Method and Apparatus for Detecting Ultra-Short Light Pulses of a Repetitive Light Pulse Signal, and for Determining the Pulse Width of the Light Pulses

• US 20080156964A1
• Filed: 03/30/2006
• Published: 07/03/2008
• Est. Priority Date: 03/30/2005
• Status: Abandoned Application

• Current Assignee: The Provost Fellows and Scholars of the College of the Holy and Undivided Trinity of Queen Elizabeth, near Dublin
• Original Assignee: The Provost Fellows and Scholars of the College of the Holy and Undivided Trinity of Queen Elizabeth, near Dublin
• Inventors: Guo, Wei-Hua, Lynch, Michael Andrew, Bradley, Ann Louise, Krug, Torsten, Donegan, John Francis
• Application Number:
  US11/910,060
• Publication Number:
  US 20080156964A1
• Time in Patent Office: Days
• US Class Current: 250/201.1
• CPC Class Codes: G01J 11/00 Measuring the characteristics of individual optical pulses or of optical pulse trains
• CPC Class Codes: G04F 13/026 Measuring duration of ultra-short light pulses, e.g. in the pico-second range; particular detecting devices therefor photometry, radiation pyrometry G01J1/00, G01J5/00; non-linear optics G02F1/35

Abstract

Apparatus for determining the pulse width of ultra-short light pulses of an input repetitive light pulse signal comprises a two-photon absorption detector (2) in the form of a microcavity (3) having an active region (4) located between top and bottom distributed Bragg reflectors (5,6). An optical fibre cable 16 directs the input light pulse signal combined with a reference repetitive light pulse signal normal to an incident surface (8) of the detector (2). The input light pulse signal is split in a polarisation light splitter (19) to form the reference light pulse signal which is passed through a delay line (23) to a polarisation light combiner (20) to be combined with the input light pulse signal, and directed at the incident surface (8) by the optical fibre cable (16). The delay line (23) is operated for alternately bringing the respective light pulses of the input and reference light pulse signals into and out of phase with each other to produce a pulsed photocurrent in the microcavity (3). A monitoring circuit (14) monitors the pulsed photocurrent, and the pulse width of the light pulses is determined as the full width half maximum of the pulsed photocurrent trace. By varying the angle of incidence at which the input and reference light pulse signals are incident on the incident surface (8), the apparatus is tuneable to input light pulse signals of different wavelengths within a predetermined range of wavelengths.

Claims

1-194. -194. (canceled)

195. Apparatus for determining the pulse width of light pulses of an input repetitive light pulse signal of repeating ultra-short light pulses, the apparatus comprising a two-photon absorption photodetector, the two-photon absorption photodetector being provided in the form of a microcavity comprising an active region and spaced apart first and second reflecting means between which the active region is located, and within which light resonates to produce a photocurrent as a result of the two-photon absorption effect, the active region and the first and second reflecting means being adapted so that the resonating lifetime of light in the microcavity is less than the pulse width of the light pulses, the pulse width of which is to be determined, a light directing means for directing the input repetitive light pulse signal into the microcavity for resonating therein, and for directing a reference repetitive light pulse signal of ultra-short repeating light pulses into the microcavity for resonating therein, and a means for progressively altering the phases relative to each other at which the light pulses of the respective input and reference light pulse signals enter the microcavity to produce a pulsed photocurrent from which the pulse width of the light pulses of the input light pulse signal is determined.

196. Apparatus as claimed in claim 195 in which the active region and the first and second reflecting means are adapted so that the resonating lifetime of light in the microcavity is in the range of 0.1 to 0.9 times the pulse width of the light pulses the pulse width of which is to be determined.

197. Apparatus as claimed in claim 196 in which the active region and the first and second reflecting means are adapted so that the resonating lifetime of light in the microcavity is in the range of 0.4 to 0.9 times the pulse width of the light pulses the pulse width of which is to be determined, and preferably, the active region and the first and second reflecting means are adapted so that the resonating lifetime of light in the microcavity is approximately 0.9 times the pulse width of the light pulses the pulse width of which is to be determined.

198. Apparatus as claimed in claim 195 in which the reflectivity of the second reflecting means is greater than the reflectivity of the first reflecting means, and preferably, the reflectivity of the first reflecting means is in the range of 0.05 to 0.99, and advantageously, the reflectivity of the first reflecting means is in the range of 0.6 to 0.99, and ideally, the reflectivity of the first reflecting means is approximately 0.95 for light pulses, the pulse width of which is to be determined of the order of one picosecond duration, and preferably, the reflectivity of the second reflecting means is in the range of 0.05 to 0.99, and advantageously, the reflectivity of the second reflecting means is in the range of 0.8 to 0.99, and ideally, the reflectivity of the second reflecting means is approximately 0.985.

199. Apparatus as claimed in claim 195 in which the first and second reflecting means are provided as first and second distributed Bragg reflectors, and preferably, the first distributed Bragg reflector comprises in the range of 1 to 15 mirror pairs, and advantageously, each mirror pair of the first distributed Bragg reflector comprises a silicon/silicon dioxide mirror pair, and ideally, each mirror pair of the first distributed Bragg reflector comprises a gallium arsenide/aluminium arsenide mirror pair.

200. Apparatus as claimed in claim 199 in which the second distributed Bragg reflector comprises in the range of 1 to 25 mirror pairs, and preferably, the second distributed Bragg reflector comprises approximately 15 mirror pairs, and advantageously, each mirror pair of the second distributed Bragg reflector comprises a gallium arsenide/aluminium arsenide mirror pair, and ideally, each mirror pair of the second distributed Bragg reflector comprises a silicon/silicon dioxide mirror pair.

201. Apparatus as claimed in claim 195 in which the perpendicular length between the first and second reflecting means of the active region is adapted to be a function of the wavelength of the light pulses, the pulse width of which is to be determined, and preferably, the perpendicular length between the first and second reflecting means of the active region is a fractional function of the wavelength of the light pulses, the pulse width of which is to be determined, and advantageously, the active region is of a material such that light of wavelength of the light pulses, the pulse width of which is to be determined resonates in the microcavity, and preferably, the active region is of a bulk semiconductor material, and preferably, the active region comprises at least one quantum well layer, and preferably, the active region comprises a plurality of barrier layers with a quantum well layer disposed between adjacent barrier layers, and advantageously, the material of each barrier layer is an alloy composition of aluminium and gallium arsenide, and preferably, the material of each quantum well layer is an alloy composition of aluminium and gallium arsenide.

202. Apparatus as claimed in claim 195 in which the first reflecting means defines an incident surface, and the light directing means is adapted for directing at least the input light pulse signal into the microcavity through the incident surface, and preferably, the light directing means is adapted for directing the reference light pulse signal into the microcavity through the incident surface, and advantageously, the reference light pulse signal is selected to be of wavelength similar to the wavelength of the input light pulse signal, and the light directing means is adapted for directing the input and reference light pulse signals at the incident surface at similar incident angles, alternatively, the reference light pulse signal is selected to be of wavelength different to the wavelength of the input light pulse signal, and the light directing means is adapted for directing the reference light pulse signal at the incident surface at an angle of incidence different to the angle of incidence at which the input light pulse signal is directed at the incident surface, and preferably, the light directing means is adapted for directing the input light pulse signal at the incident surface at an angle of incidence corresponding to the angle of incidence at which light of the wavelength of the input light pulse signal resonates in the microcavity, alternatively, the light directing means is adapted for directing the reference light pulse signal at the incident surface at an angle of incidence corresponding to the angle of incidence at which light of the wavelength of the reference light pulse signal resonates in the micro cavity.

203. Apparatus as claimed in claim 202 in which one of the two-photon absorption detector and the light directing means is moveable relative to the other for varying the angle of incidence at which at least the input light pulse signal is directed at the incident surface for facilitating tuning of the apparatus for determining the pulse width of light pulses of input light pulse signals of wavelengths within a predetermined range of wavelengths, and preferably, the two-photon absorption photodetector is adapted so that light of the highest wavelength of the predetermined range of wavelengths resonates in the microcavity when incident normal to the incident surface, and advantageously, the two-photon absorption photodetector is moveable relative to the light directing means, alternatively, the light directing means is moveable relative to the two-photon absorption photodetector.

204. Apparatus as claimed in claim 203 in which the light directing means comprises a first light directing means for directing the input light pulse signal at the incident surface, and preferably, the first light directing means is moveable relative to the two-photon absorption photodetector.

205. Apparatus as claimed in claim 204 in which the light directing means comprises a second light directing means for directing the reference light pulse signal at the incident surface independent of the first light directing means, and preferably, the second light directing means is moveable relative to the two-photon absorption photodetector, and advantageously, a monitoring means is provided for monitoring the angle of incidence at which the input light pulse signal is incident on the incident surface, and is responsive to the pulsed photocurrent and the angle of incidence at which the input light pulse signal is directed at the incident surface for determining the wavelength of the input light pulse signal.

206. Apparatus as claimed in claim 195 in which the means for progressively altering the phases relative to each other at which the light pulses of the respective input and reference light pulse signals enter the microcavity comprises a delay means, and one of the input and reference light pulse signals is passed through the delay means prior to being directed at the microcavity, and preferably, the delay means is a variable delay means for progressively varying the delay to which the one of the input and reference light pulse signals are subjected, and advantageously, the delay means comprises a delay line, and preferably, the delay line is a variable delay line, and advantageously, the reference light pulse signal is passed through the delay means, and preferably, a polarisation light combiner is provided for combining the input and reference light pulse signals prior to being directed into the microcavity, and advantageously, the reference light pulse signal is derived from the input light pulse signal, and preferably, a polarisation light splitter is provided for splitting the reference light pulse signal from the input light pulse signal, and advantageously, the reference light pulse signal is selected so that the pulse width of the light pulses thereof is similar to the pulse width of the light pulses of the input light pulse signal, and preferably, the reference light pulse signal is selected so that the repetition rate of the light pulses thereof is similar to the repetition rate of the light pulses of the input light pulse signal, and advantageously, the reference light pulse signal is selected so that the pulse width of the light pulses thereof is different to the pulse width of the light pulses of the input light pulse signal, and preferably, the reference light pulse signal is selected so that the repetition rate of the light pulses thereof is a multiple value or a fraction value of the repetition rate of the light pulses of the input light pulse signal.

207. Apparatus as claimed in claim 195 in which the apparatus is adapted for determining the pulse width of light pulses of pulse width not exceeding 500 picoseconds, and preferably, the apparatus is adapted for determining the pulse width of light pulses of pulse width not exceeding 100 picoseconds, and advantageously, the apparatus is adapted for determining the pulse width of light pulses of pulse width in the range of 10 femtoseconds to 100 picoseconds.

208. Apparatus as claimed in claim 195 in which a monitoring means is provided for monitoring the pulsed photocurrent and for determining the pulse width of the light pulses of the input light pulse signal from the monitored pulsed photocurrent, and preferably, the monitoring means is responsive to the full width half maximum of the peak value of the pulsed photocurrent for determining the pulse width of the light pulses of the input light pulse signal.

209. A method for determining the pulse width of light pulses of an input repetitive light pulse signal of repeating ultra-short light pulses, the method comprising providing a two-photon absorption detector in the form of a microcavity, whereby the microcavity comprises an active region and spaced apart first and second reflecting means between which the active region is located, and within which light resonates to produce a photocurrent as a result of the two-photon absorption effect, selecting the active region and the first and second reflecting means so that the resonating lifetime of light in the microcavity is less than the pulse width of the light pulses, the pulse width of which is to be determined, directing the input repetitive light pulse signal into the microcavity for resonating therein, directing a reference repetitive light pulse signal of ultra-short repeating light pulses into the microcavity for resonating therein, and progressively altering the phases relative to each other at which the light pulses of the respective input and reference light pulse signals enter the microcavity to produce a pulsed photocurrent from which the pulse width of the light pulses of the input light pulse signal is determined.

210. A photodetector device for detecting light of any one of a plurality of wavelengths within a predetermined range of wavelengths of an input light pulse of ultra-short duration, the photodetector device comprising a two-photon absorption detector comprising an active region within which incident light resonates to produce a detectable photocurrent as a result of the two-photon absorption effect, the two-photon absorption detector defining an incident surface for receiving incident light therethrough to the active region, and a light directing means for directing the input light pulse into the active region through the incident surface, one of the light directing means and the two-photon absorption detector being moveable relative to the other for varying the angle of incidence at which the input light pulse is incident on the incident surface for determining the wavelength of the input light pulse to which the photodetector device is responsive, so that when the light of the input light pulse contains light of the determined wavelength, the light of the input light pulse resonates in the active region to produce the detectable photocurrent.

211. A photodetector device as claimed in claim 210 in which the two-photon absorption detector is provided in the form of a microcavity comprising the active region located between spaced apart first and second reflecting means for reflecting light within the microcavity to resonate therein.

212. A photodetector device as claimed in claim 211 in which the microcavity is adapted so that light of the longest wavelength of the predetermined range of wavelengths when incident normal to the incident surface resonates within the microcavity, and preferably, the microcavity is adapted so that light of at least two wavelengths within the predetermined range of wavelengths when incident on the incident surface at similar incident angles resonates simultaneously within the microcavity, and advantageously, the first and second reflecting means are adapted for determining the wavelengths of light which resonate within the microcavity, and preferably, at least one of the first and second reflecting means comprises a distributed Bragg reflector comprising a plurality of spaced apart reflecting layers, and advantageously, the second reflecting means comprises a distributed Bragg reflector comprising at least one mirror pair, and advantageously, the first reflecting means comprises a distributed Bragg reflector comprising at least one mirror pair.

213. A photodetector device as claimed in claim 211 in which the perpendicular length between the first and second reflecting means of the active region is a function of the wavelength of light of the maximum wavelength of the predetermined range of wavelengths, and preferably, the perpendicular length between the first and second reflecting means of the active region is a fraction function of the wavelength of light of the maximum wavelength of the predetermined range of wavelengths, and advantageously, the perpendicular length between the first and second reflecting means of the active region is 458.9 nm, so that light of wavelength of 1,512 nm incident normal to the incident surface resonates in the microcavity.

214. A method for detecting light of any one of a plurality of wavelengths within a predetermined range of wavelengths of an input light pulse of ultra-short duration, the method comprising providing a two-photon absorption photodetector having an active region within which light resonates to produce a detectable photocurrent as a result of the two-photon absorption effect, the two-photon absorption detector defining an incident surface for receiving incident light therethrough to the active region, and providing a light directing means for directing the input light pulse into the active region through the incident surface, and moving one of the light directing means and the two-photon absorption detector relative to the other for varying the angle of incidence at which the input light pulse is incident on the incident surface for determining the wavelength of the input light pulse to which the photodetector device is responsive, so that when the input light pulse contains light of the determined wavelength, the input light pulse resonates in the active region to produce the detectable photocurrent.