Terahertz time-domain differentiator

• US 20040240060A1
• Filed: 02/18/2004
• Published: 12/02/2004
• Est. Priority Date: 08/27/2001
• Status: Abandoned Application

• Current Assignee: Rensselaer Polytechnic Institute
• Original Assignee: Rensselaer Polytechnic Institute
• Inventors: Stowe, Matthew C, Kersting, Roland I, Filin, Aleksey I
• Application Number:
  US10/487,204
• Publication Number:
  US 20040240060A1
• Time in Patent Office: Days
• US Class Current: 359/558
• CPC Class Codes: G01J 11/00 Measuring the characteristics of individual optical pulses or of optical pulse trains

Abstract

A device and method for differentiating an incident electromagnetic pulse. A conductive grating is provided with a sub-wavelength period, an area larger than the electromagnetic beam diameter, and a grating conductor thickness greater than the skin depth of the electromagnetic pulse. The grating conductors are oriented essentially parallel to the incident electromagnetic pulse to diffract the electromagnetic pulse. An aperture captures only the zero order diffraction of the electromagnetic pulse, which is the first time-derivative of the incident electromagnetic pulse.

Claims

1. A grating for diffraction of an incident electromagnetic wave, the grating comprising parallel conductors disposed on an optically transparent substrate to diffract the incident electromagnetic wave such that a zero order diffraction of the electromagnetic wave is the tine domain derivative of the incident electromagnetic wave when the conductors are oriented essentially parallel to the incident electromagnetic wave the electromagnetic wave having a wavelength and a skin depth in the conductors, the conductors having a period less than the wavelength, a thickness greater than the skin depth, and a length greater than the wavelength.

2. The grating of claim 1 wherein the electromagnetic wave has a frequency of greater than one terahertz.

3. The grating of claim 1 wherein the conductors comprise a pattern of metal lines formed on a transparent substrate.

4. The grating of claim 1 wherein the time domain derivative is provided without using an electrical current.

5. The grating of claim 1 wherein the period is less than the wavelength divided by the product of two and the natural log of two.

6. The grating of claim 5 wherein the incident electromagnetic wave comprises pulses having a center frequency corresponding to the wavelength, and the grating provides a spectral operational frequency range of between about 0.3 and 1.5 times the center frequency.

7. A time-domain differentiator comprising:

a signal source providing a polarized input electromagnetic wave having a wavelength a skin depth, and a beam diameter;

a grating having a grating face wit an area greater than the beam diameter and disposed to receive the polarized input electromagnetic wave incident the grating face and diffract the polarized input electromagnetic wave, providing a zero order diffraction, the grating face comprising parallel conductors having a period less than the wavelength and a thickness greater than the skin depth, the conductors being formed on an optically transparent substrate and oriented essentially parallel to the polarized input electromagnetic wave; and

an aperture sized and positioned to capture only the zero order diffraction of the diffracted polarized input electromagnetic wave, the zero order diffraction being an electromagnetic wave essentially equivalent to the time-domain derivative of the polarized input electromagnetic wave.

8. The time-domain differentiator of claim 7 wherein the electromagnetic wave has a frequency of greater than one terahertz.

9. The time-domain differentiator of claim 7 wherein the conductors comprise a pattern of metal lines formed on a transparent substrate,

10. The time-domain differentiator of claim 7 wherein the time-domain derivative is provided without using an electrical current.

11. The time-domain differentiator of claim 7 wherein the period is less than the wavelength divided by the product of two and the natural log of two.

12. The time-domain differentiator of claim 11 wherein the incident polarized input electromagnetic wave comprises pulses having a center frequency corresponding to the wavelength, and the grating provides a spectral operational frequency range of between about 0.3 and 1.5 times the center frequency.

13. A method for performing a time-domain differentiation of an electromagnetic pulse, comprising the steps of:

identifying an electromagnetic pulse to be differentiated, the pulse having a wavelength, a center frequency, a skin depth in a conductor, and a beam diameter;

providing a diffraction grating comprising spaced parallel conductive lines composed of the conductor, disposed on an optically transparent substrate, and having a period less than the wavelength, a thickness greater than the skin depth, an area greater than the beam diameter, and a length greater than the wavelength;

orienting the diffraction grating such that the electromagnetic pulse is incident to the diffraction grating and aligned with the conductive lines; and

capturing only the zero order diffraction of the incident electromagnetic pulse.

14. The method of claim 13 wherein the electromagnetic pulse has a frequency of greater than one terahertz.

15. The method of claim 13 wherein the conductors comprise a pattern of metal lines formed on a transparent substrate.

16. The method of claim 13 wherein the time-domain derivative is provided without using an electrical current.

17. The method of claim 13 wherein the period is less than the wavelength divided by the product of two and the natural log of two.

18. The method of claim 17 wherein the incident electromagnetic pulse comprises pulses having a center frequency corresponding to the wavelength, and the grating provides a spectral operational frequency range of between about 0.3 and 1.5 times the center frequency.