WO1992006561A1 - Temperature stabilization buffer for a solid state electronic component - Google Patents

Temperature stabilization buffer for a solid state electronic component Download PDF

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Publication number
WO1992006561A1
WO1992006561A1 PCT/US1991/007043 US9107043W WO9206561A1 WO 1992006561 A1 WO1992006561 A1 WO 1992006561A1 US 9107043 W US9107043 W US 9107043W WO 9206561 A1 WO9206561 A1 WO 9206561A1
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WIPO (PCT)
Prior art keywords
temperature
ccd array
solid state
ccd
electronic component
Prior art date
Application number
PCT/US1991/007043
Other languages
French (fr)
Inventor
Frank Charles Brasington
Original Assignee
E.I. Du Pont De Nemours And Company
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Filing date
Publication date
Application filed by E.I. Du Pont De Nemours And Company filed Critical E.I. Du Pont De Nemours And Company
Publication of WO1992006561A1 publication Critical patent/WO1992006561A1/en

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Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L23/00Details of semiconductor or other solid state devices
    • H01L23/34Arrangements for cooling, heating, ventilating or temperature compensation ; Temperature sensing arrangements
    • H01L23/38Cooling arrangements using the Peltier effect
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L23/00Details of semiconductor or other solid state devices
    • H01L23/34Arrangements for cooling, heating, ventilating or temperature compensation ; Temperature sensing arrangements
    • H01L23/36Selection of materials, or shaping, to facilitate cooling or heating, e.g. heatsinks
    • H01L23/373Cooling facilitated by selection of materials for the device or materials for thermal expansion adaptation, e.g. carbon
    • H01L23/3736Metallic materials
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N23/00Cameras or camera modules comprising electronic image sensors; Control thereof
    • H04N23/50Constructional details
    • H04N23/52Elements optimising image sensor operation, e.g. for electromagnetic interference [EMI] protection or temperature control by heat transfer or cooling elements
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L2924/00Indexing scheme for arrangements or methods for connecting or disconnecting semiconductor or solid-state bodies as covered by H01L24/00
    • H01L2924/0001Technical content checked by a classifier
    • H01L2924/0002Not covered by any one of groups H01L24/00, H01L24/00 and H01L2224/00

Definitions

  • This invention relates to a solid-state device, such as a CCD, where the operating temperature is kept substantially constant to stabilize dark current noise.
  • dark current is the amount of ambient current detectable in individual imaging elements when the CCD is energized in the absence of the imaging beam.
  • dark current in each element of the CCD array is measured prior to a scan and stored as an offset value for later correction of image readings.
  • Technologists working with solid- state imagers wish that the problem of dark current noise were resolved so easily, unfortunately it is not.
  • the present invention does not require significant cooling of the CCD. As it operates at near room temperature, it is much less susceptible to humidity problems. Consequently, it does not require the energy and expense of evacuating an enclosure and filling it with dry gas to keep the CCD cooled significantly below its operating environment,-
  • the present invention is a relatively inexpensive and easily-implement ble solution to a well known problem of resolving the floating dark current problem for solid state devices.
  • This invention is based on two fundamental principles. First, it is often important that the temperature of a solid state electronic component, such as a CCD array, remain substantially constant during use.
  • the dark current problem is largely related to the fact that the offset calibration values change while the CCD is in use.
  • the apparatus of Applicant's invention successfully fixes the operating temperature of the CCD array to just below room temperature so that the offset values remain a substantially accurate representation throughout image scanning and may be used to adjust the actual data.
  • This approach has been successfully employed by Applicant in an industrial non-destructive testing radiographic system comprising scanner means, interactive display means, and storage and retrieval means.
  • this invention does not require cooling of the CCD to very low temperatures, it alleviates the time-consuming, costly and difficult measures that were heretofore undertaken to enclose and "refrigerate” the CCD.
  • This invention provides” good image signal resolution at near ambient air temperatures.
  • an image detecting system comprising a CCD array and a cooling element used to control the temperature of said CCD array
  • the improvement comprises: a temperature buffering means interposed in thermal contact between said CCD and said cooling element.
  • Figure 1 represents a prior art approach to cooling of a CCD array.
  • FIG. 1 shows the invention.
  • FIG. 3 is a schematic representation of circuitry employing the invention.
  • a heat transfer means 20 is thermally connected to the rear face of solid-state CCD imager 3, that is, opposite the face where the imaging beam is received. Heat transfer means 20 is utilized to provide a substantially uniform temperature exchange from the rear face of the CCD 3 to heat buffering means 4. To be most effective, the heat transfer means 20, such as a thermal pad or thermally conductive glue, should remain in thermal contact with both heat buffering means 4 and
  • Heat buffering means 4 is comprised of a relatively highly thermally conductive material, such as aluminum or copper. It extends along the full length of CCD 3 and acts to integrate small temperature fluctuations along the CCD.
  • a thermally conductive mounting plate 5 is centered and fixed orthogonal to heat buffering means 4.
  • Thermistor 18 may be placed longitudinally into a grooved out section of mounting plate 5 such that the thermistor thermal contacts both heat buffering means 4 and mounting plate 5.
  • the thermistor's output Upon sensing a change in temperature of the heat buffering means, the thermistor's output, which is continuously compared with a reference temperature voltage, triggers the application of sufficient current to cooling element 10 to maintain the reference temperature. This feedback control is accomplished using standard servo amplifier and power control techniques which are well known in the art. See Figure 3.
  • Cooling element 10 is attached by means of a thermally conductive medium to mounting plate 5 on the side opposite heat buffering means 4. Cooling element 10 might typically be a thermoelectric cooler with the "cool” side fixed to mounting plate 5. The "hot” side of 10 is attached to heat sink 6 to vent away heat during temperature cooling and maintenance.
  • the prior art response to the variable dark current problem can be found in figure 1.
  • the emphasis is upon cooling the CCD array substantially below room temperature to about 10°C.
  • a further definition of the dark current noise problem reveals that acceptable resolution of most signals can be obtained at about room temperature if that temperature can be sustained during imaging of the light source on the CCD. Unless the image signals are very small (e.g. astronomy signals), the key to relative freedom from temperature-dependent dark noise is to maintain a constant temperature so that the offset dark current values, established in the absence of light, will remain useful for making corrections to image data values.
  • thermoelectric cooling device (312, 314, and 316) directly to non-imaging side of the CCD (220) .
  • This solution may not be satisfactory in that the size of the cooling device may be smaller than the active area of the CCD array thus permitting uneven cooling.
  • thermoelectric cooler itself is not a perfect device and due to manufacturing differences in its internal metallic junctions, there may be differences in temperature across its surface. Also, as heat from the
  • the instant invention avoids the problem of improper sizing of TE 10 to the CCD by extending heat transfer means and heat buffering means over the full length of the CCD.
  • the heat buffering means smooths out changes in temperature so that: 1) no one element in the CCD array will experience any substantial difference in temperature from any other element along the array and, 2) any change in temperature will be slight and gradual.
  • Heat buffering means 4 integrates temperature fluctuations and evenly distributes just-below-room temperature coolness of the TE as required. With the thermistor 18 being employed, it can respond to minute changes in temperature. Additionally, the operating temperature of the TE, e.g. 70 ⁇ F, makes it unlikely that condensate or "dew" will form on imaging window 13 of the CCD. Thus, the substantially constant temperature during imaging of the CCD yields a substantially constant source of dark current noise which can be adequately compensated for through use of measured offset values during calibration.

Abstract

A thermal buffer (4) is introduced between a thermoelectric cooler (10) and a CCD array (3) in order to provide for uniform temperature distribution throughout the CCD array (3) to stabilize dark current.

Description

TEMPERATURE STABILIZATION BUFFER FOR A SOLID STATE ELECTRONIC COMPONENT
BACKGRonwn OF THK TW πw TON
1. Field of Invention
This invention relates to a solid-state device, such as a CCD, where the operating temperature is kept substantially constant to stabilize dark current noise.
2. Description of the Prior Art
When utilizing a solid-state imager to read an image scan, one of the main sources of noise that affects image quality is dark current. In a CCD array, dark current is the amount of ambient current detectable in individual imaging elements when the CCD is energized in the absence of the imaging beam. Typically to minimize the effects of this noise, the dark current in each element of the CCD array is measured prior to a scan and stored as an offset value for later correction of image readings. Technologists working with solid- state imagers wish that the problem of dark current noise were resolved so easily, unfortunately it is not.
In the process of scanning an imaging beam across a CCD array, the temperature of the array rises. Dark current noise is known to double for every 10°C or so increase in temperature. An increase in the dark current noise renders offset values determined prior to the scan insufficient to compensate for a growing adverse effect upon image signal resolution. Various attempts have been made to address the temperature- induced rise in dark current. In U.S. patent 4,551,760, the inventor describes a method of cooling the CCD array to about +10°C to reduce dark current noise. He uses a thermoelectric cooler bonded to the rear surface of the CCD to maintain this low temperature and control the level of dark current attributable noise. However, while the dark current was reduced by the method, he found that condensate was apt to form on the glass face of the CCD interfering with an accurate reading of the image data. In order to avoid the condensate problem, others, who have cooled the CCD even lower, have sought to enclose the "cooled" CCD in a vacuum tight arrangement to minimize the possibility of humidity-induced condensate forming on its viewing surface. These solutions are both difficult and expensive to implement.
The present invention does not require significant cooling of the CCD. As it operates at near room temperature, it is much less susceptible to humidity problems. Consequently, it does not require the energy and expense of evacuating an enclosure and filling it with dry gas to keep the CCD cooled significantly below its operating environment,- The present invention is a relatively inexpensive and easily-implement ble solution to a well known problem of resolving the floating dark current problem for solid state devices.
SUMMARY OF THE INVENTION
This invention is based on two fundamental principles. First, it is often important that the temperature of a solid state electronic component, such as a CCD array, remain substantially constant during use. The dark current problem is largely related to the fact that the offset calibration values change while the CCD is in use. The apparatus of Applicant's invention successfully fixes the operating temperature of the CCD array to just below room temperature so that the offset values remain a substantially accurate representation throughout image scanning and may be used to adjust the actual data. This approach has been successfully employed by Applicant in an industrial non-destructive testing radiographic system comprising scanner means, interactive display means, and storage and retrieval means.
Secondly, since this invention does not require cooling of the CCD to very low temperatures, it alleviates the time-consuming, costly and difficult measures that were heretofore undertaken to enclose and "refrigerate" the CCD. This invention provides" good image signal resolution at near ambient air temperatures.
In an image detecting system comprising a CCD array and a cooling element used to control the temperature of said CCD array, wherein the improvement comprises: a temperature buffering means interposed in thermal contact between said CCD
Figure imgf000005_0001
and said cooling element.
DESCRIPTION OF THE DRAWING
Figure 1 represents a prior art approach to cooling of a CCD array.
Figure 2 shows the invention.
Figure 3 is a schematic representation of circuitry employing the invention.
DETAILED DESCRIPTION OF THE INVENTION
In Figure 2, a heat transfer means 20 is thermally connected to the rear face of solid-state CCD imager 3, that is, opposite the face where the imaging beam is received. Heat transfer means 20 is utilized to provide a substantially uniform temperature exchange from the rear face of the CCD 3 to heat buffering means 4. To be most effective, the heat transfer means 20, such as a thermal pad or thermally conductive glue, should remain in thermal contact with both heat buffering means 4 and
CCD 3.
Heat buffering means 4 is comprised of a relatively highly thermally conductive material, such as aluminum or copper. It extends along the full length of CCD 3 and acts to integrate small temperature fluctuations along the CCD. A thermally conductive mounting plate 5 is centered and fixed orthogonal to heat buffering means 4. Thermistor 18 may be placed longitudinally into a grooved out section of mounting plate 5 such that the thermistor thermal contacts both heat buffering means 4 and mounting plate 5. Upon sensing a change in temperature of the heat buffering means, the thermistor's output, which is continuously compared with a reference temperature voltage, triggers the application of sufficient current to cooling element 10 to maintain the reference temperature. This feedback control is accomplished using standard servo amplifier and power control techniques which are well known in the art. See Figure 3.
Cooling element 10 is attached by means of a thermally conductive medium to mounting plate 5 on the side opposite heat buffering means 4. Cooling element 10 might typically be a thermoelectric cooler with the "cool" side fixed to mounting plate 5. The "hot" side of 10 is attached to heat sink 6 to vent away heat during temperature cooling and maintenance. The prior art response to the variable dark current problem can be found in figure 1. The emphasis is upon cooling the CCD array substantially below room temperature to about 10°C. A further definition of the dark current noise problem reveals that acceptable resolution of most signals can be obtained at about room temperature if that temperature can be sustained during imaging of the light source on the CCD. Unless the image signals are very small (e.g. astronomy signals), the key to relative freedom from temperature-dependent dark noise is to maintain a constant temperature so that the offset dark current values, established in the absence of light, will remain useful for making corrections to image data values.
The prior art solution (Fig. 1) bonds the thermoelectric cooling device (312, 314, and 316) directly to non-imaging side of the CCD (220) . This solution may not be satisfactory in that the size of the cooling device may be smaller than the active area of the CCD array thus permitting uneven cooling. Further, the thermoelectric cooler (TE) itself is not a perfect device and due to manufacturing differences in its internal metallic junctions, there may be differences in temperature across its surface. Also, as heat from the
"hot" side of the TE (312) is conducted to cap (214) and conducted away by thermally conductive braid 216, some heat can be transferred to flaps 212 which are bonded to the CCD (210) . All of these sources provide an uneven distribution of temperatures across the CCD array and hence change the dark current noise from values measured during offset calibration.
The instant invention avoids the problem of improper sizing of TE 10 to the CCD by extending heat transfer means and heat buffering means over the full length of the CCD. The heat buffering means smooths out changes in temperature so that: 1) no one element in the CCD array will experience any substantial difference in temperature from any other element along the array and, 2) any change in temperature will be slight and gradual. Heat buffering means 4 integrates temperature fluctuations and evenly distributes just-below-room temperature coolness of the TE as required. With the thermistor 18 being employed, it can respond to minute changes in temperature. Additionally, the operating temperature of the TE, e.g. 70βF, makes it unlikely that condensate or "dew" will form on imaging window 13 of the CCD. Thus, the substantially constant temperature during imaging of the CCD yields a substantially constant source of dark current noise which can be adequately compensated for through use of measured offset values during calibration.
It is understood that the specific components utilized above are for example purposes only for teaching the invention and are not intended to limit the invention. All suitable equivalents should be contemplated as being within the scope of the appended claims.

Claims

What is claimed is:
1. In a cooling system for controlling the level of dark current in a solid state electronic component, including a thermoelectric cooler and a temperature feedback control system, the improvement comprising:
a temperature buffering means, interposed between and in thermal contact with said solid state electronic component and said thermoelectric cooler, for maintaining a substantially uniform temperature throughout said solid state electronic component.
2. The apparatus recited in claim 1, wherein;said temperature buffering means comprises a block of relatively highly thermally conductive material.
3. The apparatus recited in claim 2, wherein said buffering means is made of aluminum.
4. The apparatus recited in claim 2, wherein said buffering means is made of copper.
5. The apparatus recited in claim 1, wherein said solid state component comprises a CCD array.
6. In an image detecting system, comprising a CCD array and a cooling element used to control the temperature of said CCD array, the improvement comprising a temperature buffering means, interposed in thermal contact between said CCD array and said cooling element, for maintaining a substantially uniform temperature throughout the said CCD array.
7. In an industrial non-destructive testing reading and storage radiographic system comprising, in combination, scanner means, interactive display means, and storage and retrieval means, the improvement comprising:
said scanner means including a CCD array thermally coupled to a temperature buffer means interposed between said CCD array and a cooling means.
PCT/US1991/007043 1990-10-05 1991-10-01 Temperature stabilization buffer for a solid state electronic component WO1992006561A1 (en)

Applications Claiming Priority (2)

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US59318390A 1990-10-05 1990-10-05
US593,183 1990-10-05

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Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1994000950A1 (en) * 1992-06-19 1994-01-06 Honeywell Inc. Infrared camera with thermoelectric temperature stabilization
WO1997022860A1 (en) * 1995-12-19 1997-06-26 Lockheed-Martin Ir Imaging Systems Method and apparatus for thermal gradient stabilization of microbolometer focal plane arrays
US6249002B1 (en) 1996-08-30 2001-06-19 Lockheed-Martin Ir Imaging Systems, Inc. Bolometric focal plane array
US6515285B1 (en) 1995-10-24 2003-02-04 Lockheed-Martin Ir Imaging Systems, Inc. Method and apparatus for compensating a radiation sensor for ambient temperature variations
US6730909B2 (en) 2000-05-01 2004-05-04 Bae Systems, Inc. Methods and apparatus for compensating a radiation sensor for temperature variations of the sensor
US6791610B1 (en) 1996-10-24 2004-09-14 Lockheed Martin Ir Imaging Systems, Inc. Uncooled focal plane array sensor
US7030378B2 (en) 2003-08-05 2006-04-18 Bae Systems Information And Electronic Systems Integration, Inc. Real-time radiation sensor calibration
US8028531B2 (en) 2004-03-01 2011-10-04 GlobalFoundries, Inc. Mitigating heat in an integrated circuit
US20220240414A1 (en) * 2021-01-27 2022-07-28 Panasonic Intellectual Property Management Co., Ltd. Imaging device

Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4496982A (en) * 1982-05-27 1985-01-29 Rca Corporation Compensation against field shading in video from field-transfer CCD imagers
US4525743A (en) * 1984-03-28 1985-06-25 Rca Corporation Dark current measurement and control for cameras having field-transfer CCD imagers
US4551762A (en) * 1984-01-18 1985-11-05 Rca Corporation Dark-current level regulation in solid-state devices
US4551760A (en) * 1983-09-16 1985-11-05 Rca Corporation Television camera with solid-state imagers cooled by a thermal servo
US4562473A (en) * 1984-10-10 1985-12-31 Rca Corporation Dark current sensing with a solid-state imager having a CCD line register output
US4580168A (en) * 1982-05-27 1986-04-01 Rca Corporation Charge-storage-well dark current accumulator with CCD circuitry
US4587563A (en) * 1984-09-28 1986-05-06 Rca Corporation Cooler control for a solid-state imager camera
US4739382A (en) * 1985-05-31 1988-04-19 Tektronix, Inc. Package for a charge-coupled device with temperature dependent cooling

Patent Citations (8)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4496982A (en) * 1982-05-27 1985-01-29 Rca Corporation Compensation against field shading in video from field-transfer CCD imagers
US4580168A (en) * 1982-05-27 1986-04-01 Rca Corporation Charge-storage-well dark current accumulator with CCD circuitry
US4551760A (en) * 1983-09-16 1985-11-05 Rca Corporation Television camera with solid-state imagers cooled by a thermal servo
US4551762A (en) * 1984-01-18 1985-11-05 Rca Corporation Dark-current level regulation in solid-state devices
US4525743A (en) * 1984-03-28 1985-06-25 Rca Corporation Dark current measurement and control for cameras having field-transfer CCD imagers
US4587563A (en) * 1984-09-28 1986-05-06 Rca Corporation Cooler control for a solid-state imager camera
US4562473A (en) * 1984-10-10 1985-12-31 Rca Corporation Dark current sensing with a solid-state imager having a CCD line register output
US4739382A (en) * 1985-05-31 1988-04-19 Tektronix, Inc. Package for a charge-coupled device with temperature dependent cooling

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO1994000950A1 (en) * 1992-06-19 1994-01-06 Honeywell Inc. Infrared camera with thermoelectric temperature stabilization
US6515285B1 (en) 1995-10-24 2003-02-04 Lockheed-Martin Ir Imaging Systems, Inc. Method and apparatus for compensating a radiation sensor for ambient temperature variations
WO1997022860A1 (en) * 1995-12-19 1997-06-26 Lockheed-Martin Ir Imaging Systems Method and apparatus for thermal gradient stabilization of microbolometer focal plane arrays
US5763885A (en) * 1995-12-19 1998-06-09 Loral Infrared & Imaging Systems, Inc. Method and apparatus for thermal gradient stabilization of microbolometer focal plane arrays
US6249002B1 (en) 1996-08-30 2001-06-19 Lockheed-Martin Ir Imaging Systems, Inc. Bolometric focal plane array
US6791610B1 (en) 1996-10-24 2004-09-14 Lockheed Martin Ir Imaging Systems, Inc. Uncooled focal plane array sensor
US6730909B2 (en) 2000-05-01 2004-05-04 Bae Systems, Inc. Methods and apparatus for compensating a radiation sensor for temperature variations of the sensor
US7030378B2 (en) 2003-08-05 2006-04-18 Bae Systems Information And Electronic Systems Integration, Inc. Real-time radiation sensor calibration
US8028531B2 (en) 2004-03-01 2011-10-04 GlobalFoundries, Inc. Mitigating heat in an integrated circuit
US20220240414A1 (en) * 2021-01-27 2022-07-28 Panasonic Intellectual Property Management Co., Ltd. Imaging device
US11936966B2 (en) * 2021-01-27 2024-03-19 Panasonic Intellectual Property Management Co., Ltd. Imaging device with cooling mechanism

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