AUTOMATED DISPERSION COMPENSATION OVER A BROAD WAVELENGTH RANGE FOR COHERENT OPTICAL PULSES
The present application is directed to an apparatus and method for the automated compensation of dispersion over a broad wavelength range for coherent optical pulses. In one embodiment, the present application discloses an automatic dispersion compensating optical apparatus configured to change chirp introduced into an optical signal by an optical system in optical communication with the dispersion compensating optical apparatus and includes at least one wavelength-tunable source of coherent optical pulses configured to output at least one optical signal, at least one dispersion compensation device configured to receive the optical signal from the coherent source, and at least one controller in communication with the dispersion compensation device and configured to adjust chirp introduced into the optical signal by the dispersion compensation device as the wavelength of the optical signal is varied.
The present application is a continuation application of U.S. patent application Ser. No. 11/983,583, filed on Nov. 9, 2007, which claims priority to U.S. Provisional Patent Application Ser. No. 60/857, 871, filed Nov. 9, 2006, the contents of which are hereby incorporated by reference in their entirety herein.
BACKGROUNDSources of coherent optical pulses, such as lasers, optical parametric oscillators and amplifiers, etc., configured to produce outputs having very high peak intensities are used in a number of research applications. Such sources are commonly used in applications that include multi-photon microscopy, materials testing, and nonlinear spectroscopy. Many of these applications require high peak intensities and pulsewidths in the sub-picosecond pulse duration regime.
Typically, these sources of coherent optical pulses are used in conjunction with an optical system comprised of one or more optical components, including, without limitation, lenses, mirrors, modulators, acousto-optical modulators, optical crystals, etalons, gratings, optical fibers, and the like. The coherent optical pulses may propagate through a variety of materials, including, without limitation, air, glass, optical coatings applied to one or more optical devices, and the like. The amount of time required for the light to propagate through various optical components often varies as a function of wavelength, this property of optical components is called dispersion. As a result, a chirp may be introduced in the pulsed optical signal propagating through these components, i.e. different wavelength components are shifted in time within the pulse. As such, the pulse duration of the optical pulse becomes longer. Dispersion of an optical component is positive when longer wavelength light travels faster through the optical component than shorter wavelength light. If an optical pulse passes through an optical component with positive dispersion, the pulse becomes positively chirped, i.e. longer wavelength components are ahead of shorter wavelength components within the pulse. In ultra short coherent optical pulse applications (e.g. sub-picosecond and femtosecond) the high peak intensity optical pulse may be substantially degraded during its propagation through the optical system. For example, the peak intensity may be drastically reduced as the pulsewidth increases. Higher order distortion of the pulses is also common.
In response thereto, commonly a dispersion compensator may be positioned within the optical system. Typically, the dispersion compensator is configured to produce a dispersion of an opposite sign to the dispersion of the optical system and, ideally, of the same absolute value. For example, if the optical components within the optical system have positive dispersion and therefore introduce positive chirp into the optical signal, the dispersion compensator is configured to have negative dispersion and introduce negative chirp into the optical signal, thereby negating the positive dispersion of the optical system. Therefore, the pulsewidth in the output of the optical system is short again. While this approach has proven somewhat successful in the past, a number of shortcomings have been identified. For example, dispersion of both the optical system and the dispersion compensator changes significantly with pulse wavelength and not in the same manner. As such, applications requiring wide wavelength ranges require extensive tuning processes to produce compressed pulses over the full wavelength range of the optical system. These tuning processes tend to be time-consuming manual endeavors. Further, these tuning processes may need to be repeated frequently.
In light of the foregoing, there is an ongoing need for a system and method for automatically compensating for the dispersion for coherent optical pulses over a broad range of wavelengths.
SUMMARYThe present application is directed to an apparatus and method for the automated compensation of dispersion over a broad wavelength range for coherent optical pulses. In one embodiment, the present application discloses an automatic dispersion compensating optical apparatus configured to change chirp introduced into an optical signal by an optical system in optical communication with the dispersion compensating optical apparatus and includes at least optical parametric oscillator configured to output at least one optical signal, at least one dispersion compensation device configured to receive the optical signal from the optical parametric oscillator, and at least one controller in communication with the dispersion compensation device and configured to adjust chirp introduced into the optical signal by the dispersion compensation device as the wavelength of the optical signal is varied.
In another embodiment, the present application is directed to a method of automatically adjusting chirp of at least one optical signal to the desired value as the signal propagates through an optical system and includes providing a dispersion compensation device having at least one controller in communication therewith, directing at least one optical signal from an optical parametric oscillator into the dispersion compensation device, sending a control signal from the controller to the dispersion compensation device to automatically adjust the dispersion compensation device to introduce the desired chirp into the optical signal as the wavelength of the signal is tuned, and outputting the optical signal into an optical system in optical communication with the dispersion compensation device.
Other features and advantages of the embodiments of the apparatus and method for the automated compensation of dispersion over a broad wavelength range for coherent optical pulses as disclosed herein will become apparent from a consideration of the following detailed description.
Various embodiments of apparatus and method for the automated compensation of dispersion over a broad wavelength range for coherent optical pulses will be explained in more detail by way of the accompanying drawings, wherein:
Referring again to
In one embodiment, the dispersion compensation device 14 may be configured to introduce desired negative or positive chirp into the output optical signal 20 shown in
As shown in
Referring again to
In one embodiment the dispersion compensating optical apparatus 10 optionally may include one or more sensors 26 therein. For example, in one embodiment, the dispersion compensating optical apparatus 10 may include a first sensor 26 and at least a second sensor 26′. The first sensor 26, the second sensor 26′, or both may be configured to measure any variety of optical characteristics, including, without limitation, wavelength, pulse energy, repetition rate, pulse width, peak intensity fluorescence intensity, multi-photon fluorescence intensity, SHG intensity, 2-photon absorption, and multi-photon absorption and the like, In one embodiment, the first sensor 26 and the second sensor 26′ are configured to measure different optical characteristics of the dispersion compensated output signal 24. For example, the first sensor 26 may be configured to measure pulse width, pulse chirp, and/or peak intensity of the dispersion compensated output signal 24 while the second sensor 26′ is configured to measure the wavelength thereof. In an alternate embodiment, the first and second sensors 26, 26′ are configured to measure the same optical characteristics. Further, additional sensors may be positioned within the dispersion compensating optical apparatus 10 and the optical system 22. Similarly, the first and second sensors 26, 26′ may be positioned anywhere within the dispersion compensating optical apparatus 10 and the optical system 22.
Referring again to
In another embodiment, the first sensor 26 is used to characterize the beam in means of pulse width, pulse chirp, or peak intensity. For at least one wavelength, the user adjusts the controller 18 to change the configuration of the dispersion compensation device 14 to optimize the signal at the sensor 26. This value is stored as one configuration in a table within the controller 18. This procedure may be repeated for other wavelengths. After calibration the dispersion compensating apparatus 10 at one or more wavelengths the sensor 26 may be removed from the apparatus 10. All table entries may be used to calculate the configuration of the dispersion compensation device 14 for all other accessible wavelengths. The wavelength information may be received by the controller 18 from the coherent source 12, the second sensor 26′, or from an external source.
Claims
1-28. (canceled)
29. An automatic dispersion compensating optical apparatus configured to change the chirp introduced into an optical signal in optical communication with the dispersion compensating optical apparatus, comprising:
- at least one wavelength-tunable optical parametric oscillator configured to output at least one optical signal;
- at least one dispersion compensation device configured to receive the optical signal from the optical parametric oscillator; and
- at least one controller in communication with the dispersion compensation device and configured to adjust a chirp introduced into the optical signal by the dispersion compensation device as the wavelength of the optical signal is varied.
30. The apparatus of claim 29 wherein the wavelength of the optical signal is tunable over a range of wavelengths from about 300 nm to about 3000 nm.
31. The apparatus of claim 29 wherein the wavelength of the optical signal is tunable over a range of wavelengths from about 500 nm to about 1500 nm.
32. The apparatus of claim 29 wherein the wavelength of the optical signal is tunable over a range of wavelengths from about 600 nm to about 1300 nm.
33. The apparatus of claim 29 wherein the dispersion compensation device includes at least one optical element adjustably positioned therein.
34. The apparatus of claim 33 wherein the optical element is selected from the group consisting of prisms, gratings, etalons, chirp mirrors, spatial light modulators, lenses, optical mounts, optical stages, optical fibers, bulk materials, motors, actuators, and Gires Tournois interferometers.
35. The apparatus of claim 33 wherein the controller is in communication with the optical element.
36. The apparatus of claim 29 wherein the dispersion compensation device has a throughput of greater than about 70%.
37. The apparatus of claim 29 wherein the dispersion compensation device has a throughput of greater than about 80%.
38. The apparatus of claim 29, wherein the optical parametric oscillator generates optical signals having a pulsewidth of less than about one picosecond.
39. The apparatus of claim 29 wherein the controller is in communication with the optical parametric oscillator and configured to adjust and monitor at least one of the wavelength, pulse energy, pulse peak intensity, pulse repetition rate, and pulse width of the optical signal.
40. The apparatus of claim 29 wherein the controller includes at least one storage device therein.
41. The apparatus of claim 40 wherein the storage device is configured to store at least one table containing dispersion characteristics of at least one optical system in communication with the optical parametric oscillator.
42. The apparatus of claim 41 wherein the table is configured to be provided by a user to the storage device.
43. The apparatus of claim 41 wherein the table is pre-loaded onto the storage device.
44. The apparatus of claim 41 wherein the table is configured to be calculated within the controller from information received from at least one of a user, the optical parametric oscillator, the optical system in communication with the optical parametric oscillator, and at least one sensor in communication with the optical parametric oscillator.
45. The apparatus of claim 29 wherein the optical system is selected from the group consisting of telescopes, microscopes, lenses, mirrors, beam splitters, spatial filters, attenuators, beam profilers, gratings, etalons, acousto-optical devices, modulators, optical crystals and fibers.
46. The apparatus of claim 29 further comprising at least one sensor in communication with at least one of the optical parametric oscillator, the controller, dispersion compensation device, and the optical system, the sensor configured to measure at least one optical characteristic of the optical signal.
47. The apparatus of claim 46 wherein the sensor is configured to measure at least one optical characteristic of the optical signal, the optical characteristics selected from the group consisting of wavelength, pulse energy, repetition rate, pulse width, peak intensity, fluorescence intensity, multi-photon fluorescence intensity, SHG intensity, 2-photon absorption, and multi-photon absorption.
48. The apparatus of claim 29, wherein the optical dispersion compensation device is configured to adjust at least one dispersion type selected from the group consisting of second order dispersion (GDD: group delay dispersion), third order dispersion, fourth order dispersion, fifth order dispersion, positive dispersion, negative dispersion, and positive and negative dispersion.
49. A method of automatically adjusting chirp of at least one optical signal to the desired value as the signal propagates through an optical system, comprising:
- providing at least one dispersion compensation device having at least one controller in communication therewith;
- directing at least one optical signal from at least one tunable optical parametric oscillator into the dispersion compensation device;
- sending at least one control signal from the controller to the dispersion compensation device to automatically adjust the dispersion compensation device to introduce the desired chirp into the optical signal as the wavelength of the signal is tuned; and
- outputting the optical signal into at least one optical system in optical communication with the dispersion compensation device.
50. The method of 49 further comprising:
- storing at least one table of the dispersion characteristics of the optical system at one or more wavelengths within a storage device located within the controller;
- accessing the table stored in the storage device of the controller; and
- adjusting the dispersion compensation device using the table data to a desired value of chirp introduced into the optical signal as the wavelength is tuned.
51. The method of claim 49 further comprising calculating with the controller the dispersion of the optical system at a variety wavelengths based on the dispersion at one ore more other wavelengths.
52. The method of claim 51 further comprising loading a dispersion characteristics table into the storage device of the controller.
53. The method of claim 51 further comprising:
- providing at least one sensor in optical communication with the optical parametric oscillator;
- generating at least one dispersion characteristics table within the controller based on the data measured by the sensor; and
- adjusting the dispersion compensation device to change chirp introduced into the optical signal by the optical system as the wavelength is tuned based on the generated table.
54. The method of claim 53 further comprising measuring at least one of the wavelength, pulse energy, repetition rate, pulse width, peak intensity or any nonlinear peak-intensity-dependent signal, fluorescence intensity, multi-photon fluorescence intensity, SHG intensity, 2-photon absorption, and multi-photon absorption with the sensor.
55. The method of 49 further comprising:
- providing at least one sensor in communication with the optical system and the controller;
- sending data measured by the sensor to the controller; and
- adjusting the dispersion compensation device to optimize at least one parameter of an optical signal propagating through the optical system and measured by the sensor.
56. The method of claim 55 further comprising optimizing at least one of the pulse width, pulse energy, peak intensity or any nonlinear peak-intensity-dependent signal, fluorescence intensity, multi-photon fluorescence intensity, SHG intensity, 2-photon absorption, and multi-photon absorption.
Type: Application
Filed: May 19, 2011
Publication Date: Dec 22, 2011
Inventors: Dmitri A. Oulianov (Mountain View, CA), Stefan Marzenell (Sunnyvale, CA), Richard Boggy (Sunnyvale, CA)
Application Number: 13/111,810
International Classification: H04B 10/00 (20060101);