Microwave complementary doped-channel field-effect transistors

In this paper, the device performance and complementary inverter of the InGaP/InGaAs/GaAs doped-channel field-effect transistors (DCFETs) by two-dimensional semiconductor simulation are demonstrated. Due to the relatively large conduction (valance) band discontinuity at InGaP/InGaAs interface, it provides good confinement effect for transporting carriers in InGaAs channel layer for the n-channel (p-channel) device. The large gate turn-on voltage is achieved due to the employment of the wide energy-gap InGaP material as gate layer. The _ft$f_t$ and _fmax$f_{max}$ are of 6.5 (2.1) and 25 (5) GHz for the n-channel (p-channel) device. Furthermore, the co-integrated structures, by the combination of n- and p-channel field-effect transistors, could form a complementary inverter and the relatively large noise margins are achieved.     

Theoretical study of mechanisms for NCO with CH3 reaction

A detailed computational study has been performed at the QCISD(T)/6-311++G(d,p)//B3LYP/6-311++G(d,p) level for the NCO with CH₃ reaction by constructing singlet and triplet potential energy surfaces (PES). The results show that the title reaction is more favorable for the singlet PES than the triplet PES. On the singlet PES, the dominant channel is the barrierless addition of the O or N atom to the C atom of the methyl group to form CH₃NCO (IM1) and CH₃OCN (IM2). On the triplet PES, the favorable channel is the barrierless addition of the N atom to the C atom of the methyl group to form an intermediate CH₃NCO (³IM2), which then undergoes a N–C bond scission process to give out CH₃N + CO.     

A luminescent Pt(II) complex with a terpyridine-like ligand involving a six-membered chelate ring

The ligand 2-(8'-quinolinyl)-1,10-phenanthroline (1) was prepared in 79% yield by the Friedlander condensation of 8-amino-7-quinolinecarbaldehyde and 8-acetylquinoline. The complex [Pt(1)Cl]+ was prepared and compared with the isomeric 2-(2'-quinolinyl)-1,10-phenanthroline (2) complex. An X-ray analysis indicated that the six-membered chelate ring in the tridentate complex resulted in a relief of angle strain as well as some non-planarity in the bound ligand 1. The control system for photophysical studies is [Pt3Cl]+ where denotes 2-(2'-pyridyl)-1,10-phenanthroline. Relative to the complex of 3, in dichloromethane solution [Pt(1)Cl]+ exhibits noticeably higher energy charge-transfer absorption but slightly lower energy emission. The gap between the onset of absorption and emission is larger because the emission from [Pt(1)Cl]+ originates from a triplet excited state with substantial intra-ligand character. At room temperature in deoxygenated dichloromethane, [Pt(1)Cl]+ has an excited-state lifetime of 310 ns vs. 230 ns for [Pt(1)Cl]+. Within the series, [Pt(1)Cl]+ also exhibits the largest activation barrier for thermally induced quenching at 2730 cm(-1) in fluid dichloromethane solution. However, the barrier is only about 50% larger than that found for [Pt(1)Cl]+. There is reduced ring strain in [Pt(1)Cl]+, but inter-ligand steric interactions weaken the ligand field.     

Bi-1,10-phenanthrolines and their mononuclear Ru(II) complexes

A series of four biphen (phen = 1,10-phenanthroline) ligands, 2,2'-biphen (1), 3,3'-biphen (2), 2,2'-dimethylene-3,3'-biphen (3), and 2,3'-dimethylene-3,2'-biphen (4), is prepared by coupling and Friedl?nder methodology. The corresponding mononuclear Ru(II) complexes, [Ru(1-4)(Mebpy)(2)](2+) where Mebpy = 4,4'-dimethyl-2,2'-bipyridine, are prepared. These complexes show long wavelength electronic absorptions at 441-452 nm and emissions at 622-641 nm. Metal-based oxidations occur in the range 1.18-1.21 V, and ligand-based reductions, at -1.20 to -1.30 V. The addition of Zn(2+), Cd(2+), or Hg(2+) ions results in a strong enhancement and red shift of the luminescence of complex Ru-3. Alkali and alkaline earth metal ions barely affect the luminescence of Ru-3 while transition metal ions such as Co(2+), Cu(2+), Ni(2+), and Mn(2+) lead to efficient quenching of the Ru-3 luminescence. The luminescence of Ru-2 and Ru-4 is quenched in the presence of Zn(2+) because of a conformationally induced reduction in electronic communication between the two phen halves of the ligand. The addition of Zn(2+) has only a slight effect on the luminescence of Ru-1 because of steric hindrance toward complexation.     

New insight into the kinetic behavior of the structural formation process in agar gelation

Experimental investigations based on our custom-built torsion resonator were carried out on the kinetics and relaxation of the structural formation process in three agar–water solutions with agar concentrations of 0.75, 1.0, and 2.0 % w/w under natural cooling. An interesting temperature-dependent oscillatory decaying behavior of the structure development rate (SDR) in the agar gelation process is observed. This oscillatory SDR-decaying behavior is indicative of a sum of multiple SDR-determining relaxation processes and could be quantitatively described by a multiple-order Gaussian-like equation, i.e., $dG^{\prime }/dt\equiv \sum \nolimits _{n=0}^{m}{dG^{\prime }/dt}^{(n)}=\sum \nolimits _{n=0}^{m}K_{n}{\rm exp}[-2(T-T_{n})^{2}/W_{n}^{2}]$ . The ${\rm T}_{n}$ dependences of ${\rm W}_{n}$ in the gelation zone were also found to follow the Arrhenius law with activation energies of 39–74 kJ/mol for three investigated samples, indicating the important role of formation or fission of the hydrogen bonding interaction playing in the agar structural network formation. These findings provide insights into the mechanical properties and distinctive structure development rates of agar sols that dynamically and naturally evolve to form gels.     

Design of the IMP microbeam irradiation system for 100 MeV/u heavy ions

A state-of-the-art high energy heavy ion microbeam irradiation system is constructed at the Institute of Modern Physics of the Chinese Academy of Sciences. This microbeam system operates in both full current intensity mode and single ion mode. It delivers a predefined number of ions to pre-selected targets for research in biology and material science. The characteristic of this microbeam system is high energy and vertical irradiation. A quadrupole focusing system, in combination with a series of slits, has been designed to optimize the spatial resolution. A symmetrically achromatic system leads the beam downwards and serves simulta-neously as an energy analyzer. A high gradient quadrupole triplet finally focuses a C6+ ion beam to 1 μm in the vacuum chamber within the energy range from 10 MeV/u to 100 MeV/u. In this paper, the IMP microbeam system is described in detail. A systematic investigation of the ion beam optics of this microbeam system is presented together with the associated aberrations. Comparison is made between the IMP microbeam system and the other existing systems to further discuss the performance of this microbeam. Then the optimized initial beam parameters are given for high resolution and high hitting efficiency. At last, the experiment platform is briefly introduced.     

Non-Contact to Contact Transition： Direct Measurements of Interaction Forces between a Solid Probe and a Planar Air-Water Interface

The interaction force between a solid probe and a planar air-water interface is measured by using an atomic force microscope. It is demonstrated that during the approach of the probe to the air-water interface, the force curves decline all the time due to the van der Waals attraction and induces a stable profile of water surface raised. When the tip approaches very close to the water surface, force curves jump suddenly, reflecting the complex behaviour of the unstable water surface. With a theoretical analysis we conclude that before the tip touches water surface, two water profiles appear, one stable and the other unstable. Then, with further approaching, the tip touches water surface and the non-contact to contact transition occurs.     

Ab initio/DFT theory and multichannel RRKM study on the mechanisms and kinetics for the CH3S + CO reaction

The potential energy surface for the reaction of CH₃S with CO was calculated at the G3MP2//B3LYP/6-311++G(d,p) level. The rate constants for feasible channels leading to several products were calculated by TST and multichannel-RRKM theory. The results show that addition–elimination mechanism is dominant, while hydrogen abstraction mechanism is uncompetitive. The major channel is the addition of CO to CH₃S leading to an intermediate CH₃SCO which then decomposes to CH₃ + OCS. In the temperature range of 200–3000 K, the overall rate constants are positive temperature dependence and pressure independence, and it can be described by the expression as k = 1.10 × 10⁻¹⁶T^1.57exp(−3359/T) cm³ molecule⁻¹ s⁻¹. At temperature between 208 and 295 K, the calculated rate constants are in good agreement with the experimental upper limit data. At T = 1000 and 2000 K, the major product is CH₃ + OCS at lower pressure; while at higher pressure, the stabilization of IM1 is dominant channel.     

Theoretical study of the reaction of ethynyl radical with acetonitrile

A detailed computational study has been performed on the mechanism and kinetics of the C₂H + CH₃CN reaction. The geometries were optimized at the BHandHLYP/6–311G(d, p) level. The single-point energies were calculated using the BMC-CCSD, MC-QCISD and QCISD(T)/6–311+G(2df, 2pd) methods. Five mechanisms were investigated, namely, direct hydrogen abstraction, C-addition/elimination, N-addition/elimination, C₂H–to–CN substitution and H-migration. The kinetics of the title reaction were studied using TST and multichannel RRKM methodologies over a wide range of temperatures (150–3,000 K) and pressures (10^?4–10⁴ torr). The total rate constants show positive temperature dependence and pressure independence. At lower temperatures, the C-addition step is the most feasible channel to produce CH₃ and HCCCN. At higher temperatures, the direct hydrogen abstraction path is the dominant channel leading to C₂H₂ and CH₂CN. The calculated overall rate constants are in good agreement with the experimental data.     

DFT and ab initio study on the reaction mechanism of CH2SH + O2

The mechanism for the CH₂SH + O₂ reaction was investigated by DFT and ab initio chemistry methods. The geometries of all possible stationary points were optimized at the B3LYP/6-311+G(d,p) level, and the single point energy was calculated at the CCSD(T)/cc-pVXZ(X = D and T), G3MP2 and BMC-CCSD levels. The results indicate that the oxidation of CH₂SH by O₂ to form HSCH₂OO is a barrierless process. The most favorable channel is the rearrangement of the initial adduct HSCH₂OO (IM1) to form another intermediate H₂C(S)OOH (IM3) via a five-center transition state, and then the C–O bond fission in IM3 leads to a complex CH₂S. . .HO₂ (MC1), which finally gives out to the major product CH₂S + HO₂. Due to high barriers, other products including cis- and trans-HC(O)SH + HO could be negligible. The direct abstraction channel was also determined to yield CH₂S + HO₂, with the barrier height of 22.3, 18.1 and 15.0 kcal/mol at G3MP2, CCSD(T)/cc-pVTZ and BMC-CCSD levels, respectively, it is not competitive with the addition channel, in which all stationary points are lower than reactant energetically. The other channels to produce cis- and trans-CHSH + HO₂ are also of no importance.