Bessel beams: Effects of polarization

An approximation to a Bessel beam produced by tightly focusing linearly polarized light is known to produce a smaller central lobe than focusing plane polarized light. This is because the plane polarized wave gives a broad central lobe caused mainly by a parasitic longitudinal field component. It is known that this problem can be overcome by focusing radially polarized light. Here we demonstrate that other polarization distributions based on a linear combination of transverse electric (TE1) and transverse magnetic (TM1) fields can give a beam even narrower than for the radially polarized case. Special cases of this combination are identified, corresponding to the smallest width (TE1), and the maximum peak intensity compared with the side lobes (electric dipole polarization). Axially-symmetric forms can be generated by illumination with elliptically polarized light. A particular case is azimuthal polarization with a phase singularity, which is equivalent to TE1. For a semi-angular aperture of 60°, the TE1 case gives a central lobe width 9% narrower than for radially polarized illumination, while for plane polarized illumination it is 12% wider than the radially polarized case.     

Direct Measurement of Emission of Endogenous Ozone from Plants by GC–MS-SIM

According to recent observations antibodies can catalyze the formation of previously unknown oxidants, dihydrogen trioxide (H₂O₃) and ozone (O₃), formed in the interaction between singlet oxygen (¹O₂) and H₂O. The O₃ molecules can be detected indirectly e.g. in TLC/OPLC chromatographic spots in the simple BioArena operating system using O₃-eliminating molecules in the culture medium. It is currently supposed that plants can be used for the direct detection of O₃ during its eventual emission from stomata. Using the fresh primary leaves of different plant species O₃ could be really detected by means of GC–MS-SIM from the space above the the leaves which were prepared in a CO₂-containing headspace vessel. It has been also established that the CO₂ also contained O₃ molecules, and therefore, we had to use a correction to the observed data. These new findings indicate that not only formaldehyde but also O₃ and their related bioreactive compounds may play a crucial role in disease resistance (e.g. in the mechanism of action of antibodies), cell proliferation and differentiation.     

Study of structural and electronic transport properties of Ce-doped LaMnO3

The structural and electronic transport properties of La_1−x Ce _x MnO₃ (x=0.0–1.0) have been studied. All the samples exhibit orthorhombic crystal symmetry and the unit cell volume decreases with Ce doping. They also make a metal-insulator transition (MIT) and transition temperature increases with increase in Ce concentration up to 50% doping. The system La_0.5Ce_0.5MnO₃ also exhibits MIT instead of charge-ordered state as observed in the hole doped systems of the same composition.     

Gaschromatographische Bestimmung von Methoxyacetaldehyd neben Formaldehyd, Acetaldehyd und Glykolmethyl?ther

Zusammenfassung Eine gaschromatographische Methode zur Bestimmung von Formaldehyd, Acetaldehyd, Methoxyacetaldehyd und GlykolmethylÄther nebeneinander wurde entwickelt. Die Methode leistet gute Dienste bei der Kontrolle der ersten Stufe der Synthese von d-Cycloserin. Das Studium des Einflusses der verschiedenen Parameter auf die Ausbeute und der bei der heterogenen Katalyse verlaufenden Nebenreaktionen wird ermöglicht.

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Summary A gas-chromatographic method has been worked out for the determination of formaldehyde, acetaldehyde, methoxy acetaldehyde and glycolmethyl ether in presence of each other. It can be advantageously used for controlling the first stage of the synthesis of d-cycloserine. It also permits an investigation of the influence of the different parameters on the yield and an examination of the side-reactions involved in the heterogenous catalysis.

     

Catalytic reduction of sulfuric acid to sulfur dioxide

The reduction of H₂SO₄ to SO₂ occurs with a relatively good efficiency only at high temperatures, in the presence of catalysts. Some experimental results, regarding conversion of sulfuric acid (96 wt.%) to sulfur dioxide and oxygen, are reported. The reduction has been performed at 800 ?C 900°C and atmospheric pressure, in a tubular quartz reactor. The following commercial catalysts were tested: Pd/Al₂O₃ (5 wt.% and 0.5 wt.% Pd), Pt/Al₂O₃ (0.1 wt.% Pt) and ??-Fe₂O₃. The fresh and spent catalysts were characterized by X-Ray diffraction and BET method. The highest catalytic activity was determined for 5 wt.% Pd/Al₂O₃, a conversion of 80% being obtained for 5 hours time on stream, at 9 mL h^?1 flow rate of 96 wt.% H₂SO₄. A conversion of 64% was determined for 0.5 wt.% Pd/Al₂O₃ and 0.1 wt.% Pt/Al₂O₃. For ??-Fe₂O₃, a less expensive catalyst, a conversion of 61% for about 60 hours was obtained.      

Laser processing of bulk Al–12Si alloy: influence of microstructure on thermal properties

The feasibility of enhancing the thermal conductivity of an alloy via microstructural refinement was examined using Al–12%Si alloy as a model material. Al–12Si alloy samples were fabricated at different process parameters using laser engineered net shaping (LENS?) and the effect of microstructural features on the thermal conductivity was studied and compared with conventionally cast alloy. The large difference in melting points and laser light absorptivities of Si and Al as well as the low melt viscosity of Al–12Si alloy resulted in a very small process window to successfully fabricate bulk Al–12Si alloy samples using LENS?. Comparison of microstructural features of laser-processed samples with cast Al–12Si alloy showed significant refinement in eutectic Si for laser processed samples. Microstructural refinement not only improved the thermal conductivity of Al–12Si alloy but also compensated the detrimental effect of porosity on thermal conductivity. The thermal conductivity of cast alloy varied between 82 and 93?W/mK, which is ～21–76% lower than the values exhibited by laser-processed samples in the range 103–153?W/mK. The results of LENS? fabrication, microstructural evolution and thermal properties of Al–12Si alloy bulk structures can be extended to other immiscible alloys and metal matrix composites for a variety of engineering applications.     

Kinetics of the reactions of isopropoxy radicals with NO,NO2, and O2

A fluorescence excitation spectrum of (CH₃)₂CHO (isopropoxy radical) is reported following photolysis of isopropyl nitrite at 355 nm. Rate constants for the reaction of isopropoxy with NO, NO₂, and O₂ have been measured as a function of pressure (1–50 Torr) and temperature (25–110°C) by monitoring isopropoxy radical concentrations using laser-induced fluorescence. We have obtained the following Arrhenius expressions for the reaction of isopropoxy with NO and O₂ respectively: (1.22±0.28)×10^?11 exp[(+0.62±0.14 kcal)/RT]cm²/s and (1.51±0.70)×10^?14 exp[(?0.39±0.28)kcal/RT]cm³/s where the uncertainties represent 2σ. The results with NO₂ are more complex, but indicate that reaction with NO₂ proceeds more rapidly than with NO contrary to previous reports. The pressure dependence of the thermal decomposition of the isopropoxy radical was studied at 104 and 133°C over a 300 Torr range using nitrogen as a buffer gas. The reaction is in the fall-off region over the entire range. Upper limits for the reaction of isopropoxy with acetaldehyde, isobutane, ethylene, and trimethyl ethylene are reported.We have performed the first LIF study of the isopropoxy radical. Arrhenius parameters were measured for the reaction of i-PrO with O₂, NO, NO₂, using direct radical measurement techniques. All reactions are in their high-pressure limits at a few Torr of pressure. The rate constant for the reactions of i-PrO with NO and NO₂ reactions exhibit a small negative activation energy. Studies of the i-PrO + NO₂ reaction produce data which indicate that O(³P) reacts rapidly with i-PrO. Unimolecular decomposition studies of i-PrO indicate that the reaction is in the fall-off region between 1 and 300 Torr of N₂ and the high-pressure limit is above 1 atmosphere of N₂.