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To address the low resolution and signal-to-noise ratios on a relatively low field MR system (1.5 T), Chen and colleagues used 3T MRI to verify whether DTI could help in locating epileptogenic areas.
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The relatively low field for these signals is due to a deshielding resulting from the adjacent double bond.
The most striking effect, which is, however, largely ignored in previous literature, is the relatively low field enhancement factor obtained from the experimental Fowler-Nordheim [FN] plot.
This quantum screening effect, which describes the relatively low field enhancement factors and higher turn-on field in most nanoscale FE experiments, is particularly crucial for vacuum nanoelectronic devices.
We put forward the quantum screening effect in field emission [FE] nanodiodes, explaining relatively low field enhancement factors due to the increased potential barrier that impedes the electron Fowler-Nordheim tunneling, which is usually observed in nanoscale FE experiments.
Clinical MRI was found to be limited by the relatively low field strength and resolution compared to what was shown in experimental studies [ 33].
The disadvantages of this scanner are its relatively low field strength of 0.5 Tesla and the requirement for non-magnetic instruments and microscopes.
Room temperature polarization-electric field (P-E) curves show that the samples are not saturated with maximum remanence polarization, Pr = 0.110 μC/cm2, and a relatively low coercive field, Ec = of 7.918 kV/cm, at an applied field of 1 kV/cm was observed for 5% Nd doping.
Dependence of the nanoparticles magnetization (M) on the external magnetic field (H) is described by a narrow hysteresis loop in relatively low fields and the strong linear M increase with the further H increase.
The highest value of Pr = 0.110 μC/cm2 and a relatively low coercive field (Ec) of 7.918 kV/cm were observed for 5% Nd concentration.
A high emission current of ∼30 μA was obtained at a relatively low applied field of ∼1.75 V/μm, corresponding to an overall current density of ∼7 × 104 A/cm2.
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