The present invention relates generally to detectors for gamma-ray and X-ray detection devices.
Anisotropic conductive films (ACFs) (also referred to as anisotropic conductive adhesives (ACAs)) consist of mixtures of conductive fillers in an insulating polymer. ACFs are capable of electrically conducting in one direction (the film thickness or Z axis) and insulating in other two directions (x and y axis). ACF has become important interconnect technology for devices which are not significantly sensitive to high pressure and high temperature, such as silicon devices or substrates used in advanced display assembly, contactless smart-card module assembly, and bare chip attach on rigid and flexible substrates.
In one embodiment, a device comprises: (a) a radiation detector comprising a semiconductor substrate having opposing front and rear surfaces, a cathode electrode located on the front surface of said semiconductor substrate, and a plurality of anode electrodes on the rear surface of said semiconductor substrate, (b) a printed circuit board, and (c) an electrically conductive polymeric film disposed between the printed circuit board and the anode electrodes, wherein the polymeric film comprises electrically conductive wires electrically connecting the radiation detector with the printed circuit board.
In another embodiment, a method of electrically connecting a radiation detector to a printed circuit board comprises (a) providing a radiation detector comprising a semiconductor substrate having opposing front and rear surfaces, a cathode electrode located on the front surface of said semiconductor substrate, and a plurality of anode electrodes on the rear surface of said semiconductor substrate, (b) providing a printed circuit board, (c) providing an electrically conductive polymeric film between the printed circuit board and the plurality of anodes, and (d) bonding the radiation detector to the printed circuit board using at least one of a bonding temperature of 135° C. or less and a compressive force of about 35 psi or less.
The following definitions are used herein:
Cathode electrode: the electrode on one major surface of the detector substrate where incident gamma rays or x-rays enter the detector, i.e. positioned towards the radiation source.
Anode electrodes: segmented electrode contacts located on the rear surface of the substrate, i.e. positioned away from the radiation source.
Interpixel or inter pixel: the region or gap separating pixel electrodes. For electrode configurations with non-pixellated discrete contact segments the term is equivalently applied to the gap between contact segments.
Radiation Detector Design
Radiation detectors can be configured in a variety of ways. A common configuration comprises a cathode electrode and a plurality of anode electrodes located on opposite sides of a semiconductor plate or substrate. Typically these radiation detectors have pixilated anode electrode arrays fabricated by various deposition and lithography processes resulting in a gap between pixels, termed the interpixel gap or interpixel region.
In the preferred embodiments, the radiation detectors comprise a semiconductor material, such as a semiconductor material preferably comprising CdZnTe (CZT) or CdTe. Although other types of semiconductor materials exemplified by lead iodide, thallium bromide, gallium arsenide or silicon may be used.
More preferred is Cd(1-x)ZnxTe (where x is less than or equal to 0.5), a wide band gap ternary II-VI compound semiconductor with unique electronic properties. This type of semiconductor is useful in gamma-ray and X-ray detectors which are used as spectrometers that operate at room temperature for nuclear radiation detection, spectroscopy and medical imaging applications.
Illustrated in
Thus,
The direct lithography fabrication process is described with reference to
In step 1, shown in
In an optional step 2 shown in
In step 3, as shown in
The resist coating is hardened in step 4 by baking for 10 minutes at 90° C. This step is done to drive excess solvent out of the resist. The tile is now prepared for lithography exposure.
In step 5, as shown in
In step 6 shown in
In step 7 the remaining resist pixel pattern 314 is baked for 20 minutes at 90° C. This step is done to harden the resist further.
In step 8, shown in
In step 9 shown in
The overall combination of depositing the metal layer over the entire substrate surface at once, direct photolithography and the etching process results in the improved device interpixel resistance and performance.
In step 10 shown in
Cathode Housing (Optional)
Optionally, an electrically conductive housing may be attached to the detector cathode by (a) providing a radiation detector comprising a semiconductor substrate having opposing front and rear surfaces, a cathode electrode located on the front surface of said semiconductor substrate and a plurality of anode electrodes on the rear surface of said semiconductor substrate, (b) providing a separately formed electrically conductive housing, and (c) attaching the housing to the cathode electrode such that the housing and the cathode electrode are in electrical contact.
A non-limiting example of a housing is depicted in
As shown in
The electrically conductive housing 425 shields the detector from background electromagnetic fields (or magnetic fields). Additionally, device electric fields are focused using this housing. The housing is also preferably transparent to X-ray or gamma-ray radiation. Further, the housing preferably exhibits little or no oxidation in ambient air, such as under normal operating conditions of the detector. As such, the housing is most preferably a thin structure and comprises a material transparent to radiation, substantially impervious to background electromagnetic fields and exhibits little or no oxidation at ambient conditions.
For example the housing may be between about 50 microns and 100 microns thick. In some cases a metal foil is sufficient as a housing.
Based on the parameters set forth above, one skilled in the art may chose from a host of materials for constructing the housing. In general, metals and metallic alloys are preferred. Any suitable metal which does not substantially oxidize in air may be used. A non-limiting example of suitable metallic alloys includes stainless steel, brass (such Ni/Ti coated brass), NiCo alloys, NiFe alloys, NiFeCo alloys, NiFeMo alloys or NiFeCuMo alloys. A class of metal alloys termed “Mu-metals” is most preferred. Mu-metals are a type of NiFe alloy, particularly effective at screening static or low frequency magnetic fields. In some cases, the aforementioned alloys may be doped with other alloying elements, mechanically pre-treated (e.g. cold worked, hot worked etc.), chemically surface-treated (e.g. surface coating for corrosion resistance) or any combination thereof.
In some cases, the housing 425 is shaped to conform to geometry of the detector, more specifically, to geometry of the cathode, to which it is secured. Therefore, one skilled in the art may contemplate various curved or angular housing shapes given the shape of the detector. In a non-limiting example, the housing is a rectangular or circular-cross-sectioned (e.g. cylinder) shape.
When the housing is constructed to extend over (partially or completely) at least one side of the substrate, said at least one side is spaced from said housing. This gap is either empty or filled with an insulating material.
The housing 425 is attached to the cathode electrode 200 such that an electrical conduction path exists between the two. In a preferred case, the housing and the cathode are attached via an electrically conductive material. Most preferably, an electrically conducive polymeric material, such as a conductive epoxy applied to the inner face or surface of the housing is used.
Edge coatings 420 suitable for certain embodiments of the present application are described in U.S. application Ser. No. 11/642,819, filed on Dec. 21, 2006 which is hereby incorporated by reference in its entirely.
Detector-PCB Attachment
As described in U.S. application Ser. No. 11/642,819, the radiation detector may be connected to a readout printed circuit board (PCB), to process data obtained by the detector.
The present embodiments describe a detector device comprising a radiation detector attached to a device component such as a PCB, through an electrically conductive polymeric film. In one aspect, the electrically conductive polymeric film comprises electrically conductive wires (e.g., nanowires or metallic fibers), which are substantially aligned in the z-axis (film thickness axis) and traverse the thickness of film. In a further aspect, the electrically conductive film is an anisotropic conductive film (ACF).
In a further embodiment, a detector device comprises a CZT detector attached to a PCB through an ACF, wherein at least one bonding edge of the ACF is coated with an edge coating.
Anisotropic conductive films (ACFs) refer to a type of electrically conductive polymeric films having a polymeric matrix embedded with electrically conductive fillers. Also, an ACF conducts electricity in one direction (e.g. z-axis or film thickness) and insulates in another direction (e.g. x-y plane).
Though a number of ACFs exist in the market, to date, most are not suitable for bonding a radiation detector to a PCB. One reason, among others, is that typical application of an ACF involves compressing an ACF between two surfaces to be bonded, followed by curing. Thus, materials sensitive to high pressures and/or temperatures can not be bonded using this type of film. For example, a common type of ACF has a polymeric matrix with conductive spheres randomly distributed therein. The conductive spheres may be metal spheres (e.g. gold, silver, nickels or tin/lead mixtures) or metal coated polymer spheres. Forming a good electrical bond with this type of ACF requires large compressive forces, sometimes approaching a few hundred psi. Additionally, curing involves high temperatures, as about 150° C. or higher. Such conditions are not suitable for a CdZnTe (CZT) detector which is very sensitive to high temperatures and compressive forces.
The present inventors have found that a new type of electrically conductive film can be used to bond a detector which cannot withstand high temperatures and pressures, such as a CZT radiation detector to a PCB. This film comprises electrically conductive wires which are substantially aligned in the z-axis and traverse the thickness of film. Preferably, the wires are metallic nanowires (having a diameter of 1 micron or less) or other fibers. Also preferably, the metal nanowires have small pitch, such as less than 20 microns, for example 10-15 microns, such as 11-13 microns, which facilitates attachment of the film to small anode pixels.
In one embodiment, the density of the metallic nanowires is sufficient to conduct current between a detector anode and a PCB. In another embodiment, the density of the conductive nanowires is as high as practical without interfering with the adhesive properties of the film. In a non-limiting example, the nanowire density is up to 20 million per square inch of film. In the preferred embodiments, this film is an ACF conducting electricity across the thickness (z-axis) of the film and insulating in the plane of the film (x-y plane).
The composition of the metallic nanowires may vary so long as they remain electrically conductive. In a non-limiting example, the nanowires comprise NiO-coated Ni wires which may be slightly tilted off the z-axis depending on the polymer matrix.
The polymer matrix of the ACF preferably comprises an epoxy or a thermoplastic polymer. A favorable aspect of this ACF is that the compressive forces needed for bonding are generally at least ten times less than that for the aforementioned ACFs with conductive spheres and the ACF can be cured at a lower temperature, such as about 135° C. or less.
As mentioned, CZT detectors are sensitive to thermal and compressive loads. In order to assess device performance, the leakage current of a CZT detector device is measured under elevated temperatures and compressive forces. The test CZT detector device comprises a PCB connected to a CZT detector through a conductive plastic film used to mimic an ACF. The results are shown in the leakage current versus applied bias voltage plots in
According to an embodiment, one suitable bonding or attachment procedure involves bonding a PCB to a cleaned CZT detector by providing an ACF between the PCB and the detector anodes, and applying a compressive force of about 35 psi or less at an elevated temperature of about 135° C. or less. In a non-limiting example, the pressure is in the range of about 25 to about 35 psi. In another non-limiting example, the elevated temperature is in the range of about 90° C. to about 135° C., more preferably between 125° C. and 130° C. The duration of the elevated temperature, applied compressive force or both, is typically between five minutes and two hours including all values in this range. In some cases the temperature or applied compressive load may be applied for less than five minutes or more than two hours. A housing jig may used for alignment during the bonding step.
If desired, after the bonded device is cooled down and the compressive load is removed, an optional second anneal at a temperature between about 90° C. to about 135° C., such as between 125° C. and 130° C. may be carried out. If a thermally curable edge coating 420 is used, then the edge coating may be applied after the compressive load is removed but prior to the second anneal such that the edge coating is cured during the second anneal. If a UV curable edge coating 420 is used, then a UV radiation curing step is used.
The long term reliability of a CZT detector device is another concern when using ACF for attachment. Experiments on accelerated life test (ALT) of ACF attached samples show that device performance is stable under long term thermal cycling at high and low temperatures. However, performance can degrade under 2 hour or 24 hour hash tests at 85° C. and 85% relative humidity. One possible explanation for this effect is that moisture absorption into the ACF is responsible for the degradation. In support of this explanation, vacuum pumping experiments show that the absorbed moisture could be pumped away under the vacuum resulting in improved sample performance.
A method of reducing or preventing moisture absorption into the ACF, involves coating the bonding line of the ACF (ACF/PCB and ACF/detector interface lines) with a moisture resistant edge coating, as shown in
Based on the coating materials tested, a preferred ACF edge coating material is UV cure epoxy, since it provides the desired combination of FWHM response and leakage current. One reason for the performance of the solder mask and silicone edge coatings may be due to the weakened ACF during the relatively high temperature curing of these materials. Therefore, room temperature curing is an advantage of the UV curable epoxy. Other compatible low temperature coating materials, such as acrylic resins, are viable candidates as edge coating materials.
Although the foregoing refers to particular preferred embodiments, it will be understood that the present invention is not so limited. It will occur to those of ordinary skill in the art that various modifications may be made to the disclosed embodiments and that such modifications are intended to be within the scope of the present invention. All of the publications, patent applications and patents cited herein are incorporated herein by reference in their entirety.
| Number | Name | Date | Kind |
|---|---|---|---|
| 4479131 | Rogers et al. | Oct 1984 | A |
| 5616928 | Russell et al. | Apr 1997 | A |
| 6002134 | Lingren | Dec 1999 | A |
| 6027766 | Greenberg et al. | Feb 2000 | A |
| 6037595 | Lingren | Mar 2000 | A |
| 6046454 | Lingren et al. | Apr 2000 | A |
| 6243441 | Zur | Jun 2001 | B1 |
| 6262408 | Izumi et al. | Jul 2001 | B1 |
| 6291763 | Nakamura | Sep 2001 | B1 |
| 6310281 | Wendt et al. | Oct 2001 | B1 |
| 6340812 | Izumi et al. | Jan 2002 | B1 |
| 6340818 | Izumi et al. | Jan 2002 | B1 |
| 6342700 | Izumi et al. | Jan 2002 | B1 |
| 6344370 | Izumi et al. | Feb 2002 | B1 |
| 6350946 | Miyake et al. | Feb 2002 | B1 |
| 6372538 | Wendt et al. | Apr 2002 | B1 |
| 6392217 | Teranuma et al. | May 2002 | B1 |
| 6398624 | Izumi et al. | Jun 2002 | B1 |
| 6413581 | Greenberg et al. | Jul 2002 | B1 |
| 6512233 | Sato et al. | Jan 2003 | B1 |
| 6593577 | Izumi | Jul 2003 | B2 |
| 6722159 | Greenberg et al. | Apr 2004 | B2 |
| 6803109 | Qiu et al. | Oct 2004 | B2 |
| 6825473 | Watanabe | Nov 2004 | B2 |
| 6909100 | Sognefest et al. | Jun 2005 | B2 |
| 6949749 | Tokuda et al. | Sep 2005 | B2 |
| 6978534 | Sakaki | Dec 2005 | B2 |
| 6981758 | Cruz-Uribe et al. | Jan 2006 | B2 |
| 6995840 | Hagler | Feb 2006 | B2 |
| 6999165 | Hagler | Feb 2006 | B2 |
| 7004376 | Ashida | Feb 2006 | B2 |
| 7030169 | Kalgutkar et al. | Apr 2006 | B2 |
| 7049002 | Greenberg et al. | May 2006 | B2 |
| 7064152 | Kalgutkar et al. | Jun 2006 | B2 |
| 7117588 | Vafi et al. | Oct 2006 | B2 |
| 7125101 | Cruz-Uribe et al. | Oct 2006 | B2 |
| 7128428 | Takahashi et al. | Oct 2006 | B2 |
| 7169209 | Nakata et al. | Jan 2007 | B2 |
| 7170062 | Vuorela | Jan 2007 | B2 |
| 7189971 | Spartiotis et al. | Mar 2007 | B2 |
| 7194197 | Wendt et al. | Mar 2007 | B1 |
| 7235736 | Buller et al. | Jun 2007 | B1 |
| 7239164 | Tamaki | Jul 2007 | B2 |
| 7267850 | Coggio et al. | Sep 2007 | B2 |
| 7301155 | Tokuda et al. | Nov 2007 | B2 |
| 7348599 | Yamazaki et al. | Mar 2008 | B2 |
| 7491572 | Kim et al. | Feb 2009 | B2 |
| 20020014593 | Tokuda et al. | Feb 2002 | A1 |
| 20020074503 | Watanabe | Jun 2002 | A1 |
| 20020134943 | Izumi | Sep 2002 | A1 |
| 20030215056 | Vuorela | Nov 2003 | A1 |
| 20070075408 | Shibayama et al. | Apr 2007 | A1 |
| 20070085180 | Kim et al. | Apr 2007 | A1 |
| Number | Date | Country |
|---|---|---|
| 2001-0069358 | Jul 2001 | KR |
| 10-0539082 | Dec 2005 | KR |
| WO 2004097938 | Nov 2004 | WO |
| Number | Date | Country | |
|---|---|---|---|
| 20090321651 A1 | Dec 2009 | US |