The present invention relates generally to photodetectors, and more particularly to photodetectors for communication systems.
As semiconductor integrated circuits become more complex and run at higher speeds, there is increasing desire for efficient information flow between different parts of an IC, or even between a number of chips (or chiplets). This can be as simple as clock distribution, or more complex data transfer between processor and memory, or different logic blocks exchanging data.
Signaling within an IC or between ICs is almost always done electrically through the numerous metal levels formed lithographically above the IC (redistribution layers (RDLs) and back end of line (BEOL) layers), wiring in the package, the use of an interposer or bridge (typically fabricated from silicon or an organic laminate) inserted between the ICs and the package, the use of a printed circuit board to which multiple packaged ICs are attached, or the use of electrical cables between circuit boards within a chassis or in different chassis. However, electrical connections can suffer from signal integrity issues, including crosstalk, roll-off with frequency, and reflections at impedance discontinuities. Amelioration of the signal integrity issues may require signal regeneration and equalization, increasing circuit area and power requirements for the ICs. Additionally, power consumption generally scales with frequency, as each logic transition charges or discharges a potentially significant capacitance associated with the electrical line.
There has been a great deal of interest over several decades in using optics for clock distribution or intra- and inter-chip data distribution. For example, a synchronizing clock signal can be optically distributed with almost zero latency to many parts of a chip or a collection of chips that are co-packaged simultaneously. The optical signal can be sent through free-space, with possibly the use of mirrors or microlenses, or distributed in a waveguiding layer that is incorporated on the chip or in the package. In a more complex implementation, the data bus can be optical, connecting multiple points on the chips with optical signals.
Optical communication within a chip or between a set of chips requires appropriate optical sources and receivers. In silicon photonics, heterogeneously integrated lasers, co-packaged lasers, or an external laser is used to generate the light, while various modulator structures such as rings, Mach-Zehnder waveguide devices, or other components impose data on the CW signals. Detectors can be monolithically made in silicon by using absorbing germanium layers. Generally, a longer wavelength of 1.3 um is used for silicon photonics as it is compatible with fibers that send or receive the data elsewhere.
Generally, most photodetectors in silicon and other materials employ a p-i-n structure, where a lightly doped “intrinsic” semiconductor is sandwiched between p-doped and n-doped material. Either the built-in voltage of the diode alone or with the additional reverse bias causes an electric field to be present in the intrinsically doped “i” region. When photons are absorbed in this region and generate electron hole pairs, the electric field separates the two carriers and generates photocurrent.
Generally, p-i-n structures are made “vertically” (e.g., normal to the top surface of an IC), for example there is a top p-type region, with an intrinsic region below and all on top of n-type material. The photons have to pass through the top p-type region to be absorbed in the intrinsic region. This is not much of a problem at longer wavelengths because the absorption length of those wavelengths in Si is relatively long, and the top p-type region can thus be made quite thin compared to the absorption length of the light. But at shorter wavelengths where the absorption length in Si is much shorter, it is quite difficult to make the top p-region thin enough to be totally transparent. Any light that is absorbed in the top p-type region generally does not lead to photocurrent, as there is no electric field to separate the carriers. Any photogenerated carriers that appear in the top p-doped region generally recombine in the same region and are not detected.
Furthermore, there is a trade-off in vertical photodiodes between speed and efficiency. If the middle intrinsic region is made too thin compared to the absorption length of the photon wavelength, then not much of the light is absorbed. If is made too thick, such that all the light is absorbed, the region might be too wide for fast response; any photogenerated carriers generally should be swept out of the intrinsic region and even at saturated carrier velocities, transiting a wide intrinsic region causes a time delay and a reduction in speed.
It is frequently desirable to integrate photodiodes with CMOS electronics. However, vertical structures are generally not compatible with CMOS processes, nearly all of which are lateral surface processes on extremely thin layers.
A typical CMOS process follows the following steps. A relatively insulating wafer with low levels of doping is used and n-well and p-wells are implanted for the PMOS and NMOS structures. A thin oxide is grown to act as the gate oxide. Then a polysilicon layer is deposited and patterned to act as the gates. A second mask of photoresist blocks the p-well, while a p+ implant is used to form the source and the drain on the NMOS structure on the n-well. This mask is then removed and another photoresist mask is formed to protect the n-well, and a subsequent n+ implant is used to form the source and the drain on the NMOS structure made in the p-well. Then the resist is removed, silicided contacts are formed, and other lasers of oxide of PSG glass are made in the structure with different layers of interconnect metal.
In some embodiments a photodetector for short wavelength applications is fabricated in a fully CMOS compatible process. In some embodiments the photodetector does not include germanium or SiGe. In some embodiments the photodetector is for use with light with a wavelength much shorter than 1300 nm. In some such embodiments the photodetector is for use with blue light in the visible spectrum. In some embodiments the photodetector is for use with light with a wavelength of in the 400 nm-450 nm range, which may be transmitted through oxide, nitride or dielectric waveguides or fibers, and can be detected or absorbed in silicon easily, without the use of germanium. In some embodiments n+ and p+ regions of the photodetector are formed as part of a process of forming source and drain regions of NMOS and PMOS transistors for the photodetector. In some embodiments the n+ and p+ regions of the photodetector have implant diffusion depths of the source and drain regions of the NMOS and PMOS transistors. In some embodiments an oxide layer is provided below diffusions depths of the n+ and p+ regions of the photodetector.
Some embodiments provide a device including a CMOS compatible photodetector, comprising: a device layer including a photodetector region comprised of interdigitated p fingers and n fingers of a lateral p-i-n photodetector, the p fingers being connected to a p contact and the n fingers being connected to an n contact, the n fingers being doped with an n-type dopant and the p fingers being doped with a p-type dopant; and at least one of a buried oxide layer below the device layer, a buried doped layer below the device layer, or a p-type or n-type dopant implant at at least one edge of the photodetector region. In some embodiments the at least one of the buried oxide layer below the device layer, the buried doped layer below the device layer, or the p-type or n-type implant at at least one edge of the photodetector region comprises the buried oxide layer below the device layer. In some embodiments. In some embodiments the buried oxide layer is reflective at a wavelength of operation. In some embodiments the wavelength of operation is about 450 nm. In some embodiments a thickness of the device layer is between 3 and 5 times an absorption length of light at the wavelength of operation. In some embodiments doped regions for the p fingers and the n fingers extend at least halfway through the thickness of the device layer. In some embodiments the at least one of a buried oxide layer below the device layer or a p-type implant or n-type implant at at least one edge of the photodetector region further comprises the p-type implant or n-type implant at at least one edge of the photodetector region. In some embodiments the p-type implant or n-type implant at at least one edge of the photodetector region comprises p-type implants or n-type implants at at least opposing edges of the photodetector region. Some embodiments further comprise at least one PMOS transistor and at least one NMOS transistor in the device layer. In some embodiments the at least one of the buried oxide layer below the device layer, the buried doped layer below the device layer, or the p-type implant or n-type implant at at least one edge of the photodetector region comprises the buried doped layer below the device layer. In some embodiments the buried doped layer comprises an n-type doped layer. In some embodiments the buried doped layer comprises an p-type doped layer. Some embodiments further comprise transimpedance amplifier circuitry in the device layer. Some embodiments further comprise a waveguide positioned to provide light to the photodetector region.
Some embodiments provide a device including a CMOS compatible photodetector, comprising: a device layer including a photodetector region comprised of interdigitated p fingers and n fingers of a lateral p-i-n photodetector, the p fingers being connected to a p contact and the n fingers being connected to an n contact, the n fingers being doped with an n-type dopant and the p fingers being doped with a p-type dopant; and a photodetector isolation structure for the photodetector region. In some embodiments the photodetector isolation structure comprises a buried oxide layer below the device layer under the photodetector region. In some embodiments the photodetector isolation structure comprises a buried doped layer below the device layer under the photodetector region. In some embodiments the photodetector isolation structure comprises doped implants at opposing edges of the photodetector region. In some embodiments the photodetector isolation structure comprises a buried oxide layer below the device layer under the photodetector region and doped implants at opposing edges of the photodetector region.
These and other aspects of the invention are more fully comprehended upon review of this disclosure.
Then a polysilicon layer 137 is deposited and patterned by photoresist 135 and etched to form the gate oxide, for example as shown in
The above process produces interdigitated contacts of p+ and n+ with lightly doped semiconductor in between, and gate oxide above. In some embodiments, the interdigitated contacts are subsequently metalized. This can be accomplished by patterning the oxide to allow electrical contact to the source, drain and p and n regions of the lateral p-i-n detector. Ti can then be added, forming titanium silicide on the contacts and then following with additional metallization such as copper or gold.
The addition of a buried oxide layer 213 increases the speed of the photodetector because any carriers generated deep within the wafer are not collected. The buried oxide layer is shown in
In some embodiments, the photodetector structure comprises a buried doped layer instead of a buried oxide layer. This buried doped layer may be fabricated as an n-type implant or p-type implant. This layer serves a similar purpose to that of a buried oxide layer: any carriers generated deeper than the layer are not collected by p-i-n detector structure. In some embodiments, the buried doped layer may not be electrically connected to other structures such that it is electrically floating. In some embodiments, a p-type buried implant layer may touch the p-type fingers of the photodetector. In some embodiment, an n-type buried implant layer may touch the n-fingers of the photodetector such that it is at the same voltage as the n-type fingers.
Similarly, preferably the detector is not illuminated outside the region of the fingers. For this reason, it is preferred both to block off the light away from the finger region with metal 255, for example, and also dope the regions 230 outside, in some embodiments at edges of, the detector, for example with a p-type implant, although in some embodiments an n-type implant may be used. This is shown in
The detector quantum efficiency (QE) is simple to calculate. Generally, factors impacting QE include:
1. Surface reflectivity: Ideally the thickness of the oxide 227 is appropriate to act an as anti-reflection coating layer. Other materials, such as MgF, SiN, or other dielectric, can be deposited on the detector surface to act as an anti-reflective (AR) coating and reduce the light that is lost simply through reflection.
2. The “duty cycle” of the fingers: The finger “duty cycle” is the ratio of spacing between the fingers to the center-to-center finger spacing. As previously mentioned, light that is incident on the fingers is lost, and thus maximizing duty cycle maximizes QE.
3. Thickness of the silicon device region: Ideally this is a few times the absorption length of the light in silicon. For example, at 450 nm, the absorption length of light in silicon is about 0.2 um. Preferably the device layer should be a few times this, or say 0.6 to 1 um for vertical incidence. For proper collection of carriers, the doped region should penetrate a substantial region into the absorption region. Otherwise, there will be only weak electric fields in the lower parts of the wafer and the carriers generated there will not be efficiently collected.
In some embodiments, a waveguide is fabricated on top of a detector.
In some embodiments, the waveguide and detector are in contact over a sufficient length that most of the light in the waveguide is absorbed along the length of the detector. As light propagating in the waveguide enters the region where the waveguide is in contact with the detector, some of the light is absorbed in the detector because the detector index is higher than that of the waveguide core. Light that is not directly absorbed is reflected and absorbed farther down the waveguide when it again encounters the core-detector interface.
In some embodiments, the waveguide is terminated by a reflective coating 373 (such as a metal layer) that forms an angled mirror at the end of the waveguide. Light reflected from this mirror is absorbed by the photodetector. Such an angled mirror can easily be formed by under-etching a material with a mask and metallizing afterwards. An under-cut forms under a mask and the angle can be adjusted by varying the directionality, pressure, and reactant concentration in the etch. Similarly, a grey scale mask or nano-imprint technology can be used.
In some embodiments, the detector is monolithically integrated with a transimpedance amplifier (TIA) and/or other active electronics. In some embodiments, this detector/TIA combination is fabricated in the same substrate on which the waveguides are fabricated.
In some embodiments, the detector/TIA die are fabricated on a silicon wafer with a buried oxide layer, and the die may have been released from that wafer using a selective etch in which the buried oxide acts as an etch-stop layer and allows the die to be lifted off that wafer.
In some embodiments, the substrate to which the detector/TIA die is attached is a silicon interposer 433. In some embodiments, the substrate is designed to be used between a complex logic or memory IC, such as a FPGA or a GPU and a package and has thin wiring and through-chip vias. The output signal from the TIA is transmitted to a logic chip 441 above, or sent down through the interposer to the package 435 below.
Various interconnect schemes can be used between this chip, the logic chip, and the package. Solder bumps 457, copper pillars 461, solid-liquid diffusion bonding, or other methods. An advantage of course is that the optical signal in the waveguide can propagate longer distances without cross-talk or degradation than electrical lines.
Although the invention has been discussed with respect to various embodiments, it should be recognized that the invention comprises the novel and non-obvious claims supported by this disclosure.
This application claims the benefit of U.S. Provisional Patent Application No. 63/047,694, filed on Jul. 2, 2020, the disclosure of which is incorporated by reference herein.
Number | Date | Country | |
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63047694 | Jul 2020 | US |