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In the case of exit requirements in Taiwan the possible coercive strength of the policy is weakened at the essential point of using certifications of English ability for a real-world purpose, i.e., getting a job.
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When the external field is reversed, the value of B falls and passes through zero (point C) at a field strength known as the coercive force.
Crack growth only occurred if the applied field exceeded the coercive field strength of the material.
Ferroelectric performance in SiO2-doped HfO2 with a remanent polarization (P r) above 10 μC/cm2 and a coercive field strength (E c) of 1 MV/cm was reported [1].
A remnant polarization of 19 μC/cm2 and a coercive field strength of 1.07 MV/cm were achieved with the Pt/HZO/Ni stack annealed at 650 °C with a HZO thickness of ∼20 nm.
In this work, a Ni/Hf0.5Zr0.5O2/Ru/Si stack annealed at 550°C for 30 s in N2 ambient after the Ni top electrode has been deposited was manufactured, and it shows the best ferroelectric hysteresis loop in the dielectric thickness of 25 nm, with a remanent polarization value of 6 μC/cm2 and a coercive field strength of 2.4 MV/cm measured at 10 kHz.
Samarium cobalt has the next highest coercive field strength, at 9,200 oersted, but a magnetic flux density of 10,500 gauss and an overall energy density of 26.
This glassy alloy shows a high fracture strength ~ 4000 MPa with a plastic strain of 0.5%, a high saturation magnetization ~ 1.45 T and a low coercive force ~ 1.5 A/m.
But we have no coercive force.
Here, we successfully synthesized an Fe39Ni39B14.2Si2.75P2.75Nb2.3 BMG which exhibits large plastic strain of 7.8%, high fracture strength of 3.35 GPa and excellent soft magnetic properties, i.e., rather high saturation flux density of 0.88 T, low coercive force of 0.7 A/m and high permeability of 20800.
coercive force.
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