The present invention relates to NLDMOS arrays. In particular it relates to NLDMOS arrays with self-protection capability for use in high power applications.
Power products such as dc-dc convertors, controllers, LED drivers, LMUs etc., are typically implemented as arrays and are commonly designed using power optimization processes (POP) which optimizes the drain-source resistance Rdson versus drain breakdown voltage BVDSS, resulting in a very narrow or even negative electrostatic discharge (ESD) protection window. This is a particular problem in protecting the power pins in large and midsize arrays that have been developed using POPs. Thus, for example, Switch pins in buck and boost dc-dc converters, current sinks and LED drivers can experience high transient voltages during operation that are not much different to the pulsed safe operating area (SOA) limits. This low voltage margin, coupled with the fact that transient voltages at the pins are very fast, makes these devices unsuitable for ESD protection by separate explicit snapback clamps due to the inherent latch-up problems. Such arrays therefore have to rely on self-protection.
The first inclination would be to argue that larger arrays should provide greater self protection. However this is only partially true since the self protection capability is not a linear function of array size. The safe pulse current capabilities of an array are in fact a function of two current components: the monopolar channel current and the avalanche current component. Tests have shown that the monopolar channel current is a function of initial gate biasing as depicted in
However, gate biasing does not address the avalanche current component. At certain ESD stress levels the arrays often operate in a non-linear fashion leading to current filamentation effects and local burnout at relatively low currents. Thus the SOA of the array is not simply scalable due to local snapback effects.
According to the invention there is provided a self protected NLDMOS array comprising multiple NLDMOS devices, each NLDMOS device including an n+ drain and an n+ source, wherein an n-type deep implant is formed in the device. The device may include an n-buried layer (NBL) and the n-type deep implant may include an n-sinker extending downwardly between the n+ drain and the NBL or off-set laterally from the n+drain. The deep implant may be implemented using insulated gate bipolar transistor (IGBT) technology in which process steps used in making an n-type drift region for an IGBT are used to provide the deep implant of the NLDMOS device. The device may be implemented on a bulk substrate wherein the n-type deep implant is defined by an n-type epitaxial region below the active region. The device may be implemented using thin film or membrane technology. The n-type deep implant may have a doping level of 1018 cm−3. The n-type deep implant may be spotted or patterned. The n-type deep implant may take the form of an n-well.
Further, according to the invention, there is provided a method of controlling the ESD breakdown voltage of an NLDMOS array, that includes multiple NLDMOS devices, each NLDMOS device including an n+ drain an n+ source, and a gate between the n+ drain and the n+ source, the method comprising, forming an n-type deep implant in the device. The deep implant may be formed to extend vertically below the n+ drain or at a location on the drain side of the gate between the n+ drain and the n+ source. In order to control the breakdown voltage of the array, the location of the deep implant between the n+ drain and the n+ source may be adjusted laterally.
Tests with a 60 mm wide array as provided by the LM5008 resulted in local burnout at ESD pulses below 2 kV. At a 2 kV HBM (human body model) pulse the ESD current is about 1.33A, thus requiring a current density from the array before snapback of only 0.025 mA/μm. However this was not achieved by the array due to non-linear effects that cause local snapback. High voltage NLDMOS arrays typically are not capable or snapback without suffering irreversible damage. Thus, in the case of NLDMOS arrays a solution had to be found to avoid local snapback.
Typically the array is large enough to withstand ESD pulses provided the ESD current is balanced across the array. Unfortunately non-linearity characteristics of the array results in unbalanced current distribution and local snapback effects.
Since in the NLDMOS array the source and p-body are typically connected it is not possible to limit the critical current by reducing the parasitic npn base resistance. One approach that has been adopted in the past in the case of arrays of snapback NMOS devices is to balance the current by making use of unsilicided drain ballast regions. In the case of NPN arrays, poly emitter ballasting regions have been used as an approach in balancing current.
However, the present invention deals with arrays of NLDMOS devices. Tests that were conducted in solving this dilemma showed that simply increasing the length of surface structures such as the drain ballast region fails to address the problem. As shown in
However, as indicated above, gate bias does not address the avalanche current component. Thus a different solution had to be found for NLDMOS arrays to address avalanche current breakdown.
The present invention adopts a novel current balancing structure on the drain side of the devices. In particular, the present invention makes use of additional in depth sub-collector implants. This is best understood by considering a prior NLDMOS device.
One embodiment of the present invention is shown in
Graph 500 shows the curve for no sinker compared to graphs 502, 504, 506, 508, 510, which shows the mask at locations 9.5, 10, 11, 12, 15 μm, respectively, measured from the left opening of the drain diffusion toward the source. Thus the closer the N-sinker mask is to the source (moved to the left), the lower the breakdown voltage The curve 500 with highest Vbr has no Nsinker.
In yet another embodiment of the invention instead of using process steps for forming a sinker (as is used for instance in forming vertical BJTs) process steps for forming an n-type epitaxial drift region in an isolated gate bipolar transistor (IGBT) cell configuration were used instead thereby defining an NLDMOS with n-type deep implant.
This is best understood with reference to a prior art IGBT is shown in
Thus, in one embodiment of the invention the n-type deep implant in an NLDMOS-like structure of the invention is implemented by forming the n-type epitaxial drift region 620 using IGBT manufacturing processes IGBT.
Yet another embodiment of the invention is shown in
Yet another embodiment of the invention includes an NLDMOS-type structure implemented in thin film technology as shown in
In the embodiment of
Thus, while the invention has been defined in terms of specific embodiments, the invention is not so limited, and can be implemented in different ways without departing from the scope of the invention.