The subject matter of this application relates to transistors. More particularly, the subject matter of this application relates to PMOS and NMOS devices with depletable drain extensions.
Conventional structures used to build high voltage MOS devices, such as PMOS device 100 shown in
Some applications, however, call for both high voltage NMOS and high voltage PMOS devices on the same structure. One conventional approach has been to make the NMOS using a quasi-vertical diffused metal-oxide semiconductor device (DMOS). A quasi-vertical DMOS device, however, requires a heavy doped buried layer, a sinker, and a thick epitaxial layer with closely controlled resistivity and thickness. These structures increase the complexity and cost of processing.
Another conventional approach has been to build both NMOS and PMOS devices with depletable drain extensions. It is undesirable, however, to use the simple drain extension 110 structure illustrated in
Thus, there is need to overcome these and other problems of the prior art associated with high voltage structures that call for both high voltage NMOS and high voltage PMOS devices.
In accordance with an embodiment of the invention, there is an integrated circuit device having a complementary integrated circuit structure comprising a first MOS device. The first MOS device comprises a source doped to a first conductivity type, a drain extension doped to the first conductivity type separated from the source by a gate, and an extension region doped to a second conductivity type underlying at least a portion of the drain extension adjacent to the gate. The integrated circuit structure also comprises a second complementary MOS device comprising a dual drain extension structure.
In accordance with another embodiment there is a complementary integrated circuit structure. The complementary integrated circuit comprises a first MOS device having a first source doped to a first conductivity type and a single drain extension separated from the first source by a first gate. The complementary integrated circuit also includes a second complementary MOS device having a second source doped to a second conductivity type and a dual drain extension separated from the second source by a second gate.
In accordance with another embodiment there is a method of making a complementary integrated circuit structure. The method comprises forming a first drain extension and a second drain extension from a first layer doped to a first conductivity type in a substrate, forming a first extension region under the first drain extension and forming a second extension region under the second drain extension, wherein the first extension region and the second extension region are formed from a second layer doped to a second conductivity type, and forming a first source and a second source in the substrate. The method also includes forming a gate of a first MOS device and a gate of a second complementary MOS device over the substrate, wherein the gate of the first MOS device is formed between a portion of the first layer and the first source, and wherein the gate of the second MOS device is formed between a portion of the first layer and the second source, and further wherein the second MOS device is a dual drain extension device.
It is to be understood that both the foregoing general description and the following detailed description are exemplary and explanatory only and are not restrictive of the invention, as claimed.
The accompanying drawings, which are incorporated in and constitute a part of this specification, illustrate several embodiments of the invention and together with the description, serve to explain the principles of the invention.
FIGS. 7a and 7b is a cross-section of an integrated circuit device according to various embodiments of the present invention.
FIG. 8 is a cross-section of an integrated circuit device according to various embodiments of the present invention.
FIG. 9 is a top-view of the device of FIG. 8 according to various embodiments of the present invention.
FIG. 10 is a cross-section of a LDMOS device made in accordance with still another embodiment of the present invention.
In the following description, reference is made to the accompanying drawings that form a part thereof, and in which is shown by way of illustration specific exemplary embodiments in which the invention may be practiced. These embodiments are described in sufficient detail to enable those skilled in the art to practice the invention and it is to be understood that other embodiments may be utilized and that changes may be made without departing from the scope of the invention. The following description is, therefore, not to be taken in a limited sense.
Notwithstanding that the numerical ranges and parameters setting forth the broad scope of the invention are approximations, the numerical values set forth in the specific examples are reported as precisely as possible. Any numerical value, however, inherently contains certain errors necessarily resulting from the standard deviation found in their respective testing measurements. Moreover, all ranges disclosed herein are to be understood to encompass any and all sub-ranges subsumed therein. For example, a range of “less than 10” can include any and all sub-ranges between (and including) the minimum value of zero and the maximum value of 10, that is, any and all sub-ranges having a minimum value of equal to or greater than zero and a maximum value of equal to or less than 10, e.g., 1 to 5.
According to various embodiments, a PMOS device complementary to the NMOS device 200 can be made without adding complexity to the process. In particular, complementary devices can be made in the same substrate without having to provide separate islands doping types for each device. Moreover, each of the complementary devices can include drain extensions where both drain extensions are made with the same layer. Referring to
Accordingly, various single drain extension device designs can be combined with the dual drain extension device 200 shown in
According to various embodiments a complementary PMOS device 300 is shown in
As indicated, the PMOS device 300 can be made in the same P-type substrate in which the complementary NMOS structure 200 is made. Referring to
According to various embodiments, the P-type drain extension 310 can extend beyond the N-type extension 340 onto the P+ drain contact 320 and/or the P-type substrate. The P+ drain contact 320 can also be spaced apart from the N-type extension 340. The portion of the N-type extension 340 under the P+ source 324, the N+ body contact 322, and the gate 312, between the P+ source 324 and the P-type drain extension 310, can be the N-type body of the PMOS 300. For example, in the devices of
According to various embodiments, the P+ layer used as the P+ body contact 244 in the NDMOS device 200 can be used as the P+ source 324 and the P+ drain contact 320 in the PMOS device 300. Further, the N+ layer used as the N+ body contact 322 of the PMOS device 300 can be used as the N+ drain contact 220 and N+ source 246 in the NDMOS 200. Using this arrangement, high voltage devices can be fabricated.
According to various embodiments, the P-type drain extensions of the devices can be formed after sidewall spacers have been formed. In this case, the P-type drain extensions can be very shallow such that they do not extend the entire way under the sidewall spacers so as to not reach the drain edge of the gate. This can prevent the P-type drain extension 310 from making an electrical connection to the channel, as called for by the current carrying extension in the PMOS device 300. When the extension is formed after the sidewall spacers, the ohmic connection of the structure can be achieved by adding a P-link layer adjacent to the drain edge of the gate, as described below.
For example,
According to various embodiments, the P-link layer 450 and the P-type drain extension 410 can be designed such that the drain extension totally depletes at a drain to body reverse bias below that at which the link layer to body junction under the edge of the gate breaks down. This can ensure that the addition of the P-link layer 450 does not reduce the breakdown of the MOS structure. According to various embodiments, the length of the P-link layer can be small so it does not fully contribute to setting the breakdown voltage. In some cases, breakdown voltage in depletable drain extension structures can be approximately proportional to the length of the depletable extension. According to various embodiments, the length of the P-link layer can be from about 0.5 μm to about 5.0 μm, and in some cases can be about 1.5 μm. A wide range of doses can be used, starting with the same dose as the P-type drain extension, such as ˜1E12 ions/cm2 and ranging up to greater than 1E15 ions/cm2, as might be used for the P+ layer.
According to various embodiments, the voltage at which the P-type drain extension totally depletes can be set largely by the integrated dose of the P-type drain extension and by the doping level of the P-type and N-type extensions. The integrated dose of the P-type drain extension can be selected so as to limit the electric field at which the extension totally depletes so that depletion occurs before breakdown between the P-type drain extension and the N-type extension occurs. For some embodiments, the P extension doping can be about 1E12 ions/cm2. This can yield a one dimensional electric field at a breakdown of about 1.6E5 V/cm.
According to various embodiments, the electric field can be obtained from a first integration of Poisson's equation in one dimension
E=qNax1/∈ [1]
where E is the electric field, q is the electron charge, Na is the doping of P-type drain extension (in this case the doping is assumed to be uniform), x1 is the thickness of P-type drain extension, and ∈ is the dielectric constant of silicon.
Further,
Q=Nax1 [2]
where Q is the integrated dose of the P-type extension (in units of ions/cm2). After substituting:
E=qQ/∈ [3]
According to various embodiments, the absolute voltage in the depletion layer on one side of the junction can be given by the second integral of Possion's equation;
Vp=qNax12/2∈=qQ2/2∈Na [4]
For the P-type drain extension side,
Vn=qNdtn2/2∈ [5]
where Vn is the voltage in the depletion layer in the N-type extension, tn is the width of depletion layer in N-type extension at a voltage that just totally depletes the P-type extension, and Nd is the doping level of the N extension (which in this case is assumed to be uniform). The integrated dose in the two sides of a depletion layer are equal, therefore:
x1Na=tnNd [6]
Solving for tn:
tn=x1Na/Nd [7]
and substituting into the expression for Vn:
Vn=qNd[(x1Na)/(Nd)]2/2∈=q(x1Na)2/Nd2∈ [8]
Substituting
x1=Q/N8 [9]
Vn=qNa2(Q/Na)2/Nd2∈=qQ2/Nd2∈ [10]
And the total applied voltage is the sum of the voltages in the depletion layers on the two sides of the junction:
V=Vn+Vp [11]
=qQ2/Nd2ε+qQ2/Na2ε [12]
=qQ2/2ε((1/Nd)+(1/Na)). [13]
According to various embodiments, another PMOS device 500 is shown in
According to various embodiments, the PMOS device 500 can be formed in the well 504 formed from an N-type extension 540. Further, according to various embodiments, the well 504 can be the body of the PMOS device. Moreover, the PMOS device 500 can be made using a layer that is also used to make the bodies of low voltage PMOS devices, i.e., an N well. The well 504 can also be a shallow N body layer optionally self aligned to the gate, similar to that of the NDMOS body 242 shown in
For example, when combining the PMOS device 500 shown in
According to various embodiments, NDMOS devices, such as those described herein, can have breakdown voltages (BVDSS) ranging from about 50V to about 1200V. According to some embodiments, NDMOS devices, such as those described herein, can have breakdown voltages ranging from about 150V to greater than about 800V. Complementary devices, such as the PMOS devices described herein, can be made to operate over the same range of voltages. Still further, devices, such as those described herein, can have improved specific ON resistance, which can vary with breakdown voltage. For example, NDMOS devices disclosed herein having a breakdown voltage of about 250V can have a specific on resistance of about 3.2 Ωmm2. Complementary PMOS devices, made with a breakdown voltage of about 250V can have a specific ON resistance of about 9.6 Ωmm2.
Some conventional MOS devices that include dual drain extensions have drain contact diffusions that can be formed in the body layer of the device. The drain body breakdown voltage (BVDSS) in such a device, however, can be influenced by the plane breakdown of the drain to body (or well) junction. This can also be the case where a feature that completely eliminates junction curvature is included as part of the device. Plane breakdown is set primarily by the doping of the lightly doped side (the drain) of the junction. Breakdown increases as doping decreases.
Body doping can be constrained to a relatively high value by the need to set threshold voltage. Typical body doping for a PMOS device is about 1E15 cm−3 for a gate oxide ˜/>1000 Å. The plane junction breakdown with this doping is about 250V. Thinner gate oxides, such as, for example, about 400 Å, can require body doping ˜/>1E16 cm−3, for which the plane junction breakdown is about 50V. NMOS devices require higher body doping for a given gate oxide thickness and threshold voltage than do PMOS devices, so their breakdown voltage can be more limited than in a PMOS device.
The drain to body junction of devices described herein, however, can be the junction between the N-type extension, such as N-type extension 340 or 440 that form both body and depletable extension regions, as shown in
According to various embodiments, in the PMOS device 600, source and drain extension 610 can be formed in the N-type well 604 without the need for an N-type extension. The N-type well 604 doping profile can be adjusted such that it totally depletes the P-type extension 610.
It is contemplated to invert all conductivity types explicitly described herein to produce a dual drain extension PMOS and a single drain extension NMOS using the structures described above.
FIGS. 7a and 7b show an MOS device where P+ drain contact 712a is formed in P− type drain 712, P+ source 714 is formed in the N− body 711 and N+ body contact 711c is provided in the N− body 711. The MOS channel region 711b is in the N− body 711 below the MOS gate 716 and Gate Oxide 713. The N type top gate 721 is provided along the surface 711s of the body 711 above the P type drift region 717 which acts as a JFET channel. The lateral edge or peripheral edge of both the top gate 721 and drift region 717 extend to the drain-to-body junction 715 and preferably terminate at the junction 715. It is noted that situations may exist where the doping level in the top gate may be sufficiently high so as to render it desirable to provide a shorter top gate having a lateral extension which stops short of contacting the junction 715. In this case care should be taken to insure that any nondepleted portion of the top gate does not result in a breakdown of the top gate-to-drift region junction 717a. Proper doping of the top gate 721 will generally be a sufficient preventative step. Dashed line 721p designates the peripheral edge of top gate 721 in an embodiment where the top gate does not extend all the way to the junction 715.
The structure of FIG. 7a provides reduced ON resistance in the JFET channel 717. The reduction in ON resistance is accomplished by providing a structure which can accommodate increased drift region doping without suffering from reduced body-to-drain breakdown. This is possible because of the provision of the top gate 721. The top gate-to-channel depletion layer which holds some channel charge when reverse biased, is in addition to the channel charge held by the bottom gate to channel depletion layer of the prior art. This additional channel charge, in the form of ionized channel impurity atoms, causes the reduction in channel resistance. It is possible to provide more than twice the doping level previously acceptable due to the additional ability to hold channel change. Thus, for a drift region 717 having a doping of 1×1012 boron atoms per square centimeter in a bottom gate arrangement, the present invention will permit 2×1012 boron atoms per square centimeter. Thus, the ON resistance will be only half the ON resistance of the prior arrangement.
In order to optimize performance of the structure of the invention, the top gate 721 must be designed differently than an ordinary JFET gate. Top gate 721 should become totally depleted at a body-to-drain voltage of less than the breakdown voltage of the top gate-to-drain junction 715a. Since top gate 721 is connected to body 711, the voltage at the top gate-to-drain junction 715a will equal the voltage of the body-to-drain junction 715 voltage and the top gate-to-drain breakdown voltage should be greater than the voltage at which top gate 721 becomes totally depleted. Additionally, the top gate 721 must totally deplete before the body 711 to channel 717 depletion layer reaches the top gate 721 to channel 717 depletion layer to thereby assure that a large top gate 721 to drain 712 voltage is not developed by punch-through action from the body 711. An ordinary JFET gate never totally depletes regardless of operating conditions.
In addition to the above described characteristics of the device of the invention, it is also necessary to insure that the channel of the JFET drift region 717 contacts the inversion layer MOS surface channel. This can be accomplished as shown in FIG. 7b where an implant mask 750 having a tapered edge 751 is provided over the body 711. An implant aperture 752 is provided in mask 750 at the location where the P drift region 717 and N top gate 721 are to be formed. The aperture 752 is shown as exposing the protective oxide 753. Ion implantation is not substantially affected by the oxide 753 due to the oxide thickness of only about 0.1-0.2 micrometers, yet the oxide provides surface passivation for the underlying body 711.
The drift region 717 is ion implanted and, because of the graduated thickness of the implant mask 750 (along the edge 751), the depth of the implanted drift region 717 is graduated or tapered. In the illustration, a fairly good rounding of the drift region 717 occurs at the peripheral edges or extremities 717a, 717b of the region 717. The curved extremity 717a is of interest because at this location the channel of the JFET drift region 717 contacts the surface 711s of body 711 beyond the end 721a of top gate 721 and is desirably beneath the gate 716 of the MOS device. The top gate 721 may be ion-implanted using the implant mask 750 but at an energy level which results in a shallower implantation. This tapered profile, particularly if curved, provides improved performance.
A further extension of the invention is illustrated in FIG. 8 which shows an LDMOS device where N+ drain contact 712a is formed in an N− type substrate and an N+ source 714 and P+ body contact 711c are formed in a P− type body region 8240. The DMOS channel region 711b is in the P− body 8240 below the DMOS gate 716. The N type first drift region 8217 is provided along the surface 711s of the substrate 711 above a P− type separation region 8250. A second drift region 217a exists in the substrate 711 underneath the P− type separation region. The lateral edge of both the first drift region 8217 and the separation region 8250 extend from the gate 716 to the N+ drain contact 712a.
The structure in FIG. 8 provides reduced ON resistance by way of the second (surface) drift region 217a. To illustrate this, consider an example in which the N− region 711 has a doping of 1×1014 ions cm−3. The top gate layer 8217 has an integrated doping of about 1×1012 ions cm−2 and is preferably not more than two microns thick while maintaining full breakdown. The thickness of the N and P layers 8217, 8250 together is preferably less than ten microns and can be less than one micron. The same integrated doping in the N− body 711 requires a thickness of 100 microns. Thus, the N and P layers 8217, 8250 respectively consume only a small fraction of the N− thickness required to provide doping equal to that portion of the N layer of the prior art device.
The lateral spacing between the drain contact 712a and the channel 711b in the device described above would be approximately 30 microns. In such a device, even if a full 100 micron thick N− body 711 were provided, it would have a higher resistance than the N− first drift region 8217 provided according to the invention. This is because the average path length of current flowing from the drain contact 712a down through the thick N− body 711 and back up to the surface edge of the channel at the drain-to-body junction would be greater than the direct path through the N− first drift region.
Maximum breakdown is achieved in the invention by providing doping densities of the N and P layers 8217, 8250 such that they become totally depleted before breakdown is reached at any point along the junctions which they form with adjoining regions and before breakdown is reached at the junction between them. To insure that this occurs, the N region 8217 should have an integrated doping not exceeding approximately 1×1012 ions cm−2 and the P region 8250 should have a higher integrated doping not exceeding about 1.5 to 2×1012 ions cm−2.
To insure proper depletion of the P and N regions 8250, 8217, they must have the proper voltages applied. The N layer bias is achieved by connecting the N first drift region 8217 to the higher concentration N+ drain contact 712a by overlapping the N first drift region 8217 and drain contact 712a. The P region 8250 bias is achieved by overlapping the P region 8250 with the P− body 8240 at least at one end of the channel, thereby applying the body voltage to the P layer 8250. This is illustrated in FIG. 9.
With this structure and choice of doping levels, the desired results are achieved. When a reverse bias voltage is applied to the drain-to-body junction between P− body 8240 and N− body 711, the same reverse bias appears on both the PN− junction 8260 and the PN junction 8270. Depletion layers spread up into the N first drift region 8217 and down into the N− body 711 from the P layer 8250. In a preferred embodiment, the P and N first drift region dopings are chosen such that the N layer 8217 becomes totally depleted at a lower voltage than that at which the P layer 8250 becomes totally depleted. This insures that no residual undepleted portion of the N layer 8217 is present which could reduce breakdown voltage.
As a result of the invention, the improved DMOS device provides a reduced resistance current path in the drain which does not depend on the N− doping. This allows the N− doping to be reduced to achieve a desired breakdown voltage with good manufacturing margin, while maintaining desirable low drift region resistance. In a multi-device process which includes LDMOS devices, the N− region can be adjusted to achieve the desired characteristics of one or more of the other device types, while the N first drift region 8217 sets the drift region 8217 resistance of the LDMOS.
Still another embodiment, as illustrated in FIG. 10, provides no gap between the P− body 8240 and the P region 8221 adjacent to the channel edge. The absence of the gap prevents current from flowing in the N− body 711; so the entire drift region current path is in the N first drift region 8217. Elimination of the gap also allows the device structure to be made smaller. As with the other structure, the N and P regions may be self-aligned to the gate edge, as illustrated in FIG. 10, or not self-aligned. They may also be covered by thick or thin oxide as a design option.
While the invention has been illustrated with respect to one or more implementations, alterations and/or modifications can be made to the illustrated examples without departing from the spirit and scope of the appended claims. In addition, while a particular feature of the invention may have been disclosed with respect to only one of several implementations, such feature may be combined with one or more other features of the other implementations as may be desired and advantageous for any given or particular function. Furthermore, to the extent that the terms “including”, “includes”, “having”, “has”, “with”, or variants thereof are used in either the detailed description and the claims, such terms are intended to be inclusive in a manner similar to the term “comprising”.
Other embodiments of the invention will be apparent to those skilled in the art from consideration of the specification and practice of the invention disclosed herein. It is intended that the specification and examples be considered as exemplary only, with a true scope and spirit of the invention being indicated by the following claims.
This application claims priority to U.S. Provisional Patent Application Ser. No. 60/688,708 filed on Jun. 9, 2005, the disclosure of which is incorporated by reference herein in its entirety.This application is a continuation reissue of application Ser. No. 13/291,302 filed on Nov. 8, 2011, now U.S. Reissue Pat. No. RE 44,430, which is a reissue of application Ser. No. 12/372,172 filed on Feb. 17, 2009, now U.S. Pat. No. 7,829,954, which is a division of application Ser. No. 11/361,361 filed on Feb. 24, 2006, now U.S. Pat. No. 7,547,592, which claims benefit of U.S. provisional patent application No. 60/688,708 filed on Jun. 9, 2005, the disclosure of which is incorporated by reference herein in its entirety.
Number | Name | Date | Kind |
---|---|---|---|
4823173 | Beasom | Apr 1989 | A |
5264719 | Beasom | Nov 1993 | A |
5338960 | Beasom | Aug 1994 | A |
6894349 | Beasom | May 2005 | B2 |
6974753 | Beasom | Dec 2005 | B2 |
RE44430 | Beasom | Aug 2013 | E |
20030102512 | Chatterjee | Jun 2003 | A1 |
Entry |
---|
U.S. Patent and Trademark Office, “Image File Wrapper”, “U.S. Appl. No. 11/361,361, Downloaded Jul. 19, 2013”, pp. 1-153. |
U.S. Patent and Trademark Office, “Image File Wrapper”, “U.S. Appl. No. 12/372,172 , Downloaded Jul. 19, 2013”, pp. 1-115. |
U.S. Patent and Trademark Office, “Image File Wrapper”, “U.S. Appl. No. 13/291,302 , Downloaded Jul. 19, 2013”, pp. 1-190. |
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60688708 | Jun 2005 | US |
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Parent | 11361361 | Feb 2006 | US |
Child | 12372172 | US |
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Parent | 13291302 | Nov 2011 | US |
Child | 12372172 | US |
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Parent | 12372172 | Feb 2009 | US |
Child | 13950481 | US | |
Parent | 12372172 | Feb 2009 | US |
Child | 13291302 | US |