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For samples with fluences of 1 × 1017/cm2 and 5 × 1017/cm2, obvious flatness in the hysteresis loops can be observed, as shown in Fig. 2, identical to the behavior demonstrated for the exchange-spring magnets21.
Through this method, more discrete conductance levels could be observed, as shown in Fig. 15 [195, 195].
Because the UV light intensity is relatively low, no saturation photocurrent can be observed as shown in Fig. 3b.
When the decay time was extended to 104 s, no decay current could be observed as shown in the first light off Figure 2b.
As for the BE of Co 2p in Ni Co bimetallic catalysts, similar behaviors can also be observed, as shown in Fig. 6b.
Furthermore, the holes create more parallel filaments near the BE interface and a little decrease of set voltage and the resistance in LRS can be observed, as shown in Figures 3b and4b.
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Subsequently, cell proliferation or migration was observed, as shown in Figure 6.
With the laser modulation added, the presence of equally-spaced sidebands was observed, as shown in Figure 2a.
As an incident beam with TE polarization does not experience cloaking effect, significant splitting has been observed as shown in Figure 3e g at various incident angles.
This is one possible reason why we rarely observed standstill of the chitinases, whereas apparent stop of the movement of TrCel7A during the processive motion was observed, as shown by the dotted histogram line in Fig. 4g.
In contrast, at similar conditions where phase intermixing is observed for v1/6−30° and v1/5−30° borophene, another new structure is observed as shown in the derivative image of the bare-tip STM topography in Fig. 4a.
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