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Synopsis
Polyanionic metal clusters are produced by electron attachment in both Paul and Penning traps. After size and charge-state selection, the cluster properties are further investigated by various methods including photo-dissociation. Depending on the particular cluster species various decay modes are observed.
The multifunctional sphingosine-1-phosphate (S1P) is a lipid signaling molecule and central
regulator in the development of several cancer types. In recent years, intriguing information has
become available regarding the role of S1P in the progression of Glioblastoma multiforme (GBM),
the most aggressive and common brain tumor in adults. S1P modulates numerous cellular processes
in GBM, such as oncogenesis, proliferation and survival, invasion, migration, metastasis and stem cell
behavior. These processes are regulated via a family of five G-protein-coupled S1P receptors (S1PR1-5)
and may involve mainly unknown intracellular targets. Distinct expression patterns and multiple
intracellular signaling pathways of each S1PR subtype enable S1P to exert its pleiotropic cellular
actions. Several studies have demonstrated alterations in S1P levels, the involvement of S1PRs
and S1P metabolizing enzymes in GBM pathophysiology. While the tumorigenic actions of S1P
involve the activation of several kinases and transcription factors, the specific G-protein (Gi, Gq,
and G12/13)-coupled signaling pathways and downstream mediated effects in GBM remain to be
elucidated in detail. This review summarizes the recent findings concerning the role of S1P and its
receptors in GBM. We further highlight the current insights into the signaling pathways considered
fundamental for regulating the cellular processes in GMB and ultimately patient prognosis.
Monitoring of Calcite Precipitation in Hardwater Lakes with Multi-Spectral Remote Sensing Archives
(2017)
Background: Recently, the expression of proteinase-activated receptor 2 (PAR2) has been
shown to be essential for activin receptor-like kinase 5 (ALK5)/SMAD-mediated signaling and cell
migration by transforming growth factor (TGF)-β1. However, it is not known whether activation
of non-SMAD TGF-β signaling (e.g., RAS–RAF–MEK–extracellular signal-regulated kinase (ERK)
signaling) is required for cell migration and whether it is also dependent on PAR2. Methods: RNA
interference was used to deplete cells of PAR2, followed by xCELLigence technology to measure
cell migration, phospho-immunoblotting to assess ERK1/2 activation, and co-immunoprecipitation
to detect a PAR2–ALK5 physical interaction. Results: Inhibition of ERK signaling with the MEK
inhibitor U0126 blunted the ability of TGF-β1 to induce migration in pancreatic cancer Panc1 cells.
ERK activation in response to PAR2 agonistic peptide (PAR2–AP) was strong and rapid, while it was
moderate and delayed in response to TGF-β1. Basal and TGF-β1-dependent ERK, but not SMAD
activation, was blocked by U0126 in Panc1 and other cell types indicating that ERK activation is
downstream or independent of SMAD signaling. Moreover, cellular depletion of PAR2 in HaCaT
cells strongly inhibited TGF-β1-induced ERK activation, while the biased PAR2 agonist GB88 at 10
and 100 µM potentiated TGF-β1-dependent ERK activation and cell migration. Finally, we provide
evidence for a physical interaction between PAR2 and ALK5. Our data show that both PAR2–APand TGF-β1-induced cell migration depend on ERK activation, that PAR2 expression is crucial for
TGF-β1-induced ERK activation, and that the functional cooperation of PAR2 and TGF-β1 involves a
physical interaction between PAR2 and ALK5
Abstract
Single self-stabilized discharge filaments were investigated in the plane-parallel electrode configuration. The barrier discharge was operated inside a gap of 3 mm shielded by glass plates to both electrodes, using helium-nitrogen mixtures and a square-wave feeding voltage at a frequency of 2 kHz. The combined application of electrical measurements, ICCD camera imaging, optical emission spectroscopy and surface charge diagnostics via the electro-optic Pockels effect allowed the correlation of the discharge development in the volume and on the dielectric surfaces. The formation criteria and existence regimes were found by systematic variation of the nitrogen admixture to helium, the total pressure and the feeding voltage amplitude. Single self-stabilized discharge filaments can be operated over a wide parameter range, foremost, by significant reduction of the voltage amplitude after the operation in the microdischarge regime. Here, the outstanding importance of the surface charge memory effect on the long-term stability was pointed out by the recalculated spatio-temporally resolved gap voltage. The optical emission revealed discharge characteristics that are partially reminiscent of both the glow-like barrier discharge and the microdischarge regime, such as a Townsend pre-phase, a fast cathode-directed ionization front during the breakdown and radially propagating surface discharges during the afterglow.
Surface charge measurements on different dielectrics in diffuse and filamentary barrier discharges
(2017)
Abstract
Previously, we reported on the measurement of surface charges during the operation of barrier discharges (BDs) using the electro-optic Pockels effect of a bismuth silicon oxide (BSO) crystal. With the present work, the next milestone is achieved by making this powerful method accessible to various dielectrics which are typically used in BD configurations. The dynamics and spatial distribution of positive and negative surface charges were determined on optically transparent borosilicate glass, mono-crystalline alumina and magnesia, respectively, covering the BSO crystal. By variation of the nitrogen admixture to helium and the pressure between 500 mbar and 1 bar, both the diffuse glow-like BD and the self-stabilized discharge filaments were operated inside of a gas gap of 3 mm. The characteristics of the discharge and, especially, the influence of the different dielectrics on its development were studied by surface charge diagnostics, electrical measurements and ICCD camera imaging. Regarding the glow-like BD, the breakdown voltage changes significantly by variation of the cathodic dielectric, due to the different effective secondary electron emission (SEE) coefficients. These material-specific SEE yields were estimated using Townsend’s criterion in combination with analytical calculations of the effective ionization coefficient in helium with air impurities. Moreover, the importance of the surface charge memory effect for the self-stabilization of discharge filaments was quantified by the recalculated spatio-temporal behavior of the gap voltage.
Abstract
The presented work highlights the role of residual weakly-bound surface electrons acting as an effective seed electron reservoir that favors the pre-ionization of diffuse barrier discharges (BDs). A glow-like BD was operated in helium at a pressure of 500 mbar in between two plane electrodes each covered with float glass at a distance of
3 mm.The change in discharge development due to laser photodesorption of surface electrons was studied by electrical measurements and optical emission spectroscopy. Moreover, a 1D numerical fluid model of the diffuse discharge allowed the simulation of the laser photodesorption experiment, the estimation of the released surface electrons, and the understanding of their impact on the reaction kinetics in the volume. The breakdown voltage is clearly reduced when the laser beam at photon energy of 2.33 eV hits the cathodic dielectric that is charged with residual electrons during the discharge pre-phase. According to the adapted simulation, the laser releases only a small amount of surface electrons in the order of
10 pC. Nevertheless, this significantly supports the pre-ionization. Using a lower photon energy of 1.17 eV, the transition from the glow mode to the Townsend mode is induced due to a much higher electron yield up to 1 nC. In this case, both experiment and simulation indicate a retarded stepwise release of surface electrons initiated by the low laser photon energy.
Abstract
In this series of two papers, the E-H transition in a planar inductively coupled radio frequency discharge (13.56 MHz) in pure oxygen is studied using comprehensive plasma diagnostic methods. The electron density serves as the main plasma parameter to distinguish between the operation modes. The (effective) electron temperature, which is calculated from the electron energy distribution function and the difference between the floating and plasma potential, halves during the E-H transition. Furthermore, the pressure dependency of the RF sheath extension in the E-mode implies a collisional RF sheath for the considered total gas pressures. The gas temperature increases with the electron density during the E-H transition and doubles in the H-mode compared to the E-mode, whereas the molecular ground state density halves at the given total gas pressure. Moreover, the singlet molecular metastable density reaches 2% in the E-mode and 4% in the H-mode of the molecular ground state density. These measured plasma parameters can be used as input parameters for global rate equation calculations to analyze several elementary processes. Here, the ionization rate for the molecular oxygen ions is exemplarily determined and reveals, together with the optical excitation rate patterns, a change in electronegativity during the mode transition.
Abstract
The laser photodetachment experiment in a diffuse helium–oxygen barrier discharge is evaluated by a 1D fluid simulation. As in the experiment, the simulated discharge operates in helium with
400
ppm
oxygen admixture at
500
mbar
inside a discharge gap of
3
mm
. The laser photodetachment is included by the interaction of negative ions with a temporally and spatially dependent photon flux. The simulation with the usually applied set of reactions and rate coefficients provides a much lower negative ion density than needed to explain the impact on the discharge characteristics in the experiment. Further processes for an enhanced negative ion formation and their capabilities of reproducing the experimental results are discussed. These further processes are additional attachment processes in the volume and the negative ion formation at the negatively charged dielectric. Both approaches are able to reproduce the measured laser photodetachment effect partially, but the best agreement with the experimental results is achieved with the formation of negative ions at the negatively charged dielectric.
Abstract
In this series of two papers we present results about the E-H transition of an inductively coupled oxygen discharge driven at radio frequency (13.56 MHz) for different total gas pressures. The mode transition from the low density E-mode to the high density H-mode is studied using comprehensive plasma diagnostics. The measured electron density can be used to distinguish between the different operation modes. This paper focuses on the determination of the negative atomic ion density and the electronegativity by two experimental methods and global rate equation calculation. As a result, the electronegativity significantly decreases over two orders of magnitude from about 25 in the E-mode to about 0.1 in the H-mode. The temporal behavior of the electronegativity in pulsed ICP shows that the negative atomic ion density reaches a steady state after 10 ms. Negative atomic ions are mainly produced by the dissociative attachment with the molecular ground state. The ion–ion recombination with the positive molecular ions and the collisional detachment with the singlet molecular metastables contribute significantly to the loss of the negative atomic ions.