INFRARED SOURCE
This invention relates to a sealed infrared radiation source, comprising an emitter comprising a thin structure, e.g. a membrane or thin band, being stimulated by an electrical current conducted through said membrane, said membrane thus comprising an electrical conductor.
Usually sealed infrared sources have electrical conductors for supplying energy to the emitter which passes between the layers constituted by glass housings and silicon membrane layers, as is described in US 5.591.679. This method, however, have several disadvantages such as complicated production and temperature characteristics.
US 5.285.131 describes an infrared source in the 2 micron IR range comprising a membrane being encased hermetically by the substrate and a silicon nitride window. The emitter membrane is doped with boron to increase the efficiency of the IR emission from the source. The solution described in this patent comprises electrical coupling of the power supply to the source through layers of metallized aluminium, which complicated the production and sealing of the casing. A similar solution is shown in US 5.955.839. Both these solutions have the disadvantage of being complicated to produce, as they comprise several different materials. Other examples are shown in US 5.814.870 and 6.204.083. The use of silicon being heavily doped with Boron or Phosphor to increase the efficiency of IR radiation of a source is known and described in US 5.827.438.
It is an object of this invention to provide a infrared source being possible to mass produce using silicon technology. The source should be sealed using ordinary bonding techniques to withstand both temperature variations and other strains. The present invention relates to a source and a method for making this source being based on the idea of supplying current through the housing parts, the housing parts also being made from silicon and being bonded to the emitter part by fusion bonding or similar. The invention is more specifically described in the independent claims. Thus a hermetically sealed source is provided in a very simple process, preferably a so-called fusion bonding process. The present invention thus provides a solution being suitable for mass production were all electrical conductor paths are lead through the whole stack. Thus the source may be hermetically sealed in vacuum or in
an inert gas during production and it is possible to pack e.g. 1500 source at the time. Today the packing costs are as high as the costs for the soured, as each chip is hand picked, glued to a can, wire bonded to the can, and a top with an IR window is welded to the can. Thus the present invention gives large cost reductions. According to a preferred embodiment of the invention the emitting membrane preferably comprises a silicon layer being doped with a very high concentration of Boron or Phosphor. This doped area is in thermal contact with an electrical conductor layer on the emitter, but electrically insulated from the electrical conductor layer on the emitter. The electrical conductor layer on the emitter has sufficient resistance to serve as a heater for the highly doped silicon. While silicon usually is semitransparent in the infrared spectrum the high doping makes the silicon opaque and therefore it emits radiation in the near infrared spectrum. The absorption properties of the highly doped silicon is well known in sensors and sources, e.g. as described in US 6,169,284 and US 5.827.438. Thus the preferred embodiment of the invention comprises an emitter being made from silicon and being highly doped with Boron or Phosfor, and which is in thermal contact with a resistor heating up the emitter when a current is applied to it. Preferably the emitter is packed in a silicon housing and being surrounded by a sealed cavity. In the wording of this specification emitter/radiating part and membrane are mainly regarded describing the function and the form, respectively, of the active part of the source.
The invention will now be described with reference to the accompanying drawings, illustrating the invention by way of examples. It should be noted that the scales in the drawings are distorted to simplify their understanding. Figures la,b illustrates the membranes of two embodiments of the invention as seen from above.
Figures 2-8 illustrates a preferred method for producing the source. Figure 9 illustrates the function of the IR source. Figure 10 illustrates an alternative emitter according to the invention. In figure Ia and Ib a top view of the emitting part of two alternative versions of the invention are illustrated. In this case the emitter is provided by an EPI membrane 11 comprising a conductive poly silicon area 10. The membrane also
comprises electrical contact areas 12,13 for providing coupling to upper and lower parts of the source housing.
The membrane also comprises holes 14,15 for pressure equilibration between the two sides of the membrane. In figure Ia the holes are large so as to provide heat insulation between the radiating part 10 and the remaining part of the membrane.
In this case the emitting part 10 acts as a radiating band or strip which may be made with a chosen width depending on the intended use. The band shaped embodiment may provide fast response, but will have slow heat conduction away from the sensor, thus increasing the risk for over heating. In figure Ib the radiating part 10 has almost full contact with the surrounding walls, which improves the heat transfer ratio to the environment through the material.
The source according to the invention is produced as illustrated in the accompanying drawings, figure 2-8. According to the preferred method of production a first silicon layer 1,4 is provided on a silicon substrate 3 and being insulated from the substrate by an oxide layer 2. Holes 5 are etched in the first silicon layer for providing pressure equilibration etc corresponding to the openings 14,15 shown in figures Ia5Ib.
A chosen part 1 of the silicon layer 4 chosen to act as emitter in the source is doped with a high concentration of Boron or Phosphor to increase the efficiency, as described above.
In figure 3 an oxide layer 6 is then provided on the first silicon layer 4 and the holes 5.
As shown in figure 4 openings 7,8 are provided in the oxide layer 6. One of said openings 7,8 being in one of the holes 5 through the first silicon layer 4, so as to provide a hole directly through to the substrate 3. Another of said openings 7 is provided to obtain contact through the oxide layer 6 to the first silicon layer 4, the position of this opening not being on the highly doped part 1.
In figure 5 an electrical conductive layer 9 (e.g. doped polysilicon) is provided on the first silicon layer thus also covering the holes and openings in the upper oxide layer. Thus the electrically conductive layer provides electrical contact through the openings 7,8 to both the substrate 3 and at least a part of the first silicon layer 4.
The electrically conductive polysilicon layer is then, see figure 6 removed from the holes 5, except from the hole being provided with the opening 8 to the substrate 3, and from other parts 21 (see figure 7) along the rim of first silicon layer 11. Thus electrical coupling is obtained from the rim area 21, through the opening 7 to the polysilicon layer, passed the Boron og Phosphor doped emitter area 1, and through the opening 8 in a hole in the first silicon layer to the substrate 3.
The oxide layer 6 is also removed from the rim 21 of the first silicon layer and from the holes 5 not provided with the conductive polysilicon layer, and a cavity is etched through the substrate from below up to the lower oxide layer 2 under the Boron or Phosphor doped area 1 forming the emitter area, and the holes 5. Thus through-holes 14 are obtained connecting the cavity and the upper side of the emitter. Thus the emitter is left as a membrane enclosed in an oxide layer and being provided with an electrically conductive heater layer, e.g. of doped polysilicon.
As shown in figure 8 new silicon housing parts 16,17 are then laminated over and below the element , preferably using a bonding process. The upper housing part 16 defines a cavity and is bonded to the first silicon layer 4 along the rim 21 where the oxide layer was removed, thus providing electrical contact between the upper housing and the first silicon layer, and the lower housing part 17 is bonded to the substrate 3 thus defining a lower cavity. As mentioned above the two cavities are provided with a pressure equilibration holes between them, but are otherwise sealed, and may be filled with inert gas or vacuum to avoid oxidation. The lower housing part is provided with electrical contact with the electrically conductive layer of polysilicon through the hole provided with an opening in the silicon layer. According to an alternative embodiment the lower housing part is also provided with a cavity under the radiation element 1.
Metal layers 18,19 may then be provided on the upper and lower housing parts 16,17. One of said metallic layers should be provided with a window 20 above the emitter area 1 so as to allow the emitted infrared radiation pass through. The undoped silicon material in the housing 16 is transparent to infrared radiation. An electrical current between them indicated by the line 23 in figure 9 will then travel from the first housing part through the connection with the first silicon layer to the electrically conductive layer through the opening in the oxide, layer. It then
passes the electrically conductive layer provided on but insulated from the highly Boron or Phosphor doped membrane and through the hole in the first silicon layer and opening in the oxide layer to the substrate, and further to the lower housing part. Although the holes 5 are shown in the drawings these have limited sizes, se the holes 14,16 in figures Ia and Ib, and the electrical current path indicated by reference numeral 23 propagates around them unhindered.
Thus no separate electrical conductors are needed for providing a current to the membrane, only electrical contacts provided outside the housing. This requires only standard technology. Although the illustrated embodiment includes electrical contact 18,19 on the upper or lower surfaces of the housing other electrically equivalent solutions may of course be applied, e.g. on the sides of the housing or surfaces protruding from the sides. The important aspect of this invention being that it provides a radiation source and a method for producing this which may efficiently sealed using bonding techniques or similar. According to an alternative embodiment of the invention optical elements, such as a lens or diffractive optical elements are provided on or in the structure of one of the housing parts, thus shaping or focussing the infrared light emitted from the membrane. The diffractive optical element is especially advantageous if the light source is small or collimated, or a distance is provided between the source and the optical elements. A filter may also be added to modulate the wavelength distribution.
As mentioned above the device is primarily meant to be mass produced with silicon, being constructed by micromachining a radiation element in a silicon wafer. In another wafer a cavity is etched, so that the cavity is positioned above the radiation element. A third wafer, in which a cavity also may be etched, is laminated under the radiation element. The lamination may be performed using a so-called fusion bonding process, which provides a completely sealed coupling between the two.
As illustrated in figure 9 electrical contact is provided to the radiation element through the top wafer, which is coupled to an insulated epi-layer on the mid wafer, up from the epi-layer to a doped poly-Si layer extending above the radiation element 1, down from the poly-Si layer therough the epi-layer but insulated therefrom and further through an insulating oxide layer to the subtrate of the mid wafer and down to the bottom wafer. It is thus possible to couple directly to the top of the upper wafer
and to the surface of the bottom wafer, thus to send a current through the stack for heating the radiation element. When the radiation element is heated the IR radiation goes through the top wafer, which is transparent to IR because the doping level is low. The emitted radiation corresponds essentially to a grey body. It should be noted that the scales of the drawings above are exaggerated, especially in the ration between height and length. Typical dimensions of the radiation source is as follows:
The thickness of the radiation element: a few μm
Length/width of the radiaton element: typically in the range from a few hundred μm to a few mm.
Length/width of the chip. A couple of mm
Thickness of chip Typically l-2mm
Wafer thickness: Typically 300-500μm
The radiation source according to the invention is possible to produce using standard process steps of semiconductor technology. Silicon wafers are for example processed using
• photolithography,
• oxidation of silicon, • surface depositing,
• epitaxial growth of surface layers, implanting of conductors, resistors and etch stops with suitable atoms.
• Diffusion of implanted atoms
• Etching for freeing mechanical structures, in which the etching process is stopped against doped or implanted areas.
Processing this infrared radiation source will typically follow these steps:
• Grow highly doped silicon on a silicon substrate wafer wherein the surface silicon is insulated by an oxide. • Grow oxide on this thin highly doped silicon layer.
• Deposit a thin polysilicon film on this oxide layer.
• Make insulated electrical contact points between the poly-silicon layer and the grown silicon layer, and between the polysilicon layer and the substrate.
• Etch a 4μm thick structure from the back
• Pattern the surface layers with standard processes. • Etch cavities in the wafer to be bonded on top of the element wafer.
• Deposit aluminium contacts on the opposite side of the cavity.
• If applicable, etch cavities in the wafer to be laminated under the element wafer.
• Deposit aluminium contacts in the opposite side from the cavity and surface to be bonded with the element wafer. • Laminate the three wafers with fusion bonding.
As the emitter membrane may be subject to large temperature fluctuations it may be advantageous to the prove temperature sensors such as a temperature sensitive resistor or diode on the emitter. The sensor being provided with electrical conductors for coupling to the temperature measuring means monitoring the temperature of the emitter, said temperature measuring circuitry being provided in the housing or externally for monitoring the temperature of the emitter. Alternative other temperature measuring means may be employed to monitor the temperature of the emitting membrane, e.g. positioned in the housing. Other variations and alternatives may of course also be made by a person skilled in the art within the scope of this invention, such as providing the electrical contacts on the sides of the source housing or variations in the materials used to manufacture the unit.
As is clear from figure 9 the emitting part 10 of the source is constituted by a conductive layer 9, e.g. polysilicon, and a doped layer 1, e.g. doped with Boron og Phosphor, being separated by an insulating layer 6.
Fig. 10 illustrates an alternative emitter according to the invention. In the embodiments discussed above the current is lead through openings 12,13 in the doped layer and being insulated from this. In figure 10 the current is lead through the doped layer 31 and through an opening 35 in the insulating layer 34 separating it from the heater layer 32. This way the current is forced through a small area of the heater layer 32, providing a larger current in the area surrounding the opening and thus increasing the emitted IR intensity in this area.
In figure 10 the source is illustrated with electrodes 33 mounted on top of the emitter, but the solution in figure 9, with electrical contacts at the top and bottom may of course also be used with the necessary modifications, e.g. concerning the openings for leading the current to the heater layer. The electrodes 10 in figure 10 are ring shaped so at to provide a uniform current flow into and from the opening 35. The opening may be a complete removal of the insulating layer 34 or a thin layer may remain, especially when the drive current is pulsed or an AC current is provided.