Sentence examples for excitation left from inspiring English sources

Normalization (by area = 1) of the excitation (left) and emission (right) spectral set prior to the application of the SIMCA modelling.

Fig. 4 Room temperature (300 K) magnetic hysteresis loops of a Fe3O4 NPs, b Fe3O4@SiO2, c Fe3O4@SiO2-[Eu DBM 3Lp] Fe3O4@SiO2-[Eu DBM 3Lp]Lp]@PEI nanocomposite. Figure 5 illustrates the corrected excitation (leFe3O4@SiO2-[Eu DBM 3Lp]@PEI Fe3O4@SiO2-[Eu DBM 3Lp]@PEIomplex [Eu(DBM)3Lp] ananocompositeSiO2-[Eu(DBM)3Lp]@PEI nanocomposite as solid at room temperature.

This would require the system to be re-set once (after the 10th excitation), leaving 4 stored in the phase-change medium; hence the result is 1 remainder 4. We have performed exactly this computation using our phase-change processor.

Even for very low temperatures, before all excitations leave the chain, the equilibrium state will be a thermalized state.

When both inhibition and excitation were left intact, LTP induced by pairing was only slightly reduced by AIP (Figure 5C), as expected from the loss of the glutamatergic LTP component (Figure 2B).

Furthermore, the designs do not affect the designs of simultaneous multiple fluorescence or side scatter detection designs as the beam shaping still maintains a uniform region for excitation while leaving room for multiple collection waveguides.

Left noise excitation frequency content of 0 200 Hz, right noise excitation frequency content of 0 50 Hz.

Open image in new window Fig. 10 CWT analysis for case 3. Left noise excitation frequency content of 0 200 Hz, right noise excitation frequency content of 0 50 Hz.

Band-selective inversion pulses are characterized by almost rectangular inversion profiles, leading to full inversion for spin packets with resonance offsets within the pulse excitation bandwidth and leaving spin packets outside the excitation bandwidth largely unaffected.

Long after the excitation laser pulse has left the sample – some 60 femtoseconds later – they observed the onset of a collective movement of the atoms, that is, phonons.

The cotunneling transport can be either elastic if the transmitting electron leaves the dot in its ground state, or inelastic if the applied bias exceeds the lowest excitation energy and the dot is left in an excited state.