Analysis of Cu–Cu direct bonding and grain growth across the bonding interface
Figure 2(a) shows an IPF-Z mapping image of the Cu(500 nm)/Ti(200 nm) seed layer. The granular Cu microstructure is clearly evident, and the Cu grains have a…
Figure 2(a) shows an IPF-Z mapping image of the Cu(500 nm)/Ti(200 nm) seed layer. The granular Cu microstructure is clearly evident, and the Cu grains have a…
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The steady-state behavior of TE materials is governed by the conservation of electric charge and energy35:
$$\nabla \cdot{\boldsymbol{J}}=0$$
(1)
$$\nabla…
The eigenmodes of lasers are solutions to the Helmholtz equation under the paraxial approximation, which means that their intensity distribution remains invariant during propagation, with only a scaling effect due to beam…
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Consider the crystallographic parameters, including lattice constants, cell angles, and internal atomic positions, represented by Cγ, with γ ranging from 1 to NC. In a scenario where symmetries are ignored, NC is given by 6 +…
For the identification of the local polar structure of the designed NN-based RFEs, the detailed polar structures of both samples were carried out by transmission electron…
• Physics 18, s115
The MicroBooNE experiment’s five-year dataset has shown that an unpredicted neutrino-flavor oscillation is not the cause of anomalous results obtained by its predecessor.
MicroBooNE Collaboration
A new AI tool is giving fusion research a huge boost by spotting hidden “safe zones” inside reactors where parts are shielded from scorching plasma heat. Called HEAT-ML, the system can do in milliseconds what once took half an hour, allowing…
After more than 30 years, physicists in Finland have uncovered the heaviest nucleus ever seen to emit a proton, a rare process that sheds light on the limits of atomic matter. The discovery of 188-astatine — an oddly “watermelon-shaped”…