This invention relates generally to Geiger-mode (Gm) avalanche photodiode (APD) focal plane arrays (FPAs) and, more particularly, to architectures and methods for increasing the optical overstress tolerance thereof.
There is a potential for saturation or loss of functionality in GmAPD FPAs due to incoming high-intensity optical signals. These high-intensity signals can generate, in the GmAPD, excessively large currents, which are then injected into the read-out integrated circuit (ROIC). These large currents may result in corruption of data from the FPA or possibly result in damage to the sensor. It is desirable to avoid these effects, collectively referred to as “optical overstress,” through elements of the FPA design.
The circuit model of the GmAPD 102 includes intrinsic instantaneous series resistance “RS(t),” breakdown voltage “VB,” diode capacitance “CD,” and switch “S” to emulate the spontaneous avalanche breakdown process in the GmAPD. See, Haitz, R. H. “Model for the Electrical Behavior of a Microplasma” J. Appl. Phys. 35, 1370 (1964). ROIC unit cell 108 includes arm transistor 110, disarm transistor 112, and sense transistor 114.
GmAPD 102 is armed by externally applied voltage “VHI,” with accompanying low-impedance load resistance RL. Voltage VHI is set as follows:
Referring now to
When sense transistor 114 in ROIC unit cell 108 detects that the voltage has dropped to quench voltage VQ, disarm transistor 112 turns “on,” reducing the voltage across GmAPD 102 to VLO, as depicted in
As the voltage is reduced below breakdown voltage VB, switch S opens again and the current drops from steady-state value I0 back to zero, as depicted in
The initial spike in current/to IA scales with optical intensity in the presence of a very large optical signal due to Rs(t) decreasing when an excess of free carriers are generated within the diode. High magnitudes of this peak current ultimately cause the issues attributed to “optical overstress” upon injection into ROIC unit cell 108. As this problem is relatively unique to GmAPD FPAs due to the high impedance necessary at the ROIC input for detection of avalanche events, to the inventors' knowledge, it has not been addressed in the prior art.
Embodiments of the invention provide a way to significantly increase the tolerance of a GmAPD FPA to optical overstress.
A first approach adopted by the present inventors to address the problem of high peak current was to shut down the power supply lines in the ROIC when high current is detected. This approach proved to be ineffective, however, due to the essentially instantaneous overstress impact of the current pulse (i.e. <<10 nanoseconds). The inventors then considered a second approach wherein the magnitude of the current is reduced before the current is injected into ROIC unit cell 108.
In accordance with the illustrative embodiment, one or more limit resistor(s) are monolithically integrated within each pixel of the GmAPD FPA. The inventors recognized that, based on certain considerations related to the architecture of their GmAPD arrays, the limit resistor(s) must be monolithically integrated. In some of such embodiments, the limit resistor(s) are integrated into the GmAPD of each pixel. In some other of such embodiments, the limit resistor(s) are integrated into the ROIC unit cell of each pixel. In some further embodiments, limit resistor(s) are integrated into both the GmAPD and the ROIC unit cell of each pixel.
As a consequence of the presence of the limit resistor(s) in accordance with the present teachings, when the switch S closes at time to, the voltage V drops more slowly than in the prior art (as depicted in
Some embodiments of the invention provide a GmAPD FPA comprising a plurality of pixels, each pixel comprising: an electrical circuit including a GmAPD, a unit cell of a ROIC, and a limit resistor, wherein the limit resistor is monolithically integrated in the pixel, and wherein the limit resistor limits a magnitude of a current entering the ROIC unit cell, wherein the current is generated by the GmAPD.
Some embodiments of the invention provide a GmAPD FPA comprising a plurality of pixels, each pixel comprising: a GmAPD having a limit resistor monolithically integrated therein, the limit resistor operable to limit a magnitude of a current generated by the GmAPD, and a unit cell of a ROIC that receives the current, as limited by the limit resistor, from the GmAPD.
Some embodiments of the invention provide a method for increasing the tolerance of a GmAPD FPA to optical overstress, the method comprising increasing, within each pixel of the GmAPD FPA, the series resistance of an electrical connection between the GmAPD and a unit cell of a ROIC.
Embodiments of the invention provide a GmAPD FPA having increased tolerance optical overstress. For the sake of clarity, the embodiments of the invention are depicted and described at the pixel level. Each GmAPD FPA pixel includes a GmAPD pixel and a unit cell of an ROIC. There is a 1:1 relationship between GmAPDs and unit cells of the ROIC. Each unit cell of the ROIC provides a digital readout of the avalanche events that occur within the associated GmAPD. It is within the capabilities of those skilled in the art to appropriately scale to the level of a GmAPD FPA.
In some embodiments in which limit resistor 316A is monolithically integrated in GmAPD 302, the limit resistor is a thin-film resistor that is patterned on the GmAPD from, for example, standard-production, high-resistivity NiCr and TaN thin films.
Thus, in both embodiments depicted, the limit resistor is: (a) located in the circuit between the GmAPD and the ROIC unit cell, and (b) monolithically integrated into the GmAPD FPA pixel.
With reference to
Because sense transistor 114 in the ROIC unit cell is a voltage threshold detector, the smaller current amplitudes generated in embodiments of the invention will not degrade the circuit's ability to detect avalanches. The primary performance trade-off to be considered is avoiding degradation of the FPA timing jitter performance associated with an increase in avalanche RC time constants induced by the presence of limit resistor 316A or 316B. This places an upper limit on useful values of the limit resistor of about 100 kOhms. The lower limit of resistance of the limit resistor, which is about 1 kOhm, is determined by the minimum value that reduces the peak current to an acceptable value.
Since the existing series resistance between the GmAPD anode and the ROIC input in an APD FPA is dominated by the contact resistance of the APD anode contact, which is about 100 ohms, the aforementioned resistance range of the limit resistor (i.e., about 1 kOhm to about 100 kOhms) is expected to yield, at minimum, a factor-of-ten improvement in optical-overload tolerance. At the same time, keeping the resistance in the aforementioned range will, as previously noted, avoid unacceptable levels of degradation in timing jitter performance.
As previously noted, in embodiments of the invention, the limit resistor is monolithically integrated into the GmAPD FPA pixel. A process for monolithically integrating the limit resistor into a GmAPD, such as to form GmAPD 301 (
The fabrication operations germane to embodiments of the invention take place after epitaxial growth of the various layers (e.g., absorption layer, charge control layer, cap layer, etc.) composing an APD (hereinafter referred to in the disclosure and claims as the “APD device layers”), but before diffusing a dopant into the cap layer to form the active region of the APD. Conventional techniques are used for metal deposition, insulator deposition, patterning, etc.
Referring now to
In operation S503, an n- or p-contact metal (dependent on device type) is deposited on a portion of the active region. As needed, additional “passivation” material is deposited to fill what remains of the opening formed in the passivation layer.
In operation S504, a layer of metal, such as, without limitation, high resistivity NiCr or TaN, is deposited between the contact (i.e., contact 628) and a region in which a bond pad will be deposited. This layer of metal can be deposited, for example, via electron beam evaporation, or sputtering, and be patterned into a desired configuration using techniques known in the art. This layer of metal serves as the limit resistor.
In operation S505, additional metal is deposited in a location at which a bond pad is desired. This metal will partially (or wholly) overlap the metal serving as the limit resistor. The bond pad comprises, for example and without limitation, gold, aluminum, copper, and alloys thereof.
In operation S506, a layer of electrical insulation is deposited over the APD. Materials suitable for use as the layer of electrical insulation include, for example and without limitation, BCB, SiO2, SiNx, and Al2O3. An opening is then formed around the bond pad to enable electrical contact between the GmAPD and the ROIC.
Monolithically integrating a limit resistor into an ROIC will necessarily proceed along a somewhat different path as a consequence of the structural differences between a GmAPD and a ROIC. In light of the present teachings, those skilled in the art will be able to adapt ROIC fabrication procedures to incorporate a limit resistor.
It is to be understood that the disclosure teaches just one example of the illustrative embodiment and that many variations of the invention can easily be devised by those skilled in the art after reading this disclosure and that the scope of the present invention is to be determined by the following claims.
This application is a continuation of U.S. application Ser. No. 17/581,464, filed Jan. 21, 2022, which is a continuation of U.S. application Ser. No. 16/002,816, filed Jun. 7, 2018, which claims the benefit of U.S. Provisional Application No. 62/516,453, filed Jun. 7, 2017, the contents of all of which are hereby incorporated by reference in their entireties.
Number | Date | Country | |
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62516453 | Jun 2017 | US |
Number | Date | Country | |
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Parent | 17581464 | Jan 2022 | US |
Child | 18830316 | US | |
Parent | 16002816 | Jun 2018 | US |
Child | 17581464 | US |