Pulsed light sources

• US 7,233,607 B2
• Filed: 05/03/2005
• Issued: 06/19/2007
• Est. Priority Date: 02/18/2002
• Status: Expired due to Fees

• Current Assignee: University of Southampton
• Original Assignee: University of Southampton
• Inventors: Lefort, Laurent, Nilsson, Lars Johan Albinsson, Ibsen, Morten, Richardson, David J, Price, Jonathan Hugh Vaughan, Malinowski, Andrew
• Primary Examiner(s): Rodriguez; Armando
• Application Number:
  US11/120,476
• Publication Number:
  US 20050190802A1
• Time in Patent Office: 777 Days
• Field of Search: 372/5, 372/25, 372/30
• US Class Current: 372/25
• CPC Class Codes: H01S 3/0057 Temporal shaping, e.g. pulse compression, frequency chirping soliton generation and propagation G02F1/3513, H01S3/063 and H01S3/108
• CPC Class Codes: H01S 3/0085 Modulating the output, i.e. the laser beam is modulated outside the laser cavity
• CPC Class Codes: H01S 3/0675 Resonators including a grating structure, e.g. distributed Bragg reflectors [DBR] or distributed feedback [DFB] fibre lasers
• CPC Class Codes: H01S 3/06754 Fibre amplifiers H01S3/06708 takes precedence
• CPC Class Codes: H01S 3/06791 Fibre ring lasers fibre laser gyrometers G01C19/72
• CPC Class Codes: H01S 3/1024 for pulse generation
• CPC Class Codes: H01S 3/1118 Semiconductor saturable absorbers, e.g. semiconductor saturable absorber mirrors [SESAMs]; Solid-state saturable absorbers, e.g. carbon nanotube [CNT] based
• CPC Class Codes: H01S 3/2316 Cascaded amplifiers

Abstract

A source of pulses of coherent radiation at a wavelength of approximately 1 μm, comprises a pump source for producing pump light; a laser cavity comprising an Yb³⁺-doped gain medium arranged to receive the pump light, the laser cavity being modelocked to generate laser pulses at a defined repetition rate; a pulse detector arranged to generate a pulse selection signal indicative of the repetition rate; a pulse selector arranged to reduce the repetition rate of the laser pulses responsive to the pulse selection signal from the pulse detector by passing only selected ones of the laser pulses; and at least one optical amplifier for amplifying the laser pulses of reduced repetition rate. The at least one optical amplifier can be configured for chirped or parabolic pulse amplification.

Claims

1. A source of pulses of coherent radiation at a wavelength of approximately 1 μ

m, comprising;

a pump source for producing pump light;

a laser cavity comprising an Yb³⁺-doped gain medium arranged to receive the pump light, the laser cavity being modelocked to generate laser pulses at a defined repetition rate;

a pulse detector arranged to generate a pulse selection signal indicative of the repetition rate;

a pulse selector arranged to reduce the repetition rate of the laser pulses responsive to the pulse selection signal from the pulse detector by passing only selected ones of the laser pulses; and

at least one optical amplifier for amplifying the laser pulses of reduced repetition rate.

2. The source of pulses of coherent radiation according to claim 1, in which the pulse selector comprises a lithium niobate integrated optical intensity modulator including a Mach-Zehnder interferometer.

3. The source of pulses of coherent radiation according to claim 1, in which the Yb³⁺-doped gain medium comprises a single mode optical fiber having a core, the pump light being coupled into the core.

4. The source of pulses of coherent radiation according to claim 1, in which the laser cavity has a Fabry-Perot design.

5. The source of pulses of coherent radiation according to claim 1, in which the laser cavity is modelocked by non-linear polarization rotation switching, and comprises a semiconductor saturable absorber mirror operable to initiate modelocking and a polarization selecting arrangement to polarize the light pulses and maintain the polarization while the light pulses are inside the cavity.

6. The source of pulses of coherent radiation according to claim 1, and further comprising an amplification system containing the at least one optical amplifier, the amplification system being operable to achieve chirped pulse amplification and comprising a pulse stretcher for increasing the duration of the pulses before passing them to the at least one optical amplifier for amplification, and a pulse compressor for decreasing the duration of the amplified pulses.

7. The source of pulses of coherent radiation according to claim 6, in which the pulse stretcher comprises a chirped fiber Bragg grating.

8. The source of pulses of coherent radiation according to claim 6, in which the pulse compressor comprises a pair of diffraction gratings.

9. The source of pulses of coherent radiation according to claim 6, in which the amplification system comprises at least two optical amplifiers arranged sequentially in a cascade.

10. The source of pulses of coherent radiation according to claim 1, and further comprising an amplification system containing the at least one optical amplifier, the amplification system being operable to achieve parabolic pulse amplification and comprising a pulse compressor which decreases the duration of the pulses after the pulses have been amplified by the at least one optical amplifier.

11. The source of pulses of coherent radiation according to claim 10, in which the pulse compressor comprises a pair of diffraction gratings.

12. The source of pulses of coherent radiation according to claim 1, in which the at least one optical amplifier comprises:

an amplifier pump source for producing amplifier pump light; and

an amplification medium comprising an optical fiber having a cladding and a core, the amplification medium being arranged to receive the amplifier pump light and the laser pulses.

13. The source of pulses of coherent radiation according to claim 12, further comprising at least a second optical amplifier arranged sequentially in a cascade with said at least one optical amplifier.

14. The source of pulses of coherent radiation according to claim 12, and further comprising at least one time gating device that is responsive to the pulse selection signal and arranged to allow radiation to pass from one optical amplifier to another in synchronicity with the pulse selection signal.

15. The source of pulses of coherent radiation according to claim 13, in which the cascade of optical amplifiers comprises at least one pre-amplifier followed by at least one power amplifier.

16. The source of pulses of coherent radiation according to claim 12, and further comprising an optical isolating device associated with the pump source and operable to protect the pump source from exposure to radiation generated in or reflected from other parts of the source of pulses of coherent radiation.

17. The source of pulses of coherent radiation according to claim 16, in which one or more of the at least one optical amplifiers further comprises an optical isolating device associated with the amplifier pump source and operable to protect the amplifier pump source from exposure to radiation generated in or reflected from the remainder of the source of coherent radiation.

18. The source of pulses of optical radiation according to claim 16, in which the or each optical isolating device comprises one or more wavelength division multiplexers configured to reflect radiation having a wavelength of approximately 1 μ

m.

19. The source of pulses of coherent radiation according to claim 1, and further comprising an optical isolating device associated with the pump source and operable to protect the pump source from exposure to radiation generated in or reflected from other parts of the source of pulses of coherent radiation.

20. The source of pulses of coherent radiation according to claim 19, in which one or more of the at least one optical amplifiers further comprises an optical isolating device associated with the amplifier pump source and operable to protect the amplifier pump source from exposure to radiation generated in or reflected from the remainder of the source of coherent radiation.

21. The source of pulses of optical radiation according to claim 19, in which the optical isolating device comprises one or more wavelength division multiplexers configured to reflect radiation having a wavelength of approximately 1 μ

m.

22. A method of generating pulses of coherent radiation at a wavelength of approximately 1 μ

m, comprising;

generating pulses having a defined repetition rate from a modelocked laser oscillator having an Yb³⁺-doped gain medium;

generating a pulse selection signal indicative of the pulse repetition rate;

activating a pulse selector with the pulse selection signal;

reducing the repetition rate of the pulses by passing the pulses through the activated pulse selector; and

amplifying the pulses by passing them through at least one optical amplifier.

23. The method of generating pulses of coherent radiation according to claim 22, in which the pulse selector comprises a lithium niobate integrated optical intensity modulator including a Mach-Zehnder interferometer.

24. A source of pulses of coherent radiation at a wavelength of approximately 1 μ

m, comprising;

means for producing pump light;

means for receiving the pump light and generating laser pulses at a defined repetition rate;

means for reducing the repetition rate of the generated laser pulses by selecting members of the laser pulses;

means for stretching the pulses of reduced repetition rate;

means for amplifying the laser pulses of reduced repetition rate; and

means for compressing the laser pulses of reduced repetition rate.

25. The source of pulses of coherent radiation according to claim 24, wherein the means for receiving the pump light includes a Yb³⁺-doped gain medium.

26. The source of pulses of coherent radiation according to claim 24, wherein the means for receiving the pump light includes an optical fiber.