Pulsed light sources

• US 6,917,631 B2
• Filed: 05/13/2002
• Issued: 07/12/2005
• 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): Harvey, Mingun Oh
• Assistant Examiner(s): Jackson, Cornelius H.
• Application Number:
  US10/146,219
• Publication Number:
  US 20030156605A1
• Time in Patent Office: 1,156 Days
• Field of Search: 372/5, 372/6, 372/10, 372/18, 359/25, 359/29.01, 359/30, 359/333
• US Class Current: 372/5
• 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 laser oscillator system operable to generate laser pulses at a defined repetition rate; and

a cascade of sequentially arranged optical amplifiers arranged to receive and amplify the laser pulses, each optical amplifier comprising an amplifier pump source for producing amplifier pump light and an amplification medium comprising Yb³⁺-doped optical fiber having a cladding and a core and arranged to receive the amplifier pump light and the laser pulses,

the cascade comprising a first pre-amplifier followed by a second pre-amplifier followed by a power amplifier,

the amplification media of the pre-amplifiers comprising single mode optical fibers arranged to receive amplifier pump light into the core of the optical fibers, each pre-amplifier further comprising a Yb³⁺-doped indirectly pumped optical fiber coupled to the optical fiber of its amplification medium to absorb amplified spontaneous emission arising from the amplification medium, and arranged so that it does not receive amplifier pump light, and

the amplification medium of the power amplifier comprising a large mode area optical fiber having an inner cladding and arranged to receive amplifier pump light into the inner cladding.

2. The source of pulses of coherent radiation according to claim 1, in which the amplifier pump source of each pre-amplifier comprises one of:

a master-oscillator-power-amplifier system (MOPA);

a high-brightness single mode diode laser;

or

an optical fiber-based laser.

3. The source of pulses of coherent radiation according to claim 1, in which the amplifier pump source of the power amplifier comprises a diode laser.

4. The source of pulses of coherent radiation according to claim 1, in which the pulses have an optical mode quality of substantially M²=1 after amplification in the cascade.

5. The source of pulses of coherent radiation according to claim 1, and further comprising a pulse detector arranged to generate a pulse selection signal indicative of the repetition rate, and 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.

6. The source of pulses of coherent radiation according to claim 1, in which each optical amplifier 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 other parts of the source of coherent radiation.

7. The source of pulses of optical radiation according to claim 6, 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.

8. The source of pulses of coherent radiation according to claim 1, and further comprising a pulse compressor which decreases the duration of the amplified pulses, the cascade of optical amplifiers being arranged to achieve parabolic pulse amplification.

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

10. The source of pulses of coherent radiation according to claim 1, in which the large mode area optical fiber of the power amplifier is provided with an asymmetry in cross-section to enhance coupling of the amplifier pump light received into the inner cladding from the inner cladding to the core.

11. The source of pulses of coherent radiation according to claim 10, in which the asymmetry arises from one or more generally flat sides provided on an outer surface of the inner cladding.

12. The source of pulses of coherent radiation according to claim 10, in which the asymmetry arises from the core being axially offset from a central axis of the inner cladding.

13. The source of pulses of coherent radiation according to claim 1, and further comprising a pulse stretcher which increases the duration of the pulses before passing them to the cascade of optical amplifiers, and a pulse compressor which decreases the duration of the amplified pulses, the cascade of optical amplifiers being arranged to achieve chirped pulse amplification.

14. The source of pulses of coherent radiation according to claim 13, in which the pulse stretcher comprises a chirped fiber Bragg grating.

15. The source of pulses of coherent radiation according to claim 13, in which the pulse compressor comprises a pair of diffraction gratings.

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

m, comprising;

means for generating laser pulses at a defined repetition rate; and

a cascade of sequentially arranged optical amplifiers arranged to receive and amplify the laser pulses, each optical amplifier comprising an amplifier pump source for producing amplifier pump light and an amplification medium comprising Yb³⁺-doped optical fiber having a cladding and a core and arranged to receive the amplifier pump light and the laser pulses,

the cascade comprising a first pre-amplifier followed by a second pre-amplifier followed by a power amplifier,

the amplification media of the pre-amplifiers comprising single mode optical fibers arranged to receive amplifier pump light into the core of the optical fibers, each pre-amplifier further comprising a Yb³⁺-doped indirectly pumped optical fiber coupled to the optical fiber of its amplification medium to absorb amplified spontaneous emission arising from the amplification medium, and arranged so that it does not receive amplifier pump light, and

the amplification medium of the power amplifier comprising a large mode area optical fiber having an inner cladding and arranged to receive pump light into the inner cladding.

17. 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

an optical amplifier for amplifying the laser pulses of reduced repetition rate, said optical amplifier, said optical amplifier comprising,

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 and wherein said amplifier is arranged sequentially in a cascade comprising a first pre-amplifier followed by a second pre-amplifier followed by a power amplifier.

18. The source of pulses of coherent radiation according to claim 17, in which the amplification media of the first pre-amplifier and the second pre-amplifier comprise Yb³⁺-doped optical fiber.

19. The source of pulses of coherent radiation according to claim 17, in which the amplification media of the first pre-amplifier and the second pre-amplifier are comprise respective sections of single mode optical fibers.

20. The source of pulses of coherent radiation according to claim 17, in which the optical fibers of the amplification media of the first pre-amplifier and the second pre-amplifier are arranged to receive amplifier pump into the cores of the optical fibers.

21. The source of pulses of coherent radiation according to claim 17, in which each pre-amplifier further comprises a Yb³⁺-doped indirectly pumped optical fiber coupled to the optical fiber of its amplification medium to absorb amplified spontaneous emission arising from the amplification medium, and arranged so that it does not receive amplifier pump light.

22. The source of pulses of coherent radiation according to claim 17, in which the amplifier pump source of each pre-amplifier comprises one of:

a master-oscillator-power-amplifier system (MOPA);

a high-brightness single mode diode laser;

or

an optical fiber-based laser.

23. The source of pulses of coherent radiation according to claim 17, in which the amplification medium of the power amplifier comprises a Yb³⁺-doped large mode area optical fiber having a core and an inner cladding.

24. The source of pulses of coherent radiation according to claim 23, in which the amplifier pump source of the power amplifier comprises a diode laser.

25. The source of pulses of coherent radiation according to claim 23, in which the pulses have an optical mode quality of substantially M²1 after amplification in the power amplifier.

26. The source of pulses of coherent radiation according to claim 23, in which the large mode area fiber of the power amplifier is arranged to receive amplifier pump light into its inner cladding.

27. The source of pulses of coherent radiation according to claim 26, in which the large mode area optical fiber of the power amplifier is provided with an asymmetry in cross-section which acts to enhance coupling of the amplifier pump light received into the inner cladding from the inner cladding to the core.

28. The source of pulses of coherent radiation according to claim 27, in which the asymmetry arises from one or more generally flat sides provided on an outer surface of the inner cladding.

29. The source of pulses of coherent radiation according to claim 27, in which the asymmetry arises from the core being axially offset from a central longitudinal axis of the inner cladding.