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(Figure 4.17). The difference between phasematched and unphasematched SHG is<br />

very instructive in Figure 4.18. Minimal pump power leads to SHG light at 780<br />

nm. The conversion efficiency is much larger than at the peak to the left. For the<br />

full data set please refer to Appendix A.4.2. Note that in Figures 4.15 to 4.18, the<br />

Shg power Pump power [a.u.]<br />

Shg power Pump power [a.u.]<br />

2<br />

1.5<br />

1<br />

0.5<br />

Mapping pump wavelength to shg wavelength<br />

Shg spectrum<br />

Pump spectrum<br />

0<br />

700 720 740 760 780 800 820 840<br />

Shg wavelength [nm] Pump wavelength [nm/2]<br />

Figure 4.15: Shifted SHG<br />

2<br />

1.5<br />

1<br />

0.5<br />

Mapping pump wavelength to shg wavelength<br />

Shg spectrum<br />

Pump spectrum<br />

0<br />

700 720 740 760 780 800 820 840<br />

Shg wavelength [nm] Pump wavelength [nm/2]<br />

Figure 4.17: Insufficient pump power<br />

Shg power Pump power [a.u.]<br />

2<br />

1.5<br />

1<br />

0.5<br />

Mapping pump wavelength to shg wavelength<br />

Shg spectrum<br />

Pump spectrum<br />

0<br />

700 720 740 760 780 800 820 840<br />

Shg wavelength [nm] Pump wavelength [nm/2]<br />

Figure 4.16: Phasematched SHG<br />

Shg power Pump power [a.u.]<br />

2<br />

1.5<br />

1<br />

0.5<br />

Mapping pump wavelength to shg wavelength<br />

Shg spectrum<br />

Pump spectrum<br />

0<br />

700 720 740 760 780 800 820 840<br />

Shg wavelength [nm] Pump wavelength [nm/2]<br />

Figure 4.18: Near phasematching<br />

amplitudes of pump and SHG power have been scaled to illustrate the mappings<br />

between SHG and pump light. Yet all plots in this measurement share the same<br />

scaling factor.<br />

Irregularities in the manufacturing process may lead to a different phasematching<br />

contour for each different waveguide. Another measurement in a different waveguide<br />

has been performed to investigate possible differences. This time no amplification<br />

around 780 nm occurred as plotted in Figure 4.19. Furthermore at 800 nm a very<br />

sharp peak was excited (Figure 4.20). This peak bears no resemblance to the prior<br />

measurement and seems too narrow to result from phasematched SHG. One possible<br />

explanation is remaining pump light from the optical amplifier that pumps the OPA.<br />

This light around 800 nm may have seeded some SHG at this wavelength. Alternatively,<br />

phasematched SHG may not have occurred because of insufficient pump<br />

power. Given that we used another waveguide on the chip, it may also be possible<br />

50

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