1,427 research outputs found
Theory of valley-orbit coupling in a Si/SiGe quantum dot
Electron states are studied for quantum dots in a strained Si quantum well,
taking into account both valley and orbital physics. Realistic geometries are
considered, including circular and elliptical dot shapes, parallel and
perpendicular magnetic fields, and (most importantly for valley coupling) the
small local tilt of the quantum well interface away from the crystallographic
axes. In absence of a tilt, valley splitting occurs only between pairs of
states with the same orbital quantum numbers. However, tilting is ubiquitous in
conventional silicon heterostructures, leading to valley-orbit coupling. In
this context, "valley splitting" is no longer a well defined concept, and the
quantity of merit for qubit applications becomes the ground state gap. For
typical dots used as qubits, a rich energy spectrum emerges, as a function of
magnetic field, tilt angle, and orbital quantum number. Numerical and
analytical solutions are obtained for the ground state gap and for the mixing
fraction between the ground and excited states. This mixing can lead to valley
scattering, decoherence, and leakage for Si spin qubits.Comment: 18 pages, including 4 figure
Spin exchange in quantum rings and wires in the Wigner-crystal limit
We present a controlled method for computing the exchange coupling in
strongly correlated one-dimensional electron systems. It is based on the
asymptotically exact relation between the exchange constant and the
pair-correlation function of spinless electrons. Explicit results are obtained
for thin quantum rings with realistic Coulomb interactions, by calculating this
function via a many-body instanton approach.Comment: 7 pages, 2 figures. Changes in the text and figures to improve
readability; added reference
Electric field inside a "Rossky cavity" in uniformly polarized water
Electric field produced inside a solute by a uniformly polarized liquid is
strongly affected by dipolar polarization of the liquid at the interface. We
show, by numerical simulations, that the electric "cavity" field inside a
hydrated non-polar solute does not follow the predictions of standard Maxwell's
electrostatics of dielectrics. Instead, the field inside the solute tends, with
increasing solute size, to the limit predicted by the Lorentz virtual cavity.
The standard paradigm fails because of its reliance on the surface charge
density at the dielectric interface determined by the boundary conditions of
the Maxwell dielectric. The interface of a polar liquid instead carries a
preferential in-plane orientation of the surface dipoles thus producing
virtually no surface charge. The resulting boundary conditions for
electrostatic problems differ from the traditional recipes, affecting the
microscopic and macroscopic fields based on them. We show that relatively small
differences in cavity fields propagate into significant differences in the
dielectric constant of an ideal mixture. The slope of the dielectric increment
of the mixture versus the solute concentration depends strongly on which
polarization scenario at the interface is realized. A much steeper slope found
in the case of Lorentz polarization also implies a higher free energy penalty
for polarizing such mixtures.Comment: 9 pages, 8 figure
Cell death sensitization of leukemia cells by opioid receptor activation
Cyclic AMP (cAMP) regulates a number of cellular processes and modulates cell death induction. cAMP levels are altered upon stimulation of specific G-protein-coupled receptors inhibiting or activating adenylyl cyclases. Opioid receptor stimulation can activate inhibitory Gi-proteins which in turn block adenylyl cyclase activity reducing cAMP. Opioids such as D,L-methadone induce cell death in leukemia cells. However, the mechanism how opioids trigger apoptosis and activate caspases in leukemia cells is not understood. In this study, we demonstrate that downregulation of cAMP induced by opioid receptor activation using the opioid D,L-methadone kills and sensitizes leukemia cells for doxorubicin treatment. Enhancing cAMP levels by blocking opioid-receptor signaling strongly reduced D,L-methadone-induced apoptosis, caspase activation and doxorubicin-sensitivity. Induction of cell death in leukemia cells by activation of opioid receptors using the opioid D,L-methadone depends on critical levels of opioid receptor expression on the cell surface. Doxorubicin increased opioid receptor expression in leukemia cells. In addition, the opioid D,L-methadone increased doxorubicin uptake and decreased doxorubicin efflux in leukemia cells, suggesting that the opioid D,L-methadone as well as doxorubicin mutually increase their cytotoxic potential. Furthermore, we found that opioid receptor activation using D,L-methadone alone or in addition to doxorubicin inhibits tumor growth significantly in vivo. These results demonstrate that opioid receptor activation via triggering the downregulation of cAMP induces apoptosis, activates caspases and sensitizes leukemia cells for doxorubicin treatment. Hence, opioid receptor activation seems to be a promising strategy to improve anticancer therapies
Opioid receptor activation triggering downregulation of cAMP improves effectiveness of anti-cancer drugs in treatment of glioblastoma
Glioblastoma are the most frequent and malignant human brain tumors, having a very poor prognosis. The enhanced radio- and chemoresistance of glioblastoma and the glioblastoma stem cells might be the main reason why conventional therapies fail. The second messenger cyclic AMP (cAMP) controls cell proliferation, differentiation, and apoptosis. Downregulation of cAMP sensitizes tumor cells for anti-cancer treatment. Opioid receptor agonists triggering opioid receptors can activate inhibitory Gi proteins, which, in turn, block adenylyl cyclase activity reducing cAMP. In this study, we show that downregulation of cAMP by opioid receptor activation improves the effectiveness of anti-cancer drugs in treatment of glioblastoma. The Β΅-opioid receptor agonist D,L-methadone sensitizes glioblastoma as well as the untreatable glioblastoma stem cells for doxorubicin-induced apoptosis and activation of apoptosis pathways by reversing deficient caspase activation and deficient downregulation of XIAP and Bcl-xL, playing critical roles in glioblastomas' resistance. Blocking opioid receptors using the opioid receptor antagonist naloxone or increasing intracellular cAMP by 3-isobutyl-1-methylxanthine (IBMX) strongly reduced opioid receptor agonist-induced sensitization for doxorubicin. In addition, the opioid receptor agonist D,L-methadone increased doxorubicin uptake and decreased doxorubicin efflux, whereas doxorubicin increased opioid receptor expression in glioblastomas. Furthermore, opioid receptor activation using D,L-methadone inhibited tumor growth significantly in vivo. Our findings suggest that opioid receptor activation triggering downregulation of cAMP is a promising strategy to inhibit tumor growth and to improve the effectiveness of anti-cancer drugs in treatment of glioblastoma and in killing glioblastoma stem cells
Widespread deuteration across the IRDC G035.39-00.33
Β© 2016 The Authors. Infrared Dark Clouds (IRDCs) are cold, dense regions that are usually found within Giant Molecular Clouds. Ongoing star formation within IRDCs is typically still deeply embedded within the surrounding molecular gas. Characterizing the properties of relatively quiescent IRDCs may therefore help us to understand the earliest phases of the star formation process. Studies of local molecular clouds have revealed that deuterated species are enhanced in the earliest phases of star formation. In this paper, we test this towards IRDC G035.39-00.33. We present an 80 arcsec by 140 arcsec map of the J = 2 β 1 transition of N2D+, obtained with the Institut de Radioastronomie MillimΓ©trique 30 m telescope telescope. We find that N2D+ is widespread throughout G035.39-00.33. Complementary observations of N2H+ (1 - 0) are used to estimate the deuterium fraction, DN2H+ frac β‘ N(N2D+)/N(N2H+). We report a mean DN2H+ frac = 0.04 Β± 0.01, with a maximum of DN2H+ frac = 0.09 Β± 0.02. The mean deuterium fraction is ~3 orders of magnitude greater than the interstellar [D]/[H] ratio. High angular resolution observations are required to exclude beam dilution effects of compact deuterated cores. Using chemical modelling, we find that the average observed values of DN2H+ frac are in agreement with an equilibrium deuterium fraction, given the general properties of the cloud. This implies that the IRDC is at least ~3 Myr old, which is ~8 times longer than the mean free-fall time of the observed deuterated region
Evaluation of an Electrostatic Dust Removal System with Potential Application in Next-Step Fusion Devices
The ability to manage inventories of carbon, tritium, and high-Z elements in fusion plasmas depends on means for effective dust removal. A dust conveyor, based on a moving electrostatic potential well, was tested with particles of tungsten, carbon, glass and sand. A digital microscope imaged a representative portion of the conveyor, and dust particle size and volume distributions were derived before and after operation. About 10 cu mm volume of carbon and tungsten particles were moved in under 5 seconds. The highest driving amplitude tested of 3 kV was the most effective. The optimal driving frequency was 210 Hz (maximum tested) for tungsten particles, decreasing to below 60 Hz for the larger sand particles. Measurements of particle size and volume distributions after 10 and 100 cycles show the breaking apart of agglomerated carbon, and the change in particle distribution over short timescales 1 s)
Spectral Models for Early Time SN 2011fe Observations
We use observed UV through near IR spectra to examine whether SN 2011fe can
be understood in the framework of Branch-normal SNe Ia and to examine its
individual peculiarities. As a benchmark, we use a delayed-detonation model
with a progenitor metallicity of Z_solar/20. We study the sensitivity of
features to variations in progenitor metallicity, the outer density profile,
and the distribution of radioactive nickel. The effect of metallicity
variations in the progenitor have a relatively small effect on the synthetic
spectra. We also find that the abundance stratification of SN 2011fe resembles
closely that of a delayed detonation model with a transition density that has
been fit to other Branch-normal Type Ia supernovae. At early times, the model
photosphere is formed in material with velocities that are too high, indicating
that the photosphere recedes too slowly or that SN 2011fe has a lower specific
energy in the outer ~0.1 M_sun than does the model. We discuss several
explanations for the discrepancies. Finally, we examine variations in both the
spectral energy distribution and in the colors due to variations in the
progenitor metallicity, which suggests that colors are only weak indicators for
the progenitor metallicity, in the particular explosion model that we have
studied. We do find that the flux in the U band is significantly higher at
maximum light in the solar metallicity model than in the lower metallicity
model and the lower metallicity model much better matches the observed
spectrum.Comment: 9 pages, 14 figures, MNRAS, in press, fixed typ
Deuterium fractionation in cold dense cores in the low-mass star forming region L1688
In this work, we study deuterium fractionation in four starless cores in the
low-mass star-forming region L1688 in the Ophiuchus molecular cloud. We study
how the deuterium fraction () changes with environment, compare
deuteration of ions and neutrals, core centre and its envelope, and attempt to
reproduce the observed results with a gas-grain chemical model. We chose high
and low gas density tracers to study both core centre and the envelope. With
the IRAM 30m antenna, we mapped NH(1-0), ND(1-0),
HCO (1-0) and (2-1), DCO(2-1), and
-NHD(1-1) towards the chosen cores. The missing -NH
and NH(1-0) data were taken from the literature. To measure the
molecular hydrogen column density, dust and gas temperature within the cores,
we used the Herschel/SPIRE dust continuum emission data, the GAS survey data
(ammonia), and the COMPLETE survey data to estimate the upper limit on CO
depletion. We present the deuterium fraction maps for three species towards
four starless cores. Deuterium fraction of the core envelopes traced by
DCO/HCO is one order of magnitude lower (0.08) than that
of the core central parts traced by the nitrogen-bearing species (0.5).
Deuterium fraction increases with the gas density as indicated by high
deuterium fraction of high gas density tracers and low deuterium fraction of
lower gas density tracers and by the decrease of with core radii,
consistent with the predictions of the chemical model. Our model results show a
good agreement with observations for (ND/NH) and
R(DCO/HCO) and underestimate the (NHD/NH).Comment: 30 pages with 22 figures, accepted for publication in MNRA
ΠΠΎΠ½ΡΠΏΠ΅ΠΊΡ ΡΠΎΠ΄Π° Anopteris (Pteridophyta, Pteridaceae)
In the article a synopsis of the genus Anopteris (Prantl) Diels is given. The synopsis of Anopteris includes three species. For each species, the Latin name, basionym, nomenclatural citation, synonyms, information on locus classicus, type, habitat, and distribution are given. AnΒ original key for identification of the species of Anopteris is also prepared. The localities of occurrence of each species are precisely given.Β ΠΡΠΈΠ²Π΅Π΄Π΅Π½ ΠΊΠΎΠ½ΡΠΏΠ΅ΠΊΡ ΡΠΎΠ΄Π° Anopteris (Prantl) Diels. ΠΠΎΠ½ΡΠΏΠ΅ΠΊΡ Π²ΠΊΠ»ΡΡΠ°Π΅Ρ ΡΡΠΈ Π²ΠΈΠ΄Π°. ΠΠ»Ρ ΠΊΠ°ΠΆΠ΄ΠΎΠ³ΠΎ ΠΈΠ· Π½ΠΈΡ
ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡΡΡ Π»Π°ΡΠΈΠ½ΡΠΊΠΎΠ΅ Π½Π°Π·Π²Π°Π½ΠΈΠ΅, Π±Π°Π·ΠΈΠΎΠ½ΠΈΠΌ, Π½ΠΎΠΌΠ΅Π½ΠΊΠ»Π°ΡΡΡΠ½Π°Ρ ΡΠΈΡΠ°ΡΠ°, ΡΠΈΠ½ΠΎΠ½ΠΈΠΌΡ, ΠΎΡΠΊΡΠ΄Π° ΠΎΠΏΠΈΡΠ°Π½, ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΡ ΠΎ ΡΠΈΠΏΠ΅, Π΄Π°Π½Π½ΡΠ΅ ΠΎ ΠΌΠ΅ΡΡΠΎΠΎΠ±ΠΈΡΠ°Π½ΠΈΠΈ, ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½ΠΈΠ΅ ΠΏΠΎ ΡΡΡΠ°Π½Π°ΠΌ Ρ ΡΠΈΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ΅ΡΡ ΡΠ±ΠΎΡΠ° ΠΈ ΠΎΠ±ΡΠ΅Π΅ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½ΠΈΠ΅. ΠΠ»Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ Π²ΡΠ΅Ρ
Π²ΠΈΠ΄ΠΎΠ² ΡΠΎΠ΄Π° Anopteris ΡΠΎΡΡΠ°Π²Π»Π΅Π½ ΠΎΡΠΈΠ³ΠΈΠ½Π°Π»ΡΠ½ΡΠΉ ΠΊΠ»ΡΡ, ΡΠΊΠ°Π·Π°Π½Ρ ΠΏΠΎΠ΄ΡΠΎΠ±Π½ΡΠ΅ ΠΌΠ΅ΡΡΠ° ΠΏΡΠΎΠΈΠ·ΡΠ°ΡΡΠ°Π½ΠΈΡ.Β ΠΡΠΈΠ²Π΅Π΄Π΅Π½ ΠΊΠΎΠ½ΡΠΏΠ΅ΠΊΡ ΡΠΎΠ΄Π° Anopteris (Prantl) Diels. ΠΠΎΠ½ΡΠΏΠ΅ΠΊΡ Π²ΠΊΠ»ΡΡΠ°Π΅Ρ ΡΡΠΈ Π²ΠΈΠ΄Π°. ΠΠ»Ρ ΠΊΠ°ΠΆΠ΄ΠΎΠ³ΠΎ ΠΈΠ· Π½ΠΈΡ
ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡΡΡ Π»Π°ΡΠΈΠ½ΡΠΊΠΎΠ΅ Π½Π°Π·Π²Π°Π½ΠΈΠ΅, Π±Π°Π·ΠΈΠΎΠ½ΠΈΠΌ, Π½ΠΎΠΌΠ΅Π½ΠΊΠ»Π°ΡΡΡΠ½Π°Ρ ΡΠΈΡΠ°ΡΠ°, ΡΠΈΠ½ΠΎΠ½ΠΈΠΌΡ, ΠΎΡΠΊΡΠ΄Π° ΠΎΠΏΠΈΡΠ°Π½, ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΡ ΠΎ ΡΠΈΠΏΠ΅, Π΄Π°Π½Π½ΡΠ΅ ΠΎ ΠΌΠ΅ΡΡΠΎΠΎΠ±ΠΈΡΠ°Π½ΠΈΠΈ, ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½ΠΈΠ΅ ΠΏΠΎ ΡΡΡΠ°Π½Π°ΠΌ Ρ ΡΠΈΡΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ΅ΡΡ ΡΠ±ΠΎΡΠ° ΠΈ ΠΎΠ±ΡΠ΅Π΅ ΡΠ°ΡΠΏΡΠΎΡΡΡΠ°Π½Π΅Π½ΠΈΠ΅. ΠΠ»Ρ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ Π²ΡΠ΅Ρ
Π²ΠΈΠ΄ΠΎΠ² ΡΠΎΠ΄Π° Anopteris ΡΠΎΡΡΠ°Π²Π»Π΅Π½ ΠΎΡΠΈΠ³ΠΈΠ½Π°Π»ΡΠ½ΡΠΉ ΠΊΠ»ΡΡ, ΡΠΊΠ°Π·Π°Π½Ρ ΠΏΠΎΠ΄ΡΠΎΠ±Π½ΡΠ΅ ΠΌΠ΅ΡΡΠ° ΠΏΡΠΎΠΈΠ·ΡΠ°ΡΡΠ°Π½ΠΈΡ.
- β¦