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Behavior of a porous particle in a radiofrequency plasma under pulsed argon ion beam bombardment
The behavior of a single porous particle with a diameter of 250 μm levitating in a radiofrequency (RF) plasma under pulsed argon ion beam bombardment was investigated. The motion of the particle under the action of the ion beam was observed to be an oscillatory motion. The Fourier-analyzed motion is dominated by the excitation frequency of the pulsed ion beam and odd higher harmonics, which peak near the resonance frequency. The appearance of even harmonics is explained by a variation of the particles's charge depending on its position in the plasma sheath. The Fourier analysis also allows a discussion of neutral and ion forces. The particle's charge was derived and compared with theoretical estimates based on the orbital motion-limited (OML) model using also a numerical simulation of the RF discharge. The derived particle's charge is about 7-15 times larger than predicted by the theoretical models. This difference is attributed to the porous structure of the particle. © IOP Publishing Ltd and Deutsche Physikalische Gesellschaft
Energy influx from an rf plasma to a substrate during plasma processing
The energy influx delivered by an rf plasma to a metal substrate has been studied by a calorimetric method with a thermal probe. By changing the substrate voltage, the influence of the kinetic energy of the charge carriers to the thermal power could be determined. The measured energy influx for an argon plasma can be explained mainly by ions, electrons, and their recombination. In the case of an oxygen plasma, where the energy influx is under comparable conditions about 50% higher, also other transfer mechanisms such as surface-aided atom association and relaxation of rovibrational states have to be taken into consideration
High-resolution FTIR spectroscopy and analysis of the Ka = 0 ← 1 subbands of the fundamentals ν3 and ν6 of the dimer (HF)2
We report new far-infrared spectra of (HF)2 obtained by high resolution long-path Fourier Transform-Infrared (FTIR) spectroscopy. The origins of the two tunneling components of the Ka= 0 ← 1 subband of the in-plane symmetric bending fundamental ν3 were found to be at 450.4546 cm−1 (Γt: A+ ← B+) and at 451.4583 cm−1 (B+ ← A+), and of the Ka= 0 ← 1 subband of the out-of-plane bending fundamental ν6 at 382.0802 cm−1 (A+ ← A+) and at 383.2245 cm−1 (B+ ← B+). The Ka= 0 term values with respect to the ground state Γt = A+ term are 486.9442 cm−1 for the A+ and 486.8834 cm−1 for the B+ tunneling levels of ν3. They are 417.5053 cm−1 for the A− and 419.7140 cm−1 for the B− vibration-tunneling sublevels of ν6. The results are discussed in relation to full-dimensional quantum dynamics and predictions based on recent ab initio calculations and our empirically refined potential energy hypersurfaces. Graphical abstract
2MASS J03105986+1648155AB - A new binary at the L/T transition
The transition from the L to the T spectral type of brown dwarfs is marked by
a very rapid transition phase, remarkable brightening in the J-band and a
higher binary frequency. Despite being an active area of inquiry, this
transition regime still remains one of the most poorly understood phases of
brown dwarf evolution. We resolved the L dwarf 2MASS J03105986+1648155 for the
first time into two almost equally bright components straddling the L/T
transition. Since such a co-eval system with common age and composition
provides crucial information of this special transition phase, we monitored the
system over 3 years to derive first orbital parameters and dynamical mass
estimates, as well as a spectral type determination. We obtained resolved high
angular resolution, near-IR images with HST and the adaptive optics instrument
NACO at the VLT including the laser guide star system PARSEC. Based on two
epochs of astrometric data we derive a minimum semi-major axis of 5.2 +- 0.8
AU. The assumption of a face-on circular orbit yields an orbital period of 72
+- 4 years and a total system mass of 30-60 Mjup. This places the masses of the
individual components of the system at the lower end of the mass regime of
brown dwarfs. The achieved photometry allowed a first spectral type
determination of L9 +- 1 for each component. In addition, this seems to be only
the fifth resolved L/T transition binary with a flux reversal. While ultimate
explanations for this effect are still owing, the 2MASS J03105986+1648155
system adds an important benchmark object for improving our understanding of
this remarkable evolutionary phase of brown dwarfs. Additionally, the
observational results of 2MASS J03105986+1648155 AB derived with the new PARSEC
AO system at the VLT show the importance of this technical capability. The
updated AO system allows us to significantly extend the sample of brown dwarfs
observable with high-resolution from the ground and hence to reveal more of
their physical properties.Comment: 6 pages, 2 figures, 3 tables, accepted for publication by A&
Polarization Diagnostics for Cool Core Cluster Emission Lines
The nature of the interaction between low-excitation gas filaments at ~104 K, seen in optical line emission, and diffuse X-ray emitting coronal gas at ~107 K in the centers of galaxy clusters remains a puzzle. The presence of a strong, empirical correlation between the two gas phases is indicative of a fundamental relationship between them, though as yet of undetermined cause. The cooler filaments, originally thought to have condensed from the hot gas, could also arise from a merger or the disturbance of cool circumnuclear gas by nuclear activity. Here, we have searched for intrinsic line emission polarization in cool core galaxy clusters as a diagnostic of fundamental transport processes. Drawing on developments in solar astrophysics, direct energetic particle impact induced polarization holds the promise to definitively determine the role of collisional processes such as thermal conduction in the ISM physics of galaxy clusters, while providing insight into other highly anisotropic excitation mechanisms such as shocks, intense radiation fields, and suprathermal particles. Under certain physical conditions, theoretical calculations predict of the order of 10% polarization. Our observations of the filaments in four nearby cool core clusters place stringent upper limits ( 0.1%) on the presence of emission line polarization, requiring that if thermal conduction is operative, the thermal gradients are not in the saturated regime. This limit is consistent with theoretical models of the thermal structure of filament interfacesPeer reviewe
Cavity-Enhanced Raman Spectroscopy of Natural Gas with Optical Feedback cw-Diode Lasers
We report on improvements made on our previously introduced technique of cavity-enhanced Raman spectroscopy (CERS) with optical feedback cw-diode lasers in the gas phase, including a new mode-matching procedure which keeps the laser in resonance with the optical cavity without inducing long-term frequency shifts of the laser, and using a new CCD camera with improved noise performance. With 10 mW of 636.2 nm diode laser excitation and 30 s integration time, cavity enhancement achieves noise-equivalent detection limits below 1 mbar at 1 bar total pressure, depending on Raman cross sections. Detection limits can be easily improved using higher power diodes. We further demonstrate a relevant analytical application of CERS, the multicomponent analysis of natural gas samples. Several spectroscopic features have been identified and characterized. CERS with low power diode lasers is suitable for online monitoring of natural gas mixtures with sensitivity and spectroscopic selectivity, including monitoring H2, H2S, N2, CO2, and alkanes
The DURAbility of Basal versus Lispro mix 75/25 insulin Efficacy (DURABLE) Trial: Comparing the durability of lispro mix 75/25 and glargine
OBJECTIVE This study compared the durability of glycemic control of twice-daily insulin lispro mix 75/25 (LM75/25: 75% insulin lispro protamine suspension/25% lispro) and once-daily insulin glargine, added to oral antihyperglycemic drugs in type 2 diabetes patients
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