Liquid metal micro switches using as channels and heater cavities matching patterned thick film dielectric layers on opposing thin ceramic plates

Information

  • Patent Grant
  • 6777630
  • Patent Number
    6,777,630
  • Date Filed
    Wednesday, April 30, 2003
    21 years ago
  • Date Issued
    Tuesday, August 17, 2004
    20 years ago
Abstract
An efficient way to fabricate the channels and cavities in a LIMMS device is to form them as matching upper and lower portions each created as a patterned layer of thick film dielectric material deposited on a respective upper or lower substrate. The two portions are adhered together by a patterned layer of adhesive, and hermetically sealed around an outer perimeter. The heater resistors are mounted atop the lower layer, thus suspending them away from that substrate and exposing more of their surface area. Vias can be used to route the conductors for the heaters and the switched signal contacts through the lower substrate to cooperate with surface mount techniques using solder balls on an array of contact pads. These vias can be made hermetic by their placement within the patterned layers of dielectric material and by covering their exposed ends with pads of hermetic metal. Suitable thick film dielectric materials that may be deposited as a paste and subsequently cured include the KQ 150 and KQ 115 thick film dielectrics from Heracus and the 4141A/D thick film compositions from DuPont.
Description




BACKGROUND OF THE INVENTION




Recent developments have occurred in the field of very small switches having moving liquid metal-to-metal contacts and that are operated by an electrical impulse. That is, they are actually small latching relays that individually are SPST or SPDT, but which can be combined to form other switching topologies, such as DPDT. (Henceforth we shall, as is becoming customary, refer to such a switch as a Liquid Metal Micro Switch, or LIMMS.) With reference to

FIGS. 1-4

, we shall briefly sketch the general idea behind one class of these devices. Having done that, we shall advance to the topic that is most of interest to us, which is an improved technique for forming the needed channels and cavities of such switches fabricated on a substrate.




Refer now to

FIG. 1A

, which is a top sectional view of certain elements to be arranged within a cover block


1


of suitable material, such as glass. The cover block


1


has within it a closed-ended channel


7


in which there are two small movable distended droplets (


12


,


13


) of a conductive liquid metal, such as mercury. The channel


7


is relatively small, and appears to the droplets of mercury to be a capillary, so that surface tension plays a large part in determining the behavior of the mercury. One of the droplets is long, and shorts across two adjacent electrical contacts extending into the channel, while the other droplet is short, touching only one electrical contact. There are also two cavities


5


and


6


, within which are respective heaters


3


and


4


, each of which is surrounded by a respective captive atmosphere (


10


,


11


) of a suitable gas, such as N


2


. Cavity


5


is coupled to the channel


7


by a small passage


8


, opening into the channel


7


at a location about one third or one fourth the length of the channel from its end. A similar passage


9


likewise connects cavity


6


to the opposite end of the channel. The idea is that a temperature rise from one of the heaters causes the gas surrounding that heater to expand, which splits and moves a portion of the long mercury droplet, forcing the detached portion to join the short droplet. This forms a complementary physical configuration (or mirror image), with the large droplet now at the other end of the channel. This, in turn, toggles which two of the three electrical contacts are shorted together. After the change the heater is allowed to cool, but surface tension keeps the mercury droplets in their new places until the other heater heats up and drives a portion of the new long droplet back the other way. Since all this is quite small, it can all happen rather quickly; say, on the order of a millisecond, or less. The small size also lends itself for use amongst controlled impedance transmission line structures that are part of circuit assemblies that operate well into the microwave region.




To continue, then, refer now to

FIG. 1B

, which is a sectional side view of

FIG. 1A

, taken through the middle of the heaters


3


and


4


. New elements in this view are the bottom substrate


2


, which may be of a suitable ceramic material, such as that commonly used in the manufacturing of hybrid circuits having thin film, thick film or silicon die components. A layer


14


of sealing adhesive bonds the cover block


1


to the substrate


2


, which also makes the cavities


5


and


6


, passages


8


and


9


, and the channel


7


, each moderately gas tight (and also mercury proof, as well!). Layer


14


may be of a material called CYTOP (a registered trademark of Asahi Glass Co., and available from Bellex International Corp., of Wilmington, Del.). Also newly visible are vias


15


-


18


which, besides being gas tight, pass through the substrate


2


to afford electrical connections to the ends of the heaters


3


and


4


. So, by applying a voltage between vias


15


and


16


, heater


3


can be made to become very hot very quickly. That in turn, causes the region of gas


10


to expand through passage


8


and begin to force long mercury droplet


12


to separate, as is shown in FIG.


2


. At this time, and also before heater


3


begins to heat, long mercury droplet


12


physically bridges and electrically connects contact vias


19


and


20


, after the fashion shown in FIG.


1


C. Contact via


21


is at this time in physical and electrical contact with the small mercury droplet


13


, but because of the gap between droplets


12


and


13


, is not electrically connected to via


20


.




Refer now to

FIG. 3A

, and observe that the separation into two parts of what used to be long mercury droplet


12


has been accomplished by the heated gas


10


, and that the right-hand portion (and major part of) the separated mercury has joined what used to be smaller droplet


13


. Now droplet


13


is the larger droplet, and droplet


12


is the smaller. Referring to

FIG. 3B

, note that it is now contact vias


20


and


21


that are physically bridged by the mercury, and thus electrically connected to each other, while contact via


19


is now electrically isolated.




The LIMMS technique described above has a number of interesting characteristics, some of which we shall mention in passing. They make good latching relays, since surface tension holds the mercury droplets in place. They operate in all attitudes, and are reasonably resistant to shock. Their power consumption is modest, and they are small (less than a tenth of an inch on a side and perhaps only twenty or thirty thousandths of an inch high). They have decent isolation, are reasonably fast with minimal contact bounce. There are versions where a piezo-electrical element accomplishes the volume change, rather than a heated and expanding gas. There also exist certain refinements that are sometimes thought useful, such as bulges or constrictions in the channel or the passages. Those interested in such refinements are referred to the Patent literature, as there is ongoing work in those areas. See, for example, U.S. Pat. No. 6,323,447 B1.




To sum up our brief survey of the starting point in LIMMS technology that is presently of interest to us, refer now first to FIG.


4


and then to FIG.


5


. In

FIG. 4

there is shown an exploded view


32


of a slightly different arrangement of the parts, although the operation is just as described in connection with

FIGS. 1-3

. In particular, note that in this arrangement the heaters (


3


,


4


) and their cavities (


5


,


6


) are each on opposite sides of the channel


7


. Another new element to note in

FIG. 4

is the presence of contact electrodes


22


,


23


and


24


. These are (preferably thin film) depositions of metal that are electrically connected to the vias (


19


,


20


and


21


, respectively). They not only serve to ensure good ohmic contact with the droplets of liquid metal, but they are also regions for the liquid metal to wet against, which provides some hysteresis in the pressures required to move the droplets. This helps ensure that the contraction caused by the cooling (and contraction) of the heated (and expanded) operating medium does not suck the droplet back toward where it just came from. The droplets of liquid metal are not shown in the figure.




If contact electrodes


22


-


24


are to be produced by a thin film process, then they will most likely need to be fabricated after any thick film layers of dielectric material are deposited on the substrate (as will occur in connection with many of the remaining figures). This order of operations is necessitated if the thick film materials to be deposited need high firing temperatures to become cured; those temperatures can easily be higher than what can be withstood by a layer of thin film metal. Also, if the layer of thin film metal is to depart from the surface of the substrate and climb the sides of a channel, then it might be helpful if the transition were not too abrupt.





FIG. 5

is a simplified exploded view


25


of a LIMMS device whose heater cavities, liquid metal channel and their interconnecting passages are formed in a layer of dielectric material between two substrates, instead of being recesses in a cover block. The figure shows a portion of a substrate


26


, which may be of ceramic or glass, and which serves as a base upon which to fabricate the LIMMS device. Various metal conductors


27


-


31


, which may be of gold, are deposited on the top surface of the substrate


26


, or they may be what remains from a patterned removal of an entire metal sheet originally present on the surface of the substrate. The latter case cooperates nicely in instances where some of the conductors are to be co-planar transmission lines formed with the presence of a ground plane. Mercury amalgamates with gold, however, and if enough mercury is present, will dissolve it. It is therefore desirable to protect the gold with a covering of another metal, such as chromium or molybdenum. (Owing to the possibility of mercury smears during assembly, a complete over-covering of all the gold is more desirable than simply covering the exposed pads where the droplet or slug of mercury might be expected to touch the gold during normal operation.) In the figure, conductors


27


and


28


are drive lines for heater resistors


34


and


35


, respectively. Conductors


29


,


30


and


31


are switched signal lines that might also be parts of a controlled impedance transmission line structure.




Now note patterned layer


36


. It is applied over the various conductors


27


-


31


, and may be of KQ 150 or KQ 115 thick film dielectric material from Heraeus, or the 4141A/D thick film compositions from DuPont. These are materials that are applied as pastes and then cured under heat at prescribed temperatures for prescribed lengths of time. Depending upon the particular material, they may be applied as an undifferentiated sheet, cured and then patterned (say, by laser or chemical etching) or they may be patterned upon their initial application (via a screening process). In any event, the patterning produces the heater cavities


44


and


45


, the liquid metal channel


46


and their interconnecting passages.




The conventional thick film processes used to print patterned layers of the dielectric material allows considerable control over the finished thickness of a cured layer of dielectric material (say, in the range of five to ten thousandths of an inch), and achieving sufficient uniformity of thickness is not a major difficulty. However, there are limits to how thin and how thick an uncured printed layer can be, and it may be necessary to apply (print) multiple layers to achieve a particular overall depth for layer


36


. For the KQ material that is to be printed on using a fine mesh (screen) of stainless steel, a printed uncured layer is on the order of one to two thousandths of an inch in thickness. The KQ material shrinks in thickness by an amount of about thirty percent during the curing process. It is possible to print several uncured layers, one on top of the other, and then fire the whole works, or, the application sequence could be print—fire—print—fire . . . , or even print—print . . . print—fire—print—print . . . During the firing for curing the steep side walls and relatively sharp edges possible for the uncured printed layers become sloped and rounded, respectively. The resulting trapezoidal cross-sectional shape of the liquid metal channel


46


may be a significant influence in determining a desired thickness for layer


36


. In this connection, the view shown in

FIG. 5

is a considerable simplification, in that, for simplicity of the drawing, the heater cavities


44


and


45


, liquid metal channel


46


, and their interconnecting passages (not numbered in

FIG. 5

, but are shown as


8


and


9


in

FIGS. 1 and 2

) are all depicted as having steep side walls and sharp edges. It makes the basic subject matter of the drawing much easier to appreciate. When using printed KQ, however, the actual situation is much close to what is shown in

FIGS. 6-9

. Note the sloping side walls of the various patterned layers of dielectric material. Steep sidewalls and sharp edges are not necessarily bad, and can be obtained with other fabrication techniques, although that may also have an effect on the method used to create metalized regions, such as


41


-


43


that are to ascend such steep side walls.




Once layer


36


has been formed and patterned, metallic regions


41


-


43


are deposited. These correspond to metallic contacts


22


-


24


of

FIG. 4

, and serve to improve electrical contact with the liquid metal and to provide a surface that can be wetted by the liquid metal (for latching). Regions


41


-


43


may be deposited by thin film techniques, in which case it may be important that any high temperature firings needed to cure the dielectric layer


36


have already been performed.




If desired, a strip of metal


37


may be applied around the perimeter of the LIMMS device. Such a strip


37


is part of an hermetic seal with a cover plate


38


and is formed of solder or glass frit. The hermetic seal may also involve there being a beveled edge


39


along the perimeter of the cover plate


38


. Cover plate


38


is preferably of ceramic, although one could use glass, as well. On the underside of the cover plate is applied a patterned layer


40


of adhesive, such as CYTOP. The patterning of the adhesive layer


40


matches that of the dielectric layer


36


that it is to mate against, and is shown by the dotted lines. Also shown as dotted lines are metalized regions


47


,


48


and


49


that correspond to the regions


41


-


43


formed in the channel


46


. Metalized regions


47


-


49


offer additional surface for wetting at the various locations of the liquid metal, and may also be deposited by thin film techniques.




To assemble the LIMMS shown in view


25


of

FIG. 5

, the channel


46


would receive its droplets of liquid metal (not shown) and, while in an atmosphere of a suitable gas, such as N


2


, the cover plate


38


would be affixed against the substrate


26


bearing the patterned layer


36


of dielectric material. Then the hermetic seal would be formed.




We are always interested in techniques that improve device capability, reduce device fabrication cost, reduce the costs associated with connecting the device to a surrounding circuit, reduce device power consumption or increase the reliability of the device and its various interconnections with other circuitry. The speed of operation and power consumption of a LIMMS device would be favorably affected if more of the operating gas were in contact with the heater resistor and if less of the heater resistor's heat were captured by the substrate. Heater resistors that are affixed directly to traces or pads formed on the substrate are very close to the substrate, reducing the resistor area available to heat the gas and waste power by heating the substrate. Moreover, forming recesses in sheet of ceramic or glass is an onerous task, and one that may involve nasty chemicals that are not easily handled. Also, it may be that such forming requires process capabilities that not otherwise needed, so that if another existing process could be used instead, a certain simplification in manufacturing logistics is obtained. And there is the promise that if an existing process is re-used, the resulting structure will have thermal expansion characteristics that are quite compatible with the other structures. For these reasons, we should like to re-visit how the heaters are mounted, and perhaps get rid of the recesses dug into the cover block. The use on the bottom substrate of a patterned layer of dielectric forming cavities, channels and interconnecting passages is an attractive starting point. But then what?




SUMMARY OF THE INVENTION




An attractive solution to the problem of efficient fabrication of the channels and cavities in a LIMMS device is to form them as matching upper and lower portions each created as a patterned layer of thick film dielectric material deposited on a respective upper or lower substrate. The two portions are adhered together by a patterned layer of adhesive, and hermetically sealed around an outer perimeter. The heater resistors are mounted atop the lower layer, thus suspending them away from that substrate and exposing more of their surface area. Vias can be used to route the conductors for the heaters and the switched signal contacts through the lower substrate to cooperate with surface mount techniques using solder balls on an array of contact pads. Such vias are not normally hermetic, but can be made so by their placement within the patterned layers of dielectric material. If desired, the upper substrate and its patterned dielectric layer could be replaced by a conventional flat substrate that has had recesses formed therein.




This plan depends upon the use of a suitable dielectric material, which must be strong, adheres well to the substrate, is impervious to contaminants, is capable of being patterned, and if also desired, which can be metalized for soldering. It should also have well controlled and suitable properties as a dielectric. Given a choice, a lower dielectric constant (K) is preferable over a higher one. Suitable thick film dielectric materials that may be deposited as a paste and subsequently cured include the KQ 150 and KQ 115 thick film dielectrics from Heraeus and the 4141A/D thick film compositions from DuPont.











BRIEF DESCRIPTION OF THE DRAWINGS





FIGS. 1A-C

are various sectional views of a prior art SPDT Liquid Metal Micro Switch (LIMMS), and wherein for convenience, while the heaters are shown as located on opposite ends of the channel, they are also shown as being on the same side thereof;





FIG. 2

is a sectional view similar to that of

FIG. 1A

, at the start of an operational cycle;





FIGS. 3A-B

are sectional views of the LIMMS of

FIGS. 1A-C

at the conclusion of the operation begun in

FIG. 2

;





FIG. 4

is an exploded view of a prior art SPDT LIMMS similar to what is shown in

FIGS. 1-3

, but where the heaters are disposed both on opposite sides and on opposite ends of the channel;





FIG. 5

is a simplified exploded view of a prior art LIMMS device that is fabricated with a ceramic cover plate disposed atop a layer of patterned thick film dielectric;





FIG. 6

is a simplified cross sectional view of a LIMMS device having a recessed cover block and sequentially applied multiple patterned layers of dielectric material that not only form a heater cavity but also serve to suspend the heater resistor away from a lower substrate, and which uses vias and ascending pads to bring the resistor's electrical connections out on the bottom surface of the lower substrate to allow surface mounting with an array of solder balls;





FIG. 7

is a simplified cross sectional view of a LIMMS device having a recessed cover block and a patterned layer of dielectric material that not only forms a heater cavity but also serves to suspend the heater resistor away from a lower substrate, and which uses unitary vias to bring the resistor's electrical connections through the combined dielectric layer and substrate out onto the bottom surface of the lower substrate to allow surface mounting with an array of solder balls;





FIG. 8

is a simplified cross sectional view similar to that of

FIG. 7

, except that the recessed cover block is replaced by an upper substrate having channels and cavities formed in a patterned layer of dielectric material; and





FIG. 9

is a simplified cross sectional view similar to that of

FIG. 8

, except that it is for a region of the LIMMS device having a liquid metal channel.











DESCRIPTION OF A PREFERRED EMBODIMENT




Refer now to

FIG. 6

, wherein is shown a simplified representation


33


of a cross section taken through a heater cavity for a LIMMS device constructed with the heater resistor therein


66


suspended above the substrate


50


. The substrate


50


may be of ceramic or of glass, and it has had holes


54


and


55


drilled or otherwise formed therein to act as vias for the conductors that carry the electrical signals that drive the heater resistor


66


. What is contemplated is the possibility of a larger arrangement (not itself depicted) wherein there may be carried by the substrate


50


many other LIMMS devices or other circuit elements (after the manner of complete circuit assemblies mounted on the substrate to form a so-called hybrid circuit) having, in total, a large number of conductors to be dealt with, so that it is desirable to use ball grid surface mount techniques to connect those conductors to the larger outer environment. On the other hand, we do not rule out the possibility that the number of conductors is still modest, or even small, but that it is nevertheless desirable for some other reasons to employ the surface mount ball grid technique. (These reasons might include, but are not limited to, the pre-existence in the manufacturing environment of a surface mount process for the larger part—the hybrid—being built, an absence or aversion to wire bonding in favor of the solder ball idea, and a possibility that the density of the hybrid is so high that it is desirable to minimize the amount of surface real estate devoted to interconnection between parts.) In any event, the reader will appreciate that the application of vias is an effective way to get signals from one side of a substrate to another, for whatever reason.




To continue, the underside of the substrate


50


has a patterned layer of metal, very possibly of gold, of which regions


51


,


52


,


53


,


58


and


59


are representative. Elements


51


-


53


may be simply a ground plane or serve as portions of controlled impedance transmission line structures, such as co-planar transmission lines. Alternatively, one or more of


51


-


53


might be absent. Elements


58


and


59


are pads that connect to metallic plugs


56


and


57


, respectively. Those plugs are formed in the holes


54


and


55


and serve as the actual electrical connection of the via from one side of substrate


50


to the other. Pads


58


and


59


carry solder balls


60


and


61


that are central to the surface mount ball grid technique: they re-flow against a matching pattern of mounting pads upon the application of heat during the process of attaching (by soldering) the part in

FIG. 6

to a larger part (not shown) that carries it. It will be appreciated that there may be a layer of solder resist (not shown) that assists in avoiding unwanted connection between


51


-


53


and any conductive surface proximate after mounting.




And now to a topic of some interest. While the regions


51


-


53


might be the remnants of an undifferentiated sheet originally covering the entire bottom surface of the substrate


50


and patterned by etching, the subsequent manner of forming a plug/pad combination (


54


/


58


,


57


/


59


) is as follows. First, the associated hole is drilled and the hole filled (plugged) with a powdered composition including the metal, such as gold. It is then made hard and permanent by the application of heat, as in sintering. There is some shrinkage of the plug as it is fired, both longitudinally along its axis and in diameter. The diameter shrinkage creates a non-hermetic seal, which is also compounded by the porosity of the plug.




After the plug is formed the bottom pad (


58


,


59


) is printed using, for example, a powered thick film composition of PtPdAg, which is then fired. The plug and the pad make electrical contact owing to their intimate proximity. The PtPdAg is, after curing, an effective hermetic seal across the (bottom) end of the via. The PtPdAg pad is thin, and if soldered to in the immediate region of the via plug, permits leaching of the via plug's metal through the pad and into the solder. This can embrittle the solder, which causes reliability problems. This leads us to use an enlarged or elongated pad with the solder ball offset from the plug.




For additional hermetic protection we are inclined to also individually seal the top end of each via as it emerges from (or enters into) the substrate. And, we want to suspend the heater resistor


66


that is associated with these vias. Mindful that processing steps cost money, we would appreciate it if there were a way to accomplish two goals by combing steps common to both goals.




After having formed the vias and their pads


58


and


59


, we apply regions


62


and


63


of patterned thick film dielectric material. That application is a printing and firing step involving, for example, either the (afore-mentioned in the Summary) KQ material from Heraeus or the DuPont product. (Note the sloped sides of the regions


62


and


63


; they arise as explained the Background during the firing that cures the multiple printed layers of the dielectric material.) Then we print and fire gold or silver bearing pads


64


and


65


from the vias to top surfaces of regions


62


and


63


, respectively. They are in turn covered by any protective metallic layer (chromium or molybdenum) needed to protect against mercury or mercury vapor. These pads are hermetic. The sloping sides leading down toward the vias are useful at this point, as printing on a slope is quite possible, while printing along a vertical portion of a steep transition is problematic. Next, regions of dielectric


67


and


68


are formed, proceeding right up the sloping portion of the pads


64


and


65


, respectively. Notice that the entire top of the vias are enclosed by the dielectric material. It is a glass-like substance after it is cured, and quite suitable as an hermetic seal. The result is a good hermetic seal in a pad that is impervious to attack from the mercury, and whose surface well above the substrate (for affixing a suspended heater resistor


66


).




Subsequently, heater resistor


66


is affixed in place. Suitable resistors include known semiconductor composites as well as other known materials, and there are various known ways of electrically and physically attaching them to the pads (


64


,


65


). In due course a cover plate


70


(which may be of glass, or perhaps ceramic) having suitable recesses (for the heater cavities and perhaps the liquid metal channels and their interconnecting passages) and bearing a matching pattern of CYTOP is attached. One way to form the patterning of the cover plate and the layer of CYTOP is to apply a layer of the CYTOP to the underside of the cover plate and then use an abrasive blasting process to pattern both at the same time. Known techniques may be used to accomplish an additional hermetic seal between the perimeter of the cover plate


70


and the substrate


50


.




Refer now to

FIG. 7

, wherein is shown a cross section


79


similar to that


33


of

FIG. 6

, save that the vias and the layer of dielectric material are formed in a somewhat different manner. The difference is that a single patterned layer


71


of dielectric material is formed before the holes


71


and


72


are drilled for the vias. When those holes are drilled they made are all the way straight through both the substrate


50


and the layer of dielectric


71


. We next form long via plugs


75


and


76


. Then offset bottom pads


58


and


59


are formed, as are top pads


73


and


74


. In all other aspects

FIGS. 6 and 7

are essentially the same.




We now use

FIG. 7

as a point of departure for a further improvement. We would like to dispense with a top cover plate


70


having recessed cavities and/or channels therein. How that may be accomplished is shown and discussed in connection with

FIGS. 8 and 9

.




Referring now to

FIG. 8

, shown therein is a cross sectional view


80


whose lower portion (from adhesive layer


69


and resistor


66


downward) is the same as in

FIG. 7

, but which does not incorporate the recessed top cover plate


70


. In its place there is a top substrate


78


bearing a patterned layer


77


of dielectric material, that may be either the KQ material from Heraeus or the DuPont product. The patterning of dielectric layer


77


matches whatever recesses, channels, passages and cavities that would have been in the cover plate


70


, had it been used instead. The upper substrate and its patterned dielectric layer


77


are attached by the patterned adhesive layer


69


, as before. It will, of course, be appreciated that technique of

FIG. 8

(the forming of recesses, channels, passages and cavities in a dielectric layer patterned on an upper substrate) could also be used with the technique of

FIG. 6

to replace the cover plate


70


.




Finally, refer now to

FIG. 9

, which is a cross sectional view


81


of LIMMS device fabricated in the manner of

FIG. 8

, but where the sectional view is taken through channel containing the movable liquid metal droplet (or slug). It will be appreciated, then, that in this view substrate


50


has the deposited and then patterned layer


71


of dielectric (which includes a void under the heater resistor


66


of

FIG. 8

, but does not have such a void as part of the heater channel shown in

FIG. 9

, although it might). The underside of substrate


50


may have patterned metallic regions


83


-


87


that correspond to


51


-


53


of FIG.


8


. In the same way, the three vias in

FIG. 9

are formed with holes


88


-


90


that contain plugs


91


-


93


, and that are respectively in ohmic contact with pads


94


-


97


, and also respectively with pads


100


-


102


. Solder balls


97


-


99


are offset from their respective plugs


91


-


93


. Upper substrate


78


may optionally have the patterned remnants


82


and


83


of metal that serve either as a ground shield, ground plane or as signal conductors.




Now note metallic regions


103


-


105


. These are depositions that are intended to provide a wetting action to the movable metallic droplet, as mentioned earlier. They are not there to provide electrical contact, so that we have for that, for instance, region


103


does not touch pad


100


. It does not touch because region


103


does not extend over the lip of layer


77


toward the region occupied by the layer


69


of CYTOP. Now, it likely would not hurt anything if region


103


did extent to the left and was covered by the CYTOP: the CYTOP is resilient and the layer of metal forming region


103


is thin.




Recall that if the moving metal is mercury and the pads


100


-


102


and their associated regions


103


-


105


are of gold (or another metal that reacts with mercury), then those surfaces of gold must be protected from amalgamation and being dissolved by covering layers of suitable protection, say, of chromium or molybdenum.



Claims
  • 1. An electrical switching assembly comprising:a first non-conductive substrate having first and second surfaces; a first layer of dielectric material deposited upon the first surface of the first non-conductive substrate and patterned to create heater cavities, a liquid metal channel and passages connecting the heater cavities to locations along the liquid metal channel; a second non-conductive substrate having a first surface; a second layer of dielectric material deposited upon the first surface of the second non-conductive substrate and patterned to match at least the heater cavities of the first layer of dielectric material; a layer of adhesive deposited on the second layer of dielectric material and patterned to match the pattern of the first layer of dielectric material; and the surfaces of first and second non-conducting substrates facing each other and being brought into contact through the intervening first and second layers of dielectric material and the layer of adhesive.
  • 2. An electrical switching assembly as in claim 1 wherein at least one of the first and second non-conductive substrates is of glass.
  • 3. An electrical switching assembly as in claim 1 wherein at least one of the first and second non-conductive substrates is of ceramic.
  • 4. An electrical switching assembly as in claim 1 further comprising conductive vias through the first non-conductive substrate and first layer of dielectric material, an end of each conductive via being within the heater cavity.
  • 5. An electrical switching assembly as in claim 4 further comprising pads inside the heater cavity that cover the vias and a heater resistor suspended between the pads.
  • 6. An electrical switching assembly as in claim 4 further comprising conductive vias through the first non-conductive substrate and first layer of dielectric material, an end of each conductive via being within the liquid metal channel.
  • 7. An electrical switching assembly as in claim 1 wherein the first and second layers of dielectric material are deposited with thick film techniques.
  • 8. An electrical switching assembly comprising:a first non-conductive substrate having first and second surfaces; a layer of dielectric material deposited upon the first surface of the first non-conductive substrate and patterned to create heater cavities, a liquid metal channel and passages connecting the heater cavities to locations along the liquid metal channel; a second non-conductive substrate having a first surface patterned to match at least the heater cavities of the first layer of dielectric material; a layer of adhesive deposited on the first surface of the second non-conductive substrate and patterned to match the pattern of the layer of dielectric material; and the surfaces of first and second non-conducting substrates facing each other and being brought into contact through the intervening layer of dielectric material and the layer of adhesive.
  • 9. An electrical switching assembly as in claim 8 wherein at least one of the first and second non-conductive substrates is of glass.
  • 10. An electrical switching assembly as in claim 8 wherein at least one of the first and second non-conductive substrates is of ceramic.
  • 11. An electrical switching assembly as in claim 8 further comprising conductive vias through the first non-conductive substrate and first layer of dielectric material, an end of each conductive via being within the heater cavity.
  • 12. An electrical switching assembly as in claim 11 further comprising pads inside the heater cavity that cover the vias and a heater resistor suspended between the pads.
  • 13. An electrical switching assembly as in claim 11 further comprising conductive vias through the first non-conductive substrate and first layer of dielectric material, an end of each conductive via being within the liquid metal channel.
  • 14. An electrical switching assembly as in claim 8 wherein the first and second layers of dielectric material are deposited with thick film techniques.
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