CA2103412A1 - Passive temperature-insensitive fabry-perot etalons - Google Patents
Passive temperature-insensitive fabry-perot etalonsInfo
- Publication number
- CA2103412A1 CA2103412A1 CA002103412A CA2103412A CA2103412A1 CA 2103412 A1 CA2103412 A1 CA 2103412A1 CA 002103412 A CA002103412 A CA 002103412A CA 2103412 A CA2103412 A CA 2103412A CA 2103412 A1 CA2103412 A1 CA 2103412A1
- Authority
- CA
- Canada
- Prior art keywords
- etalon
- air gap
- fiber
- length
- slab
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Abandoned
Links
- BJQHLKABXJIVAM-UHFFFAOYSA-N bis(2-ethylhexyl) phthalate Chemical compound CCCCC(CC)COC(=O)C1=CC=CC=C1C(=O)OCC(CC)CCCC BJQHLKABXJIVAM-UHFFFAOYSA-N 0.000 claims abstract description 62
- 239000000835 fiber Substances 0.000 claims abstract description 33
- 230000003287 optical effect Effects 0.000 claims abstract description 9
- 239000013307 optical fiber Substances 0.000 claims description 4
- 239000011343 solid material Substances 0.000 claims 5
- 230000008859 change Effects 0.000 description 11
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 4
- 230000000694 effects Effects 0.000 description 3
- 230000007423 decrease Effects 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 2
- 239000011521 glass Substances 0.000 description 2
- 230000007246 mechanism Effects 0.000 description 2
- 239000000377 silicon dioxide Substances 0.000 description 2
- 230000008901 benefit Effects 0.000 description 1
- 230000015556 catabolic process Effects 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000006731 degradation reaction Methods 0.000 description 1
- 230000001419 dependent effect Effects 0.000 description 1
- 239000013013 elastic material Substances 0.000 description 1
- 239000002657 fibrous material Substances 0.000 description 1
- 239000000463 material Substances 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000035945 sensitivity Effects 0.000 description 1
- 230000003595 spectral effect Effects 0.000 description 1
- 239000012780 transparent material Substances 0.000 description 1
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29379—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means characterised by the function or use of the complete device
- G02B6/29395—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means characterised by the function or use of the complete device configurable, e.g. tunable or reconfigurable
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J3/00—Spectrometry; Spectrophotometry; Monochromators; Measuring colours
- G01J3/12—Generating the spectrum; Monochromators
- G01J3/26—Generating the spectrum; Monochromators using multiple reflection, e.g. Fabry-Perot interferometer, variable interference filters
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29346—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means operating by wave or beam interference
- G02B6/29358—Multiple beam interferometer external to a light guide, e.g. Fabry-Pérot, etalon, VIPA plate, OTDL plate, continuous interferometer, parallel plate resonator
- G02B6/29359—Cavity formed by light guide ends, e.g. fibre Fabry Pérot [FFP]
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/28—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals
- G02B6/293—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means
- G02B6/29379—Optical coupling means having data bus means, i.e. plural waveguides interconnected and providing an inherently bidirectional system by mixing and splitting signals with wavelength selective means characterised by the function or use of the complete device
- G02B6/29398—Temperature insensitivity
Abstract
PASSIVE TEMPERATURE-INSENSITIVE FABRY-PEROT ETALONS
ABSTRACT
Both the fiber and the bulk Fabry-Perot etalons can be made temperature insensitive by the addition of a compensator element. This element adjusts the optical length of the air-gap in the etalon cavity so as to compensate for any changes in the optical length of the fiber or the etalon slab due to ambient temperature changes.
ABSTRACT
Both the fiber and the bulk Fabry-Perot etalons can be made temperature insensitive by the addition of a compensator element. This element adjusts the optical length of the air-gap in the etalon cavity so as to compensate for any changes in the optical length of the fiber or the etalon slab due to ambient temperature changes.
Description
2iO3~12 ':.' :
PASSIVE TEMPERATURE-INSENSITIVE FABRY-PEROT ETALONS
FIET,IL OF THE l yvFN~TlQ~
The invention relates to passive arrangements for tuning Fabry-Perot etalons, and for making the resonant wavelengths of such devices insensitive to temperature ., S changes.
; .~, ~; .
" ~C~QI~N~ F T~l~
In wavelength-division muldplexed systems, there is a need for filters capable of separating the different wavelength channels. As these filters must often operate at different locadons, there is a funher need for wavelength standards in order to avoid channel collisions and to maintain system transparency. Specifically, such filters must be capable of maintaining their preset frequencies in environments in which the temperature may change. While Fabry-Perot etalons are convenient for this purpose in lightwave systems, they have the disadvantage that they tend to be temperature sensidve. One soludon to this problem is to design filters that can be preset to a lS desired wavelength, and then place them in a temperature-controlled environment in - order to avoid temperature-dependent effects. A preferred alternadve approach would be to design an etalon that is passively compensated for temperature fluctuations solely by vinue of its physical configuradon. Such a filter is then completely passive, and does not require headng elements and acdve controls to maintain its wavelength setdng in an environment in which the temperature tends to vary.
In U.S. Patent 4,861,136, an etalon is disclosed which comprises a waveguiding pordon and a non-waveguiding (i.e., air gap) pordon. It is an advantage of such an etalon that its frequency can be readily tuned simply by changing the length of the gap. However, as noted above, the opdcal length of the cavity also varies as a funcdon of temperature, thereby detuning the filter.
Accordingly, it is the object of the present invendon to provide passive temperature compensadon in a Fabry-Perot etalon.
BR~F,F n~pTU~rY OF THJ~ VF.~TlON 2103~ l 2 The opdcal length and, hence, the resonant wavelength of a Fabry-Perot etalon tends to change as a funcdon of temperature. In accordance with the present inven-don, compensators are provided that serve to counter this change in opdcal wave-S length. In an etalon comprising a length of fiber and an air gap, the compensators modify the length of the air gap in a sense to cancel any change in the length of the filter.
In a typical embodiment, the compensators are lengths of rotary connector capillaries in which the opdcal fiber is embedded. The lengths of the capillaries are precisely maintained by means of a spacing sleeve.
, In a second embodiment of the invendon, passive temperature compensation is - obtained in a Fabry-Perot slab etalon.
....
Passive tuning means are disclosed for presetting the etalon to the desired wavelength.
BRI~F nE~I~ (~E THE~R~i FIG. 1 shows a prior art Fabry-Perot etalon comprising a length of opdcal .
fiber;
FIG. 2 shows a prior art Fabry-Perot etalon comprising a length of optical fiberand an air gap;
FIG. 3 shows a passive, temperature-insensidve Fabry-Perot fiber etalon in , accordance with the present invendon including passive compensators and a spacing sleeve;
FIG. 4 shows an arrangement for maintaining the desired contact between the S spacing sleeve and the compensators, and for providing a means for pretuning the etalon to its desired wavelength;
FIG. S shows a passive. temperature-compensated Fabry-Perot slab etalon in accordance with the present invention.
D~
Referring to the drawing, FIG. I shows a prior art fiber Fabry-Perot etalon (FFP) 10 comprising a length of optical fiber 11 disposed between a pair of partially reflecting surfaces 12 and 13. Input and output fibers 14 and 15 couple optical -; 5 signals into and out of the etalon.
All the fibers are shown embedded in lengths of precision rotary connector capillaries 16, 17 and 18. The endre assembly is typically maintained in alignment by means of a split alignment sleeve 19.
The temperature sensitivity of such a structure is due to the dependence of the optical length nL of the etalon on the temperature T, as given by ~ = (na + ~L (1) where: D, is the index of refracdon of the fiber core;
anlaT is the temperature coefficient of n;
-I 15 is the thermal expansion coefficient of the fiber;
,~ and L is the physical length of the fiber.
For silica fibers, to a good approximadon, n= 1.46 ~ntifffT = 1.0 x 10'5C' and = 0.5 x 10~C '.
'ff This results in a temperature dependence of the resonant frequency of the f, etalon at 1.5 m wavelength of 1.4GHzC ' for any length of etalon.
f Ill addidon to its inherent temperature sensidvity, tuning the cavity requires some mechanism for changing the opdcal length of the cavity.
One illustrative tuning arrangement employing piezoelectric elements is disclosed in an ardcle by J. Stone and L.W. Stulz entdtled "Pigtailed High-Finesse - ~ 4 Tunable Fibre Fabry-Perot Interferometers With Large, Medium And ~al~ i~ree Spectral Ranges," published in the July 16, 1987 issue of Electrorli~l~t~, Vol. 23, No. 15, pp. 781-783. The problem with such a tuning arrangement is that the piezoelectric elements themselves are temperature sensitive, thus further complicating the problem.
FIG. 2, now to be considered, shows a modification of the simple structure of r FTG. 1, designed lo facilitate tuning. In this prior art structure (see U.S. Patent 4,861,136, assigned to applicant's assignee), the etalon includes both a section of fiber and a non-guiding portion, or gap. Referring more specifically to the figure, the etalon cavity comprises the region 20 bounded by the partially reflecting surfaces 21 and 22.
.~ A portion of region 20 includes a length of fiber 23. The balance of the cavity is the -~s air gap 24.
Coupling into and out of tbe etalon is by means of fibers 25 and 26.
As in FIG. 1, all the flbers are shown embedded in lengths of precision rotary connector capillaries 27, 28 and 29, and the entire assembly is maintained in proper alignment by means of a split alignment sleeve 30.
While the etalon shown in FIG. 2 can be conveniently tuned by changing the length of gap 24, it can also be just as easily detuned due to the temperature sensidvity of fiber 23, and the capillaries 27 and 28. If, for example, the wavelength ~;
were to increase, the length of fiber 23 would also increase, thereby decreasing the length of the gap 24. Sirnultaneously the capillaries 27 and 28 would also increase thereby tending to reduce the length of gap 24.
However, the effect of any change in the lengths of the capillaries is unpredict-able inasmuch as they are not fixed at any point along their lengths relative to the air s gap and are, therefore, free to move in either longitudinal direcdon. As2alcQn~ 12 quence, the temperature sensidvity of this structure is unpredictable.
FIG. 3, now to be considered, illustrates a passive, temperature-insensitive Fabry-Perot etalon in accordance with the present invendon, where the term "passive,"
S as used herein, means the absence of any externally applied voltages or currents.
Basically, the structure is designed such that any change in the opdcal length of the -~ etalon, as a funcdon of temperature, is compensated by the thermal changes in other lengths of glass. To accomplish this compensadon, the rotary capillaries 27 and 28 of the prior art etalon illustrated in FIG. 2 are ground down to form a region of reduced .~ 10 diameter, or annular step, and a spacing sleeve is placed between the corners of the ; step to fix the relatdve positions of the two capillaries and the etalon. This is illustrat-ed in FIG. 3 wherein the rotary capillaries 31 and 32 include annular steps 33 and 34, . respecdvely. A spacing sleeve 35 is placed between, and in contact with the steps.
~;
The effect of this arrangement is to fix the positions of the reduced diameter portions of the capillaries reladve to the etalon. As will be explained herein below, these S provide the compensadng components for the etalon. The latter include a guided portion, provided by fiber length 38, and an unguided pordon provided by gap 39.Reflecdve surfaces 40 and 41 define the physical length L of the cavity. The optical length OL of the etalon cavity is OL = nLF I LA (2) where: LF jS the length of the fiber;
LA is the air gap;
and n is the refracdve index of the fiber.
` 6 The length of the spacing sleeve L, is Ll = Ll + L2 + LF + LA ( ) where: Ll and L2 are the lengths of the reduced diarneter regions 36 and 37 of ` the capillaries.
When the temperature changes, e.g. increases, the physical length of the fiber increases, thereby decreasing the length of the air gap. In addidon, the refractive ;;i index of the fiber material changes. Simultaneously, the length of the sleeve 35 , increases as do the lengths of the reduced diameter regions 36 and 37. The resulting net change in the optical length of the etalon is given by ~i. 10 aT [(n-l)F + ~a ]LF + C4L~ - o~G(LI + L2) (4) where: aF is the expansion coefficient of the fiber;
c~, is the expansion coefficient of the spacing sleeve;
aG is the expansion coefficient of the capillaries.
The change of resonant wavelength with temperature is ~T aT LF
where: ~ is the wavelength.
It will be noted that equation (4) includes both positive and negative tertns.
, Equation (4), therefore, can be set equal to zero, provided cl, is not too large, and a relation among the parameters determined for which there is no net change in theopdcal length of the etalon as the temperature changes.
FIG. 4 shows an arrangement for maintaining the desired contact between the spacing sleeve and the compensators, and a passive tuning mechanism for pretuning the etalon to its desired wavelength. In this illustrative embodiment, the tuner comprises an assembly bracket 50 which makes a slide fit with capillaries 51 and 52 The latter are provided with shoulders 53 and 54. Springs 55 and 56, placed between the bracket arms and the capillary shoulders, force the capillaries against the spacing sleeve 57. Tuning is accomplished by means of a threaded screw 58, pushing against the alignment sleeve 59. This has the effect of dlting the etalon mirrors and thereby changing the opdcal length of the cavity. This is accomplished by rotadng the - capillaries 51 and 52 about axes perpendicular to the plane of the figure at the slide fits. Since the change in the length of the air gap 60 required to cover a free spectral-range is only half of the opdcal wavelength, very little rotadon of the capillaries is re-quired. Hence, the degradation due to tildng of the mirrors is negligible.
It will be noted that inasmuch as both the tuning and compensadon are accomplished with passive elements, the etalon can De preset at the factory, potted, if desired, and requires no further adjustments or attendon when placed into service.
;, FM. 5 illustrates the applicadon of the principles of the present invention to a buLlc etalon. In this embodiment, the cavity regio~l includes a slab 65 of transparent material, such as silica, and an air gap fonned between slab 65 and a second slab of ,; glass 68. The latter slab is the thermal compensator, as will be explained herein , below. Pardally reflecdng surfaces 67 and 69 on the outside surface of slab 65 and 3 the inside surface of slab 69 respecdvely define the resonant cavity.
The air space between slabs 65 and 68 is maintained by means of springs 70 ~! and 71 or an annular ring of an elastic material. The endre assembly is held together by means of clamps 72 and 73.
As in the cæ of the fiber etalon, as the temperature changes, e.g., increases, slab 65 expands and its refracdve index n increases. These changes increæ the opdcal length of the cavity.
Sirnultaneously, however, the increase in the size of the slab decreases the width of the air gap. This decreæs the opdcal length of the cavity. While this compensates somewhat for the increase produced by the slab, it is generally insuffi-cient to fully compensate. Full compensadon is effected by the compensator slab 68 whose size also increases with increasing temperature. Clamped at one end, the compensator expands inwardly so as to further decrease the width of the air gap. By suitable selection of materials and lengths, the net change in resonant frequenQy o~the cavity as a function of frequency can be reduced to zero at the wavelength of interest.
To tune the etalon, the entire structure is rotated so that the cavity mirrors are not normal to the light direction. Thus, both tuning and thermal compensation can be S achieved by totally passive means.
. In all cases it is understood that the above-described arrangements are illustra- ~ `
tive of but a small number of the many possible specific embodiments which can represent applications of the principles of the invention. For example, in the embodi-ment of FIG. S the clarnps can be glued to the etalon slab and the compensator slab.
:~ 10 Alternatively, the compensator slab and the clamp can be threaded so that the slab can be screwed into position. Thus, numerous and varied other arrangements can readily be devised by those skilled in the art.
;O
' .
..
PASSIVE TEMPERATURE-INSENSITIVE FABRY-PEROT ETALONS
FIET,IL OF THE l yvFN~TlQ~
The invention relates to passive arrangements for tuning Fabry-Perot etalons, and for making the resonant wavelengths of such devices insensitive to temperature ., S changes.
; .~, ~; .
" ~C~QI~N~ F T~l~
In wavelength-division muldplexed systems, there is a need for filters capable of separating the different wavelength channels. As these filters must often operate at different locadons, there is a funher need for wavelength standards in order to avoid channel collisions and to maintain system transparency. Specifically, such filters must be capable of maintaining their preset frequencies in environments in which the temperature may change. While Fabry-Perot etalons are convenient for this purpose in lightwave systems, they have the disadvantage that they tend to be temperature sensidve. One soludon to this problem is to design filters that can be preset to a lS desired wavelength, and then place them in a temperature-controlled environment in - order to avoid temperature-dependent effects. A preferred alternadve approach would be to design an etalon that is passively compensated for temperature fluctuations solely by vinue of its physical configuradon. Such a filter is then completely passive, and does not require headng elements and acdve controls to maintain its wavelength setdng in an environment in which the temperature tends to vary.
In U.S. Patent 4,861,136, an etalon is disclosed which comprises a waveguiding pordon and a non-waveguiding (i.e., air gap) pordon. It is an advantage of such an etalon that its frequency can be readily tuned simply by changing the length of the gap. However, as noted above, the opdcal length of the cavity also varies as a funcdon of temperature, thereby detuning the filter.
Accordingly, it is the object of the present invendon to provide passive temperature compensadon in a Fabry-Perot etalon.
BR~F,F n~pTU~rY OF THJ~ VF.~TlON 2103~ l 2 The opdcal length and, hence, the resonant wavelength of a Fabry-Perot etalon tends to change as a funcdon of temperature. In accordance with the present inven-don, compensators are provided that serve to counter this change in opdcal wave-S length. In an etalon comprising a length of fiber and an air gap, the compensators modify the length of the air gap in a sense to cancel any change in the length of the filter.
In a typical embodiment, the compensators are lengths of rotary connector capillaries in which the opdcal fiber is embedded. The lengths of the capillaries are precisely maintained by means of a spacing sleeve.
, In a second embodiment of the invendon, passive temperature compensation is - obtained in a Fabry-Perot slab etalon.
....
Passive tuning means are disclosed for presetting the etalon to the desired wavelength.
BRI~F nE~I~ (~E THE~R~i FIG. 1 shows a prior art Fabry-Perot etalon comprising a length of opdcal .
fiber;
FIG. 2 shows a prior art Fabry-Perot etalon comprising a length of optical fiberand an air gap;
FIG. 3 shows a passive, temperature-insensidve Fabry-Perot fiber etalon in , accordance with the present invendon including passive compensators and a spacing sleeve;
FIG. 4 shows an arrangement for maintaining the desired contact between the S spacing sleeve and the compensators, and for providing a means for pretuning the etalon to its desired wavelength;
FIG. S shows a passive. temperature-compensated Fabry-Perot slab etalon in accordance with the present invention.
D~
Referring to the drawing, FIG. I shows a prior art fiber Fabry-Perot etalon (FFP) 10 comprising a length of optical fiber 11 disposed between a pair of partially reflecting surfaces 12 and 13. Input and output fibers 14 and 15 couple optical -; 5 signals into and out of the etalon.
All the fibers are shown embedded in lengths of precision rotary connector capillaries 16, 17 and 18. The endre assembly is typically maintained in alignment by means of a split alignment sleeve 19.
The temperature sensitivity of such a structure is due to the dependence of the optical length nL of the etalon on the temperature T, as given by ~ = (na + ~L (1) where: D, is the index of refracdon of the fiber core;
anlaT is the temperature coefficient of n;
-I 15 is the thermal expansion coefficient of the fiber;
,~ and L is the physical length of the fiber.
For silica fibers, to a good approximadon, n= 1.46 ~ntifffT = 1.0 x 10'5C' and = 0.5 x 10~C '.
'ff This results in a temperature dependence of the resonant frequency of the f, etalon at 1.5 m wavelength of 1.4GHzC ' for any length of etalon.
f Ill addidon to its inherent temperature sensidvity, tuning the cavity requires some mechanism for changing the opdcal length of the cavity.
One illustrative tuning arrangement employing piezoelectric elements is disclosed in an ardcle by J. Stone and L.W. Stulz entdtled "Pigtailed High-Finesse - ~ 4 Tunable Fibre Fabry-Perot Interferometers With Large, Medium And ~al~ i~ree Spectral Ranges," published in the July 16, 1987 issue of Electrorli~l~t~, Vol. 23, No. 15, pp. 781-783. The problem with such a tuning arrangement is that the piezoelectric elements themselves are temperature sensitive, thus further complicating the problem.
FIG. 2, now to be considered, shows a modification of the simple structure of r FTG. 1, designed lo facilitate tuning. In this prior art structure (see U.S. Patent 4,861,136, assigned to applicant's assignee), the etalon includes both a section of fiber and a non-guiding portion, or gap. Referring more specifically to the figure, the etalon cavity comprises the region 20 bounded by the partially reflecting surfaces 21 and 22.
.~ A portion of region 20 includes a length of fiber 23. The balance of the cavity is the -~s air gap 24.
Coupling into and out of tbe etalon is by means of fibers 25 and 26.
As in FIG. 1, all the flbers are shown embedded in lengths of precision rotary connector capillaries 27, 28 and 29, and the entire assembly is maintained in proper alignment by means of a split alignment sleeve 30.
While the etalon shown in FIG. 2 can be conveniently tuned by changing the length of gap 24, it can also be just as easily detuned due to the temperature sensidvity of fiber 23, and the capillaries 27 and 28. If, for example, the wavelength ~;
were to increase, the length of fiber 23 would also increase, thereby decreasing the length of the gap 24. Sirnultaneously the capillaries 27 and 28 would also increase thereby tending to reduce the length of gap 24.
However, the effect of any change in the lengths of the capillaries is unpredict-able inasmuch as they are not fixed at any point along their lengths relative to the air s gap and are, therefore, free to move in either longitudinal direcdon. As2alcQn~ 12 quence, the temperature sensidvity of this structure is unpredictable.
FIG. 3, now to be considered, illustrates a passive, temperature-insensitive Fabry-Perot etalon in accordance with the present invendon, where the term "passive,"
S as used herein, means the absence of any externally applied voltages or currents.
Basically, the structure is designed such that any change in the opdcal length of the -~ etalon, as a funcdon of temperature, is compensated by the thermal changes in other lengths of glass. To accomplish this compensadon, the rotary capillaries 27 and 28 of the prior art etalon illustrated in FIG. 2 are ground down to form a region of reduced .~ 10 diameter, or annular step, and a spacing sleeve is placed between the corners of the ; step to fix the relatdve positions of the two capillaries and the etalon. This is illustrat-ed in FIG. 3 wherein the rotary capillaries 31 and 32 include annular steps 33 and 34, . respecdvely. A spacing sleeve 35 is placed between, and in contact with the steps.
~;
The effect of this arrangement is to fix the positions of the reduced diameter portions of the capillaries reladve to the etalon. As will be explained herein below, these S provide the compensadng components for the etalon. The latter include a guided portion, provided by fiber length 38, and an unguided pordon provided by gap 39.Reflecdve surfaces 40 and 41 define the physical length L of the cavity. The optical length OL of the etalon cavity is OL = nLF I LA (2) where: LF jS the length of the fiber;
LA is the air gap;
and n is the refracdve index of the fiber.
` 6 The length of the spacing sleeve L, is Ll = Ll + L2 + LF + LA ( ) where: Ll and L2 are the lengths of the reduced diarneter regions 36 and 37 of ` the capillaries.
When the temperature changes, e.g. increases, the physical length of the fiber increases, thereby decreasing the length of the air gap. In addidon, the refractive ;;i index of the fiber material changes. Simultaneously, the length of the sleeve 35 , increases as do the lengths of the reduced diameter regions 36 and 37. The resulting net change in the optical length of the etalon is given by ~i. 10 aT [(n-l)F + ~a ]LF + C4L~ - o~G(LI + L2) (4) where: aF is the expansion coefficient of the fiber;
c~, is the expansion coefficient of the spacing sleeve;
aG is the expansion coefficient of the capillaries.
The change of resonant wavelength with temperature is ~T aT LF
where: ~ is the wavelength.
It will be noted that equation (4) includes both positive and negative tertns.
, Equation (4), therefore, can be set equal to zero, provided cl, is not too large, and a relation among the parameters determined for which there is no net change in theopdcal length of the etalon as the temperature changes.
FIG. 4 shows an arrangement for maintaining the desired contact between the spacing sleeve and the compensators, and a passive tuning mechanism for pretuning the etalon to its desired wavelength. In this illustrative embodiment, the tuner comprises an assembly bracket 50 which makes a slide fit with capillaries 51 and 52 The latter are provided with shoulders 53 and 54. Springs 55 and 56, placed between the bracket arms and the capillary shoulders, force the capillaries against the spacing sleeve 57. Tuning is accomplished by means of a threaded screw 58, pushing against the alignment sleeve 59. This has the effect of dlting the etalon mirrors and thereby changing the opdcal length of the cavity. This is accomplished by rotadng the - capillaries 51 and 52 about axes perpendicular to the plane of the figure at the slide fits. Since the change in the length of the air gap 60 required to cover a free spectral-range is only half of the opdcal wavelength, very little rotadon of the capillaries is re-quired. Hence, the degradation due to tildng of the mirrors is negligible.
It will be noted that inasmuch as both the tuning and compensadon are accomplished with passive elements, the etalon can De preset at the factory, potted, if desired, and requires no further adjustments or attendon when placed into service.
;, FM. 5 illustrates the applicadon of the principles of the present invention to a buLlc etalon. In this embodiment, the cavity regio~l includes a slab 65 of transparent material, such as silica, and an air gap fonned between slab 65 and a second slab of ,; glass 68. The latter slab is the thermal compensator, as will be explained herein , below. Pardally reflecdng surfaces 67 and 69 on the outside surface of slab 65 and 3 the inside surface of slab 69 respecdvely define the resonant cavity.
The air space between slabs 65 and 68 is maintained by means of springs 70 ~! and 71 or an annular ring of an elastic material. The endre assembly is held together by means of clamps 72 and 73.
As in the cæ of the fiber etalon, as the temperature changes, e.g., increases, slab 65 expands and its refracdve index n increases. These changes increæ the opdcal length of the cavity.
Sirnultaneously, however, the increase in the size of the slab decreases the width of the air gap. This decreæs the opdcal length of the cavity. While this compensates somewhat for the increase produced by the slab, it is generally insuffi-cient to fully compensate. Full compensadon is effected by the compensator slab 68 whose size also increases with increasing temperature. Clamped at one end, the compensator expands inwardly so as to further decrease the width of the air gap. By suitable selection of materials and lengths, the net change in resonant frequenQy o~the cavity as a function of frequency can be reduced to zero at the wavelength of interest.
To tune the etalon, the entire structure is rotated so that the cavity mirrors are not normal to the light direction. Thus, both tuning and thermal compensation can be S achieved by totally passive means.
. In all cases it is understood that the above-described arrangements are illustra- ~ `
tive of but a small number of the many possible specific embodiments which can represent applications of the principles of the invention. For example, in the embodi-ment of FIG. S the clarnps can be glued to the etalon slab and the compensator slab.
:~ 10 Alternatively, the compensator slab and the clamp can be threaded so that the slab can be screwed into position. Thus, numerous and varied other arrangements can readily be devised by those skilled in the art.
;O
' .
..
Claims (11)
1. A Fabry-Perot etalon comprising: a region of solid material and an air gap located between, and bounded by a pair of partially reflecting surfaces;
passive means for tuning said etalon;
and passive compensator means, responsive to changes in temperature, for varying the optical length of said air gap.
passive means for tuning said etalon;
and passive compensator means, responsive to changes in temperature, for varying the optical length of said air gap.
2. The etalon according to claim 1 wherein said region of solid material is a section of optical fiber.
3. The etalon according to claim 1 wherein said region of solid material is a slab.
4. The etalon according to claim 1 wherein:
said region of solid material is a length of optical fiber embedded in a rotary connector capillary;
said passive compensator means includes input and output fiber sections coupled to said etalon and embedded in sections of rotary connector capillaries;and a spacing sleeve for maintaining the ends of said capillaries in fixed positions relative to said etalon.
said region of solid material is a length of optical fiber embedded in a rotary connector capillary;
said passive compensator means includes input and output fiber sections coupled to said etalon and embedded in sections of rotary connector capillaries;and a spacing sleeve for maintaining the ends of said capillaries in fixed positions relative to said etalon.
5. A Fabry-Perot etalon comprising:
a fixed length of optical fiber embedded in a rotary capillary tube and an air gap disposed between a pair of partially reflecting surfaces;
one of said reflecting surfaces being disposed between an end of said fixed length of fiber located away from said air gap, and an end of a second fiber;
the second reflecting surface being disposed across an end of a third fiber located adjacent to said air gap and opposite the other end of said length of fiber;
said second and third fibers being embedded in sections of connector capillary tubes whose diameters abruptly increase from a first value adjacent to said etalon to a second larger value at distances away from said etalon, forming a pair of annular steps;
and an annular spacing sleeve disposed along said etalon between said steps.
a fixed length of optical fiber embedded in a rotary capillary tube and an air gap disposed between a pair of partially reflecting surfaces;
one of said reflecting surfaces being disposed between an end of said fixed length of fiber located away from said air gap, and an end of a second fiber;
the second reflecting surface being disposed across an end of a third fiber located adjacent to said air gap and opposite the other end of said length of fiber;
said second and third fibers being embedded in sections of connector capillary tubes whose diameters abruptly increase from a first value adjacent to said etalon to a second larger value at distances away from said etalon, forming a pair of annular steps;
and an annular spacing sleeve disposed along said etalon between said steps.
6. The etalon according to claim 5 wherein the distance L1 between said one reflecting surface and its nearest step, and the distance L2 between said secondreflecting surface and its nearest step are selected to minimize the changes in the optical length of said etalon at a given operating frequency as a function of tempera-ture.
7. The etalon according to claim 6 including a U shaped assembly bracket having first and second apertures for receiving said connector capillaries including said second and third fibers;
said apertures being large enough to form a slide fit and thereby to permit saidcapillaries to move longitudinally within said apertures;
said capillaries further have shoulders disposed therealong between said apertures and said etalon;
and springs located between said apertures and said shoulders thereby forcing said spacing sleeve to make contact with said annular steps.
said apertures being large enough to form a slide fit and thereby to permit saidcapillaries to move longitudinally within said apertures;
said capillaries further have shoulders disposed therealong between said apertures and said etalon;
and springs located between said apertures and said shoulders thereby forcing said spacing sleeve to make contact with said annular steps.
8. The etalon according to claim 7 including:
an aligning sleeve extending between said capillaries for aligning all of said fibers;
and means pressing against the side of aligning sleeve for tuning said etalon.
an aligning sleeve extending between said capillaries for aligning all of said fibers;
and means pressing against the side of aligning sleeve for tuning said etalon.
9. The etalon according to claim 1 wherein:
said solid material is a slab. and said compensator is a slab;
and wherein said air gap is formed between said etalon slab and said compen-sator slab.
said solid material is a slab. and said compensator is a slab;
and wherein said air gap is formed between said etalon slab and said compen-sator slab.
10. The etalon according to claim 9 wherein:
a first partially reflecting surface is located along one side of said etalon slab;
a second partially reflecting surface is located along one side of said compen-sator;
said one side of said compensator being adjacent to said air gap;
pliable means, located between said slabs, for maintaining said air gap;
and clamping means for forcing said slabs toward each other.
a first partially reflecting surface is located along one side of said etalon slab;
a second partially reflecting surface is located along one side of said compen-sator;
said one side of said compensator being adjacent to said air gap;
pliable means, located between said slabs, for maintaining said air gap;
and clamping means for forcing said slabs toward each other.
11. The etalon according to claim 10 including means for tilting the planes of said reflecting surfaces relative to the direction of light propagation.
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US08/080,458 US5384877A (en) | 1993-06-21 | 1993-06-21 | Passive temperature-insensitive fabry-perot etalons |
| US080,458 | 1993-06-21 |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| CA2103412A1 true CA2103412A1 (en) | 1994-12-22 |
Family
ID=22157519
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| CA002103412A Abandoned CA2103412A1 (en) | 1993-06-21 | 1993-11-18 | Passive temperature-insensitive fabry-perot etalons |
Country Status (4)
| Country | Link |
|---|---|
| US (1) | US5384877A (en) |
| EP (1) | EP0629886A1 (en) |
| JP (1) | JPH0727943A (en) |
| CA (1) | CA2103412A1 (en) |
Families Citing this family (14)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US6310690B1 (en) * | 1999-02-10 | 2001-10-30 | Avanex Corporation | Dense wavelength division multiplexer utilizing an asymmetric pass band interferometer |
| US6304383B1 (en) * | 1999-09-17 | 2001-10-16 | Corning Incorporated | Controlled stress thermal compensation for filters |
| JP4104802B2 (en) | 2000-01-26 | 2008-06-18 | 富士通株式会社 | Gain equalization apparatus, wavelength characteristic variable apparatus and optical amplifier using air gap type etalon |
| US6860633B2 (en) * | 2001-11-30 | 2005-03-01 | Schott Technologies, Inc. | Thermal expansion measurements using Fabry-Perot etalons |
| US20040001258A1 (en) * | 2002-06-28 | 2004-01-01 | Mandeep Singh | Solid state etalons with low thermally-induced optical path length change |
| US6844975B2 (en) * | 2002-10-09 | 2005-01-18 | Jds Uniphase Corporation | Etalon devices employing multiple materials |
| US7050671B1 (en) * | 2003-01-17 | 2006-05-23 | Jds Uniphase Corporation | Tunable compensation of chromatic dispersion using etalons with tunable optical path length and non-tunable reflectivity |
| JP4046037B2 (en) | 2003-07-22 | 2008-02-13 | 豊田合成株式会社 | Drawer device |
| CN102053361A (en) * | 2010-11-24 | 2011-05-11 | 福州高意通讯有限公司 | Adjustable etalon |
| CN103048781A (en) * | 2011-10-11 | 2013-04-17 | 福州高意通讯有限公司 | MEMS (Micro-Electro Mechanical System) adjustable etalon |
| CN103792658B (en) * | 2014-02-18 | 2016-03-30 | 苏州旭创科技有限公司 | Optical standard tool |
| CN104698585B (en) * | 2015-04-01 | 2017-07-11 | 武汉理工大学 | Adjustable optic fibre F P wave filters |
| GB2563405A (en) * | 2017-06-13 | 2018-12-19 | Oclaro Tech Ltd | Tuneable filter |
| CN107817043B (en) * | 2017-09-22 | 2019-09-17 | 暨南大学 | A kind of air micro chamber fibre optic hydrophone and production method and signal detecting method |
Family Cites Families (6)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4830451A (en) * | 1986-03-05 | 1989-05-16 | American Telephone And Telegraph Company | Technique and apparatus for fabricating a fiber Fabry-Perot etalon |
| US4861136A (en) * | 1987-07-15 | 1989-08-29 | American Telephone And Telegraph Company | Optical communication systems using fabry-perot cavities |
| US5073004A (en) * | 1990-05-18 | 1991-12-17 | At&T Bell Laboratories | Tunable optical filter |
| US5061857A (en) * | 1990-11-09 | 1991-10-29 | The United States Of America As Represented By The Secretary Of The Navy | Waveguide-binding sensor for use with assays |
| US5212745A (en) * | 1991-12-02 | 1993-05-18 | Micron Optics, Inc. | Fixed and temperature tuned fiber fabry-perot filters |
| US5212746A (en) * | 1991-12-02 | 1993-05-18 | Micron Optics, Inc. | Single wafered ferrule fiber fabry-perot filters |
-
1993
- 1993-06-21 US US08/080,458 patent/US5384877A/en not_active Expired - Lifetime
- 1993-11-18 CA CA002103412A patent/CA2103412A1/en not_active Abandoned
-
1994
- 1994-06-07 EP EP94304100A patent/EP0629886A1/en not_active Withdrawn
- 1994-06-20 JP JP6159669A patent/JPH0727943A/en active Pending
Also Published As
| Publication number | Publication date |
|---|---|
| EP0629886A1 (en) | 1994-12-21 |
| JPH0727943A (en) | 1995-01-31 |
| US5384877A (en) | 1995-01-24 |
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| Date | Code | Title | Description |
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| EEER | Examination request | ||
| FZDE | Discontinued |