IP Library Granted Patent US 10,175,111
Granted Patent B2
US 10,175,111 · App. 15/524,488 · Granted Jan 8, 2019

Method and apparatus for characterization of terahertz radiation

Inventors: Tsuneyuki Ozaki (Brossard, CA); Gargi Sharma (Brampton, CA); Kanwarpal Singh (Brampton, CA)
Assignee: Institut National de la Recherche Scientifique
G01J3/42G01J3/0218G01J3/0224
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Quick Facts
Patent No.
US 10,175,111
App. No.
15/524,488
Granted
Jan 8, 2019
Kind
B2
Abstract

A method for characterizing terahertz radiation using spectral domain interferometry, comprising overlapping a pump beam and a terahertz beam in a detecting crystal; obtaining two probe pulses by propagating the probe beam into a polarization maintaining single-mode optical fiber after the detecting crystal; and measuring a change in the optical path difference between the two probe pulses. The system comprises a detection crystal, where a terahertz pulse and a probe beam are made to overlap; a polarization-maintaining optical fiber propagating the probe beam after the detection crystal and outputting two probe pulses; and a spectrometer where the two probe pulses interfere.

Claims (36)

1. A method for characterizing terahertz radiation using spectral domain interferometry, comprising:

overlapping a probe beam and a terahertz beam in a detecting crystal;

obtaining two probe pulses by propagating the probe beam into a polarization maintaining single-mode optical fiber after the detecting crystal; and

measuring a change in the optical path difference between the two probe pulses.

2. The method of claim 1 , comprising, before said overlapping the probe beam and the terahertz beam in the detecting crystal:

splitting an input broadband light beam into the pump beam and the probe beam; and

using the pump beam to generate the terahertz beam in a terahertz source.

3. The method of claim 1 , comprising, before said propagating the probe beam into the polarization maintaining single-mode optical fiber, converting a linear polarization state of the probe beam to a circular polarization state.

4. The method of claim 1 , wherein the probe beam is coupled into the polarization-maintaining optical fiber, with a polarization direction thereof set along the birefringent axes of the polarization-maintaining optical fiber.

5. The method of claim 1 , to wherein said obtaining two probe pulses further comprises passing the two pulses exiting the polarization-maintaining optical fiber to a polarizer.

6. The method of claim 1 , to wherein said obtaining two probe pulses further comprises passing the two pulses exiting the polarization-maintaining optical fiber to a polarizer, the polarizer being positioned with a transmission axis thereof at 45° with respect to the birefringent axes of the polarization-maintaining optical fiber.

7. The method of claim 1 , wherein said measuring a change in the optical path difference between the two probe pulses comprises observing interferences between the two probe pulses.

8. The method of claim 1 , comprising, before said overlapping the probe beam and the terahertz beam in the detecting crystal:

splitting an input broadband light beam into the pump beam and the probe beam; and

using the pump beam to generate the terahertz beam in a terahertz source by one of: i) an optical method and ii) four-wave mixing.

9. The method of claim 1 , comprising, before said overlapping the probe beam and the terahertz beam in the detecting crystal:

splitting an input broadband light beam into the pump beam and the probe beam; and

using the pump beam to generate the terahertz beam in a THz source by optical rectification in a nonlinear crystal.

10. The method of claim 1 , further comprising delaying the probe beam.

11. A spectral domain interferometry system for characterizing terahertz radiation, comprising:

a detection crystal, where a terahertz pulse and a probe beam are made to overlap;

a polarization-maintaining optical fiber propagating the probe beam after said detection crystal and outputting two probe pulses; and

a spectrometer where the two probe pulses interfere.

12. The system of claim 11 , further comprising:

an input broadband light beam;

a beam splitter splitting said input beam into a pump beam and the probe beam; and

a terahertz source;

wherein the pump beam is used to generate the terahertz pulse in said terahertz source.

13. The system of claim 11 , further comprising a quarter-wave plate before said polarization-maintaining optical fiber to convert a linear polarization state of the probe beam to a circular polarization state.

14. The system of claim 11 , wherein a polarization direction of the probe beam is set along the birefringent axes of the polarization-maintaining optical fiber.

15. The system of claim 11 , further comprising a polarizer after said polarization-maintaining optical fiber.

16. The system of claim 11 , wherein said terahertz source is a non-linear crystal.

17. The system of claim 11 , wherein said terahertz source is one of: ZnTe, GaP and GaSe.

18. The system of claim 11 , wherein said terahertz source is a four-wave mixing unit.

19. The system of claim 11 , wherein said terahertz source is a non-linear crystal of a thickness in a range between 10 micrometers and 2 millimeters.

20. The system of claim 11 , further comprising an optical delay line used to match the probe beam in space and time with the terahertz pulse.

Assignments (3)
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 4, 2017
From: SHARMA, GARGI
To: INSTITUT NATIONAL DE LA RECHERCHE SCIENTIFIQUE
Reel/Frame 042242/0563 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 4, 2017
From: SINGH, KANWARPAL
To: INSTITUT NATIONAL DE LA RECHERCHE SCIENTIFIQUE
Reel/Frame 042242/0662 →
ASSIGNMENT OF ASSIGNOR'S INTEREST Recorded May 4, 2017
From: OZAKI, TSUNEYUKI
To: INSTITUT NATIONAL DE LA RECHERCHE SCIENTIFIQUE
Reel/Frame 042242/0774 →
Continuity (2)
Provisional Application 62076826 · Nov 7, 2014
Related Publication 20170336262A1 · Nov 23, 2017
Cited By (2)
US 12,474,262 US 12,687,489