Patent Application
20170302048
The field of the present invention relates to stabilized laser sources. In particular, one or more examples of a stabilized non-reciprocal fiber-ring Brillouin laser source, and methods of their use, are disclosed herein.
Examples of laser sources or methods of their use are disclosed in:
Each reference, patent, and publication listed above is incorporated by reference as if fully set forth herein.
A laser source comprises a fiber-ring optical resonator, a pump laser source, and a frequency-locking mechanism. The fiber-ring optical resonator includes an optical circulator and an optical coupler, and is characterized by a Brillouin shift frequency νB. The optical circulator is arranged so as to (i) limit to a single round trip propagation of an optical signal around the fiber-ring optical resonator in a forward direction, and (ii) permit resonant propagation of an optical signal around the fiber-ring optical resonator in a backward direction. The pump laser source produces a pump optical signal at a pump optical frequency ν1, and (i) launches into the fiber-ring optical resonator via the optical circulator a first input portion of the pump optical signal to propagate in the forward direction, and (ii) launches into the fiber-ring optical resonator via the optical coupler a second input portion of the pump optical signal to propagate in the backward direction. The frequency-locking mechanism couples the pump laser source and the fiber-ring optical resonator by controlling the pump optical frequency ν1 to maintain resonant propagation of the second input portion of the pump optical signal around the fiber-ring optical resonator in the backward direction. The fiber-ring optical resonator is arranged so as to produce from the first input portion of the pump optical signal a Brillouin laser optical signal, at a Brillouin laser frequency ν1S=ν1−νB, that resonantly propagates around the fiber-ring optical resonator in the backward direction. The optical coupler directs out of the fiber-ring optical resonator (i) an output portion of the second input portion of the pump optical signal, at the pump optical frequency ν1, to act as an optical feedback signal to the frequency-locking mechanism, and (ii) an output portion of the Brillouin laser optical signal, at the Brillouin laser frequency ν1S, to act as optical output of the laser source.
The laser source can further include a second pump laser source that produces a second pump optical signal at a second pump optical frequency ν2, and launches into the fiber-ring optical resonator via the optical circulator a first input portion of the second pump optical signal to propagate in the forward direction. The fiber-ring optical resonator is arranged so as to produce from the first input portion of the second pump optical signal a second Brillouin laser optical signal, at a second Brillouin laser frequency ν2S=ν2−νB, that resonantly propagates around the fiber-ring optical resonator in the backward direction. The optical coupler is arranged so as to direct out of the fiber-ring optical resonator an output portion of the second Brillouin laser optical signal, at the second Brillouin laser frequency ν2S, to act as second optical output of the laser source. A second input portion of the pump optical signal can be launched into the fiber-ring optical resonator via the optical coupler to propagate in the backward direction, and a second frequency-locking mechanism can couple the second pump laser source and the fiber-ring optical resonator by controlling the second pump optical frequency ν2 to maintain resonant propagation of the second input portion of the second pump optical signal around the fiber-ring optical resonator in the backward direction.
The optical output signals at the optical output frequencies ν1S and ν2S can be employed to generate an output electrical signal at an optical difference frequency |ν1S−ν2S| by directing the optical output signals onto a photodetector; the output electrical signal exhibits reduced phase noise. An electrical frequency divider can be employed to divide the optical difference frequency |ν1S−ν2S| of the output electrical signal to achieve still further phase noise reduction.
An optical or electro-optical frequency divider can be employed to generate, from the optical output signals at the optical output frequencies ν1S and ν2S, an output electrical signal at a frequency fD. The integer N that is closest to |ν1S−ν2S|/fD is the nominal frequency division ratio of the optical or electro-optical frequency divider. The output electrical signal at the frequency fD exhibits phase noise reduced by about a factor of N2 relative to phase noise of the optical difference frequency |ν1S−ν2S|.
Objects and advantages pertaining to stabilized laser sources may become apparent upon referring to the example embodiments illustrated in the drawings and disclosed in the following written description or appended claims, and shall fall within the scope of the present disclosure or appended claims.
This Summary is provided to introduce a selection of concepts in a simplified form that are further described below in the Detailed Description. This Summary is not intended to identify key features or essential features of the claimed subject matter, nor is it intended to be used as an aid in determining the scope of the claimed subject matter.
The embodiments depicted are shown only schematically: all features may not be shown in full detail or in proper proportion, certain features or structures may be exaggerated relative to others for clarity, and the drawings should not be regarded as being to scale. The embodiments shown are only examples: they should not be construed as limiting the scope of the present disclosure or appended claims.
An example of an inventive laser source 10 is illustrated schematically in
The pump laser source 200 produces a pump optical signal 20 characterized by a pump optical frequency ν1. A first input portion 22 of the pump optical signal 20 is launched into the fiber-ring optical resonator 100, via the optical circulator 110, to propagate in the forward direction; that first portion 22 of the pump optical signal 20 makes only a single round trip around the fiber-ring optical resonator 100 before being rejected by the circulator 110. A second input portion 24 of the pump optical signal 20 is launched into the fiber-ring optical resonator 100, via the optical coupler 120, to propagate in the backward direction; that second portion 24 of the pump optical signal 20 makes multiple round trips around the fiber-ring optical resonator 100 through the circulator 110. The frequency-locking mechanism 300 couples the pump laser source 200 and the fiber-ring optical resonator 100 by controlling the pump optical frequency ν1 (via an electrical laser-control signal 28) to maintain resonant propagation of the second input portion 24 of the pump optical signal 20 around the fiber-ring optical resonator 100 in the backward direction. The optical coupler 120 directs out of the fiber-ring optical resonator 100 an output portion 26 of the second input portion 24 of the pump optical signal 20, at the pump optical frequency ν1; at least a portion of the optical signal 26 acts as an optical feedback signal to the frequency-locking mechanism 300.
The fiber-ring optical resonator 100 is characterized by a Brillouin shift frequency νB (that varies proportionally with the pump optical frequency ν1), and produces from the first input portion 22 of the pump optical signal 20 a Brillouin laser optical signal 80 at a Brillouin laser frequency ν1S=ν1−νB. The backward-propagating Brillouin laser optical signal 80 is at least partly transmitted by the optical circulator 100 upon each round trip around the fiber-ring resonator 100, and so can resonantly propagate around the fiber-ring optical resonator 100 in the backward direction (i.e., counterpropagating with respect to the first input portion 22 of the pump laser signal 20). The optical coupler 120 directs out of the fiber-ring optical resonator 100 an output portion 82 of the Brillouin laser optical signal 80 at the Brillouin laser frequency ν1S; at least a portion of the optical signal 82 acts as optical output of the laser source 10. In some examples, the optical coupler 120 is a 95/5 coupler (i.e., about 5% of the power circulating in the fiber-ring resonator 100 exits on each round trip); other suitable coupling ratios can be employed.
In some examples, the pump optical frequency ν1 is between about 75 THz and about 750 THz (i.e., the pump wavelength in vacuum is between about 400 nm and about 4 μm); in some examples, the pump optical frequency ν1 is between about 120 THz and about 430 THz (i.e., the pump wavelength in vacuum is between about 700 nm and about 2.5 μm); in some examples, the pump optical frequency ν1 is between about 150 THz and about 300 THz (i.e., the pump wavelength in vacuum is between about 1 μm and about 2 μm). Any suitable pump laser source can be employed (e.g., a semiconductor, solid state, fiber, or dye laser), either directly or after any suitable frequency shifting (e.g., via phase modulation, one or more nonlinear optical processes, and so forth) or after any suitable amplification (e.g., using a semiconductor, solid state, fiber, or dye amplifier). In some examples a fiber laser operating at about 1550 nm is employed, amplified by a fiber amplifier. The fiber-ring optical resonator 100 typically comprises silica optical fiber that is characterized by a Brillouin shift frequency νB of about 10.9 GHz when pumped at about 1550 nm. Other suitable optical fiber material(s) can be employed, and those other fiber materials can exhibit other corresponding Brillouin shift frequencies. The optical circulator 110 and the optical coupler 120 can be of any suitable type or construction. In some examples, the optical coupler 120 can be a fused-fiber coupler.
The presence of the optical circulator 110 in the fiber-ring resonator 100 causes the resonator 100 to exhibit non-reciprocal behavior (e.g., unidirectional resonant propagation in the backward direction versus only a single round trip in the forward direction). In a bidirectional resonator (e.g., a fiber-ring resonator that does not include an optical circulator, or a microdisk resonator), intracavity power buildup in the reverse direction (relative the pump signal propagation), and output power at the Brillouin laser frequency (ν1S=ν1−νB), are limited by onset of resonant oscillation in the forward direction at another Brillouin laser frequency ν1−2νB (pumped by intracavity power at the Brillouin laser frequency ν1S=ν1−νB). Multiple cascaded orders of Brillouin laser oscillation, propagating around the resonator in alternating directions and spaced by the Brillouin shift frequency νB, can occur simultaneously in a single bidirectional resonator pumped by a single pump signal. In contrast, in the non-reciprocal fiber-ring resonator 100 (non-reciprocal due to the presence of the optical circulator 110 incorporated into the resonator 100), resonant propagation in the forward direction is prevented, so that no higher orders of Brillouin laser oscillation can occur. This non-reciprocal behavior of the fiber-ring resonator 100 has the effect of enabling higher buildup of intracavity power of the Brillouin laser signal 80 and higher output power at the Brillouin laser wavelength ν1S=ν1−νB. That increase in laser power can be desirable in its own right, and can also be desirable because Schawlow-Townes noise in a Brillouin laser oscillator typically is inversely proportional to its output power. The disclosed non-reciprocal arrangement of the fiber-ring resonator 100, that suppresses higher-order Brillouin laser oscillation and therefore enables higher output power at the Brillouin laser wavelength ν1S=ν1−νB, results in lower Schawlow-Townes noise in the Brillouin laser output 82 than would be achievable otherwise.
In some examples, the threshold for Brillouin laser oscillation is on the order of a few tens of milliwatts of power in the pump optical signal, and about a hundred milliwatts of pump optical power yields about 10 milliwatts of corresponding Brillouin laser output power. Other thresholds or conversion efficiencies can be achieved or employed.
Schawlow-Townes noise of the Brillouin laser signal 80 and optical output 82 also is inversely related to the spatial volume of the resonant optical mode of the Brillouin laser signal 80 supported by the fiber-ring optical resonator 100. A longer fiber-ring resonator 100 therefore produces Brillouin laser output that exhibits correspondingly less Schawlow-Townes noise than the Brillouin laser output of a shorter but otherwise equivalent fiber-ring resonator. In some examples, the fiber-ring optical resonator 100 includes an optical fiber greater than or equal to about 10 meters long, with a corresponding free spectral range less than about 20 MHz; in some examples, the fiber-ring optical resonator 100 includes an optical fiber greater than or equal to about 40 meters long, with a corresponding free spectral range less than about 5 MHz; in some examples, the fiber-ring optical resonator 100 includes an optical fiber greater than or equal to about 100 meters long, with a corresponding free spectral range less than about 2 MHz; in some examples, the fiber-ring optical resonator 100 includes an optical fiber greater than or equal to about 200 meters long, with a corresponding free spectral range less than about 1 MHz; in some examples, the fiber-ring optical resonator 100 includes an optical fiber greater than or equal to about 500 meters long, with a corresponding free spectral range less than about 0.4 MHz.
Silica optical fiber typically is employed in the fiber-ring resonator 100, and exhibits stimulated Brillouin gain with a bandwidth of about 50 MHz. A fiber-ring resonator 100 with a free spectral range less than 50 MHz, including those described above, typically can produce Brillouin laser output (at the Brillouin laser frequency ν1S=ν1−νB) without requiring a frequency-locking mechanism, because at least one resonant mode of the fiber-ring cavity will sufficiently overlap the stimulated Brillouin gain spectral profile at the Brillouin-shifted pump optical frequency ν1−νB. The stimulated Brillouin gain spectral profile varies sufficiently rapidly near its peak so that typically only one resonant mode at a time supports resonant Brillouin laser oscillation. However, in response to fluctuations or drift of the pump optical frequency ν1, the resonant Brillouin laser signal typically will intermittently hop from one resonant mode of the fiber-ring resonator 100 to another, which is undesirable if the laser source 10 is to be used as or incorporated into a stable frequency reference.
The frequency-locking mechanism 300 substantially prevents such mode-hopping of the Brillouin laser oscillation 80 in the fiber-ring resonator 100. Any suitable frequency-locking mechanism can be employed. In some examples, the frequency-locking mechanism 300 includes a Pound-Drever-Hall mechanism (e.g., as in
In the examples shown, the second input portion 24 of the pump optical signal 20 is launched into the fiber-ring optical resonator 100 by the optical coupler 120 (which acts as an output coupler and directs the output portion 82 of the Brillouin laser signal 80 out of the fiber-ring resonator 100), and the optical coupler 120 also directs an output portion 26 of the backward-propagating signal 24 out of the fiber-ring resonator 100; in other examples, an optical coupler separate from the optical coupler 120 can be employed for launching the second input portion 24 into the fiber-ring resonator or to direct the output portion 26 out of the fiber-ring resonator 100. In the examples shown, an optical splitter 130 can be employed to divide the optical signals directed out of the fiber-ring resonator 100 by the coupler 120 (i.e., optical signals 26 and 82); one fraction propagates to the frequency-locking mechanism 300, while the other fraction propagates along the optical output path of the laser source 10. The fraction of the output portion 26 of the resonantly propagating input portion 24, at the pump optical frequency ν1, that is directed by the splitter 130 to the frequency-locking mechanism 300 acts as an optical feedback signal to the frequency-locking mechanism 300.
In some examples (e.g., wherein a Pound-Drever-Hall frequency locking mechanism 300 is employed), the second input portion 24 of the pump optical signal 20 is directed through a portion of the frequency-locking mechanism 300 on its way to being launched into the fiber-ring optical resonator 100. In the specific example of a Pound-Drever-Hall mechanism 300 (e.g., as in
In a silica fiber-ring resonator 100 that is about 10 meters long or longer (i.e., with a free spectral range less than about 20 MHz), the frequency-locking mechanism serves to ensure resonant oscillation of the Brillouin laser signal 80, and also to prevent mode-hopping and to reduce phase noise of the optical output 82 of the laser source 10. In a shorter fiber-ring resonator 100, however, wherein the free spectral range is larger than the stimulated Brillouin gain bandwidth, the frequency-locking mechanism 300 is also used to ensure that the Brillouin laser frequency ν1S=ν1−νB substantially coincides with a resonant mode of the fiber-ring resonator 100. This can be accomplished in some examples by (i) arranging the fiber-ring resonator 100 so that an integer multiple of its free spectral range is about equal to its Brillouin shift frequency νB (e.g., about 10.9 GHz in silica fiber pumped at 1550 nm), and then (ii) using the frequency-locking mechanism 300 to lock the pump optical frequency ν1 to a resonant mode of the fiber-ring resonator 100.
The second pump laser source 210 can be provided in a variety of ways. In the example illustrated schematically in
In the example illustrated schematically in
The scheme described in the preceding example can be carried further (resulting in an optical spectrum resembling the example shown in
In another example (illustrated schematically in
An example is shown in
In a given laser source 10, both frequency-locking mechanisms 300/310 can operate in the same manner (e.g., both Pound-Drever-Hall mechanisms, as in the example of
If needed or desired, additional pump laser sources, operating at corresponding additional, different pump optical frequencies, can be employed to generate additional optical outputs from the laser source 10.
The laser source 10, when operated to produce two optical outputs 82/92 at respective optical frequencies ν1S and ν2S, can be arranged so as to exhibit fluctuations of an output optical difference frequency |ν2S−ν1S| only within an operationally acceptable bandwidth. The term “operationally acceptable” is necessarily a context-sensitive descriptor, and can vary from one instance to the next based on such considerations as minimum required performance criteria for a given use, or limitations of space, cost, complexity, power consumption, or maintenance. In some examples, the laser source 10 can be arranged so as to exhibit fluctuations of an output optical difference frequency |ν2S−ν1S|, over about a 0.1 second timescale, only within a bandwidth less than about 100 Hz. In some examples, the laser source 10 can be arranged so as to exhibit fluctuations of an output optical difference frequency |ν2S−ν1S|, over about a 0.1 second timescale, only within a bandwidth less than about 0.1 Hz. The use of a single fiber-ring resonator 100 to generate output optical signals at both optical frequencies ν1S and ν2S significantly reduces noise in the signal at the output optical difference frequency |ν2S−ν1S|, because many sources of so-called technical noise (i.e., noise arising from instabilities in environment or equipment, as opposed to quantum noise inherent in the physics of the system) are shared between the two optical outputs 82/92, and therefore cancel out at the optical difference frequency.
One application of the laser source 10, when arranged to produce two optical outputs 82/92 at the two optical frequencies ν1S and ν2S, is to produce a stable electrical reference signal 99 in the radio-frequency or microwave-frequency range (e.g., 100s of MHz to 100s of GHz). One simple way to generate such an electrical signal 99 (e.g., as in the example of
The laser source 10 is arranged so as to exhibit phase noise of the electrical output signal 99 at the output optical difference frequency |ν1S−ν2S| less than an operationally acceptable reference phase noise level. As noted above, “operationally acceptable” is a context-sensitive limitation. In some examples, the laser source 10 can be arranged so as to exhibit phase noise of the electrical output signal 99 at the output optical difference frequency |ν1S−ν2S| less than about −90 dBc/Hz at 1 kHz offset frequency and less than about −110 dBc/Hz at 10 kHz offset frequency. In some examples, the laser source 10 can be arranged so as to exhibit phase noise of the electrical output signal 99 at the output optical difference frequency |ν1S−ν2S| less than about −110 dBc/Hz at 1 kHz offset frequency and less than about −130 dBc/Hz at 10 kHz offset frequency. Examples of noise spectra for electrical signals 99 generated in this way are shown in
Still further reductions of phase noise can be achieved by generating optical output signals 82/92 at corresponding output optical frequencies ν1S and ν2S that are more than about 100 GHz apart, and employing optical or electro-optical frequency division to produce an electrical output signal 97 at a frequency fD. The frequency fD is about equal to |ν1S−ν2S|/N, where N is an integer that defines the division factor of the divider. In some examples, the two optical outputs 82/92 from the laser source 10 (at respective optical frequencies ν1S and ν2S) are directed into an optical frequency divider 503 of any suitable type (e.g., as in
The output optical frequencies ν1S and ν2S can be selected so that the output optical difference frequency |ν1S−ν2S| is greater than about 300 GHz, greater than about 1 THz, greater than about 10 THz, or greater than about 100 THz. The frequency fD of the output electrical signal 97 can be between about 0.3 GHz and about 300 GHz, between about 1 GHz and about 100 GHz, or between about 5 GHz and about 50 GHz; frequencies between about 5 GHz and about 50 GHz are commonly desired. The frequency fD of the electrical output signal 97 is about equal to |ν1S−ν2S|/N, where N is an integer that defines the nominal division factor of the optical divider 503 or the electro-optical divider 507. The reduction of phase noise in the output electrical signal 97 at the frequency fD is reduced, relative to the phase noise of the output optical difference frequency |ν1S−ν2S|, by roughly a factor of aν1S−ν2S|/fD)2 (i.e., roughly N2). For example, for output optical frequencies ν1S and ν2S separated by about 300 GHz and fD at about 10 GHz, the reduction of phase noise is about 900-fold; for output optical frequencies ν1S and ν2S separated by about 1 THz and fD at about 10 GHz, the reduction of phase noise is about 10,000-fold. The laser source 10 or the optical or electro-optical frequency divider 503 or 507 is arranged so as to limit phase noise of the electrical output signal at the frequency fD to less than an operationally acceptable reference phase noise level (which is context-sensitive). In some examples, the laser source 10 or the divider 503 or 507 can be stabilized so as to limit phase noise of the electrical output signal at the frequency fD to less than about [−90−20·log(|ν1S−ν2S|/fD)] dBc/Hz at 1 kHz offset frequency and less than about [−110−20·log(|ν1S−ν2S|/fD)] dBc/Hz at 10 kHz offset frequency. In some examples, the laser source 10 or the divider 503 or 507 can be stabilized so as to limit phase noise of the electrical output signal at the frequency fD to less than about [−110−20·log(|ν1S−ν2S|/fD)] dBc/Hz at 1 kHz offset frequency and less than about [−130−20·log(|ν1S−ν2S|/fD)] dBc/Hz at 10 kHz offset frequency.
In addition to the preceding, the following examples fall within the scope of the present disclosure or appended claims:
A laser source comprising: (a) a fiber-ring optical resonator including an optical circulator and an optical coupler, wherein the fiber-ring optical resonator is characterized by a Brillouin shift frequency νB, and wherein the optical circulator is arranged so as to (i) limit to a single round trip propagation of an optical signal around the fiber-ring optical resonator in a forward direction, and (ii) permit resonant propagation of an optical signal around the fiber-ring optical resonator in a backward direction; (b) a pump laser source that arranged so as to (i) produce a pump optical signal characterized by a pump optical frequency ν1, (ii) launch into the fiber-ring optical resonator via the optical circulator a first input portion of the pump optical signal to propagate in the forward direction, and (iii) launch into the fiber-ring optical resonator via the optical coupler a second input portion of the pump optical signal to propagate in the backward direction; and (c) a frequency-locking mechanism coupling the pump laser source and the fiber-ring optical resonator, wherein the frequency-locking mechanism is arranged so as to control the pump optical frequency ν1 to maintain resonant propagation of the second input portion of the pump optical signal around the fiber-ring optical resonator in the backward direction, wherein: (d) the fiber-ring optical resonator is arranged so as to produce from the first input portion of the pump optical signal a Brillouin laser optical signal, at a Brillouin laser frequency ν1S=ν1−νB, that resonantly propagates around the fiber-ring optical resonator in the backward direction; and (e) the optical coupler is arranged so as to direct out of the fiber-ring optical resonator (i) an output portion of the second input portion of the pump optical signal, at the pump optical frequency ν1, to act as an optical feedback signal to the frequency-locking mechanism, and (ii) an output portion of the Brillouin laser optical signal, at the Brillouin laser frequency ν1S, to act as optical output of the laser source.
The laser source of Example 1 wherein the pump optical frequency ν1 is between about 75 THz and about 750 THz.
The laser source of Example 1 wherein the pump optical frequency ν1 is between about 120 THz and about 430 THz.
The laser source of Example 1 wherein the pump optical frequency ν1 is between about 150 THz and about 300 THz.
The laser source of any one of Examples 1 through 4 wherein the frequency-locking mechanism includes a Pound-Drever-Hall mechanism.
The laser source of any one of Examples 1 through 4 wherein the frequency-locking mechanism includes a Hänsch-Couillaud mechanism.
The laser source of any one of Examples 1 through 6 wherein the fiber-ring optical resonator includes an optical fiber greater than or equal to about 40 meters long.
The laser source of any one of Examples 1 through 6 wherein the fiber-ring optical resonator includes an optical fiber greater than or equal to about 100 meters long.
The laser source of any one of Examples 1 through 6 wherein the fiber-ring optical resonator includes an optical fiber greater than or equal to about 200 meters long.
The laser source of any one of Examples 1 through 6 wherein the fiber-ring optical resonator includes an optical fiber greater than or equal to about 500 meters long.
The laser source of any one of Examples 1 through 10 wherein the fiber-ring optical resonator comprises silica optical fiber and the Brillouin shift frequency νB is about 10.9 GHz.
A method employing the laser source of any one of Examples 1 through 11, the method comprising: (A) launching from the pump laser source into the fiber-ring optical resonator via the optical circulator the first input portion of the pump optical signal, at the pump optical frequency ν1, to propagate in the forward direction and thereby produce, from the first input portion of the pump optical signal, the Brillouin laser optical signal, at the Brillouin laser frequency ν1S=ν1−νB, that resonantly propagates around the fiber-ring optical resonator in the backward direction; (B) launching into the fiber-ring optical resonator via the optical coupler the second input portion of the pump optical signal to propagate in the backward direction; (C) using the optical coupler, directing out of the fiber-ring optical resonator the output portion of the second input portion of the pump optical signal, at the pump optical frequency ν1, to act as the optical feedback signal to the frequency-locking mechanism; (D) using the frequency-locking mechanism, controlling the pump optical frequency ν1 to maintain resonant propagation of the second input portion of the pump optical signal around the fiber-ring optical resonator in the backward direction; and (E) using the optical coupler, directing out of the fiber-ring optical resonator the output portion of the Brillouin laser optical signal, at the Brillouin laser frequency ν1S, to act as the optical output of the laser source.
The laser source of any one of Examples 1 through 11 wherein: (b′) the laser source further comprises a second pump laser source that is arranged so as to (i) produce a second pump optical signal characterized by a second pump optical frequency ν2, and (ii) launch into the fiber-ring optical resonator via the optical circulator a first input portion of the second pump optical signal to propagate in the forward direction; (d′) the fiber-ring optical resonator is arranged so as to produce from the first input portion of the second pump optical signal a second Brillouin laser optical signal, at a second Brillouin laser frequency ν2S=ν2−νB, that resonantly propagates around the fiber-ring optical resonator in the backward direction; and (e′) the optical coupler is arranged so as to direct out of the fiber-ring optical resonator an output portion of the second Brillouin laser optical signal, at the second Brillouin laser frequency ν2S, to act as second optical output of the laser source.
The laser source of Example 13 wherein the pump frequency ν1 and the second pump frequency ν2 are each between about 75 THz and about 750 THz.
The laser source of Example 13 wherein the pump frequency ν1 and the second pump frequency ν2 are each between about 120 THz and about 430 THz.
The laser source of Example 13 wherein the pump frequency ν1 and the second pump frequency ν2 are each between about 150 THz and about 300 THz.
The laser source of any one of Examples 13 through 16 wherein the laser source is arranged so as to exhibit fluctuations of an output optical difference frequency |ν2S−ν1S| only within an operationally acceptable bandwidth.
The laser source of any one of Examples 13 through 16 wherein the laser source is arranged so as to exhibit fluctuations of an output optical difference frequency |ν2S−ν1S|, over about a 0.1 second timescale, only within a bandwidth less than about 100 Hz.
The laser source of any one of Examples 13 through 16 wherein the laser source is arranged so as to exhibit fluctuations of an output optical difference frequency |ν2S−ν1S|, over about a 0.1 second timescale, only within a bandwidth less than about 0.1 Hz.
The laser source of any one of Examples 13 through 19 wherein the second pump laser source includes at least one phase modulator operated at a frequency fM and arranged so as to generate, from at least a portion of the pump optical signal at the pump optical frequency ν1, the second pump optical signal at the second pump optical frequency ν2, and the second pump optical frequency is either ν2=ν1+fM or ν2=ν1−fM.
The laser source of any one of Examples 13 through 19 wherein pump laser source and the second pump laser source include a single pump laser, operated at an optical frequency ν0, and at least one phase modulator, operated at a frequency fM and arranged so as to generate, from at least a portion of optical output of the single pump laser at the optical frequency ν0, the pump optical signal and the second pump optical signal, and wherein either (i) the pump optical frequency is ν1=ν0−fM and the second pump optical frequency is ν2=ν0+fM, or (ii) the pump optical frequency is ν1=ν0+fM and the second pump optical frequency is ν2=ν0−fM.
The laser source of any one of Examples 13 through 19 wherein pump laser source and the second pump laser source include a single pump laser, operated at an optical frequency ν0, and at least one phase modulator, operated at a frequency fM and arranged so as to generate, from at least a portion of optical output of the single pump laser at the optical frequency ν0, the pump optical signal and the second pump optical signal, and wherein the pump optical frequency is ν1=ν0±N1fM and the second pump optical frequency is ν2=ν0±N2fM, wherein N1 and N2 are integers.
A method employing the laser source of any one of Examples 13 through 22, the method comprising: (A) launching from the pump laser source into the fiber-ring optical resonator via the optical circulator the first input portion of the pump optical signal, at the pump optical frequency ν1, to propagate in the forward direction and thereby produce, from the first input portion of the pump optical signal, the Brillouin laser optical signal, at the Brillouin laser frequency ν1S=ν1−νB, that resonantly propagates around the fiber-ring optical resonator in the backward direction; (A′) launching from the second pump laser source into the fiber-ring optical resonator via the optical circulator the first input portion of the second pump optical signal, at the pump optical frequency ν2, to propagate in the forward direction and thereby produce, from the first input portion of the second pump optical signal, the second Brillouin laser optical signal, at the frequency ν2S=ν2−νB, that resonantly propagates around the fiber-ring optical resonator in the backward direction; (B) launching into the fiber-ring optical resonator via the optical coupler the second input portion of the pump optical signal to propagate in the backward direction; (C) using the optical coupler, directing out of the fiber-ring optical resonator the output portion of the second input portion of the pump optical signal to act as the optical feedback signal to the frequency-locking mechanism; (D) using the frequency-locking mechanism, controlling the pump optical frequency ν1 to maintain resonant propagation of the second input portion of the pump optical signal around the fiber-ring optical resonator in the backward direction; (E) using the optical coupler, directing out of the fiber-ring optical resonator the output portion of the Brillouin laser optical signal to act as the optical output of the laser source; and (E′) directing out of the fiber-ring optical resonator the output portion of the second Brillouin laser optical signal to act as the second optical output of the laser source.
The laser source of any one of Examples 13 through 22 wherein: (b″) the second pump laser source is arranged so as to launch into the fiber-ring optical resonator via the optical coupler a second input portion of the second pump optical signal to propagate in the backward direction; (c″) the laser source further comprises a second frequency-locking mechanism coupling the second pump laser source and the fiber-ring optical resonator, wherein the second frequency-locking mechanism is arranged so as to control the second pump optical frequency ν2 to maintain resonant propagation of the second input portion of the second pump optical signal around the fiber-ring optical resonator in the backward direction; and (e″) the optical coupler is arranged so as to direct out of the fiber-ring optical resonator an output portion of the second input portion of the second pump optical signal to act as an optical feedback signal to the second frequency-locking mechanism.
A method employing the laser source of Example 24, the method comprising: (A) launching from the pump laser source into the fiber-ring optical resonator via the optical circulator the first input portion of the pump optical signal, at the pump optical frequency ν1, to propagate in the forward direction and thereby produce, from the first input portion of the pump optical signal, the Brillouin laser optical signal, at the Brillouin laser frequency ν1S=ν1−νB, that resonantly propagates around the fiber-ring optical resonator in the backward direction; (A′) launching from the second pump laser source into the fiber-ring optical resonator via the optical circulator the first input portion of the second pump optical signal, at the second pump optical frequency ν2, to propagate in the forward direction and thereby produce, from the first input portion of the second pump optical signal, the second Brillouin laser optical signal, at the second Brillouin laser frequency ν2S=ν2−νB, that resonantly propagates around the fiber-ring optical resonator in the backward direction; (B) launching into the fiber-ring optical resonator via the optical coupler the second input portion of the pump optical signal to propagate in the backward direction; (B′) launching into the fiber-ring optical resonator via the optical coupler the second input portion of the second pump optical signal to propagate in the backward direction; (C) using the optical coupler, directing out of the fiber-ring optical resonator the output portion of the second input portion of the pump optical signal to act as the optical feedback signal to the frequency-locking mechanism; (C′) using the optical coupler, directing out of the fiber-ring optical resonator the output portion of the second input portion of the second pump optical signal to act as the optical feedback signal to the second frequency-locking mechanism; (D) using the frequency-locking mechanism, controlling the pump optical frequency ν1 to maintain resonant propagation of the second input portion of the pump optical signal around the fiber-ring optical resonator in the backward direction; (D′) using the frequency-locking mechanism, controlling the second pump optical frequency ν2 to maintain resonant propagation of the second input portion of the second pump optical signal around the fiber-ring optical resonator in the backward direction; (E) using the optical coupler, directing out of the fiber-ring optical resonator the output portion of the Brillouin laser optical signal to act as the optical output of the laser source; and (E′) directing out of the fiber-ring optical resonator the output portion of the second Brillouin laser optical signal to act as the second optical output of the laser source.
The laser source of any one of Examples 13 through 22 or Example 24 wherein an output optical difference frequency |ν1S−ν2S| is less than about 100 GHz, and the laser source further comprises a photodetector arranged so as to receive the output and the second output of the laser source and to generate therefrom an electrical output signal at the output optical difference frequency |ν1S−ν2S|.
The laser source of Example 26 further comprising an electrical frequency divider arrange so as to provide a divided electrical output signal at the frequency |ν1S−ν2S|/N, wherein N is an integer.
The laser source of any one of Examples 26 or 27 wherein the laser source is arranged so as to exhibit phase noise of the electrical output signal at the output optical difference frequency |ν1S−ν2S| less than an operationally acceptable reference phase noise level.
The laser source of any one of Examples 26 or 27 wherein the laser source is arranged so as to exhibit phase noise of the electrical output signal at the output optical difference frequency |ν1S−ν2S| less than about −90 dBc/Hz at 1 kHz offset frequency and less than about −110 dBc/Hz at 10 kHz offset frequency.
The laser source of any one of Examples 26 or 27 wherein the laser source is arranged so as to exhibit phase noise of the electrical output signal at the output optical difference frequency |ν1S−ν2S| less than about −110 dBc/Hz at 1 kHz offset frequency and less than about −130 dBc/Hz at 10 kHz offset frequency.
A method employing the laser source of any one of Examples 26 through 30, the method comprising: (A) receiving at the photodetector the optical output and the second optical output of the laser source; and (B) using the photodiode, generating from the optical output and the second optical output the electrical output signal at the output optical difference frequency |ν1S−ν2S|.
The laser source of any one of Examples 13 through 22 or Example 24 wherein an output optical difference frequency |ν1S−ν2S| is greater than about 100 GHz, and the laser source further comprises an optical or electro-optical frequency divider that is arranged so as to receive the optical output and the second optical output of the laser source and to generate therefrom a stabilized electrical output signal at an electrical output frequency fD that is less than the output optical difference frequency |ν1S−ν2S|.
The laser source of Example 32 wherein the output optical difference frequency |ν1S−ν2S| is greater than about 300 GHz, greater than about 1 THz, greater than about 10 THz, or greater than about 100 THz.
The laser source of any one of Examples 32 or 33 wherein the frequency fD is between about 0.3 GHz and about 300 GHz, between about 1 GHz and about 100 GHz, or between about 5 GHz and about 50 GHz.
The laser source of any one of Examples 32 through 34 wherein the laser source or the optical or electro-optical frequency divider is arranged so as to limit phase noise of the electrical output signal at the frequency fD to less than an operationally acceptable reference phase noise level.
The laser source of any one of Examples 32 through 34 wherein the laser source or the optical or electro-optical frequency divider is stabilized so as to limit phase noise of the electrical output signal at the frequency fD to less than about [−90−20·log(|ν1S−ν2S|/fD)] dBc/Hz at 1 kHz offset frequency and less than about [−110−20·log(|ν1S−ν2S|/fD)] dBc/Hz at 10 kHz offset frequency.
The laser source of any one of Examples 32 through 34 wherein the laser source or the optical or electro-optical frequency divider is stabilized so as to limit phase noise of the electrical output signal at the frequency fD to less than about [−110−20·log(|ν1S−ν2S|/fD)] dBc/Hz at 1 kHz offset frequency and less than about [−130−20·log(|ν1S−ν2S|/fD)] dBc/Hz at 10 kHz offset frequency.
A method employing the laser source of any one of Examples 32 through 37, the method comprising: (A) receiving at the optical or electro-optical frequency divider the optical output and the second optical output of the laser source; and (B) using the received optical output and the received second optical output, generating with the optical or electro-optical frequency divider the stabilized electrical output signal at the frequency fD.
It is intended that equivalents of the disclosed example embodiments and methods shall fall within the scope of the present disclosure or appended claims. It is intended that the disclosed example embodiments and methods, and equivalents thereof, may be modified while remaining within the scope of the present disclosure or appended claims.
In the foregoing Detailed Description, various features may be grouped together in several example embodiments for the purpose of streamlining the disclosure. This method of disclosure is not to be interpreted as reflecting an intention that any claimed embodiment requires more features than are expressly recited in the corresponding claim. Rather, as the appended claims reflect, inventive subject matter may lie in less than all features of a single disclosed example embodiment. Thus, the appended claims are hereby incorporated into the Detailed Description, with each claim standing on its own as a separate disclosed embodiment. However, the present disclosure shall also be construed as implicitly disclosing any embodiment having any suitable set of one or more disclosed or claimed features (i.e., a set of features that are neither incompatible nor mutually exclusive) that appear in the present disclosure or the appended claims, including those sets that may not be explicitly disclosed herein. In addition, for purposes of disclosure, each of the appended dependent claims shall be construed as if written in multiple dependent form and dependent upon all preceding claims with which it is not inconsistent. It should be further noted that the scope of the appended claims does not necessarily encompass the whole of the subject matter disclosed herein.
For purposes of the present disclosure and appended claims, the conjunction “or” is to be construed inclusively (e.g., “a dog or a cat” would be interpreted as “a dog, or a cat, or both”; e.g., “a dog, a cat, or a mouse” would be interpreted as “a dog, or a cat, or a mouse, or any two, or all three”), unless: (i) it is explicitly stated otherwise, e.g., by use of “either . . . or,” “only one of,” or similar language; or (ii) two or more of the listed alternatives are mutually exclusive within the particular context, in which case “or” would encompass only those combinations involving non-mutually-exclusive alternatives. For purposes of the present disclosure and appended claims, the words “comprising,” “including,” “having,” and variants thereof, wherever they appear, shall be construed as open ended terminology, with the same meaning as if the phrase “at least” were appended after each instance thereof, unless explicitly stated otherwise. For purposes of the present disclosure or appended claims, when terms are employed such as “about equal to,” “substantially equal to,” “greater than about,” “less than about,” and so forth, in relation to a numerical quantity, standard conventions pertaining to measurement precision and significant digits shall apply, unless a differing interpretation is explicitly set forth. For null quantities described by phrases such as “substantially prevented,” “substantially absent,” “substantially eliminated,” “about equal to zero,” “negligible,” and so forth, each such phrase shall denote the case wherein the quantity in question has been reduced or diminished to such an extent that, for practical purposes in the context of the intended operation or use of the disclosed or claimed apparatus or method, the overall behavior or performance of the apparatus or method does not differ from that which would have occurred had the null quantity in fact been completely removed, exactly equal to zero, or otherwise exactly nulled.
For purposes of the present disclosure and appended claims, any labelling of elements, steps, limitations, or other portions of an example or claim (e.g., first, second, etc., (a), (b), (c), etc., or (i), (ii), (iii), etc.) is only for purposes of clarity, and shall not be construed as implying any sort of ordering or precedence of the portions so labelled. If any such ordering or precedence is intended, it will be explicitly recited in the example or claim or, in some instances, it will be implicit or inherent based on the specific content of the example or claim. In the appended claims, if the provisions of 35 USC §112(f) are desired to be invoked in an apparatus claim, then the word “means” will appear in that apparatus claim. If those provisions are desired to be invoked in a method claim, the words “a step for” will appear in that method claim. Conversely, if the words “means” or “a step for” do not appear in a claim, then the provisions of 35 USC §112(f) are not intended to be invoked for that claim.
If any one or more disclosures are incorporated herein by reference and such incorporated disclosures conflict in part or whole with, or differ in scope from, the present disclosure, then to the extent of conflict, broader disclosure, or broader definition of terms, the present disclosure controls. If such incorporated disclosures conflict in part or whole with one another, then to the extent of conflict, the later-dated disclosure controls.
The Abstract is provided as required as an aid to those searching for specific subject matter within the patent literature. However, the Abstract is not intended to imply that any elements, features, or limitations recited therein are necessarily encompassed by any particular claim. The scope of subject matter encompassed by each claim shall be determined by the recitation of only that claim.
This application claims benefit of U.S. provisional App. No. 62/270,756 filed Dec. 22, 2015 in the names of Jiang Li and Kerry Vahala, said provisional application being hereby incorporated by reference as if fully set forth herein.
This invention was made with Government support under Contract Nos. W31P4Q-14-1-0001 and W911QX-13-C-0140 awarded by the U.S. Army Contracting Command. The Government has certain rights in the invention.
| Number | Date | Country | |
|---|---|---|---|
| 62270756 | Dec 2015 | US |
