It is shown that the maximum superconducting transition temperature, T c for ZrP1.25Se0.75 is increased from 5.8 K to 7.2 K by partially substituting a non-magnetic rare earth atom Lu for Zr and on the other hand is d...
It is shown that the maximum superconducting transition temperature, T c for ZrP1.25Se0.75 is increased from 5.8 K to 7.2 K by partially substituting a non-magnetic rare earth atom Lu for Zr and on the other hand is decreased by substituting other non-magnetic rare earth atoms Y and La. Obviously, T c is raised when lattice constants in the a-axis and the c-axis increase with replacing Zr. Its implications for further increasing T c are discussed.
Conventional flip chip technologies such as the mass reflow (Mr) process and the thermal compression bonding (TCB) process are commonly used technologies in the micro assembly field. However, there is a continuous nee...
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Conventional flip chip technologies such as the mass reflow (Mr) process and the thermal compression bonding (TCB) process are commonly used technologies in the micro assembly field. However, there is a continuous need for next generation interconnection technology to achieve a low form factor with increasing die and substrate complexities. Moreover, very thin 3d integrated packages and 2.5d packages with thin interposerdie promise advanced interconnection technologies for mobile and wearable applications. With this point of view, the most important factor in interconnection is optimal thermal energy control for soldering. However, a conventional Mr process cannot provide any selectivity and controlled thermal energy transferring with the traditional convection reflow. Its high thermal budget makes warpage an issue, aside from other side effects. To overcome the Mr process problems, recent researches and industries have focused on developing a TCB process with non-conductive paste (NCP) or non-conductive film (NCF) due to TCB's unique advantages of low mechanical and thermal stress. However, the productivity of the TCB process is not comparably to the conventional process. Laser-assisted bonding (LAB) with beam homogenizer is considered to be the next generation interconnection technologydue to its excellent thermal selectivity, extremely fast ramping up speed with purely controlled wavelength. This LAB process offers a very stable interconnection quality as well as robust functional andreliability result. Interestingly, it also achieves excellent results with thin coreless substrate due to its selective heating area availability. This paper will discuss the laser heating mechanism, multi-chip & component bonding availability and advantage of LAB from an assembly industrial perspective.
The experimental CrFeMoNbTaTiZr alloys were designed based on the extremely low bio-toxicity of the chemical elements. They are currently used as a basis for alloying of classical alloys used in medical device manufac...
The experimental CrFeMoNbTaTiZr alloys were designed based on the extremely low bio-toxicity of the chemical elements. They are currently used as a basis for alloying of classical alloys used in medical device manufacturing. From this alloying system, were obtained in a Vacuum Arc remelting (VAr) equipment six alloys: CrFeMoNbTaTi, CrFeMoNbTaZr, CrFeMoTaTiZr, CrFeTaNbTiZr, CrTaNbTiZrMo and FeTaNbTiZrMo. The microstructural analysis of the obtained alloys have been performed by optical and SEM microscopy. The microhardness tests show results in the range of 575 – 1337 HV0.2 / 10. In order to improve the mechanical properties heat treatment procedures have been applied.
The method to attach seed to crucible lid as well as seed quality is very important for obtaining high quality crystals. Therefore, modified seeding method was developed for improving adhesive layer between seed and g...
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ISBN:
(纸本)9781509026142
The method to attach seed to crucible lid as well as seed quality is very important for obtaining high quality crystals. Therefore, modified seeding method was developed for improving adhesive layer between seed and graphite crucible lid. SiC single crystal grown with modified seeding methoddefinitely exhibited lower micropipe density (MPd) and lower full width at half maximum (FWHM) values comparing with values from conventional seeding method. Etch pit density of SiC crystal was successfully decreased with using the modified seeding method.
We present a novel algorithm that can determine rotation-related parameters of a target using FMCW (frequency modulated continuous wave) radars, not utilizing inertia information of the target. More specifically, th...
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We present a novel algorithm that can determine rotation-related parameters of a target using FMCW (frequency modulated continuous wave) radars, not utilizing inertia information of the target. More specifically, the proposed algorithm estimates the angular velocity vector of a target as a function of time, as well as the distances of scattering points in the wing tip from the rotation axis, just by analyzing doppler spectrograms obtained from three or more radars. The obtained parameter values will be useful to classify targets such as hostile warheads or missiles forreal-time operation, or to analyze the trajectory of targets under test for the instrumentation radar operation. The proposed algorithm is based on the convex optimization to obtain the rotation-related parameters. The performance of the proposed algorithm is assessed through Monte Carlo simulations. Estimation performance of the proposed algorithm depends on the target andradar geometry and improves as the number of iterations of the convex optimization steps increases.
SiC powders having different purities were prepared by carbothermal reduction underdifferent conditions from traditional process and SiC single crystals were grown by the PVT method from the powders. After crystal gr...
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In the present study we investigated the electronic structure of the valence skipping compoundrbTlX3 (X=F,Cl,Br) from first principles. Combined with structural optimization, we confirmed that the charge-density-wave...
In the present study we investigated the electronic structure of the valence skipping compoundrbTlX3 (X=F,Cl,Br) from first principles. Combined with structural optimization, we confirmed that the charge-density-wave (CdW) is formed in all of these three compounds, and the Tl atoms in two different sites take the valence Tl1+ and Tl3+. We investigated the evolution of the CdW gap as a function of the volume and the atomic position, and found that this CdW gap can be collapsed by applying pressure with only few GPa forrbTlBr3. In this metallic phase a large charge-fluctuation and a large electron-phonon interaction is expected.
In this study, the current fluctuations were measured at the hydrothermal fields in the Okinawa Trough (Hatoma Knoll, Irabu Knoll, and Iheya North field) to characterize the fluid environment. The purpose of this stud...
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ISBN:
(纸本)9781509015276
In this study, the current fluctuations were measured at the hydrothermal fields in the Okinawa Trough (Hatoma Knoll, Irabu Knoll, and Iheya North field) to characterize the fluid environment. The purpose of this study was to reveal the fluctuations of the deep-sea currents using an acoustic doppler current profiler (AdCP), and to correlate them with the development of a bottom mixed layer as predicted by a numerical model. An AdCP (Teledyne rd Instruments Workhorse Sentinel, 300 kHz) was installed on the seabed at the Hatoma Knoll (depth about 1500 m), Irabu Knoll (depth about 2000 m), and Iheya North field (depth about 1000 m). For each observation point, the deep-sea current data were successfully recovered in the layer at depths between the seafloor and 40-60 m above the seafloor. Notably, the measurement results obtained at the Hatoma Knoll and Iheya North field showed a remarkably interesting fluctuation. during a time period of approximately 3 h, the range in the depths at which the currents were successfully recorded increased in a pulse form, up to around the upper layer at 120 m, allowing measurements in almost all of the layers. The time period of this pulse corresponded to the shift from an ebb tide to high tide. With the exception of these pulses, the currents could only be recorded from the seafloor to about a 40 m layer. This result indicated that a suitable environment for AdCP measurements was formed only within this range. To investigate the cause, a numerical model experiment was performed for the bottom turbulence and subsequent occurrence of vertical mixing of the suspended particulate matter in the Okinawa Trough using a large-eddy simulation (LES) model. The simulatedresults suggested that the semidiurnal tide periodically enhances the bottom turbulence at intervals of approximately 6 h, with the result that the bottom mixed layer thickness increases to a maximum of approximately 40-60 m. It was concluded that a suitable environment for AdCP
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