CA2020219C - Radiation switching arrangement with moving deflecting element - Google Patents
Radiation switching arrangement with moving deflecting elementInfo
- Publication number
- CA2020219C CA2020219C CA002020219A CA2020219A CA2020219C CA 2020219 C CA2020219 C CA 2020219C CA 002020219 A CA002020219 A CA 002020219A CA 2020219 A CA2020219 A CA 2020219A CA 2020219 C CA2020219 C CA 2020219C
- Authority
- CA
- Canada
- Prior art keywords
- optical
- deflecting element
- mirror
- port
- arrangement
- 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.)
- Expired - Lifetime
Links
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
- G02B6/35—Optical coupling means having switching means
- G02B6/351—Optical coupling means having switching means involving stationary waveguides with moving interposed optical elements
- G02B6/3524—Optical coupling means having switching means involving stationary waveguides with moving interposed optical elements the optical element being refractive
-
- 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
- G02B6/32—Optical coupling means having lens focusing means positioned between opposed fibre ends
-
- 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
- G02B6/35—Optical coupling means having switching means
- G02B6/351—Optical coupling means having switching means involving stationary waveguides with moving interposed optical elements
- G02B6/3512—Optical coupling means having switching means involving stationary waveguides with moving interposed optical elements the optical element being reflective, e.g. mirror
- G02B6/3514—Optical coupling means having switching means involving stationary waveguides with moving interposed optical elements the optical element being reflective, e.g. mirror the reflective optical element moving along a line so as to translate into and out of the beam path, i.e. across the beam path
-
- 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
- G02B6/35—Optical coupling means having switching means
- G02B6/351—Optical coupling means having switching means involving stationary waveguides with moving interposed optical elements
- G02B6/3524—Optical coupling means having switching means involving stationary waveguides with moving interposed optical elements the optical element being refractive
- G02B6/3528—Optical coupling means having switching means involving stationary waveguides with moving interposed optical elements the optical element being refractive the optical element being a prism
-
- 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
- G02B6/35—Optical coupling means having switching means
- G02B6/354—Switching arrangements, i.e. number of input/output ports and interconnection types
- G02B6/3562—Switch of the bypass type, i.e. enabling a change of path in a network, e.g. to bypass a failed element in the network
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- 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
- G02B6/36—Mechanical coupling means
- G02B6/3628—Mechanical coupling means for mounting fibres to supporting carriers
- G02B6/3648—Supporting carriers of a microbench type, i.e. with micromachined additional mechanical structures
- G02B6/3652—Supporting carriers of a microbench type, i.e. with micromachined additional mechanical structures the additional structures being prepositioning mounting areas, allowing only movement in one dimension, e.g. grooves, trenches or vias in the microbench surface, i.e. self aligning supporting carriers
-
- 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
- G02B6/36—Mechanical coupling means
- G02B6/3628—Mechanical coupling means for mounting fibres to supporting carriers
- G02B6/3684—Mechanical coupling means for mounting fibres to supporting carriers characterised by the manufacturing process of surface profiling of the supporting carrier
- G02B6/3692—Mechanical coupling means for mounting fibres to supporting carriers characterised by the manufacturing process of surface profiling of the supporting carrier with surface micromachining involving etching, e.g. wet or dry etching steps
-
- 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
- G02B6/36—Mechanical coupling means
- G02B6/3628—Mechanical coupling means for mounting fibres to supporting carriers
- G02B6/3684—Mechanical coupling means for mounting fibres to supporting carriers characterised by the manufacturing process of surface profiling of the supporting carrier
- G02B6/3696—Mechanical coupling means for mounting fibres to supporting carriers characterised by the manufacturing process of surface profiling of the supporting carrier by moulding, e.g. injection moulding, casting, embossing, stamping, stenciling, printing, or with metallic mould insert manufacturing using LIGA or MIGA techniques
Abstract
A three or four-port electromagnetic radiation signal beam switching arrangement, such as for simple optical re-routing or for Local Area Network (LAN) loop switching, is achieved with a moving deflecting element having a planar deflecting surface that is constrained to move parallel to itself, into and out of the signal beam. The arrangement can be fabricated in a silicon optical workbench technology.
Description
RADIATION SWITCHING ARRANGEMENT WITH MOVING
DEFLECTING ELEMENT
Technical Field This invention relates to the field of the switching of beams of 5 electromagnetic radiation and more particularly to arrangements for the switching of optical beams by switching the output of one optical port selectively into either one of a pair of other optical ports, where each port is typically either an exit or an entry end of an optical fiber (optical waveguide).
Back~round of the Invention In telecc,.-.,.. ~-ic~tion or other systems using electromagnetic radiation signal beams, it is often desirable to switch a beam of electromagnetic r~ ti~-narriving at an input optical port selectively into either one of a pair of output ports--for example, to switch an optical signal beam arriving at the output end of an input optical fiber selectively into either one of a pair of exit optical fibers depending upon 15 a switching control signal at any moment of time. More specifically, in a teleco~u, ication switching system, it is often desired to reroute an optical colllmullication path--that is, to switch an optical path (IA), running from a given input fiber (I) to a first output optical fiber (A), into a second path (IB), running from the input fiber (I) to a second output optical fiber (B), and to switch the second path 20 (IB) back into the first path (IA).
For another example, a local area network (LAN) typically includes a main co",puler station (M) and an optical fiber LAN loop (ring) composed of fiber segments arranged in a loop, together with local stations (X, Y, Z...) located at the junctions of successive fiber segments. Each of the local stations typically 25 compri~es a separate local personal computer or the like. Optical switching arrangements are required to bypass local stations that are defective or to bypass all local stations in cases where a defect in the loop itself occurs.
Prior art is exemplified by the optical switching arrangement described in a paper by M. Nunoshita et al, published in Optics Letters, vol. 4, No. 1, pp. 27-28 30 (1979). In that paper, optical switches for the above-described purposes employed a moving lens to switch the optical paths. But such switches are very clumsy and costly, primarily because of the need to move relatively heavy piece parts rather quiclcly. Moreover, the conventional machine-made parts required for these switches lack sufficient precision of optical alignrnent to be used in conjunction with optical 35 fibers unless undesirably costly and time-consuming alignment procedures for each switch are performed. Furthermore, long-term stability and reliability are problematical because of aging phenomena associated with parts having differing mechanical andthermal properties. In addition, these switches do not enable temporarily non-acc~cced 5 (off-line) local stations in a LAN to perform desired self-testing operations in conjunction with the local optical source, unless extra added complexity is introduced:
for example, the added complexity of extra fiber, which can be added as described in Electro-Optic Products, Application Note 102, Figure 4 therein, published by Siecor Corp., Research Triangle Park, NC 27709. Furthermore, in the switches described in 10 that Siecor publication, mechanical stops are required, which tend to wear out in use and which cause the optical components to vibrate immediately after switchings in such a direction as to jitter the beam undesirably.
It would therefore be desirable to have an optical signal switching arrangement, and more generally an electromagnetic signal switching arrangement,15 which mitigates the above shortcomings in the prior art.
Summary of the Invention The foregoing shortcomings are mitigated by an electromagnetic radiation switching arrangement which comprises:
(a) a radiation deflecting element having a planar deflecting surface;
DEFLECTING ELEMENT
Technical Field This invention relates to the field of the switching of beams of 5 electromagnetic radiation and more particularly to arrangements for the switching of optical beams by switching the output of one optical port selectively into either one of a pair of other optical ports, where each port is typically either an exit or an entry end of an optical fiber (optical waveguide).
Back~round of the Invention In telecc,.-.,.. ~-ic~tion or other systems using electromagnetic radiation signal beams, it is often desirable to switch a beam of electromagnetic r~ ti~-narriving at an input optical port selectively into either one of a pair of output ports--for example, to switch an optical signal beam arriving at the output end of an input optical fiber selectively into either one of a pair of exit optical fibers depending upon 15 a switching control signal at any moment of time. More specifically, in a teleco~u, ication switching system, it is often desired to reroute an optical colllmullication path--that is, to switch an optical path (IA), running from a given input fiber (I) to a first output optical fiber (A), into a second path (IB), running from the input fiber (I) to a second output optical fiber (B), and to switch the second path 20 (IB) back into the first path (IA).
For another example, a local area network (LAN) typically includes a main co",puler station (M) and an optical fiber LAN loop (ring) composed of fiber segments arranged in a loop, together with local stations (X, Y, Z...) located at the junctions of successive fiber segments. Each of the local stations typically 25 compri~es a separate local personal computer or the like. Optical switching arrangements are required to bypass local stations that are defective or to bypass all local stations in cases where a defect in the loop itself occurs.
Prior art is exemplified by the optical switching arrangement described in a paper by M. Nunoshita et al, published in Optics Letters, vol. 4, No. 1, pp. 27-28 30 (1979). In that paper, optical switches for the above-described purposes employed a moving lens to switch the optical paths. But such switches are very clumsy and costly, primarily because of the need to move relatively heavy piece parts rather quiclcly. Moreover, the conventional machine-made parts required for these switches lack sufficient precision of optical alignrnent to be used in conjunction with optical 35 fibers unless undesirably costly and time-consuming alignment procedures for each switch are performed. Furthermore, long-term stability and reliability are problematical because of aging phenomena associated with parts having differing mechanical andthermal properties. In addition, these switches do not enable temporarily non-acc~cced 5 (off-line) local stations in a LAN to perform desired self-testing operations in conjunction with the local optical source, unless extra added complexity is introduced:
for example, the added complexity of extra fiber, which can be added as described in Electro-Optic Products, Application Note 102, Figure 4 therein, published by Siecor Corp., Research Triangle Park, NC 27709. Furthermore, in the switches described in 10 that Siecor publication, mechanical stops are required, which tend to wear out in use and which cause the optical components to vibrate immediately after switchings in such a direction as to jitter the beam undesirably.
It would therefore be desirable to have an optical signal switching arrangement, and more generally an electromagnetic signal switching arrangement,15 which mitigates the above shortcomings in the prior art.
Summary of the Invention The foregoing shortcomings are mitigated by an electromagnetic radiation switching arrangement which comprises:
(a) a radiation deflecting element having a planar deflecting surface;
2 0 (b) moving means for moving the deflecting element such that the planar surface thereof moved parallel to itself from a first region to a second region and from the second to the first region;
(c) first, second, and third radiation ports that are respectively located such that when the deflecting element is in the first region a radiation signal beam 2 5 arriving at the switching arrangement at the first port propagates through the location of the second position and enters into the second port, and such that when the deflecting element is moved by the moving means into the second region the signal beam arriving at the first port is deflected by the planar surface of the deflecting element into the third port, and 3 o (d) a substrate having a major planar surface and having first, second, and third waveguide alignment recesses therein at the surface thereof which determine respective first, second, and third port positions of the first, second, and third ports, respectively, and having a pair of deflecting element alignment recesses therein at the surface thereof for aligning the deflecting element with ~3~ 2020219 respect to the first, second, and third port positions.
Typically each port comprises an end of a waveguide, such as a millim--ter waveguide or an optical waveguide (fiber).
In a specific embolim~ont, the radiation is optical, the deflecting element S is a mirror, and the n~s~ /e ports are l~,;,pccl,~e ends of optical fibers. The mirror is held by a holder (header) which has a pair or recesses. This pair of recesses is aligned to another pair of recesses, for aligning the mirror, which have been lithographed in a silicon substrate, and each of a pair of ball-bearings fits into a respective of the pair of aligned recesses. The fibers are aligned with respect to one 10 another and to the mirror by setting the respective fibers into respective elongated recesses for aligning optical fibers. The fibers are aligned to one another and with respect to the mirror by setting the respective fibers into respective elongatedrecesses, adapted for aligning optical fibers, all of which have been lithographed in the silicon substrate simult~neously with the recesses into which the ball-bearings fit 15 In this way, the desirable alignment precision of "silicon wolL~nch" technology is achieved. Also, advantageously a planar reflecting surface of the mirror is constrained by the ball-bearings to move parallel to itself, so that jitter of the optical beam is avoided when the mirror stops moving during a switching operation, even if the mirror stops suddenly.
This switching arrangement can be modified in order to have an optical ~wilching arrangement suitable for an optical fiber loop in a LAN. Specifically, to the just described arrangement there is added a fourth port in the form of a fourth optical fiber segment which is set in yet another elongated recess in the substrate. At the same time, a local optical source is located at the local station and is positioned 25 so as to deliver a second optical signal beam to this fourth fiber segment, and a local photodetector is located at the local station and is positional so as to receive the optical beam after entering into and propagating through the third fiber segment. In this way, the optical beam arriving at the first pon stems from the LAN loop, and the second optical beam arriving at the fourth port stems from the local optical source, 30 and the switching arrangement can be used in a LAN as described above, with the added feature that when the deflecting element of a local station is in the first region (off-line) self-testing operations at that local station can be performed with adesirably lower effective optical intensity by virtue of the offset of the third and fourth fiber segments.
-~4- 2020219 Brief Description of the Drawin~
This invention together with its fea~ ;s, characteristics, and advantages -may be better understood from the following detailed description when read in conjunction with the drawings in which FIG. 1 is a schem~tic diagram of a three-port optical ~ ching arrangement in accordance with a specific embalim~nt of the invention;
FIG. 2 is a schematic diagram of the embo lim~nt shown in FIG. 1 with a mirror moved into the optical path;
~ FIG. 3 is an assembly view of a switching assembly, comprising the 10 embodiment shown in FIGS. 1 and 2, integrated in silicon workbench technology, in accordance with another specific embodiment in the invention;
FIG. 4 is a cross section view of a portion of the embodiment shown in FIGS. 1 and 2 (with optical fibers not in place, only for the sake of clarity) in accordance with a specific embodiment of the invention;
FIG. 5 is an assembly view of a four-port optical switching assembly suitable for use in a LAN, in accordance with another specific embodiment of theinvention;
FIG. 6 is a top view of the embodiment shown in FIG. 6 with the mirror out of the optical path;
FIG. 7 is a top view of the embodiment shown in FIG. 6 with the mirror in the optical path;
FIG. 8 is a diagram of a LAN in accordance with another embodiment of the invention;
FIG. 9 is a diagram of a typical local station which is off^line in the 25 LAN shown in FIG. 8;
FIG. 10 is a diagram of a typical local station which is on-line in the LAN shown in FIG. 8; and FIG. 11 is a cross-section diagram of an optical coupler in accordance with another embodiment of the invention.
FIGS. 12-13 are top views a part of a four-port optical switching assembly, in accordance with yet another specific embodiment of the invention;
FIG. 14 is a perspective view, partially in cross section, of a mirror suitable for use in a four-port optical switching assembly, in accordance with still another specific embodiment; and FIGS. 15-16 are top views of a four-port optical ~wi~ching assembly, in accordance with yet another specific embodiment of the invention;
FIGS. 17-18 are top views of part of a three-port optical switching assembly, in accordance with still another specific embodiment of the invention; and FIGS. 19-20 are top views of part of a four-port optical switching assembly, in accordance with still another specific embo-1iment of the invention.
Only for the sake of clarity, none of the drawings is to scale.
Detailed Des~ tion As shown in FIGS. 1 and 2, a three-port (one input, two output) optical ~wilchi~lg arrangement 10 (FIG. 1) or 20 (FIG. 2) has a mirror M which is positioned either out of the optical path (E;IG. 1) or in the optical path (FIG. 2). In both ~ihl~tion~ (FIGS. 1 and 2), the switching arrangement 10, 20 has first, second and third optical ports Pl, P2, and P3, which are formed by respective proximate ends of Srst, second, and third optical fiber segments Fl, F2, and F3. The switching arrangement 10, 20 further comprises first, second and third lenslets Ll, L2, and L3 which serve to collimate the respective optical beams em~n~ting from the first fiber Fl, entering into the second Sber F2 (FIG. 1), or entering into the third fiber F3 (FIG. 2). Optical radiation for the optical beams is supplied by a light source L and is collected by utili7~tion means Ul (FIG. 1) or U2 (FIG. 2). The mirror M (FIG.2) 20 has a frontal planar reflecting surface MSI and may also have another reflecting surface parallel thereto, such as rear planar reflecting surface MS2.
The switching arrangement 10, 20 can advantageously be integrated in a silicon workbench technology assembly, to form an optical switching assembly 30 (FIG. 3). Here the same reference labels are used as were used in FIGS. 1 and 2 to 25 refer to the same or similar elements or piece-parts.
On a major planar surface PS of a silicon substrate S, for alignment purposes there is a plurality of recesses (indentations or grooves) that are cut into the substrate S, including a mirror recess MR into which fits the mirror M. Other recesses cut into the substrate S include: first, second, and third fiber recesses FRl, 30 FR2, FR3; first, second, and third lenslet recesses LRl, LR2, and LR3; and first and second substrate ball recesses SBRl and SBR2 for receiving and holding in place a pair of identical ball-bearings B 1 and B2. The mirror M is integral with a silicon header (holder) H. This header has a pair of mirror ball-bearing recesses MBRl and MBR2 that are registerable with a pair of identical substrate-ball-bearing recesses 35 SBRl and SBR2 for receiving and holding in place the ball-bearings B 1 and B2. To prevent scratching of the mirror surface MS 1, the mirror recess MR is made -sufficiently wide to prevent the reflecting surface(s) of the mirror from touching the sides of this mirror recess MR especially when the mirror moves in and out of this recess. The mirror recess MR and the ball-bearing recesses SBRl, SBR2, MBRl, and MBR2 are all mutu~lly located for the desired mutual ~lignm~ont of the mirror 5 surface MSl, the lenslets Ll, L2, and L3, and the fiber segments Fl, F2, and F3.
FIG. 4 is a cross section view of the portion the header H and substrate S
in~ te~l by the line 4-4 in FIG. 3. Here in FIG. 4, the front header surface cross section FHS is typically a <110> plane of a mono-crystalline silicon body of which the header H is composed, and the mirror M is an integral part of the ~me silicon 10 body, as formed by known lithographic masking and anisotropic etching techniques.
The front substrate surface FSS cross section of the substrate S is typically a <100>
plane of a monocrystalline silicon body of which the substrate S is composed.
The header H can move in a rotary motion about the axis formed by joining the centers of the ball-bearings B 1 and B2. Hence the planar surface MS 1 15 (and MS2) of the mirror M is constrained to move parallel to itself, i.e., with no lateral displacement. Thus the right-hand edge of the mirror M (FIGS. 3 and 4) can move smoothly into and out of the mirror recess MR, depending upon a suitable force G (or distribution of forces) applied at a point (or region) at the top of the header H located to the left of the aforementioned axis through the ball-bearings B 1 20 and B2. This force G is applied in accordance with a function of time that is suitable for the desired switching. The force G gives rise to a counle,~lockwise torque when G is directed downward as shown in FIG. 4, and hence tends to move the relevant part of the mirror M (where the light beam is incident) out of the optical path in the switching arrangement 10, 20; and this force G gives rise to a clockwise torque when 25 G is directed upward (not shown), and hence tends to move the mirror M into the optical path. Thus, during switching operations, the direction of G determines the movement of the mirror M to produce the condition of the ~wilching arrangement 10 vs. 20 (FIG. 1 vs. FIG. 2).
It should be noted that jittering (random) motion of the mirror M
30 upward or downward does not impair optical alignment, because the alignment is completely determined by the identic~l ball-bearings Bl and B2 fitting into the identical recesses SBRl and SBR2 which are located and aligned such that the mirror is constrained to move in a direction perpendicular to the place defined by the fibers Fl, F2, and F3. In this way, mechanical vibrations which tend to produce 35 relative motion between the substrate and the mirror do not adversely affect the optical tr~nsmi~sion, because the otherwise adverse transverse relative motion is suppressed by the rigidity of ball-bearings B 1 and B2 in the recesses SBRl and SBR2.
The lenslets Ll, L2, and L3 are typically made of sapphire (n=1.7) or of high index (about 1.7 to 1.9) glass. The ball bearings B 1 and B2 are conveniently 5 made of the same material as are the lenslets.
FIG. 5 shows an assembly view of a four-port (two input, two output) optical switching ~csembly 50 suitable for use in a LAN. The ~cs~mbly 50 can be viewed as being derived from the previously described optical switching assembly30 by the addition of a fourth port formed by fiber segment F4 fitting into fiber 10 recess FR4, together with lenslet L4 fitting into lenslet recess LR4, plus a second mirror surface MS2 of the mirror M parallel to the first surface MS 1.
FIG. 6 shows a top view of the assembly 50 when the mirror M is out of the optical path (off-line, by-pass mode). As in~ ate~d in FIG. 6, when the mirror M
is located in a position which is thus outside of the optical path, optical radiation 15 exiting from the first fiber segment Fl then passes the swilchi-lg arrangement 60 into the second fiber F2. At the same time, an optical beam propagating in the fourthfiber segment F4 from another light source (not shown) passes into the fiber segment F3 but with an ~tten~latecl optical intensity (infli~ate~ by a dotted line), owing to a deliberately selected offset distance _ of fiber segment F3 relative to fiber segment 20 F4 (together with the same offset in their respective lenslets L3 and L4). The thus attenuated beam entering into the fiber segment F3, is useful for self-tesdng operadons as more fully described below. An absorber A can be added, if need be,to absorb the (excess) light coming from the fiber segment F4, i.e., to absorb the light which does not enter into the fiber segment F3.
FIG. 7 shows a top view of the ~wilchillg assembly 50 (FIG. 5) when the mirror is in the path of the optical beam (acdve mode). As indicated in FIG. 7, when the mirror M is thus moved into the opdcal path, the opdcal beam exidng from thefiber segment Fl is passed into the switching arrangement 70 where it is reflected by the first surface MS 1 of the mirror M and directed into the third fiber segment F3.
30 At the same time, light exiting from the fiber segment F4 is reflected by the second surface MS2 of the mirror M and enters into ~he fiber segment F2. By making the thickness (distance between frontside and ba~cide) of the mirror M equal to d/~ (=d cos 45 ), if the arrangement 60 is aligned properly, so also will the arrangement 70 be aligned properly. In pardcular, in FIG. 6 subst~nti~lly all of the 35 beam exiting from Fl will enter into F2, and only a pordon of the cross secdon of the beam exidng from F4 will enter into F3; whereas in FIG. 7 subst~nti~lly all of the beam exiting from Fl will enter with F3, and substantially all of the beam exiting from F4 will enter into F2.
FIG. 8 shows a LAN loop 800 composed of a plurality of similar local stations exemplified by a typical local station composed of node 80 together with the S four-port optical ~witching assembly 50 described above. For example, there are a total of six such local stations interconnected by six fiber segm~ntc. One of the stations may typically function as a main station, but in any event it operates in similar manner as the others insofar as relevant here.
FIG. 9 shows a typical local station which is in the off-line condition 10 (by-pass mode). As in tic~teA in FIG. 9, when the mirror (not shown) in the switching assembly 50 is not in the optical path, a trAnsmitter Tx, such as a light ernitting diode (LED), sends a light beam into fiber segment F4 which is partially propagated by the ~wilchihlg assembly 50 (as per FIG. 6) into fiber segment F3 and ultimately to a utilization means, such as a PIN photodiode receiver Rx, whereas15 optical radiation propagating through fiber segment Fl passes through the switch 50 nnflictllrbed and enters into the fiber segment F2. The beam thus propag~ting from Fl to F2 goes on to the next local station, whereas the beam propagating from F4 to F3 can be used for testing the photo-electronics of the node 80. Thus the situation of the node 80 in FIG. 9 is the off-line (by-pass) mode.
Fig. 10 shows the typical local station in its on-line condition (active mode), i.e., with the mirror in the optical path. As indicated in FIG. 10, when the rnirror M (not shown) is moved into the optical path, the optical beam e-m~n~ting from fiber segment Fl enters into the receiver Rx, whereas the optical beam em~n~ting from the tr~n~.-.;lter Tx enters into the fiber segment F2. Thus, the 25 situation depicted in FIG. 10 is the on-line mode of the node 80, wherein theelectronics of the node 80 utilizes and processes the information on the beam çm~n~ting from the fiber segment F1, and in response thereto the node 80 then transmits its own processed information to the fiber segment F4.
FIG. 11 is a design of an optical coupling arrangement, for coupling 30 together a pair of fiber segments, such as F1 and F2, to their respective lenslets Ll and L2 in the above-described switching arrangelllen~s. More specifically, for example, the space between the fiber segment Fl and its lenslet Ll is filled with a transparent medium R1, such as silicone rubber, having a refractive index which is approximately equal to that of the segment Fl, typically about 1.5. In this way,35 unwanted reflections at the interface of F1 with R1 are avoided. At the same time the more desirable collim~ted beam optics (parallel beam between L1 and L2) is -9- 20XU~19 achieved rather than converging beam optics (rays coming to a focus ~l~..xn Ll and L2). Similarly, the space between L2 and F2 is ~led with a similar tran~ale.lt medium R2.
Note that in FIGS. 6 and 7, the offset ~lict~nce _ arises in the ~witching S assembly 60 because of the non-vanishing thirlrness of the mirror M. This offset causes optical loss into the absorber A, which can be undesirable in cases where the redirection of optical intensity, as is desired in self-testing, is not desired. To avoid this possibly undesirable situation, the optics of the assembly can be mo~lifi~ for example, as shown in FIGS. 12-13 or 14 or 15-16 or 17-18 or 19-20. In all these 10 FIGURES, the same reference labels are used to denote elementc that are similar to those described above. In particular, all the lenslets are set in respective recesses in the substrate S (FIG. 5) as are the associated fibers, the recesses being located at respective positions that are determined by silicon workbench technology.
FIGS. 12-13 depict the lenslets Ll, L2, L3, and L4 in a configuration for 15 use in a switching assembly of the kind described above (FIG. 5). The rem~inder of the assembly (not shown in FIGS. 12-13) should be understood to be the same as the ~wilching ~csem~ly 50 shown in FIG. 5. Here in FIGS. 12-13, a pair of auxiliary mirrors AMl and AM2 are fixedly attached either to the substrate S (FIG. 5) or to the header H and are oriented parallel to the mirror M, whereby the optical path20 between the fibers F4 and F3 does not suffer from any offset, as is desir~
FIG. 14 depicts a mirror 140 which, when used as the mirror M attached to the header H in the switching assembly 50 (FIG. 5), likewise avoids the offset.
Here in FIG. 14, the mirror 140 includes a silicon parallel slab 144 having its front surface MSl coated with a thin layer 141 made of suitable transparent material, 25 typically silicon dioxide, having a thickness such that it acts as an anti-reflection co~ting The bottom half of the rear surface MS2 of the slab 144 is likewise coated with a simil~rly thin layer 142 of the transparent m~teri~l, whereas the top half of the rear surface MS2 is coated with a thin reflecting layer 143, made of suitable optically reflecting m~teri~l, such as a metal having a thickness of about lOOnm. This mirror 30 140 can then be used in the switching assembly 50 in the following m~nner To put the assembly with the mirror 140 into the by-pass mode depicted in FIG. 6, the mirror 140 is moved upward into a position such that the optical paths among thelenslets pass through bottom (transparent) half of the mirror 140. In this way, the dielectric portion of merely the mirror deflects (refracts) the beam slightly and 35 directs the beam along the appropliate optical path. To achieve the active mode (FIG. 7), the mirror 140 is moved downward such that the optical paths pass through -the top (reflecting) half of the mirror 140--while the bottom half of the mirror is sinl~te~l in the mirror recess MR (E~IG. 5). In this way the mirror 140 reflects the optical beams incident upon the front and rear sl~ ces of the reflecting layer 142, which has negligible thickness and hence introduces negligible offset.
FIGS. 15-16 depict an arrangement of lenslets and fibers to avoid the offset, in accordance with yet another embo limP-nt Here in FIGS. lS-16, the fibers F1, F2, F3, and F4 serve the same respective functions as in FIGS. 6-7, but they are all located on the same (front) side of mirror M. On the other (rear) side of the mirror M, auxiliary fibers AF1, AF2, and AF3--together with auxiliary lenslets AL1, AL2, and AL3--are located (FIG. 16) in respective alignment with these fibers F1, F2, and F3. Note that only three main lenslets L1, L2, and L3 are required, the lenslet L1 doing double duty by passing two mllt l~lly orthogonal beams simlllt~neously. The auxiliary fiber AF1 is connected at its rear end by a connecting fiber CF1 to the rear end of the auxiliary fiber AF3, and the allxili~ry fiber AF2 is 15 connected at its rear end by a connecting fiber CF4 to the rear end of the auxiliary fiber AF4. In this way, when the mirror M is moved into a position located in the paths of the optical beams, as shown in FIG. 15, the by-pass (off-line) mode is obtained. In particular, light exiting from Fl goes to F2 by way of a path through L1, reflection by mirror M, and through L2; and light exiting from F4 goes to F3 by 20 way of a path through L1, reflection by mirror M, and through L3. And when the mirror M is moved into a position located outside of the paths of the optical beams, as shown in FIG. 16, the active (on-line) mode is achieved. That is, light exiting from F1 goes to F3 via Ll, AL1, AFl, CFl, AF3, AL2, and L3; and light exiting from F4 goes to F2 via Ll, AL4, AF4, CF2, AF2, AL2, and L2.
It should be understood that the location of all the lenslets and fibers shown in FIGS. 15-16 again are determined by recesses in the substrate S (FIG. 5), advantageously in accordance with silicon workbench technology, and that the position of the mirror M in FIGS. 15-16 is determined by ball-bearings (not shown in FIGS. 15-16) located in recesses, i.e., in the same way as the position of the mirror 30 M in FIG. 5.
It should also be understood that in FIGS. 15-16 the positions of the fibers F2 and F3 can be interchanged, and at the same time the respective lenslets L2 and L3 are interchanged. In that case, the active (on-line) mode is obtained in the configuration shown in FIG. 15, whereas the by-pass (off-line) mode is obtained in 35 the configuration shown in FIG. 16.
Instead of the reflecting mirror M, an optically refracting elem~nt can be - used, for example, in the form of a parallel refracting slab (plate) RS, i.e., a parallel plate composed of an optically refracting medium--as illustrated, for example, in the three-port configuration shown in FIGS. 17-18 (fibers Fl, F2, F3 not shown) and in S the four-port configuration shown in FIGS. 19-20 (fibers Fl, F2, F3, F4 not shown).
It should be understood here that optical fibers (not shown in FIGS. 17-18 or FIGS.
19-20) should be aligned as shown in FIGS. 3 and 5. In particular (FIGS. 17-18),refracting slab RS is ~si~ned --for example, as to thickness and refractive index--such that, when it is moved into the optical path as constrained by ball-be~nngc B 1 10 and B2 in their respective recesses (FIG. 4), it refracts the optical beam by an amount sl.fficient to deliver the beam to a different lenslet--e.g., to the lenslet L3 (E;IG. 18) instead of L2 (FIG. 17). Note that the front and rear planar surfaces of the refracting slab RS are both constrained to move parallel to themselves, respectively.
In nG. 20, ALl and AL2 are auxiliary lenslets connected by a 15 connecting fiber CF, whereby the arrangement (FIGS. 19-20) can be used in a four-port optical switching assembly similar to the one depicted in nG. ~7.
Notice that in connection with all cases described above, the position and orient~tion of the min~r M or 140 (FIG. 14), or of the parallel refracting slab RS
(FIG. 18), is dcle ...;.-ed by the positions of ball-bearings Bl and B2 which fit into 20 the recesses SBRl and SBR2. These positions of these ball-bearings in these recesses reliably determine an axis around which the mirror M rotates in response to the applied force(s) G indicated in FIG. 4. The silicon workber ch technology, in which the recesses for the mirror, ball-bearings, fibers, and lenslets are all simult~neously formed by reliable lithography, ensures precise relative alignment of 25 all fibers, lçncletc, and the mirror on a mass productive basis--i.e., the .cimult~neous manufacture of a plurality of substrates with all their recesses aligned by means of conventional lithographic techniques. Likewise it should be understood that the position and orientation of the refracting slab RS (FIGS. 18 and 20) is similarly dele~ ed by ball bearings (not shown) which fit into recesses in the substrate S as 30 depicted in FIGS. 3-5, for example.
Although the invention has been described in detail in terms of specific embo lin-~nts, various modifications can be made without departing from the scope of the invention. For example, the lenslets can be omitted by making the edges of the fiber segments spherical, rather than flat, to collimate the exiting optical beam.
35 Also, a single mirror M or refracting slab RS can siml-lt~neously be used in conjunction with more than the single set of three (or four) ports--i.e., with an array of fibers containing a plurality of sets of such fibers, each set comprising three (or - four) fibers operating similarly to F1, F2, F3 (and F4).
Instead of offsetting (FIGS. 6 and 7) the fiber segments F3 and F4 (together with lenslets L3 and F4) by the distance d, the (center of the) mirror could 5 be offset, in order to reduce the amount of optical radiation entering into the fiber segment F3 from the fiber segment F4 during the off-line mode.
At some sacrifice of long-term stability, reliability, and optical insertion loss, the header H can be a st~mre~ metal or molded plastic body having projections that fit into recesses in the silicon substrate, while the ball-bearings are omitted.
Instead of optical signals, other forms of elec~ agnetic r~i~tion signals can be used, spanning from optical to millimeter waves with applvpl;ate changes in the materials of the lenslets, mirror, and waveguides.
(c) first, second, and third radiation ports that are respectively located such that when the deflecting element is in the first region a radiation signal beam 2 5 arriving at the switching arrangement at the first port propagates through the location of the second position and enters into the second port, and such that when the deflecting element is moved by the moving means into the second region the signal beam arriving at the first port is deflected by the planar surface of the deflecting element into the third port, and 3 o (d) a substrate having a major planar surface and having first, second, and third waveguide alignment recesses therein at the surface thereof which determine respective first, second, and third port positions of the first, second, and third ports, respectively, and having a pair of deflecting element alignment recesses therein at the surface thereof for aligning the deflecting element with ~3~ 2020219 respect to the first, second, and third port positions.
Typically each port comprises an end of a waveguide, such as a millim--ter waveguide or an optical waveguide (fiber).
In a specific embolim~ont, the radiation is optical, the deflecting element S is a mirror, and the n~s~ /e ports are l~,;,pccl,~e ends of optical fibers. The mirror is held by a holder (header) which has a pair or recesses. This pair of recesses is aligned to another pair of recesses, for aligning the mirror, which have been lithographed in a silicon substrate, and each of a pair of ball-bearings fits into a respective of the pair of aligned recesses. The fibers are aligned with respect to one 10 another and to the mirror by setting the respective fibers into respective elongated recesses for aligning optical fibers. The fibers are aligned to one another and with respect to the mirror by setting the respective fibers into respective elongatedrecesses, adapted for aligning optical fibers, all of which have been lithographed in the silicon substrate simult~neously with the recesses into which the ball-bearings fit 15 In this way, the desirable alignment precision of "silicon wolL~nch" technology is achieved. Also, advantageously a planar reflecting surface of the mirror is constrained by the ball-bearings to move parallel to itself, so that jitter of the optical beam is avoided when the mirror stops moving during a switching operation, even if the mirror stops suddenly.
This switching arrangement can be modified in order to have an optical ~wilching arrangement suitable for an optical fiber loop in a LAN. Specifically, to the just described arrangement there is added a fourth port in the form of a fourth optical fiber segment which is set in yet another elongated recess in the substrate. At the same time, a local optical source is located at the local station and is positioned 25 so as to deliver a second optical signal beam to this fourth fiber segment, and a local photodetector is located at the local station and is positional so as to receive the optical beam after entering into and propagating through the third fiber segment. In this way, the optical beam arriving at the first pon stems from the LAN loop, and the second optical beam arriving at the fourth port stems from the local optical source, 30 and the switching arrangement can be used in a LAN as described above, with the added feature that when the deflecting element of a local station is in the first region (off-line) self-testing operations at that local station can be performed with adesirably lower effective optical intensity by virtue of the offset of the third and fourth fiber segments.
-~4- 2020219 Brief Description of the Drawin~
This invention together with its fea~ ;s, characteristics, and advantages -may be better understood from the following detailed description when read in conjunction with the drawings in which FIG. 1 is a schem~tic diagram of a three-port optical ~ ching arrangement in accordance with a specific embalim~nt of the invention;
FIG. 2 is a schematic diagram of the embo lim~nt shown in FIG. 1 with a mirror moved into the optical path;
~ FIG. 3 is an assembly view of a switching assembly, comprising the 10 embodiment shown in FIGS. 1 and 2, integrated in silicon workbench technology, in accordance with another specific embodiment in the invention;
FIG. 4 is a cross section view of a portion of the embodiment shown in FIGS. 1 and 2 (with optical fibers not in place, only for the sake of clarity) in accordance with a specific embodiment of the invention;
FIG. 5 is an assembly view of a four-port optical switching assembly suitable for use in a LAN, in accordance with another specific embodiment of theinvention;
FIG. 6 is a top view of the embodiment shown in FIG. 6 with the mirror out of the optical path;
FIG. 7 is a top view of the embodiment shown in FIG. 6 with the mirror in the optical path;
FIG. 8 is a diagram of a LAN in accordance with another embodiment of the invention;
FIG. 9 is a diagram of a typical local station which is off^line in the 25 LAN shown in FIG. 8;
FIG. 10 is a diagram of a typical local station which is on-line in the LAN shown in FIG. 8; and FIG. 11 is a cross-section diagram of an optical coupler in accordance with another embodiment of the invention.
FIGS. 12-13 are top views a part of a four-port optical switching assembly, in accordance with yet another specific embodiment of the invention;
FIG. 14 is a perspective view, partially in cross section, of a mirror suitable for use in a four-port optical switching assembly, in accordance with still another specific embodiment; and FIGS. 15-16 are top views of a four-port optical ~wi~ching assembly, in accordance with yet another specific embodiment of the invention;
FIGS. 17-18 are top views of part of a three-port optical switching assembly, in accordance with still another specific embodiment of the invention; and FIGS. 19-20 are top views of part of a four-port optical switching assembly, in accordance with still another specific embo-1iment of the invention.
Only for the sake of clarity, none of the drawings is to scale.
Detailed Des~ tion As shown in FIGS. 1 and 2, a three-port (one input, two output) optical ~wilchi~lg arrangement 10 (FIG. 1) or 20 (FIG. 2) has a mirror M which is positioned either out of the optical path (E;IG. 1) or in the optical path (FIG. 2). In both ~ihl~tion~ (FIGS. 1 and 2), the switching arrangement 10, 20 has first, second and third optical ports Pl, P2, and P3, which are formed by respective proximate ends of Srst, second, and third optical fiber segments Fl, F2, and F3. The switching arrangement 10, 20 further comprises first, second and third lenslets Ll, L2, and L3 which serve to collimate the respective optical beams em~n~ting from the first fiber Fl, entering into the second Sber F2 (FIG. 1), or entering into the third fiber F3 (FIG. 2). Optical radiation for the optical beams is supplied by a light source L and is collected by utili7~tion means Ul (FIG. 1) or U2 (FIG. 2). The mirror M (FIG.2) 20 has a frontal planar reflecting surface MSI and may also have another reflecting surface parallel thereto, such as rear planar reflecting surface MS2.
The switching arrangement 10, 20 can advantageously be integrated in a silicon workbench technology assembly, to form an optical switching assembly 30 (FIG. 3). Here the same reference labels are used as were used in FIGS. 1 and 2 to 25 refer to the same or similar elements or piece-parts.
On a major planar surface PS of a silicon substrate S, for alignment purposes there is a plurality of recesses (indentations or grooves) that are cut into the substrate S, including a mirror recess MR into which fits the mirror M. Other recesses cut into the substrate S include: first, second, and third fiber recesses FRl, 30 FR2, FR3; first, second, and third lenslet recesses LRl, LR2, and LR3; and first and second substrate ball recesses SBRl and SBR2 for receiving and holding in place a pair of identical ball-bearings B 1 and B2. The mirror M is integral with a silicon header (holder) H. This header has a pair of mirror ball-bearing recesses MBRl and MBR2 that are registerable with a pair of identical substrate-ball-bearing recesses 35 SBRl and SBR2 for receiving and holding in place the ball-bearings B 1 and B2. To prevent scratching of the mirror surface MS 1, the mirror recess MR is made -sufficiently wide to prevent the reflecting surface(s) of the mirror from touching the sides of this mirror recess MR especially when the mirror moves in and out of this recess. The mirror recess MR and the ball-bearing recesses SBRl, SBR2, MBRl, and MBR2 are all mutu~lly located for the desired mutual ~lignm~ont of the mirror 5 surface MSl, the lenslets Ll, L2, and L3, and the fiber segments Fl, F2, and F3.
FIG. 4 is a cross section view of the portion the header H and substrate S
in~ te~l by the line 4-4 in FIG. 3. Here in FIG. 4, the front header surface cross section FHS is typically a <110> plane of a mono-crystalline silicon body of which the header H is composed, and the mirror M is an integral part of the ~me silicon 10 body, as formed by known lithographic masking and anisotropic etching techniques.
The front substrate surface FSS cross section of the substrate S is typically a <100>
plane of a monocrystalline silicon body of which the substrate S is composed.
The header H can move in a rotary motion about the axis formed by joining the centers of the ball-bearings B 1 and B2. Hence the planar surface MS 1 15 (and MS2) of the mirror M is constrained to move parallel to itself, i.e., with no lateral displacement. Thus the right-hand edge of the mirror M (FIGS. 3 and 4) can move smoothly into and out of the mirror recess MR, depending upon a suitable force G (or distribution of forces) applied at a point (or region) at the top of the header H located to the left of the aforementioned axis through the ball-bearings B 1 20 and B2. This force G is applied in accordance with a function of time that is suitable for the desired switching. The force G gives rise to a counle,~lockwise torque when G is directed downward as shown in FIG. 4, and hence tends to move the relevant part of the mirror M (where the light beam is incident) out of the optical path in the switching arrangement 10, 20; and this force G gives rise to a clockwise torque when 25 G is directed upward (not shown), and hence tends to move the mirror M into the optical path. Thus, during switching operations, the direction of G determines the movement of the mirror M to produce the condition of the ~wilching arrangement 10 vs. 20 (FIG. 1 vs. FIG. 2).
It should be noted that jittering (random) motion of the mirror M
30 upward or downward does not impair optical alignment, because the alignment is completely determined by the identic~l ball-bearings Bl and B2 fitting into the identical recesses SBRl and SBR2 which are located and aligned such that the mirror is constrained to move in a direction perpendicular to the place defined by the fibers Fl, F2, and F3. In this way, mechanical vibrations which tend to produce 35 relative motion between the substrate and the mirror do not adversely affect the optical tr~nsmi~sion, because the otherwise adverse transverse relative motion is suppressed by the rigidity of ball-bearings B 1 and B2 in the recesses SBRl and SBR2.
The lenslets Ll, L2, and L3 are typically made of sapphire (n=1.7) or of high index (about 1.7 to 1.9) glass. The ball bearings B 1 and B2 are conveniently 5 made of the same material as are the lenslets.
FIG. 5 shows an assembly view of a four-port (two input, two output) optical switching ~csembly 50 suitable for use in a LAN. The ~cs~mbly 50 can be viewed as being derived from the previously described optical switching assembly30 by the addition of a fourth port formed by fiber segment F4 fitting into fiber 10 recess FR4, together with lenslet L4 fitting into lenslet recess LR4, plus a second mirror surface MS2 of the mirror M parallel to the first surface MS 1.
FIG. 6 shows a top view of the assembly 50 when the mirror M is out of the optical path (off-line, by-pass mode). As in~ ate~d in FIG. 6, when the mirror M
is located in a position which is thus outside of the optical path, optical radiation 15 exiting from the first fiber segment Fl then passes the swilchi-lg arrangement 60 into the second fiber F2. At the same time, an optical beam propagating in the fourthfiber segment F4 from another light source (not shown) passes into the fiber segment F3 but with an ~tten~latecl optical intensity (infli~ate~ by a dotted line), owing to a deliberately selected offset distance _ of fiber segment F3 relative to fiber segment 20 F4 (together with the same offset in their respective lenslets L3 and L4). The thus attenuated beam entering into the fiber segment F3, is useful for self-tesdng operadons as more fully described below. An absorber A can be added, if need be,to absorb the (excess) light coming from the fiber segment F4, i.e., to absorb the light which does not enter into the fiber segment F3.
FIG. 7 shows a top view of the ~wilchillg assembly 50 (FIG. 5) when the mirror is in the path of the optical beam (acdve mode). As indicated in FIG. 7, when the mirror M is thus moved into the opdcal path, the opdcal beam exidng from thefiber segment Fl is passed into the switching arrangement 70 where it is reflected by the first surface MS 1 of the mirror M and directed into the third fiber segment F3.
30 At the same time, light exiting from the fiber segment F4 is reflected by the second surface MS2 of the mirror M and enters into ~he fiber segment F2. By making the thickness (distance between frontside and ba~cide) of the mirror M equal to d/~ (=d cos 45 ), if the arrangement 60 is aligned properly, so also will the arrangement 70 be aligned properly. In pardcular, in FIG. 6 subst~nti~lly all of the 35 beam exiting from Fl will enter into F2, and only a pordon of the cross secdon of the beam exidng from F4 will enter into F3; whereas in FIG. 7 subst~nti~lly all of the beam exiting from Fl will enter with F3, and substantially all of the beam exiting from F4 will enter into F2.
FIG. 8 shows a LAN loop 800 composed of a plurality of similar local stations exemplified by a typical local station composed of node 80 together with the S four-port optical ~witching assembly 50 described above. For example, there are a total of six such local stations interconnected by six fiber segm~ntc. One of the stations may typically function as a main station, but in any event it operates in similar manner as the others insofar as relevant here.
FIG. 9 shows a typical local station which is in the off-line condition 10 (by-pass mode). As in tic~teA in FIG. 9, when the mirror (not shown) in the switching assembly 50 is not in the optical path, a trAnsmitter Tx, such as a light ernitting diode (LED), sends a light beam into fiber segment F4 which is partially propagated by the ~wilchihlg assembly 50 (as per FIG. 6) into fiber segment F3 and ultimately to a utilization means, such as a PIN photodiode receiver Rx, whereas15 optical radiation propagating through fiber segment Fl passes through the switch 50 nnflictllrbed and enters into the fiber segment F2. The beam thus propag~ting from Fl to F2 goes on to the next local station, whereas the beam propagating from F4 to F3 can be used for testing the photo-electronics of the node 80. Thus the situation of the node 80 in FIG. 9 is the off-line (by-pass) mode.
Fig. 10 shows the typical local station in its on-line condition (active mode), i.e., with the mirror in the optical path. As indicated in FIG. 10, when the rnirror M (not shown) is moved into the optical path, the optical beam e-m~n~ting from fiber segment Fl enters into the receiver Rx, whereas the optical beam em~n~ting from the tr~n~.-.;lter Tx enters into the fiber segment F2. Thus, the 25 situation depicted in FIG. 10 is the on-line mode of the node 80, wherein theelectronics of the node 80 utilizes and processes the information on the beam çm~n~ting from the fiber segment F1, and in response thereto the node 80 then transmits its own processed information to the fiber segment F4.
FIG. 11 is a design of an optical coupling arrangement, for coupling 30 together a pair of fiber segments, such as F1 and F2, to their respective lenslets Ll and L2 in the above-described switching arrangelllen~s. More specifically, for example, the space between the fiber segment Fl and its lenslet Ll is filled with a transparent medium R1, such as silicone rubber, having a refractive index which is approximately equal to that of the segment Fl, typically about 1.5. In this way,35 unwanted reflections at the interface of F1 with R1 are avoided. At the same time the more desirable collim~ted beam optics (parallel beam between L1 and L2) is -9- 20XU~19 achieved rather than converging beam optics (rays coming to a focus ~l~..xn Ll and L2). Similarly, the space between L2 and F2 is ~led with a similar tran~ale.lt medium R2.
Note that in FIGS. 6 and 7, the offset ~lict~nce _ arises in the ~witching S assembly 60 because of the non-vanishing thirlrness of the mirror M. This offset causes optical loss into the absorber A, which can be undesirable in cases where the redirection of optical intensity, as is desired in self-testing, is not desired. To avoid this possibly undesirable situation, the optics of the assembly can be mo~lifi~ for example, as shown in FIGS. 12-13 or 14 or 15-16 or 17-18 or 19-20. In all these 10 FIGURES, the same reference labels are used to denote elementc that are similar to those described above. In particular, all the lenslets are set in respective recesses in the substrate S (FIG. 5) as are the associated fibers, the recesses being located at respective positions that are determined by silicon workbench technology.
FIGS. 12-13 depict the lenslets Ll, L2, L3, and L4 in a configuration for 15 use in a switching assembly of the kind described above (FIG. 5). The rem~inder of the assembly (not shown in FIGS. 12-13) should be understood to be the same as the ~wilching ~csem~ly 50 shown in FIG. 5. Here in FIGS. 12-13, a pair of auxiliary mirrors AMl and AM2 are fixedly attached either to the substrate S (FIG. 5) or to the header H and are oriented parallel to the mirror M, whereby the optical path20 between the fibers F4 and F3 does not suffer from any offset, as is desir~
FIG. 14 depicts a mirror 140 which, when used as the mirror M attached to the header H in the switching assembly 50 (FIG. 5), likewise avoids the offset.
Here in FIG. 14, the mirror 140 includes a silicon parallel slab 144 having its front surface MSl coated with a thin layer 141 made of suitable transparent material, 25 typically silicon dioxide, having a thickness such that it acts as an anti-reflection co~ting The bottom half of the rear surface MS2 of the slab 144 is likewise coated with a simil~rly thin layer 142 of the transparent m~teri~l, whereas the top half of the rear surface MS2 is coated with a thin reflecting layer 143, made of suitable optically reflecting m~teri~l, such as a metal having a thickness of about lOOnm. This mirror 30 140 can then be used in the switching assembly 50 in the following m~nner To put the assembly with the mirror 140 into the by-pass mode depicted in FIG. 6, the mirror 140 is moved upward into a position such that the optical paths among thelenslets pass through bottom (transparent) half of the mirror 140. In this way, the dielectric portion of merely the mirror deflects (refracts) the beam slightly and 35 directs the beam along the appropliate optical path. To achieve the active mode (FIG. 7), the mirror 140 is moved downward such that the optical paths pass through -the top (reflecting) half of the mirror 140--while the bottom half of the mirror is sinl~te~l in the mirror recess MR (E~IG. 5). In this way the mirror 140 reflects the optical beams incident upon the front and rear sl~ ces of the reflecting layer 142, which has negligible thickness and hence introduces negligible offset.
FIGS. 15-16 depict an arrangement of lenslets and fibers to avoid the offset, in accordance with yet another embo limP-nt Here in FIGS. lS-16, the fibers F1, F2, F3, and F4 serve the same respective functions as in FIGS. 6-7, but they are all located on the same (front) side of mirror M. On the other (rear) side of the mirror M, auxiliary fibers AF1, AF2, and AF3--together with auxiliary lenslets AL1, AL2, and AL3--are located (FIG. 16) in respective alignment with these fibers F1, F2, and F3. Note that only three main lenslets L1, L2, and L3 are required, the lenslet L1 doing double duty by passing two mllt l~lly orthogonal beams simlllt~neously. The auxiliary fiber AF1 is connected at its rear end by a connecting fiber CF1 to the rear end of the auxiliary fiber AF3, and the allxili~ry fiber AF2 is 15 connected at its rear end by a connecting fiber CF4 to the rear end of the auxiliary fiber AF4. In this way, when the mirror M is moved into a position located in the paths of the optical beams, as shown in FIG. 15, the by-pass (off-line) mode is obtained. In particular, light exiting from Fl goes to F2 by way of a path through L1, reflection by mirror M, and through L2; and light exiting from F4 goes to F3 by 20 way of a path through L1, reflection by mirror M, and through L3. And when the mirror M is moved into a position located outside of the paths of the optical beams, as shown in FIG. 16, the active (on-line) mode is achieved. That is, light exiting from F1 goes to F3 via Ll, AL1, AFl, CFl, AF3, AL2, and L3; and light exiting from F4 goes to F2 via Ll, AL4, AF4, CF2, AF2, AL2, and L2.
It should be understood that the location of all the lenslets and fibers shown in FIGS. 15-16 again are determined by recesses in the substrate S (FIG. 5), advantageously in accordance with silicon workbench technology, and that the position of the mirror M in FIGS. 15-16 is determined by ball-bearings (not shown in FIGS. 15-16) located in recesses, i.e., in the same way as the position of the mirror 30 M in FIG. 5.
It should also be understood that in FIGS. 15-16 the positions of the fibers F2 and F3 can be interchanged, and at the same time the respective lenslets L2 and L3 are interchanged. In that case, the active (on-line) mode is obtained in the configuration shown in FIG. 15, whereas the by-pass (off-line) mode is obtained in 35 the configuration shown in FIG. 16.
Instead of the reflecting mirror M, an optically refracting elem~nt can be - used, for example, in the form of a parallel refracting slab (plate) RS, i.e., a parallel plate composed of an optically refracting medium--as illustrated, for example, in the three-port configuration shown in FIGS. 17-18 (fibers Fl, F2, F3 not shown) and in S the four-port configuration shown in FIGS. 19-20 (fibers Fl, F2, F3, F4 not shown).
It should be understood here that optical fibers (not shown in FIGS. 17-18 or FIGS.
19-20) should be aligned as shown in FIGS. 3 and 5. In particular (FIGS. 17-18),refracting slab RS is ~si~ned --for example, as to thickness and refractive index--such that, when it is moved into the optical path as constrained by ball-be~nngc B 1 10 and B2 in their respective recesses (FIG. 4), it refracts the optical beam by an amount sl.fficient to deliver the beam to a different lenslet--e.g., to the lenslet L3 (E;IG. 18) instead of L2 (FIG. 17). Note that the front and rear planar surfaces of the refracting slab RS are both constrained to move parallel to themselves, respectively.
In nG. 20, ALl and AL2 are auxiliary lenslets connected by a 15 connecting fiber CF, whereby the arrangement (FIGS. 19-20) can be used in a four-port optical switching assembly similar to the one depicted in nG. ~7.
Notice that in connection with all cases described above, the position and orient~tion of the min~r M or 140 (FIG. 14), or of the parallel refracting slab RS
(FIG. 18), is dcle ...;.-ed by the positions of ball-bearings Bl and B2 which fit into 20 the recesses SBRl and SBR2. These positions of these ball-bearings in these recesses reliably determine an axis around which the mirror M rotates in response to the applied force(s) G indicated in FIG. 4. The silicon workber ch technology, in which the recesses for the mirror, ball-bearings, fibers, and lenslets are all simult~neously formed by reliable lithography, ensures precise relative alignment of 25 all fibers, lçncletc, and the mirror on a mass productive basis--i.e., the .cimult~neous manufacture of a plurality of substrates with all their recesses aligned by means of conventional lithographic techniques. Likewise it should be understood that the position and orientation of the refracting slab RS (FIGS. 18 and 20) is similarly dele~ ed by ball bearings (not shown) which fit into recesses in the substrate S as 30 depicted in FIGS. 3-5, for example.
Although the invention has been described in detail in terms of specific embo lin-~nts, various modifications can be made without departing from the scope of the invention. For example, the lenslets can be omitted by making the edges of the fiber segments spherical, rather than flat, to collimate the exiting optical beam.
35 Also, a single mirror M or refracting slab RS can siml-lt~neously be used in conjunction with more than the single set of three (or four) ports--i.e., with an array of fibers containing a plurality of sets of such fibers, each set comprising three (or - four) fibers operating similarly to F1, F2, F3 (and F4).
Instead of offsetting (FIGS. 6 and 7) the fiber segments F3 and F4 (together with lenslets L3 and F4) by the distance d, the (center of the) mirror could 5 be offset, in order to reduce the amount of optical radiation entering into the fiber segment F3 from the fiber segment F4 during the off-line mode.
At some sacrifice of long-term stability, reliability, and optical insertion loss, the header H can be a st~mre~ metal or molded plastic body having projections that fit into recesses in the silicon substrate, while the ball-bearings are omitted.
Instead of optical signals, other forms of elec~ agnetic r~i~tion signals can be used, spanning from optical to millimeter waves with applvpl;ate changes in the materials of the lenslets, mirror, and waveguides.
Claims (19)
1. An electromagnetic radiation switching arrangement which comprises:
(a) a radiation deflecting element having a planar deflecting surface;
(b) moving means for moving the deflecting element such that the planar deflecting surface thereof can be moved parallel to itself from a first region to a second region and from the second to the first region;
(c) first, second, and third radiation ports that are respectively located such that when the deflecting element is in the first region a radiation signal beam arriving at the switching arrangement at the first port propagates through the location of the second position and enters into the second port, and such that when the deflecting element is moved by the moving means into the second region the signal beam arriving at the first port is deflected by the planar surface of the deflecting element into the third port, and (d) a substrate having a major planar surface and having first, second, and third waveguide alignment recesses therein at the surface thereof which determine respective first, second, and third port positions of the first, second, and third ports, respectively, and having a pair of deflecting element alignment recesses therein at the surface thereof for aligning the deflecting element with respect to the first, second, and third port positions.
(a) a radiation deflecting element having a planar deflecting surface;
(b) moving means for moving the deflecting element such that the planar deflecting surface thereof can be moved parallel to itself from a first region to a second region and from the second to the first region;
(c) first, second, and third radiation ports that are respectively located such that when the deflecting element is in the first region a radiation signal beam arriving at the switching arrangement at the first port propagates through the location of the second position and enters into the second port, and such that when the deflecting element is moved by the moving means into the second region the signal beam arriving at the first port is deflected by the planar surface of the deflecting element into the third port, and (d) a substrate having a major planar surface and having first, second, and third waveguide alignment recesses therein at the surface thereof which determine respective first, second, and third port positions of the first, second, and third ports, respectively, and having a pair of deflecting element alignment recesses therein at the surface thereof for aligning the deflecting element with respect to the first, second, and third port positions.
2. The arrangement of claim 1 in which the electromagnetic radiation is optical radiation in which the radiation signal beam is a first optical beam, in which the first, second, and third waveguide alignment recesses are elongated fiber alignment recesses, and in which the first, second, and third ports comprise, respectively, first, second, and third optical fiber segments which are set in the first, second, and third elongated recesses, respectively, the first, second, and third elongated recesses having respectively first, second, and third axes that are mutually oriented for propagation of the first optical beam emanating from the first fiber segment to the second and third fiber segments.
3. The arrangement of claim 2 further including a fourth optical port comprising a fourth fiber segment set in a fourth elongated waveguide alignment recess in the substrate, the fourth elongated waveguide alignment recess having an axis which is aligned such that when the deflecting element is situated in the first region a second optical signal beam, supplied by a local optical source and arriving at the fourth port, propagates through the second region and enters into the third port, and when the deflecting element is moved to the second region the second opticalbeam is deflected by the deflecting element and enters into the second port.
4. The arrangement of claim 3 further including a photodetector which is positioned to receive an optical beam after entering into and propagating through the third fiber segment, in which the deflecting element is a mirror having frontside and backside planes that are spaced apart by a first distance, and in which the fourth recess is set with an offset distance with respect to the third recess such that when the mirror is situated in the first region only a part of the cross section of the second optical beam arriving at the fourth port enters into the third fiber segment and when the mirror is moved into the second region substantially all of the cross section of the optical beam arriving at the fourth port enters into the second fiber segment.
5. The arrangement of claim 4 further comprising fifth, sixth, seventh, and eighth recesses in the surface of the substrate having first, second, third and fourth optical lenses, respectively, set therein at respective locations that are aligned with respect to the first, second, third, and fourth ports, respectively.
6. The arrangement of claim 3 further comprising fifth, sixth, seventh, and eighth recesses in the surface of the substrate having first, second, third and fourth optical lenses, respectively, set therein at respective locations that are aligned with respect to the first, second, third, and fourth ports, respectively.
7. The arrangement of claim 3 further comprising fourth, fifth, and sixth recesses in the surface of the substrate having first, second, and third optical lenses, respectively, set therein at respective locations that are aligned with respect to the first, second, and third ports, respectively.
8. The arrangement of claim 2 in which the electromagnetic radiation is optical radiation and which further comprises fourth, fifth, and sixth recesses in the surface of the substrate having first, second, and third optical lenses, respectively, set therein at respective locations that are aligned with respect to the first, second, and third ports, respectively.
9. The arrangement of claim 1 further comprising fourth, fifth, and sixth recesses in the surface of the substrate having first, second, and third optical lenses, respectively, set therein at respective locations that are aligned with respect to the first, second, and third ports, respectively.
10. The arrangement of claim 1 in which the means for moving the mirror urges motion in a first direction that is parallel to the frontside plane and in which the first direction is perpendicular to a plane determined by the optical beams.
11. A communication system including the arrangement recited in claim 1 and further including (a) utilization means for utilization optical radiation, and (b) optical transmission means for gathering the optical beam entering into the second port and propagating it to the utilization means.
12. A communication system including the switching arrangement recited in claim 2 and further including:
utilization means for utilizing optical radiation emanating from the second fiber segment after propagating therethrough.
utilization means for utilizing optical radiation emanating from the second fiber segment after propagating therethrough.
13. A communication system including the switching arrangement recited in claim 4 and further including:
utilization means for utilizing optical signals emanating from the second fiber segment after propagating therethrough.
utilization means for utilizing optical signals emanating from the second fiber segment after propagating therethrough.
14. The system of claim 1 in which the deflecting element is a mirror.
15. The system of claim 2 in which the deflecting element is a mirror.
16. The system of claim 4 in which the deflecting element is a mirror.
17. The system of claim 1 in which the deflecting element is a parallel plate refracting element.
18. The system of claim 2 in which the deflecting element is a parallel plate refracting element.
19. The system of claim 4 in which the deflecting element is a parallel plate refracting element.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US07/385,331 US4932745A (en) | 1989-07-25 | 1989-07-25 | Radiation switching arrangement with moving deflecting element |
US385,331 | 1989-07-25 |
Publications (2)
Publication Number | Publication Date |
---|---|
CA2020219A1 CA2020219A1 (en) | 1991-01-26 |
CA2020219C true CA2020219C (en) | 1995-02-28 |
Family
ID=23520973
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CA002020219A Expired - Lifetime CA2020219C (en) | 1989-07-25 | 1990-06-29 | Radiation switching arrangement with moving deflecting element |
Country Status (6)
Country | Link |
---|---|
US (1) | US4932745A (en) |
EP (1) | EP0410619B1 (en) |
JP (1) | JP2594377B2 (en) |
CA (1) | CA2020219C (en) |
DE (1) | DE69026876T2 (en) |
HK (1) | HK179696A (en) |
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-
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-
1990
- 1990-06-29 CA CA002020219A patent/CA2020219C/en not_active Expired - Lifetime
- 1990-07-17 DE DE69026876T patent/DE69026876T2/en not_active Expired - Lifetime
- 1990-07-17 EP EP90307774A patent/EP0410619B1/en not_active Expired - Lifetime
- 1990-07-20 JP JP2190940A patent/JP2594377B2/en not_active Expired - Lifetime
-
1996
- 1996-09-26 HK HK179696A patent/HK179696A/en not_active IP Right Cessation
Also Published As
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EP0410619A3 (en) | 1992-05-13 |
HK179696A (en) | 1996-10-04 |
DE69026876T2 (en) | 1996-12-05 |
JPH0359611A (en) | 1991-03-14 |
EP0410619A2 (en) | 1991-01-30 |
DE69026876D1 (en) | 1996-06-13 |
JP2594377B2 (en) | 1997-03-26 |
EP0410619B1 (en) | 1996-05-08 |
CA2020219A1 (en) | 1991-01-26 |
US4932745A (en) | 1990-06-12 |
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