Generation of stabilized, ultra-short light pulses and the use thereof for synthesizing optical frequencies
First Claim
1. A process for the operation of a laser device having a resonator configuration with a light path, comprising the steps of:
- generating light pulses circulating in the resonator configuration, said light pulses consisting of spectral components corresponding to multiple longitudinal modes of the resonator configuration;
compensating for the group velocity dispersion of said light pulses; and
inputting a predetermined linear dispersion into the light path of the resonator configuration, so that at least one mode possesses a predetermined frequency or the mode separation between the modes possesses a predetermined value;
said step of inputting a predetermined linear dispersion comprising at least one of a tilting of a transparent plane, a pushing in of a pair of prisms in the light path of the resonator configuration, a setting of the effective pumping power for the pumping of the active medium of the laser device, or a change of the geometric configuration of the laser device relative to a pump laser.
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Abstract
A process for operation of a laser device (1) is described, whereby circulating light pulses each comprising spectral components according to a plurality of longitudinal modes of a resonator configuration (3) are generated in the resonator configuration (3) and subjected to a compensation of group velocity dispersion, and a predetermined linear dispersion is introduced into the light path of the resonator configuration (3), so that at least one mode has a predetermined frequency and/or the mode distance between the modes has a predetermined value. Furthermore, regulations for stabilizing the laser device on the basis of this process and applications of the regulations for the generation for stabilized, ultra-short light pulses, generation of optical frequencies and in the frequency and/or time measuring technique as well as in the spectroscopy are described.
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Citations
28 Claims
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1. A process for the operation of a laser device having a resonator configuration with a light path, comprising the steps of:
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generating light pulses circulating in the resonator configuration, said light pulses consisting of spectral components corresponding to multiple longitudinal modes of the resonator configuration;
compensating for the group velocity dispersion of said light pulses; and
inputting a predetermined linear dispersion into the light path of the resonator configuration, so that at least one mode possesses a predetermined frequency or the mode separation between the modes possesses a predetermined value;
said step of inputting a predetermined linear dispersion comprising at least one of a tilting of a transparent plane, a pushing in of a pair of prisms in the light path of the resonator configuration, a setting of the effective pumping power for the pumping of the active medium of the laser device, or a change of the geometric configuration of the laser device relative to a pump laser. - View Dependent Claims (3, 4, 5, 6, 7, 8, 9)
the output frequency of an optical reference frequency generator (240), a higher harmonic or an even number fraction of the output frequency or of the higher harmonic, a frequency multiple of a lower frequency reference mode of the light pulses, or a fractional frequency of a higher frequency reference mode of the light pulses. -
4. Process according to claim 3, whereby in the mode control loop (I) light pulse of the laser device (1) and light with the reference frequency (fref) are superposed and directed to a photosensitive element (211), whose electrical output signal shows a modulation at a beat frequency corresponding to the distance of the frequency of the first reference mode (M1) from the reference frequency (fref), whereby a control (214) is provided, which sets the linear dispersion of the resonator configuration (3) so that the beat signal is minimal or possesses a predetermined beat frequency.
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5. Process according to claim 4, whereby the optical reference frequency generator (240) is a stabilized continuous wave laser.
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6. Process according to claim 3, whereby the optical reference frequency generator (240) is stabilized in a reference laser control loop (III) in relation to a second higher frequency reference mode (M2) of the light pulses.
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7. Process according to claim 1 or claim 2, whereby the liner dispersion is introduced into the resonator configuration (3) within the framework of a mode control loop (Ia, Ib) depending upon the deviation of the multiplied frequency of a first reference laser (240a), which is phase coupled with a first lower frequency reference mode (M1) of the light pulses, from the frequency of a second reference laser (240b), which is phase coupled in a reference laser control loop (III) with a second higher frequency reference mode (M2) of the light pulses.
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8. Process according to claim 7 whereby the second reference laser (24 Gb) is phase coupled with the second higher frequency reference mode (M2) of the light pulses through a scaling stage.
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9. Process according to claim 1 or 2, whereby the resonator length of the laser device (1) is regulated within the framework of a repetition frequency control loop (II), in which the repetition frequency (fr) of the light pulses is superposed with a radio frequency derived from a radio frequency generator reference (25), whereby a control (224) is provided for, which sets the resonator length of the laser device (1) so that the oscillating signal formed by the superposition is minimal or possesses a predetermined beat frequency.
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2. A process for the operation of a laser device having a resonator configuration with a light path, comprising the steps of:
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generating light pulses circulating in the resonator configuration, said light pulses consisting of spectral components corresponding to multiple longitudinal modes of the resonator configuration;
compensating for the group velocity dispersion of said light pulses; and
inputting a predetermined linear dispersion into the light path of the resonator configuration, so that at least one mode possesses a predetermined frequency or the mode separation between the modes possesses a predetermined value;
said step of inputting a predetermined linear dispersion comprising changing a spectrally specific effective resonator length in a resonator branch, through which the light pulses traverse spectrally spatially separated after the compensation of the group velocity dispersion. - View Dependent Claims (10, 11, 12, 13, 14)
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15. A laser device for production of short light pulses, having a resonator configuration with
an active medium; -
a resonator formed with an optical fiber or with a plurality of mirrors, including an incoupling mirror for the coupling in of pump light to the active medium and two or more tilted mirrors for directing resonating light to an outcoupling mirror for the output of light pulses;
a compensating mechanism for the compensation of the group velocity dispersion of the light pulses;
a dispersion setting device for the input of a predetermined linear dispersion into the light path of the resonator configuration; and
said dispersion setting device comprising at least one of a transparent plate with a tilting mechanism, a pair of prisms with a sliding mechanism, which are included in the resonator configuration, an apparatus for the variation of the effective pump power of a pump laser, or an apparatus for the variation of the geometrical configuration of the laser device relative to the pump laser. - View Dependent Claims (17, 18, 19, 20, 21, 22, 23, 24, 25, 26, 27, 28)
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16. A laser device for production of short light pulses, having a resonator configuration with
an active medium; -
a resonator formed with an optical fiber or with a plurality of mirrors, including an incoupling mirror for the coupling in of pump light to the active medium and two or more tilted mirrors for directing resonating light to an outcoupling mirror for the output of light pulses;
a compensating mechanism for the compensation of the group velocity dispersion of the light pulses;
a dispersion setting device for the input of a predetermined linear dispersion into the light path of the resonator configuration; and
said dispersion setting device comprising a pivoting mechanism on a tilted mirror functioning as a resonator end mirror and being located in a branch of the resonator on the side of the compensating mechanism facing away from the active medium.
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Specification