USRE41801E1 - Thin-film thermoelectric device and fabrication method of same - Google Patents
Thin-film thermoelectric device and fabrication method of same Download PDFInfo
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- USRE41801E1 USRE41801E1 US10/404,144 US40414498A USRE41801E US RE41801 E1 USRE41801 E1 US RE41801E1 US 40414498 A US40414498 A US 40414498A US RE41801 E USRE41801 E US RE41801E
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- 238000000034 method Methods 0.000 title claims abstract description 32
- 238000004519 manufacturing process Methods 0.000 title claims abstract description 20
- 239000010409 thin film Substances 0.000 title description 22
- 239000000463 material Substances 0.000 claims abstract description 47
- 239000011159 matrix material Substances 0.000 claims abstract description 22
- 239000000758 substrate Substances 0.000 claims description 20
- 238000000059 patterning Methods 0.000 claims description 8
- 238000010248 power generation Methods 0.000 claims description 8
- 239000002096 quantum dot Substances 0.000 claims description 7
- 238000000926 separation method Methods 0.000 claims description 7
- 238000000151 deposition Methods 0.000 claims description 5
- 238000009792 diffusion process Methods 0.000 claims description 2
- 239000004020 conductor Substances 0.000 claims 2
- 238000005468 ion implantation Methods 0.000 claims 1
- 238000001816 cooling Methods 0.000 description 17
- 239000010408 film Substances 0.000 description 17
- 238000001465 metallisation Methods 0.000 description 14
- 238000010586 diagram Methods 0.000 description 7
- 230000008901 benefit Effects 0.000 description 4
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- 238000003892 spreading Methods 0.000 description 4
- 238000005229 chemical vapour deposition Methods 0.000 description 3
- 238000005530 etching Methods 0.000 description 3
- 238000012856 packing Methods 0.000 description 3
- 230000007480 spreading Effects 0.000 description 3
- 238000012986 modification Methods 0.000 description 2
- 230000004048 modification Effects 0.000 description 2
- 238000012545 processing Methods 0.000 description 2
- 238000011160 research Methods 0.000 description 2
- 239000007858 starting material Substances 0.000 description 2
- 238000013459 approach Methods 0.000 description 1
- 238000006243 chemical reaction Methods 0.000 description 1
- 230000007123 defense Effects 0.000 description 1
- 230000008021 deposition Effects 0.000 description 1
- 238000013461 design Methods 0.000 description 1
- 230000001627 detrimental effect Effects 0.000 description 1
- 238000011982 device technology Methods 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 230000008020 evaporation Effects 0.000 description 1
- 238000003780 insertion Methods 0.000 description 1
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- 238000002955 isolation Methods 0.000 description 1
- 238000000608 laser ablation Methods 0.000 description 1
- 239000002184 metal Substances 0.000 description 1
- 238000004377 microelectronic Methods 0.000 description 1
- 238000001451 molecular beam epitaxy Methods 0.000 description 1
- 238000002360 preparation method Methods 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
- 235000012431 wafers Nutrition 0.000 description 1
Images
Classifications
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- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y10/00—Nanotechnology for information processing, storage or transmission, e.g. quantum computing or single electron logic
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N10/00—Thermoelectric devices comprising a junction of dissimilar materials, i.e. devices exhibiting Seebeck or Peltier effects
- H10N10/10—Thermoelectric devices comprising a junction of dissimilar materials, i.e. devices exhibiting Seebeck or Peltier effects operating with only the Peltier or Seebeck effects
- H10N10/13—Thermoelectric devices comprising a junction of dissimilar materials, i.e. devices exhibiting Seebeck or Peltier effects operating with only the Peltier or Seebeck effects characterised by the heat-exchanging means at the junction
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N10/00—Thermoelectric devices comprising a junction of dissimilar materials, i.e. devices exhibiting Seebeck or Peltier effects
- H10N10/10—Thermoelectric devices comprising a junction of dissimilar materials, i.e. devices exhibiting Seebeck or Peltier effects operating with only the Peltier or Seebeck effects
- H10N10/17—Thermoelectric devices comprising a junction of dissimilar materials, i.e. devices exhibiting Seebeck or Peltier effects operating with only the Peltier or Seebeck effects characterised by the structure or configuration of the cell or thermocouple forming the device
-
- H—ELECTRICITY
- H10—SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N—ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
- H10N10/00—Thermoelectric devices comprising a junction of dissimilar materials, i.e. devices exhibiting Seebeck or Peltier effects
- H10N10/80—Constructional details
- H10N10/81—Structural details of the junction
- H10N10/817—Structural details of the junction the junction being non-separable, e.g. being cemented, sintered or soldered
-
- Y—GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10—TECHNICAL SUBJECTS COVERED BY FORMER USPC
- Y10S—TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
- Y10S257/00—Active solid-state devices, e.g. transistors, solid-state diodes
- Y10S257/93—Thermoelectric, e.g. peltier effect cooling
Definitions
- the present invention relates to thin-film thermoelectric devices and methods of manufacturing such devices, and particularly to thin-film thermoelectric devices with high utilization efficiency and high cooling/packing density and methods of manufacturing such devices.
- thermoelectric thin films have been used to form high-performance thermoelectric devices.
- Superlattice thermoelectric materials and quantum-well and quantum-dot structured materials have been proposed.
- the thin-film thermoelectric devices should also be scalable to a variety of heat loads and manufacturable in large volume (area).
- the methods used to manufacture the devices must be amenable to automation, compatible with cascading or multi-staging (leading to a smaller ⁇ T per stage for a higher coefficient of performance in a refrigerator or for higher efficiency in a power generator) and is equally applicable to both cooling and power generation.
- the device technology would enable the insertion of high-ZT thin-films (i.e. films with a figure of merit ZT greater than one) into high performance cooling devices while keeping the current levels compatible with present-day coolers and similar power generation devices.
- An object of the present invention is to provide a thin-film thermoelectric device and a method of manufacturing the device that achieves high material utilization efficiency.
- Another object of the present invention is to provide a thin-film thermoelectric device and a method of manufacturing the device that achieves high cooling/packing density.
- a further object of the present invention is to provide a thin-film thermoelectric device and a method of manufacturing the device that is scalable to a variety of heat loads.
- a still further object of the present invention to provide and manufacture large area thin-film thermoelectric devices.
- thermoelectric elements that can be used with low-cost power supplies.
- thermoelectric device having a plurality of thermoelectric elements (i.e. a plurality of thermoelements) formed using thin films in the range of microns to tens of microns.
- the elements may be arranged in a matrix pattern with adjacent rows having opposite conductivity type.
- the elements are disposed on a header with a pattern of conductive members. Pairs of adjacent elements of opposite conductivity type are disposed on and connected by the conductive members.
- a second header with a second pattern of conductive members is disposed on top of the elements. The conductive members of the second header connect adjacent pairs of connected elements so that the pairs are connected in series.
- thermoelectric device a method of forming a thermoelectric device.
- thin films having a thickness on the order of microns to tens of ductivity type may be formed on different substrates or one film may be formed and later selectively doped to provide regions of opposite conductivity.
- the film or films are disposed on the first header and the substrates removed. When films of opposite conductivity type are used, they are arranged in an alternating manner.
- the films are patterned to provide a plurality of thermoelectric elements in a matrix pattern. Pairs of elements, one of each conductivity type are disposed on respective conductive members on the first header. A second header is disposed on the top of the elements. Conductive members on the second header contact the pairs such that the pairs are connected in series.
- the device and method according to the invention are scalable to a variety of heat loads and is manufacturable in volume. They are amenable to automation and are compatible with cascading or multistaging. Further, the device and method are applicable to both cooling and power generation.
- FIGS. 1A and 1B are diagrams of n and p type starting materials, respectively, illustrating a step of manufacturing according to the invention
- FIGS. 2A and 2B are diagrams of segments of the n and p type starting materials, respectively, illustrating a step of manufacturing according to the invention
- FIG. 3 is a diagram of assembled segments illustrating a step of manufacturing according to the invention.
- FIG. 4 is a plan view of a header for contacting the assembled segments
- FIG. 5 is a diagram of n and p thin film sections disposed on the header of FIG. 3 illustrating a step of manufacturing according to the invention
- FIG. 6 is a diagram of a n and p sections disposed on the header of FIG. 3 after patterning, and illustrating a step of manufacturing according to the invention
- FIG. 7 is a diagram of a n and p sections of FIG. 6 after metallization and illustrating a step of manufacturing according to the invention
- FIG. 8 is a plan view of a header for attachment to the n and p sections.
- FIG. 9 is a diagram of the device according to the invention having n and p elements with the headers of FIGS. 4 and 8 attached.
- FIG. 1 illustrating a step in the process of manufacturing a thin-film thermoelectric device according to the invention.
- the device according to the invention is called a Bipolarity-Assembled, Series Inter-Connected, Thin-Film Thermoelectric Device (BASIC-TFTD). It utilizes thin films of thickness in the range of microns to tens of microns, grown or deposited on a substrate using techniques such as metallorganic chemical vapor deposition (MOCVD), chemical vapor deposition (CVD), molecular beam epitaxy (MBE) and other epitaxial/non-epitaxile processes.
- MOCVD metalorganic chemical vapor deposition
- CVD chemical vapor deposition
- MBE molecular beam epitaxy
- the thin films can consist of thin-film superlattice or non-superlattice thermoelectric materials, quantum-well (two-dimensional quantum-confined) and quantum-dot (three dimensional quantum-confined type) structured materials, and non-quantum-confined materials. Also, materials that are peeled from bulk materials can also be used.
- n-type and p-type films 11 and 12 formed as described above are formed on substrates 10 .
- Substrates 10 may have the same conductivity type as the overlying films 11 or 12 .
- the films 11 and 12 are shown as multi-layered structures but could also be a single-layer structure. Typical dimensions of these wafers could be 2 cm ⁇ 2 cm (width ⁇ length), but other sizes are possible.
- the substrates are typically a few mils thick and the film 11 and 12 are typically 5 to 20 ⁇ m in thickness.
- the films 11 and 12 are metallized, their respective upper surfaces providing a low-resistance contact, such as a low-resistance Peltier contact.
- the substrates 10 are separated by, for example, scribing, into many segments 20 and 21 .
- a typical width of the segments 1 to 5 mm.
- the size of the substrates 10 before and after separation in segments can be varied depending upon the requirements of the resulting devices.
- the segments 20 and 21 are bonded onto a cooling header or a power header 30 with alternating conductivity in FIG. 3 .
- the header can made of, for example, BeO.
- the bonding may be carried out using a conventional bonding method. Note that the substrates are facing upward and that the segments 20 and 21 have a finite separation, in this case of about 10 ⁇ m.
- the bonding pattern of the header 30 for an exemplary 8 ⁇ 9 thermoelement matrix, upon which the segments are bonded is shown in FIG. 4 .
- the surfaces of the cooling header/power header 30 that come in contact with the n- and p-type segments have to be metallized prior to assembly to provide the necessary low-resistance electrical connection between adjacent n- and p-type segments.
- the header includes a metallization for bonding an n-type segment of size a 1 , a metallization for bonding a p-type segment of size a 2 , and a metallization for series-connecting n- and p-type segments to form a couple,
- the metallizations have a width a 3 and are separated in the in the length direction by a gap of size b 2 and in the width direction by a gap of size c. Typical dimensions for a 1 , a 2 , b 1 , b 2 and c are given in FIG. 4 .
- FIG. 4 indicates ranges in dimensions a 1 , a 2 , a 3 , b 1 , b 2 , and c with, according to the present invention, a 1 ranging from 1 mm to 5 mm, a 2 ranging from 1 mm to 5 mm, a 3 ranging from 5 to 50 ⁇ m, b 1 and b 2 approximately 10 ⁇ m, and c ranging from ⁇ 2 to 10 ⁇ m.
- the n- and p-type segments are attached to a mounting surface of the cooling/power header 30 (i.e. an interconnecting member between the n- and p-type segments) with the opposed major surfaces of the deposited film in each segment arranged parallel to the mounting surface of the cooling/power header 30 .
- the substrates from each of the p- and n-segments are removed selectively without affecting the films 11 and 12 . This can typically be achieved by using selective etchants for substrates. Similar substrates, if used for both the n- and p-type segments 20 and 21 , can be removed in a single substrate removal process. After this process the BASIC-TFTD device structure would look as shown in FIG. 5 where two pairs of n, p segments are shown for convenience. The segments 11 and 12 , after substrate removal, are supported on the cooling/power header 30 for stability and handling.
- the overlying films 11 and 12 consisting of the afore-mentioned thin-film materials are arranged such the deposited films have opposed major surfaces separated by a total thickness of the deposited films such that at least one of the major surfaces is in contact with the cooling/power header 30 .
- the segments 11 and 12 are patterned in the y-direction into sections 60 and 61 .
- This step maybe carried out using photolithographic patterning followed by etching, or by laser ablation, for example.
- the device at this stage is shown in FIG. 6 .
- Typical parameters of the sections, for two examples, are given as:
- a 3 and c can easily be achieved with conventional microelectronic processing/etching. Also, b, c ⁇ a 1 , a 2 , and a 3 .
- the invention also provides several advantages. The material removed in etching is very small, leading to good material utilization efficiency high cooling/packing density can be achieved.
- Low resistivity contact metallization is then evaporated on upper surface of the n- and p-type sections, as shown in FIG. 7 .
- this step either the same metallization can be used for both of the n- and p-type section, or different metallizations can be used (separate evaporations), depending on the contact resistivity requirements.
- a top, pre-patterned metallization header 90 is then attached to the metallized sections.
- Shown in FIG. 8 is a schematic of the metallization pattern of the metallized header that will serve on the heat-sink side.
- An 8 ⁇ 9 thermoelement matrix metallization pattern is needed for this header, to correspond the metallization pattern of header 30 (see FIG. 4 ).
- the metal members of the metallization pattern provide a low-resistance contact to the sections 60 and 61 .
- the two leads, A and B are shown.
- a positive voltage would be applied to lead A and a negative (or ground) voltage would be applied to lead B for cooling.
- the metallization pattern pads contacting ntype and ptype elements are shown by parentheses. The spacing of the patterns matches that of the sections.
- thermoelements are thermally in parallel (between heat-sink and heat-source) and electrically in series.
- thermoelements For this 8 ⁇ 9 matrix of thermoelements, four each of the n- and p-type elements (identified by “y”) do not participate in the current transport through the thickness of the film They only serve to provide the electrical connection and uniform mechanical strength in the arrange men t of the thermoelements.
- the aspect ratios of the sections can be adjusted.
- the aspect ratios can be selected to provide a desired geometry while satisfying the above m>>n condition.
- the aspect ratios can be selected to insure low-current operation, allowing the use of low-cost power supplies for connection to the headers 30 and 90 .
- the material (superlattice or non-superlattice) for the n- and p-type elements can be different, as is usually the case in many conventional bulk materials. However, if the materials are the same for n- and p-type elements, and if one polarity can be typed-converted to another (p to n or n to p) by a technique, for example impurity-diffusion, without disordering the superlattice or introducing other detrimental effects, then a Bipolar Diffused, Series Interconnected, Thin-Film Thermoelectric Device (BDSIC-TFTD) can be constructed which does not require the assembly step shown in FIG. 3 (i.e. by direct deposition).
- BDSIC-TFTD Bipolar Diffused, Series Interconnected, Thin-Film Thermoelectric Device
- the type-conversion can be performed at a convenient stage in the manufacturing process, such as when the device has the structure shown in FIGS. 5 and 6 .
- Such a device can potentially be manufactured even more cost-effectively, with additional advantages and flexibility in the design of the device parameters.
- the backside of an integrated circuit chip may be used as the cooling or power header.
- the backside especially if it is electrically conducting, needs to be suitably modified to confine the electrical current to the thermoelectric element.
- suitable preparation is p-n junction isolation in the backside of the chip whereby the current is made to flow through the intended thermoelectric electric elements, i.e. is confined to the elements, and is not shunted by the conducting backside of the chip.
- Other modifications of the backside are possible to achieve similar confinement of the current.
- the backside of the chip should be of good thermal conductivity.
- the backside then may be used to extract heat which could be used for other purposes such as power generation.
- the power generated using the heat could be used provide power to other circuits or to other cooling devices.
- the BASIC-TFTD according to the invention is scalable to a variety of heat loads and is manufacturable in large volume (area). It is amenable to automation, is compatible with cascading or multi-staging (leading to a smaller ⁇ T per stage for a higher coefficient of performance in a refrigerator or for higher efficiency in a power generator) and is equally applicable to both cooling and power generation.
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- Theoretical Computer Science (AREA)
- Crystallography & Structural Chemistry (AREA)
- Cooling Or The Like Of Semiconductors Or Solid State Devices (AREA)
Abstract
Description
EXAMPLE 1 | a1, a2 ˜1 mm | Area = a1 × a3 = 0.0005 cm2 | ||
a3 ˜50 mm | ||||
EXAMPLE 2 | a1, a2 ˜5 mm | Area = a1 × a3 = 0.005 cm2 | ||
a3 ˜100 mm | ||||
This efficiency will nearly approach unity when n is large and m is large. For example, in the 8×9 matrix, −89% utilization of material is obtained. For a 25×23 element matrix, >96% utilization of material is achieved. Assuming ideal heat-spreading on the heat-sink side header and the source-side header, the heat spreading in the “non-useful” elements would be about the same as the “useful” elements. Thus, we can expect module efficiency≅(intrinsic couple efficiency×material utilization efficiency) discussed above. By choosing m>>n (if system constraints permit) a non-square geometry will minimize the difference between module and intrinsic couple efficiency. This, of course, assumes ideal heat spreading between the thermoelement and the headers. A completed device according to the invention, having a set of
Claims (56)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
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US10/404,144 USRE41801E1 (en) | 1997-03-31 | 1998-03-31 | Thin-film thermoelectric device and fabrication method of same |
Applications Claiming Priority (3)
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US4284597P | 1997-03-31 | 1997-03-31 | |
US10/404,144 USRE41801E1 (en) | 1997-03-31 | 1998-03-31 | Thin-film thermoelectric device and fabrication method of same |
PCT/US1998/006150 WO1998044562A1 (en) | 1997-03-31 | 1998-03-31 | Thin-film thermoelectric device and fabrication method of same |
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US09/381,963 Reissue US6300150B1 (en) | 1997-03-31 | 1998-03-31 | Thin-film thermoelectric device and fabrication method of same |
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USRE41801E1 true USRE41801E1 (en) | 2010-10-05 |
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US10/404,144 Expired - Lifetime USRE41801E1 (en) | 1997-03-31 | 1998-03-31 | Thin-film thermoelectric device and fabrication method of same |
US09/381,963 Ceased US6300150B1 (en) | 1997-03-31 | 1998-03-31 | Thin-film thermoelectric device and fabrication method of same |
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US09/381,963 Ceased US6300150B1 (en) | 1997-03-31 | 1998-03-31 | Thin-film thermoelectric device and fabrication method of same |
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AU (1) | AU6783598A (en) |
WO (1) | WO1998044562A1 (en) |
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Also Published As
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AU6783598A (en) | 1998-10-22 |
WO1998044562A1 (en) | 1998-10-08 |
US6300150B1 (en) | 2001-10-09 |
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