡΡ Π·Π°ΡΡΠΎΡΠΎΠ²ΡΠ²Π°ΡΠΈ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΡ Π‘ΠΠ-ΠΠΠΠ‘ Π΄Π»Ρ Π΄ΠΎΡΠ»ΡΠ΄ΠΆΠ΅Π½Ρ Π²Π·Π°ΡΠΌΠΎΠ΄ΡΡ ΠΏΠ»Π°Π·ΠΌΠΎΠ²ΠΈΡ
ΠΏΠΎΡΠΎΠΊΡΠ² Π· W-ΠΌΡΡΠ΅Π½Π½Ρ, ΡΠΊΡ ΡΠΊΠ»Π°Π΄Π°ΡΡΡ Π΄Π΅ΡΠΊΡ Π²Π½ΡΡΡΡΡΠ½Ρ ΡΠ°ΡΡΠΈΠ½ΠΈ ΡΠ΅ΡΠΌΠΎΡΠ΄Π΅ΡΠ½ΠΎΠ³ΠΎ ΡΠ΅Π°ΠΊΡΠΎΡΡ.ΠΡΠ΅Π΄ΡΡΠ°Π²Π»Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΡ
ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ ΠΏΠΎ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΠΎΠ³ΠΎ ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΠΎ-ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΏΠΎΡΠΎΠΊΠ° Ρ Π²ΠΎΠ»ΡΡΡΠ°ΠΌΠΎΠ²ΠΎΠΉ ΠΌΠΈΡΠ΅Π½ΡΡ. ΠΠΌΠΏΡΠ»ΡΡΠ½ΡΠ΅ Π΄Π΅ΠΉΡΠ΅ΡΠΈΠ΅Π²ΡΠ΅ ΠΏΠΎΡΠΎΠΊΠΈ ΠΏΠ»Π°Π·ΠΌΡ Π³Π΅Π½Π΅ΡΠΈΡΠΎΠ²Π°Π»ΠΈΡΡ Π²Π½ΡΡΡΠΈ Π‘ΠΠ-ΠΠΠΠ‘ (ΡΡΠ΅ΡΠΆΠ½Π΅Π²ΠΎΠΉ ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΡΠΉ ΠΈΠ½ΠΆΠ΅ΠΊΡΠΎΡ), ΠΊΠΎΡΠΎΡΡΠΉ ΡΠ°ΡΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ Π² ΠΠ―Π Π² Π¨Π²Π΅ΡΠΊΠ΅. ΠΠ·ΠΌΠ΅ΡΠ΅Π½ΠΈΡ ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈΡΡ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΏΠ΅ΠΊΡΡΠΎΡΠΊΠΎΠΏΠΈΠΈ ΠΈ ΠΊΠΎΡΠΏΡΡΠΊΡΠ»ΡΡΠ½ΠΎΠΉ Π΄ΠΈΠ°Π³Π½ΠΎΡΡΠΈΠΊΠΈ. Π‘ΡΡΡΠΊΡΡΡΠ½ΡΠ΅ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΎΠ±Π»ΡΡΠ°Π΅ΠΌΠΎΠΉ ΠΌΠΈΡΠ΅Π½ΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π»ΠΈΡΡ Ρ ΠΏΠΎΠΌΠΎΡΡΡ SEM. ΠΠ΅ΡΠ΅Π΄ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°ΠΌΠΈ Ρ Π²ΠΎΠ»ΡΡΡΠ°ΠΌΠΎΠ²ΠΎΠΉ ΠΌΠΈΡΠ΅Π½ΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ»ΠΈΡΡ ΡΠ°Π±ΠΎΡΠΈΠ΅ ΡΡΠ»ΠΎΠ²ΠΈΡ, ΠΊΠΎΠ³Π΄Π° Π³Π΅Π½Π΅ΡΠΈΡΠΎΠ²Π°Π»ΠΈΡΡ ΡΠΈΡΡΡΠ΅ Π΄Π΅ΠΉΡΠ΅ΡΠΈΠ΅Π²ΡΠ΅ ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΡΠ΅ ΠΏΠΎΡΠΎΠΊΠΈ. ΠΠ»Ρ ΡΡΠΎΠΉ ΡΠ΅Π»ΠΈ Π±ΡΠ» Π²ΡΠ±ΡΠ°Π½ ΡΠ°ΠΊ Π½Π°Π·ΡΠ²Π°Π΅ΠΌΡΠΉ ΡΠ΅ΠΆΠΈΠΌ βΠΌΠ΅Π΄Π»Π΅Π½Π½ΠΎΠΉ ΠΈΠ»ΠΈ PID-ΠΌΠΎΠ΄Ρβ (ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ ΠΎΡΠ°ΠΆΠ΄Π΅Π½ΠΈΡ). Π§Π°ΡΡΠΈΡΠ½ΠΎΠ΅ Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ ΡΠ΄Π΅Π»ΡΠ»ΠΎΡΡ ΠΈΠ΄Π΅Π½ΡΠΈΡΠΈΠΊΠ°ΡΠΈΠΈ ΡΠΏΠ΅ΠΊΡΡΠ°Π»ΡΠ½ΡΡ
Π»ΠΈΠ½ΠΈΠΉ WI ΠΈ WII. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ, ΠΎΠΏΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΡΠΏΠ΅ΠΊΡΡΡ ΠΈ Π΄ΡΡΠ³ΠΈΠ΅ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ, ΠΏΡΠΎΠ΄Π΅ΠΌΠΎΠ½ΡΡΡΠΈΡΠΎΠ²Π°Π»ΠΈ ΠΏΡΠΈΠΌΠ΅Π½ΠΈΠΌΠΎΡΡΡ ΡΡΡΠ°Π½ΠΎΠ²ΠΊΠΈ Π‘ΠΠ-ΠΠΠΠ‘ Π΄Π»Ρ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠΉ Π²Π·Π°ΠΈΠΌΠΎΠ΄Π΅ΠΉΡΡΠ²ΠΈΡ ΠΏΠ»Π°Π·ΠΌΠ΅Π½Π½ΡΡ
ΠΏΠΎΡΠΎΠΊΠΎΠ² Ρ W-ΠΌΠΈΡΠ΅Π½ΡΡ, ΠΊΠΎΡΠΎΡΡΠ΅ ΡΠΎΡΡΠ°Π²Π»ΡΡΡ Π½Π΅ΠΊΠΎΡΠΎΡΡΠ΅ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΠ΅ ΡΠ°ΡΡΠΈ ΡΠ΅ΡΠΌΠΎΡΠ΄Π΅ΡΠ½ΠΎΠ³ΠΎ ΡΠ΅Π°ΠΊΡΠΎΡΠ°
Unifying the Phase Diagrams of the Magnetic and Transport Properties of La_(2-x)Sr_xCuO_4, 0 < x < 0.05
An extensive experimental and theoretical effort has led to a largely
complete mapping of the magnetic phase diagram of La_(2-x)Sr_xCuO_4, and a
microscopic model of the spin textures produced in the x < 0.05 regime has been
shown to be in agreement with this phase diagram. Here we use this same model
to derive a theory of the impurity-dominated, low temperature transport. Then,
we present an analysis of previously published data for two samples: x = 0.002
data from Chen et. al., and x = 0.04 data from Keimer et. al. We show that the
transport mechanisms in the two systems are the same, even though they are on
opposite sides of the observed insulator-to-metal transition. Our model of
impurity effects on the impurity band conduction, variable-range hopping
conduction, and coulomb gap conduction, is similar to that used to describe
doped semiconductors. However, for La_(2-x)Sr_xCuO_4 we find that in addition
to impurity-generated disorder effects, strong correlations are important and
must be treated on a equal level with disorder. On the basis of this work we
propose a phase diagram that is consistent with available magnetic and
transport experiments, and which connects the undoped parent compound with the
lowest x value for which La_(2-x)Sr_xCuO_4 is found to be superconducting, x
about 0.06.Comment: 7 pages revtex with one .ps figur
Time-domain characterization and correction of on-chip distortion of control pulses in a quantum processor
We introduce Cryoscope, a method for sampling on-chip baseband pulses used to
dynamically control qubit frequency in a quantum processor. We specifically use
Cryoscope to measure the step response of the dedicated flux control lines of
two-junction transmon qubits in circuit QED processors with the temporal
resolution of the room-temperature arbitrary waveform generator producing the
control pulses. As a first application, we iteratively improve this step
response using optimized real-time digital filters to counter the
linear-dynamical distortion in the control line, as needed for high-fidelity,
repeatable one- and two-qubit gates based on dynamical control of qubit
frequency
Entropy of vortex cores on the border of the superconductor-to-insulator transition in an underdoped cuprate
We present a study of Nernst effect in underdoped in
magnetic fields as high as 28T. At high fields, a sizeable Nernst signal was
found to persist in presence of a field-induced non-metallic resistivity. By
simultaneously measuring resistivity and the Nernst coefficient, we extract the
entropy of vortex cores in the vicinity of this field-induced
superconductor-insulator transition. Moreover, the temperature dependence of
the thermo-electric Hall angle provides strong constraints on the possible
origins of the finite Nernst signal above , as recently discovered by Xu
et al.Comment: 5 Pages inculding 4 figure
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