Home Publications Presentations Tutorials Images Animations Group Members Diversions Links |
Shaping of a Terahertz Pulse
|
![]() |
Here, the screen thickness of the filter is much less than the slit width, so the filtering results from the longer wavelengths diffracting more severely after the pulse leaves the filter.
The adjustable slit filter was formed between the edges of two razor blades oriented parallel to the direction of polarization of the THz pulse. The slit width shown above was 0.5 mm. The filter was 10 cm from the emitter, ensuring an approximately planar wavefront over the slit widths of interest.
To verify our experimental findings, we numerically simulated the propagation of the THz pulse through the slit using the Finite - Difference Time - Domain method (FDTD). To facilitate direct comparison of experiments and simulations, we used actual experimental parameters together with the measured input field as the starting point for these simulations.
Terahertz pulses have become important to the atomic physics community because they provide an ultra-short, single-directional "kick" to the atoms with which they interact.
More information on the diffraction of terahertz radiation by an aperture can be found
in the papers:
Spatiotemporal shaping of terahertz pulses
Jake Bromage, Stojan Radic, G. P. Agrawal, C. R. Stroud, Jr.,
P. M. Fauchet, and Roman Sobolewski
Opt. Lett. 22, 627 (1997).
Spatiotemporal shaping of half-cycle terahertz pulses
by diffraction through conductive apertures of finite thickness
Jake Bromage, Stojan Radic, G. P. Agrawal, C. R. Stroud, Jr.,
P. M. Fauchet, and Roman Sobolewski.
JOSA B 15, 1953 (1998).
|
Previous Animation: Fractional Revival of High Momentum Wave Packet In a Square Well |
Animations |
Next Animation: Shaping a THZ pulse by a thick screen |


