Apparatus and method for the generation of high-power femtosecond pulses from a fiber amplifier
First Claim
1. An apparatus for generating high-power optical pulses, comprising:
- an optical source which generates signal light;
a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source,wherein pulse compression takes place in said nonlinear fiber amplifier; and
a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, said frequency converter providing the high-power optical pulses at an output thereof.
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Abstract
An apparatus generates femtosecond pulses from laser amplifiers by nonlinear frequency conversion. The implementation of nonlinear frequency-conversion allows the design of highly nonlinear amplifiers at a signal wavelength (SW), while still preserving a high-quality pulse at an approximately frequency-doubled wavelength (FDW). Nonlinear frequency-conversion also allows for limited wavelength tuning of the FDW. As an example, the output from a nonlinear fiber amplifier is frequency-converted. By controlling the polarization state in the nonlinear fiber amplifier and by operating in the soliton-supporting dispersion regime of the host glass, an efficient nonlinear pulse compression for the SW is obtained. The generated pulse width is optimized by utilizing soliton compression in the presence of the Raman-self-frequency shift in the nonlinear fiber amplifier at the SW. High-power pulses are obtained by employing fiber amplifiers with large core-diameters. The efficiency of the nonlinear fiber amplifier is optimized by using a double clad fiber (i.e., a fiber with a double-step refractive index profile) and by pumping light directly into the inner core of this fiber. Periodically poled LiNbO3 (PPLN) is used for efficient conversion of the SW to a FDW. The quality of the pulses at the FDW can further be improved by nonlinear frequency conversion of the compressed and Raman-shifted signal pulses at the SW. The use of Raman-shifting further increases the tuning range at the FDW. For applications in confocal microscopy, a special linear fiber amplifier is used.
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Citations
51 Claims
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1. An apparatus for generating high-power optical pulses, comprising:
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an optical source which generates signal light; a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source, wherein pulse compression takes place in said nonlinear fiber amplifier; and a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, said frequency converter providing the high-power optical pulses at an output thereof. - View Dependent Claims (2, 3, 4, 5, 6, 7, 8, 9, 12, 13, 14, 15, 16, 17, 18, 19, 20, 21, 22, 25, 26, 27)
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10. An apparatus for generating high-power optical pulses, comprising:
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an optical source which generates signal light; a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source; a fiber pulse compressor disposed to compress the optical pulses output from said nonlinear fiber amplifier; wherein the refractive index distribution of said pulse compressor is approximately invariant along the fiber length; and a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, said frequency converter providing the high-power optical pulses at an output thereof. - View Dependent Claims (11)
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23. An apparatus for generating high-power optical pulses, comprising:
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an optical source which generates signal light; a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source, wherein the amplifier fiber is a double-clad fiber, and wherein pump light and the signal light are launched into a core of the amplifier fiber; and a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, said frequency converter providing the high-power optical pulses at an output thereof.
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24. An apparatus for generating high-power optical pulses, comprising:
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an optical source which generates signal light; a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source, wherein said nonlinear amplifier comprises a multi-mode amplifier fiber, and wherein the signal light is predominantly launched into the fundamental mode of said multi-mode amplifier fiber; and a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, said frequency converter providing the high-power optical pulses at an output thereof.
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28. An apparatus for generating high-power optical pulses, comprising:
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an optical source which generates high power optical pulses; a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the high power pulses generated by said optical source; and a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, and which provides high-power optical pulses at a frequency-converted wavelength, wherein a spectral acceptance bandwidth of said frequency converter is smaller than an extent of the spectrum of the optical pulses from said optical source, and wherein said frequency converter converts energy from a portion of the spectrum of the optical pulses, from said optical source that is greater than the spectral acceptance bandwidth of said frequency converter, into the spectral acceptance bandwidth of said frequency converter. - View Dependent Claims (29)
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30. An apparatus for generating high-power optical pulses, comprising:
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an optical source which generates signal light; a fiber amplifier which receives the signal light generated by said optical source; a nonlinear fiber compressor which receives optical pulses produced by said amplifier, wherein the nonlinear fiber compressor has a refractive index distribution which is approximately invariant along the fiber length; and a periodically poled frequency converter which receives optical pulses compressed by said nonlinear fiber compressor and which produces the high-power optical pulses at a frequency-converted wavelength.
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31. An apparatus for generating high-power optical pulses, comprising:
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means for generating signal light; optical fiber means for nonlinearly amplifying the signal light; optical fiber means for pulse compressing the signal light, wherein the optical fiber means has a refractive index distribution which is approximately invariant along the fiber length; and means for frequency converting optical pulses produced by said means for nonlinearly amplifying and compressing, said means for frequency converting producing the high-power optical pulses at an output thereof. - View Dependent Claims (32, 33)
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34. A method for generating high-power optical pulses, comprising the steps of:
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generating a signal light; simultaneously nonlinearly amplifying and pulse compressing the signal light to produce amplified and pulse-compressed optical pulses; and frequency converting the amplified optical pulses to produce the high-power optical pulses at a different wavelength from the signal light. - View Dependent Claims (35, 36, 37)
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38. A method for generating high-power optical pulses, comprising the steps of:
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generating a signal light, nonlinearly amplifying the signal light to produce amplified optical pulses, wherein a double-clad fiber, pumped by an optical pumping means performs nonlinear amplification, further comprising the step of launching pump light and signal light directly into the inner core of said double-clad fiber, and frequency converting the amplified optical pulses to produce the high-power optical pulses at a different wavelength from the signal light.
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39. An apparatus for generating optical pulses, comprising:
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a fiber laser source for generating signal light; a multi-mode fiber amplifier for amplifying the signal light; means for preferentially launching a fundamental mode of said multi-mode amplifier, said multi-mode amplifier Raman-shifting said fundamental mode; and frequency conversion means for generating amplified output light at a doubled frequency.
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40. An apparatus for generating optical pulses, comprising:
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a pulse laser source for generating signal light; a multi-mode fiber amplifier for amplifying the signal light; means for preferentially launching a fundamental mode of said multi-mode amplifier, said multi-mode amplifier Raman-shifting said fundamental mode; and frequency conversion means for generating amplified output light.
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41. An apparatus for generating optical pulses, comprising:
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a pulse laser source for generating signal light; a multi-mode fiber amplifier for amplifying the signal light predominately in a fundamental mode thereof; a means for Raman-shifting said fundamental mode; and frequency conversion means for frequency-converting at least a Raman-shifted fundamental mode output of said multi-mode fiber amplifier.
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42. An apparatus for generating optical pulses, comprising:
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an optical source for generating signal light in the form of short optical pulses, and having an emission bandwidth; a nonlinear amplifier for amplifying the signal light; and a nonlinear frequency converting element having an acceptance bandwidth which is smaller than said emission bandwidth, and being capable of frequency-converting signal light within a bandwidth larger than said acceptance bandwidth.
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43. An apparatus for generating high-power optical pulses, comprising:
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a fiber laser source for generating signal light in the form of femtosecond regime optical pulses, and having a broad-band emission bandwidth; an amplifier for amplifying the signal light; and a nonlinear crystal having an acceptance bandwidth which is smaller than said broad-band emission bandwidth, and being capable of frequency-converting input light within a bandwidth larger than said acceptance bandwidth, for generating narrow-band frequency-converted light from broad-band signal light.
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44. An apparatus for generating high-power optical pulses, comprising:
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a fiber laser source for generating signal light in the form of broad-band femtosecond regime optical pulses; an amplifier for amplifying the signal light; and a nonlinear crystal for frequency converting said broad-band signal light into narrow-band frequency-converted light. - View Dependent Claims (45)
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46. An apparatus for generating optical pulses, comprising:
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an optical source for generating signal light in the form of short optical pulses, and having an emission bandwidth; an amplifier for amplifying the signal light; and a nonlinear element having a tunable acceptance bandwidth which is smaller than said emission bandwidth, and being capable of frequency-converting said signal light within a bandwidth larger than said acceptance bandwidth. - View Dependent Claims (47)
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48. An apparatus for generating optical pulses, comprising:
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an optical source for generating signal light in the form of short optical pulses, and having an emission bandwidth; a nonlinear frequency converting element having an acceptance bandwidth which is smaller than said emission bandwidth, and being capable of frequency-converting signal light within a bandwidth larger than said acceptance bandwidth.
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49. An apparatus for generating high-power optical pulses for use in two-photon confocal microscopy, comprising:
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an optical source which generates signal light; a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source, wherein pulse compression takes place in said nonlinear fiber amplifier, and said nonlinear fiber amplifier is a polarization maintaining fiber; and a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, said frequency converter providing the high-power optical pulses at an output thereof.
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50. An apparatus for generating high-power optical pulses for use in two-photon confocal microscopy, comprising:
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an optical source which generates signal light; a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source, wherein pulse compression takes place in said nonlinear fiber amplifier, and said nonlinear fiber amplifier is a contradirectionally pumped amplifier, and wherein the core diameter and the group-velocity are approximately constant along the amplifier length; and a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, said frequency converter providing the high-power optical pulses at an output thereof.
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51. An apparatus for generating ultra-short, high-power optical pulses, comprising:
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an optical source which generates signal light; a nonlinear fiber amplifier, having a nonlinear phase delay, which receives the signal light generated by said optical source, wherein pulse compression takes place in said nonlinear fiber amplifier; and a frequency converter which receives optical pulses output from said nonlinear fiber amplifier, said frequency converter providing the high-power optical pulses in Thz range at an output thereof for use in injection seeding of high-power amplifiers.
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Specification