151
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Margolis HS. Spectroscopic applications of femtosecond optical frequency combs. Chem Soc Rev 2012; 41:5174-84. [PMID: 22722917 DOI: 10.1039/c2cs35163c] [Citation(s) in RCA: 11] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/21/2022]
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152
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Ishizawa A, Nishikawa T, Mizutori A, Takara H, Nakano H, Sogawa T, Takada A, Koga M. Generation of 120-fs laser pulses at 1-GHz repetition rate derived from continuous wave laser diode. OPTICS EXPRESS 2011; 19:22402-22409. [PMID: 22109116 DOI: 10.1364/oe.19.022402] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/31/2023]
Abstract
We report the first demonstration of continuous-wave laser diode based 100-fs-class pulse lasers operating at a gigahertz repetition rate without a mode-locking technique. We describe the performance of a 1-W, 120-fs optical pulse train at 1 GHz and a 1-W, 80-fs optical pulse train at 250 MHz by using a simple configuration. Sub-100-fs pulse durations are achieved by using a progressive expansion of the spectrum in the self-phase modulation process in an erbium-doped fibre amplifier. Our scheme can achieve continuously tunable repetition rate in the range of ± 20%, and develop powerful tools for use in nanomechanical systems and nanobiotechnology.
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Affiliation(s)
- Atsushi Ishizawa
- NTT Basic Research Laboratories, NTT Corporation, 3-1 Morinosato Wakamiya, Atsugi, Kanagawa 243-0198, Japan.
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153
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Moon HS, Ryu HY, Lee SH, Suh HS. Precision spectroscopy of Rb atoms using single comb-line selected from fiber optical frequency comb. OPTICS EXPRESS 2011; 19:15855-15863. [PMID: 21934948 DOI: 10.1364/oe.19.015855] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/31/2023]
Abstract
We demonstrated the selection of a single comb-line from an optical frequency comb (OFC) of a mode-locked femtosecond fiber laser with a 250 MHz pulse repetition rate, and applied for precision spectroscopy of Rb atoms at 1529 nm. The single comb-line was selected from the fiber-OFC with a 1.5 GHz mode-spacing using spectral-mode-filtering and femtosecond laser injection-locking. When the repetition rate of the mode-locked femtosecond fiber laser was scanned over the range of 382.6 Hz at 250 MHz, we observed the double-resonance optical pumping spectra of the 5S(1/2)-5P(3/2)-4D(3/2) transition of Rb atoms using the selected comb-line of an OFC scanned over the range of 300 MHz at 196,037,213.8 MHz.
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Affiliation(s)
- Han Seb Moon
- Department of Physics, Pusan National University, Busan 609-735, Korea.
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154
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Stark SP, Steinmetz T, Probst RA, Hundertmark H, Wilken T, Hänsch TW, Udem T, Russell PSJ, Holzwarth R. 14 GHz visible supercontinuum generation: calibration sources for astronomical spectrographs. OPTICS EXPRESS 2011; 19:15690-15695. [PMID: 21934930 DOI: 10.1364/oe.19.015690] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/31/2023]
Abstract
We report the use of a specially designed tapered photonic crystal fiber to produce a broadband optical spectrum covering the visible spectral range. The pump source is a frequency doubled Yb fiber laser operating at a repetition rate of 14 GHz and emitting sub-5 pJ pulses. We experimentally determine the optimum core diameter and achieve a 235 nm broad spectrum. Numerical simulations are used to identify the underlying mechanisms and explain spectral features. The high repetition rate makes this system a promising candidate for precision calibration of astronomical spectrographs.
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Affiliation(s)
- S P Stark
- Max Planck Institut for the Science of Light, Guenther-Scharowsky Str. 1, D-91058 Erlangen, Germany.
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155
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Del'Haye P, Herr T, Gavartin E, Gorodetsky ML, Holzwarth R, Kippenberg TJ. Octave spanning tunable frequency comb from a microresonator. PHYSICAL REVIEW LETTERS 2011; 107:063901. [PMID: 21902324 DOI: 10.1103/physrevlett.107.063901] [Citation(s) in RCA: 33] [Impact Index Per Article: 2.4] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/24/2011] [Indexed: 05/31/2023]
Abstract
We report the generation of an octave-spanning optical frequency comb in a continuous wave laser pumped microresonator. The generated comb spectrum covers the wavelength range from 990 to 2170 nm without relying on additional external broadening. Continuous tunability of the generated frequency comb over more than an entire free spectral range is demonstrated. Moreover, the linewidth of individual optical comb components and its relation to the pump laser phase noise is studied. The ability to derive octave-spanning spectra from microresonator comb generators represents a key step towards f-2f self-referencing of microresonator-based optical frequency combs.
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Affiliation(s)
- P Del'Haye
- Max-Planck-Institut für Quantenoptik, Garching, Germany
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156
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Foster MA, Levy JS, Kuzucu O, Saha K, Lipson M, Gaeta AL. Silicon-based monolithic optical frequency comb source. OPTICS EXPRESS 2011; 19:14233-14239. [PMID: 21934787 DOI: 10.1364/oe.19.014233] [Citation(s) in RCA: 16] [Impact Index Per Article: 1.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/31/2023]
Abstract
We demonstrate the generation of broad-bandwidth optical frequency combs from a CMOS-compatible integrated microresonator. We characterize the comb quality using a novel self-referencing method and verify that the comb line frequencies are equidistant over a bandwidth of 115 nm (14.5 THz), which is nearly an order of magnitude larger than previous measurements.
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Affiliation(s)
- Mark A Foster
- School of Applied and Engineering Physics, 160 Clark Hall, Cornell University, Ithaca, New York 14853, USA
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157
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Abstract
The series of precisely spaced, sharp spectral lines that form an optical frequency comb is enabling unprecedented measurement capabilities and new applications in a wide range of topics that include precision spectroscopy, atomic clocks, ultracold gases, and molecular fingerprinting. A new optical frequency comb generation principle has emerged that uses parametric frequency conversion in high resonance quality factor (Q) microresonators. This approach provides access to high repetition rates in the range of 10 to 1000 gigahertz through compact, chip-scale integration, permitting an increased number of comb applications, such as in astronomy, microwave photonics, or telecommunications. We review this emerging area and discuss opportunities that it presents for novel technologies as well as for fundamental science.
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Affiliation(s)
- T J Kippenberg
- Swiss Federal Institute of Technology Lausanne (EPFL), Lausanne, CH-1015, Switzerland.
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158
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Uzan JP. Varying Constants, Gravitation and Cosmology. LIVING REVIEWS IN RELATIVITY 2011; 14:2. [PMID: 28179829 PMCID: PMC5256069 DOI: 10.12942/lrr-2011-2] [Citation(s) in RCA: 83] [Impact Index Per Article: 5.9] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Accepted: 03/23/2011] [Indexed: 05/27/2023]
Abstract
Fundamental constants are a cornerstone of our physical laws. Any constant varying in space and/or time would reflect the existence of an almost massless field that couples to matter. This will induce a violation of the universality of free fall. Thus, it is of utmost importance for our understanding of gravity and of the domain of validity of general relativity to test for their constancy. We detail the relations between the constants, the tests of the local position invariance and of the universality of free fall. We then review the main experimental and observational constraints that have been obtained from atomic clocks, the Oklo phenomenon, solar system observations, meteorite dating, quasar absorption spectra, stellar physics, pulsar timing, the cosmic microwave background and big bang nucleosynthesis. At each step we describe the basics of each system, its dependence with respect to the constants, the known systematic effects and the most recent constraints that have been obtained. We then describe the main theoretical frameworks in which the low-energy constants may actually be varying and we focus on the unification mechanisms and the relations between the variation of different constants. To finish, we discuss the more speculative possibility of understanding their numerical values and the apparent fine-tuning that they confront us with.
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Affiliation(s)
- Jean-Philippe Uzan
- Institut d’Astrophysique de Paris, UMR-7095 du CNRS, Université Pierre et Marie Curie, 98 bis bd Arago, 75014 Paris, France
- Department of Mathematics and Applied Mathematics, Cape Town University, Rondebosch, 7701 South Africa
- National Institute for Theoretical Physics (NITheP), Stellenbosch, 7600 South Africa
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159
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Chang G, Chen LJ, Kärtner FX. Fiber-optic Cherenkov radiation in the few-cycle regime. OPTICS EXPRESS 2011; 19:6635-6647. [PMID: 21451691 DOI: 10.1364/oe.19.006635] [Citation(s) in RCA: 6] [Impact Index Per Article: 0.4] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/30/2023]
Abstract
Fiber-optic Cherenkov radiation has emerged as a wavelength conversion technique to achieve isolated spectrum in the visible wavelength range. Most published results have reinforced the impression that CR forms a narrowband spectrum with poor efficiency. We both theoretically and experimentally investigate fiber-optic Cherenkov radiation excited by few-cycle pulses. We introduce the coherence length to quantify the Cherenkov-radiation bandwidth and its dependence on propagation distance. Detailed numerical simulations verified by experimental results reveal three unique features that are absent when pumped with often-used, long pulses; that is, continuum generation (may span one octave in connection with the pump spectrum), high conversion efficiency (up to 40%), and broad bandwidth (70 nm experimentally obtained) for the isolated Cherenkov radiation spectrum. These merits allow achieving broadband visible-wavelength spectra from low-energy ultrafast sources which opens up new applications (e.g. precision calibration of astronomical spectrographs).
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Affiliation(s)
- Guoqing Chang
- Department of Electrical Engineering and Computer Science, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139, USA.
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160
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Chen LJ, Chang G, Li CH, Benedick AJ, Philips DF, Walsworth RL, Kärtner FX. Broadband dispersion-free optical cavities based on zero group delay dispersion mirror sets. OPTICS EXPRESS 2010; 18:23204-23211. [PMID: 21164661 DOI: 10.1364/oe.18.023204] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/30/2023]
Abstract
A broadband dispersion-free optical cavity using a zero group delay dispersion (zero-GDD) mirror set is demonstrated. In general zero-GDD mirror sets consist of two or more mirrors with opposite group delay dispersion (GDD), that when used together, form an optical cavity with vanishing dispersion over an enhanced bandwidth in comparison with traditional low GDD mirrors. More specifically, in this paper, we show a realization of such a two-mirror cavity, where the mirrors show opposite GDD and simultaneously a mirror reflectivity of 99.2% over 100 nm bandwidth (480 nm - 580 nm).
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Affiliation(s)
- Li-Jin Chen
- Research Laboratory of Electronics, Massachusetts Institute of Technology, Cambridge, MA 02139, USA.
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161
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Benedick AJ, Chang G, Birge JR, Chen LJ, Glenday AG, Li CH, Phillips DF, Szentgyorgyi A, Korzennik S, Furesz G, Walsworth RL, Kärtner FX. Visible wavelength astro-comb. OPTICS EXPRESS 2010; 18:19175-19184. [PMID: 20940813 DOI: 10.1364/oe.18.019175] [Citation(s) in RCA: 11] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/30/2023]
Abstract
We demonstrate a tunable laser frequency comb operating near 420 nm with mode spacing of 20-50 GHz, usable bandwidth of 15 nm and output power per line of ~20 nW. Using the TRES spectrograph at the Fred Lawrence Whipple Observatory, we characterize this system to an accuracy below 1m/s, suitable for calibrating high-resolution astrophysical spectrographs used, e.g., in exoplanet studies.
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Affiliation(s)
- Andrew J Benedick
- Research Laboratory of Electronics, Massachusetts Institute of Technology, 77 Mass Ave, Cambridge, MA 02139, USA.
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162
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Pekarek S, Fiebig C, Stumpf MC, Oehler AEH, Paschke K, Erbert G, Südmeyer T, Keller U. Diode-pumped gigahertz femtosecond Yb:KGW laser with a peak power of 3.9 kW. OPTICS EXPRESS 2010; 18:16320-16326. [PMID: 20721018 DOI: 10.1364/oe.18.016320] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/29/2023]
Abstract
We present a diode-pumped Yb:KGW laser with a repetition rate of 1 GHz and a pulse duration of 281 fs at a wavelength of 1041 nm. A high brightness distributed Bragg reflector tapered diode laser is used as a pump source. Stable soliton modelocking is achieved with a semiconductor saturable absorber mirror (SESAM). The obtained average output power is 1.1 W and corresponds to a peak power of 3.9 kW and a pulse energy of 1.1 nJ. With harmonic modelocking we could increase the pulse repetition rate up to 4 GHz with an average power of 900 mW and a pulse duration of 290 fs. This Yb:KGW laser has a high potential for stable frequency comb generation.
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Affiliation(s)
- Selina Pekarek
- Department of Physics, Institute of Quantum Electronics, ETH Zurich, 8093 Zurich, Switzerland.
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163
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Chang G, Li CH, Phillips DF, Walsworth RL, Kärtner FX. Toward a broadband astro-comb: effects of nonlinear spectral broadening in optical fibers. OPTICS EXPRESS 2010; 18:12736-12747. [PMID: 20588402 DOI: 10.1364/oe.18.012736] [Citation(s) in RCA: 20] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/29/2023]
Abstract
We propose and analyze a new approach to generate a broadband astro-comb by spectral broadening of a narrowband astro-comb inside a highly nonlinear optical fiber. Numerical modeling shows that cascaded four-wave-mixing dramatically degrades the input comb's side-mode suppression and causes side-mode amplitude asymmetry. These two detrimental effects can systematically shift the center-of-gravity of astro-comb spectral lines as measured by an astrophysical spectrograph with resolution approximately 100,000; and thus lead to wavelength calibration inaccuracy and instability. Our simulations indicate that this performance penalty, as a result of nonlinear spectral broadening, can be compensated by using a filtering cavity configured for double-pass. As an explicit example, we present a design based on an Yb-fiber source comb (with 1 GHz repetition rate) that is filtered by double-passing through a low finesse cavity (finesse = 208), and subsequent spectrally broadened in a 2-cm, SF6-glass photonic crystal fiber. Spanning more than 300 nm with 16 GHz line spacing, the resulting astro-comb is predicted to provide 1 cm/s (approximately 10 kHz) radial velocity calibration accuracy for an astrophysical spectrograph. Such extreme performance will be necessary for the search for and characterization of Earth-like extra-solar planets, and in direct measurements of the change of the rate of cosmological expansion.
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Affiliation(s)
- Guoqing Chang
- Department of Electrical Engineering and Computer Science and Research Laboratory of Electronics, Massachusetts Institute of Technology, 77 Mass Ave Cambridge MA 02139 USA.
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164
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Li CH, Glenday AG, Benedick AJ, Chang G, Chen LJ, Cramer C, Fendel P, Furesz G, Kärtner FX, Korzennik S, Phillips DF, Sasselov D, Szentgyorgyi A, Walsworth RL. In-situ determination of astro-comb calibrator lines to better than 10 cm s(-1). OPTICS EXPRESS 2010; 18:13239-13249. [PMID: 20588453 DOI: 10.1364/oe.18.013239] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/29/2023]
Abstract
Improved wavelength calibrators for high-resolution astrophysical spectrographs will be essential for precision radial velocity (RV) detection of Earth-like exoplanets and direct observation of cosmological deceleration. The astro-comb is a combination of an octave-spanning femtosecond laser frequency comb and a Fabry-Pérot cavity used to achieve calibrator line spacings that can be resolved by an astrophysical spectrograph. Systematic spectral shifts associated with the cavity can be 0.1-1 MHz, corresponding to RV errors of 10-100 cm/s, due to the dispersive properties of the cavity mirrors over broad spectral widths. Although these systematic shifts are very stable, their correction is crucial to high accuracy astrophysical spectroscopy. Here, we demonstrate an in-situ technique to determine the systematic shifts of astro-comb lines due to finite Fabry-Pérot cavity dispersion. The technique is practical for implementation at a telescope-based spectrograph to enable wavelength calibration accuracy better than 10 cm/s.
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Affiliation(s)
- Chih-Hao Li
- Department of Physics, Harvard University, USA.
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165
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Quinlan F, Ycas G, Osterman S, Diddams SA. A 12.5 GHz-spaced optical frequency comb spanning >400 nm for near-infrared astronomical spectrograph calibration. THE REVIEW OF SCIENTIFIC INSTRUMENTS 2010; 81:063105. [PMID: 20590223 DOI: 10.1063/1.3436638] [Citation(s) in RCA: 7] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/29/2023]
Abstract
A 12.5 GHz-spaced optical frequency comb locked to a global positioning system disciplined oscillator for near-infrared (IR) spectrograph calibration is presented. The comb is generated via filtering a 250 MHz-spaced comb. Subsequent nonlinear broadening of the 12.5 GHz comb extends the wavelength range to cover 1380-1820 nm, providing complete coverage over the H-band transmission window of earth's atmosphere. Finite suppression of spurious sidemodes, optical linewidth, and instability of the comb has been examined to estimate potential wavelength biases in spectrograph calibration. Sidemode suppression varies between 20 and 45 dB, and the optical linewidth is approximately 350 kHz at 1550 nm. The comb frequency uncertainty is bounded by +/-30 kHz (corresponding to a radial velocity of +/-5 cm/s), limited by the global positioning system disciplined oscillator reference. These results indicate that this comb can readily support radial velocity measurements below 1 m/s in the near IR.
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Affiliation(s)
- F Quinlan
- National Institute of Standards and Technology, 325 Broadway, Boulder, Colorado 80305, USA.
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166
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Wilken T, Lovis C, Manescau A, Steinmetz T, Pasquini L, Lo Curto G, Hänsch TW, Holzwarth R, Udem T. High-precision calibration of spectrographs. ACTA ACUST UNITED AC 2010. [DOI: 10.1111/j.1745-3933.2010.00850.x] [Citation(s) in RCA: 91] [Impact Index Per Article: 6.1] [Reference Citation Analysis] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/28/2022]
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167
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Smíd R, Cíp O, Cízek M, Mikel B, Lazar J. Conversion of stability of femtosecond mode-locked laser to optical cavity length. IEEE TRANSACTIONS ON ULTRASONICS, FERROELECTRICS, AND FREQUENCY CONTROL 2010; 57:636-640. [PMID: 20211782 DOI: 10.1109/tuffc.2010.1459] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/28/2023]
Abstract
In this contribution we propose a scheme for a generation of precise displacements through conversion of relative stability of components of a femtosecond laser into the length of a Fabry-Perot cavity. The spacing of mirrors of a Fabry-Perot interferometer represents a mechanical length standard referenced to stable optical frequency of a femtosecond mode-locked laser. With the help of a highly selective optical filter, it is possible to get only a few discrete spectral components. By tuning and locking the Fabry-Perot cavity to a selected single component it is possible to get a mechanical length standard with the uncertainty of the repetition frequency of the femtosecond laser. To verify the method, an auxiliary single-frequency laser is locked to the resonance mode of the cavity and simultaneously it is optically mixed with an independent optical frequency standard He-Ne-I2. The stability of the beat-frequency between these 2 lasers represents the stability of the Fabry-Perot cavity length. The stability recording evaluated through Allan variances for one hour of operation is presented. The pilot experimental setup is able to generate the length standard in the order of 0.01 nm for 20 min of integration time.
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Affiliation(s)
- Radek Smíd
- Institute of Scientific Instruments of the Academy of Sciences of the Czech Republic, Brno, Czech Republic.
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168
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Adler F, Thorpe MJ, Cossel KC, Ye J. Cavity-enhanced direct frequency comb spectroscopy: technology and applications. ANNUAL REVIEW OF ANALYTICAL CHEMISTRY (PALO ALTO, CALIF.) 2010; 3:175-205. [PMID: 20636039 DOI: 10.1146/annurev-anchem-060908-155248] [Citation(s) in RCA: 91] [Impact Index Per Article: 6.1] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/29/2023]
Abstract
Cavity-enhanced direct frequency comb spectroscopy combines broad bandwidth, high spectral resolution, and ultrahigh detection sensitivity in one experimental platform based on an optical frequency comb efficiently coupled to a high-finesse cavity. The effective interaction length between light and matter is increased by the cavity, massively enhancing the sensitivity for measurement of optical losses. Individual comb components act as independent detection channels across a broad spectral window, providing rapid parallel processing. In this review we discuss the principles, the technology, and the first applications that demonstrate the enormous potential of this spectroscopic method. In particular, we describe various frequency comb sources, techniques for efficient coupling between comb and cavity, and detection schemes that utilize the technique's high-resolution, wide-bandwidth, and fast data-acquisition capabilities. We discuss a range of applications, including breath analysis for medical diagnosis, trace-impurity detection in specialty gases, and characterization of a supersonic jet of cold molecules.
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Affiliation(s)
- Florian Adler
- JILA, National Institute of Standards and Technology, Department of Physics, University of Colorado, Boulder, 80309-0440, USA.
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169
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Affiliation(s)
- Albrecht Bartels
- Center for Applied Photonics, University of Konstanz, Universitätsstraße 10, 78457 Konstanz, Germany
| | - Dirk Heinecke
- Center for Applied Photonics, University of Konstanz, Universitätsstraße 10, 78457 Konstanz, Germany
- National Institute of Standards and Technology (NIST), 325 Broadway Mail Stop 847, Boulder, CO 80305, USA
| | - Scott A. Diddams
- National Institute of Standards and Technology (NIST), 325 Broadway Mail Stop 847, Boulder, CO 80305, USA
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170
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Lim J, Knabe K, Tillman KA, Neely W, Wang Y, Amezcua-Correa R, Couny F, Light PS, Benabid F, Knight JC, Corwin KL, Nicholson JW, Washburn BR. A phase-stabilized carbon nanotube fiber laser frequency comb. OPTICS EXPRESS 2009; 17:14115-14120. [PMID: 19654821 DOI: 10.1364/oe.17.014115] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/28/2023]
Abstract
A frequency comb generated by a 167 MHz repetition frequency erbium-doped fiber ring laser using a carbon nanotube saturable absorber is phase-stabilized for the first time. Measurements of the in-loop phase noise show an integrated phase error on the carrier envelope offset frequency of 0.35 radians. The carbon nanotube fiber laser comb is compared with a CW laser near 1533 nm stabilized to the nu(1) + nu(3) overtone transition in an acetylene-filled kagome photonic crystal fiber reference, while the CW laser is simultaneously compared to another frequency comb based on a Cr:Forsterite laser. These measurements demonstrate that the stability of a GPS-disciplined Rb clock is transferred to the comb, resulting in an upper limit on the locked comb's frequency instability of 1.2 x 10(-11) in 1 s, and a relative instability of <3 x 10(-12) in 1 s. The carbon nanotube laser frequency comb offers much promise as a robust and inexpensive all-fiber frequency comb with potential for scaling to higher repetition frequencies.
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Affiliation(s)
- Jinkang Lim
- Department of Physics, Kansas State University, Manhattan, KS 66506, USA
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171
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McFerran JJ. Echelle spectrograph calibration with a frequency comb based on a harmonically mode-locked fiber laser: a proposal. APPLIED OPTICS 2009; 48:2752-2759. [PMID: 19424399 DOI: 10.1364/ao.48.002752] [Citation(s) in RCA: 12] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/27/2023]
Abstract
Details for constructing an astronomical frequency comb suitable as a wavelength reference for échelle spectrographs associated with optical telescopes are outlined. The source laser for the frequency comb is a harmonically mode-locked fiber laser with a central wavelength of 1.56 microm. The means of producing a repetition rate greater than 7 GHz and a peak optical power of approximately 8 kW are discussed. Conversion of the oscillator light into the visible can occur through a two-step process of (i) nonlinear conversion in periodically poled lithium niobate and (ii) spectral broadening in photonic crystal fiber. While not necessarily octave spanning in spectral range to permit the use of an f -to- 2f interferometer for offset frequency control, the frequency comb can be granted accuracy by linking the mode spacing and a comb tooth to separate frequency references. The design avoids the use of a Fabry-Perot cavity to increase the mode spacing of the frequency comb; however, the level of supermode suppression and sideband asymmetry in the fiber oscillator and in the subsequent frequency conversion stages are aspects that need to be experimentally tested.
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Affiliation(s)
- J J McFerran
- School of Physics, Mailstop M013, The University of Western Australia, Nedlands, 6009, WA, Australia.
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172
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Hundertmark H, Rammler S, Wilken T, Holzwarth R, Hänsch TW, Russell PSJ. Octave-spanning supercontinuum generated in SF6-glass PCF by a 1060 nm mode-locked fibre laser delivering 20 pJ per pulse. OPTICS EXPRESS 2009; 17:1919-1924. [PMID: 19189022 DOI: 10.1364/oe.17.001919] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/27/2023]
Abstract
We report the generation of an octave-spanning supercontinuum in SF6-glass photonic crystal fiber using a diode-pumped passively mode-locked fs Yb-fiber laser oscillating at 1060 nm. The pulses (energy up to 500 pJ and duration 60 fs) were launched into a 4 cm length of PCF (core diameter 1.7 microm and zero-dispersion wavelength approximately 1060 nm). Less than 20 pJ of launched pulse energy was sufficient to generate a supercontinuum from 600 nm to 1450 nm, which represents the lowest energy so far reported for generation of an octave-spanning supercontinuum from a 1 microm pump. Since the laser pulse energy scales inversely with the repetition rate, highly compact and efficient sources based on SF6-glass PCF are likely to be especially useful for efficient spectral broadening at high repetition rates (several GHz), such as those needed for the precise calibration of astronomical spectrographs, where a frequency comb spacing >10 GHz is required for the best performance.
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Affiliation(s)
- H Hundertmark
- Max-Planck-Research-Group (IOIP), University of Erlangen-Nuremberg, Erlangen, Germany.
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173
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Affiliation(s)
- Sebastian Lopez
- Departamento de Astronomía, Universidad de Chile, Casilla 36-D, Santiago, Chile
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