Apparatus and methods using highly optically dispersive media
View Patent ↗According to the invention, a highly optically dispersive medium is one in which the absolute value of the group index of refraction of the medium is equal to or greater than four. An optical spectroscopic parameter detection and/or measurement apparatus may be in the form of an interferometer, a spectral interferometer, a spectrometer, a wavemeter, a tunable narrowband filter The embodied devices include a highly dispersive medium that appropriately can facilitate either a slow-light effect or a fast-light effect, which is disposed in a propagation path of an electro-magnetic (EM) input field and, a detector disposed in a manner to detect an output field resulting from the input filed interaction with the highly dispersive medium. Methods involve measuring a spectroscopic parameter using an optical spectroscopic parameter detection and/or measurement apparatus that incorporates a highly dispersive medium.
1. A spectroscopic parameter detection and/or measurement apparatus, comprising:
means for optically generating at least two parts of an input electromagnetic (EM) field and generating an output field;
a highly optically dispersive medium capable of supporting one of a slow-light and a fast-light optical phenomenon cooperatively engaged with said means; and
an output field detector component disposed along an output field propagation path of the apparatus.
2. The apparatus of claim 1 , wherein said means is a two-beam interferometer including an input field divider, a first arm providing a first input field propagation path, a second arm providing a second input field propagation path, an optical path length compensator disposed in at least one of the first and second propagation paths, and an input field combiner, wherein the highly dispersive medium is disposed in at least one of the first and second propagation paths.
3. The apparatus of claim 1 , wherein said means is a Mach-Zehnder interferometer.
4. The apparatus of claim 3 , wherein the highly dispersive medium is a slow-light medium.
5. The apparatus of claim 1 , wherein said means is a Michelson interferometer.
6. The apparatus of claim 5 , wherein the highly dispersive medium is a slow-light medium.
7. The apparatus of claim 1 , wherein said means is a Twyman-Green interferometer.
8. The apparatus of claim 7 , wherein the highly dispersive medium is a slow-light medium.
9. The apparatus of claim 1 , wherein the highly dispersive medium comprises a plurality of optically dispersive media including at least one highly optically dispersive medium.
10. The apparatus of claim 1 , wherein the highly dispersive medium is characterized by a group index of refraction, n g , where the absolute value of n g is equal to or greater than four.
11. The apparatus of claim 1 , wherein the highly dispersive medium is in the form of an atomic vapor.
12. The apparatus of claim 1 , wherein the highly dispersive medium is in the form of a wave-guiding fiber.
13. The apparatus of claim 1 , wherein the highly dispersive medium is in the form of a microstructure fiber.
14. The apparatus of claim 1 , wherein the highly dispersive medium is in the form of a solid media.
15. The apparatus of claim 1 , wherein the highly dispersive medium is in the form of an integrated lightwave structure.
16. The apparatus of claim 1 , wherein the highly dispersive medium is in the form of a liquid medium.
17. The apparatus of claim 1 , wherein the highly dispersive medium is in the form of a meta-material.
18. The apparatus of claim 1 , wherein the highly dispersive medium is in the form of a condensate.
19. The apparatus of claim 1 , wherein said means is a multiple-beam interferometer.
20. The apparatus of claim 19 , further comprising an output field imaging system disposed intermediate the highly dispersive medium and the detector component.
21. The apparatus of claim 19 , wherein said means is a Fabry-Perot interferometer.
22. The apparatus of claim 21 , wherein the highly dispersive medium is a slow-light medium.
23. The apparatus of claim 19 , wherein said means is a wedged shear interferometer.
24. The apparatus of claim 23 , wherein the highly dispersive medium is a slow-light medium.
25. The apparatus of claim 1 , wherein said means comprises a diffraction grating.
26. The apparatus of claim 25 , wherein the highly dispersive medium is disposed intermediate an exit surface of the diffraction grating and the detector component.
27. The apparatus of claim 25 , wherein the highly dispersive medium is a slow-light medium.
28. The apparatus of claim 25 , wherein the diffraction grating is a transmission grating.
29. The apparatus of claim 25 , wherein the diffraction grating is a reflection grating.
30. The apparatus of claim 25 , comprising a plurality of diffraction gratings.
31. The apparatus of claim 25 , wherein the diffraction grating is a non-periodic grating.
32. The apparatus of claim 1 , wherein the apparatus is a spectroscopic interferometer.
33. The apparatus of claim 1 , wherein the apparatus is a wavelength shift-measuring apparatus.
34. The apparatus of claim 1 , wherein the apparatus is a frequency shift-measuring apparatus.
35. The apparatus of claim 1 , wherein the apparatus is a tunable filter.
36. The apparatus of claim 1 , wherein the apparatus is a wavelength division multiplexer.
37. An improved two-beam spectroscopic interferometer, comprising a highly optically dispersive medium disposed in at least one input field propagation path of the interferometer.
38. The interferometer of claim 37 , wherein the highly optically dispersive medium is a slow-light medium characterized by a group index of refraction having a value that is equal to or greater than four.
39. The interferometer of claim 37 , wherein the highly optically dispersive medium is a fast-light medium characterized by a group index of refraction having a value that is equal to or less than negative four.
40. An improved multi-beam spectroscopic interferometer, comprising a highly optically dispersive medium disposed in an input field propagation path of the interferometer.
41. The interferometer of claim 40 , wherein the highly optically dispersive medium is a slow-light medium characterized by a group index of refraction having a value that is equal to or greater than four.
42. The interferometer of claim 40 , wherein the highly optically dispersive medium is a fast-light medium characterized by a group index of refraction having a value that is equal to or less than negative four.
43. The interferometer of claim 40 , comprising a Fabry-Perot etalon.
44. The interferometer of claim 40 , comprising a wedge-plate.
45. The interferometer of claim 40 , comprising a curved surface.
46. A method for measuring a spectroscopic parameter of an EM input field, comprising:
propagating the EM input field through a spectroscopic parameter measuring apparatus that includes a highly dispersive medium disposed in a propagation path of at least an optical component of the input field; and
detecting an EM output field generated by the interaction of the EM input field with the highly dispersive medium, wherein said output field presents an indicia of the spectroscopic parameter to be measured.
47. The method of claim 46 , comprising detecting an indicia of spectral resolution.
48. The method of claim 46 , comprising detecting an indicia of spectral bandwidth.
49. The method of claim 46 , comprising detecting an indicia of finesse.