3.3 Comparison of Rotatable Polarisation to Projection via Wire-Grid Polarisers
53
Fig. 3.5 Polarisation-resolved time-domain waveforms of THz pulses generated at a ψ em = 0 ◦ , b
ψ em = 40 ◦ , c ψ em = 90 ◦ , d ψ em = 130 ◦ , and e ψ em = 180 ◦ . f Ellipticity and g orientation angle
of the THz pulses as the emitter is rotated in 2.5 ◦ steps over a 180 ◦ rotation
53
Fig. 3.5 Polarisation-resolved time-domain waveforms of THz pulses generated at a ψ em = 0 ◦ , b
ψ em = 40 ◦ , c ψ em = 90 ◦ , d ψ em = 130 ◦ , and e ψ em = 180 ◦ . f Ellipticity and g orientation angle
of the THz pulses as the emitter is rotated in 2.5 ◦ steps over a 180 ◦ rotation