1. Field
Circuit devices and methods for forming circuit devices.
2. Background
A metal oxide semiconductor field effect transistor (MOSFET) of an integrated circuit such as a multiprocessor or other circuit. The transistor includes a source and drain junction region formed in a semiconductor substrate and a gate electrode formed on a surface of the substrate. A gate length is the distance between the source and drain junction region. Within the substrate, the region of the substrate beneath the gate electrode and between the source and drain junction regions is generally referred to as a channel with a channel length being the distance between the source and drain junctions. An active area including the gate electrode and the junction regions is typically defined by shallow trench isolation (STI) structures formed in the substrate defining a perimeter. The distance between two STI in a direction perpendicular to the channel (on the same substrate plane) is generally referred to as a channel width. In this aspect, trenches are etched vertically into the silicon substrate and a dielectric material (e.g., an oxide) is deposited within the trench. The term “vertical” as used herein is understood to mean substantially perpendicular to a surface of the substrate.
As noted above, many transistor devices are formed in a semiconductor substrate. To improve the conductivity of the semiconductor material of the substrate, dopants are introduced (e.g., implanted) into the substrate. An N-type transistor device may have source and drain regions (and gate electrode) doped with an N-type dopant such as arsenic. The N-type junction regions are formed in a well that has previously been formed in the semiconductor substrate as a P-type conductivity. A P-type dopant is boron.
A transistor device works generally in the following way. Carriers (e.g., electrons, holes) flow between source junction and drain junction by the establishment of contacts on the substrate to the source and drain junction between which a potential voltage difference has been applied. To establish carrier flow, a sufficient voltage must be applied also to the gate electrode to form an inversion layer of carriers in the channel. This minimum amount of voltage is generally referred to as a threshold voltage (VT).
In general, in Very Large Scale Integrated (VLSI) circuits a variety of device lengths and widths are used (where “width” is the device dimension measured in the direction perpendicular to current flow and “length” is the device dimension measured in the direction of current flow). For an effective VLSI circuit design, it is desired that performance characteristics like threshold voltage VT, leakage current Ioff (i.e. current per micron of device width flowing between source and drain junctions in “off-state” when transistor is switched off) and drive current Ion (i.e. current per micron of device width flowing between source and drain junctions in “on-state” or when transistor is switched on) are well controlled and remain constant.
If drive current decreases on narrow width devices, designers typically will need to add additional device width to their layout to compensate for the drive current loss if high performance is required on the narrow width devices used. Once this is done on the millions of narrow devices present, it will result in undesirable increased microchip area. On the other hand if drive current Ion increases on narrow width devices due to a decrease in VT and increase in leakage current Ioff, designers will typically experience undesired high current leakage and high power consumption in circuit blocks which makes use of narrow width devices such as for example a SRAM (Static Random Access Memory) array.
Typically, for long devices (about 500-1000 nanometers channel length L), Ioff increases while VT decreases when going from wide to narrow width MOSFET. This effect is known as Inverse Narrow Width Effect (INWE) and is mainly due to the gate electrode wrapping around the isolation edges and high trench slopes that result in fringing (i.e., higher) electrical field at the STI edges. In contrast, in the case of short devices (about 30-70 nanometers channel length L), despite the type of isolation used, the opposite of INWE is observed and VT increases while Ioff decreases when going from wide to narrow width MOSFET. Ideally, the threshold voltage should be constant along the gate width especially for the short devices (about 30-70 nanometers channel length L) that are mostly used in state of the art VLSI.
To set the threshold voltage of the short devices (about 30-70 nanometers channel length L), locally implanted dopants may be introduced under the gate edges by tilted implants. Such implants are referred to as “halo” implants and are normally performed after gate patterning in a direction parallel to the channel length direction (perpendicular to the device width direction). The implanted dopant however tends to raise the doping concentration at both active region ends in the device width direction due to the implanted species segregation properties into the oxide material of which the STI trenches are formed. In this aspect, a piling up of the dopant at STI edge regions may be seen.
In the case where the dopant concentrations below the gate vary, so does a threshold voltage along the width of the gate. In particular in short channel length narrow width devices, as a result of diffusion and the piling up of the halo dopant toward the STI region, the threshold voltage at the edge regions of the gate electrode may be greater than at the center region. In wide devices this non uniform distribution does not significantly affect overall threshold voltage because the gate edges make up only a small fraction of the entire gate. In narrow devices, however, since the gate is much narrower, the contribution of the edges is much more significant. Thus, in narrow width devices (e.g., on the order of 500 nanometers width or less), the overall threshold voltage of the gate is increased to a greater degree due to the edges than in wide devices.
In addition, threshold voltage may be sensitive to STI step topography at STI edges that cause a poly gate to be thicker and a poly length to be patterned longer at device edges. Since threshold voltage varies with poly length, a local variation in poly length occurring at STI edge regions will change the average threshold voltage. This change in threshold voltage will be, larger on narrow width devices where the gate edges make up a large fraction of the entire gate.
The features, aspects, and advantages of the invention will become more thoroughly apparent from the following detailed description, appended claims, and accompanying drawings in which:
Referring to the figures,
Overlying a surface of substrate 102 (a top surface as viewed) in
Overlying a surface of mask layer 120 in
Wells 105, 110 and 115 may be P-type or N-type. For example, well 110 may be a P-type well formed in one region of substrate 102 while wells 105 and 115 may be N-type formed in a second and third region of substrate 102. P-type well 110 is formed by introducing a dopant such as boron, into substrate 102. N-type wells 105, 115 are formed by introducing a dopant such as arsenic, phosphorus, or antimony into substrate 102. Representatively, the transistor device formed by the foregoing description in well 110 is an NMOSFET, formed in a P-type well. In an alternative embodiment, the transistor device is a PMOSFET, formed in an N-type well.
After dielectric layer 510 is formed, dielectric layer 510 is polished resulting in a planar surface of structure 100 as shown in
In one embodiment, a narrow device width may be in the range of approximately 0.1-0.5 microns and a wide device width may be in the range of approximately 1-10 microns. Dopants 810 may be of a P-type or N-type species depending respectively on whether it is desired to increase or to decrease the VT of the narrow width NMOS devices with respect to the VT of the wide width NMOS devices.
In an ideal embodiment, device performance (ID) remains constant regardless of the width (z) of the device. In reality, however, as the width (z) of the device decreases, the performance decreases dramatically. It is this performance decrease that, in one aspect, may be balanced and in another aspect overcompensated to achieve the target performance level. Thus, the energy and dose of the implant must be optimized to appropriately balance the ion distribution within the well and achieve target VT.
In one embodiment, the species of the dopant is chosen in order to compensate or to boost a nonuniform distribution of dopant along the substrate surface after doping of the substrate well. In another embodiment, species of the dopant is chosen in order to compensate or to boost a nonuniform distribution of dopant along a substrate surface after a halo implant performed after poly gate formation. A nonuniform distribution refers to a distribution differing by 50 to 100 percent. Alternatively, the dopant is introduced to compensate for a performance decrease with respect to wide ones cause by a thicker poly gate at STI edges and a poly length patterned longer at device edges. In one embodiment an opposite species type to the halo may be selected if one wants to reduce the overall VT of the narrow device with respect to the VT of the wide width devices.
Nonuniform ion distribution occurs, in one aspect, during thermocycles of the fabrication process. In the case of a P-type well, boron dopants tend to diffuse toward dielectric material 510 (e.g., SiO2) in trench 210. Thus, a larger concentration of boron tends to form along edges of well 110 than at the center. This increased boron concentration near edges of a width dimension of a gate electrode tends to increase the voltage that must be applied to the edges to turn the device on as compared to that required along the center portion of a width dimension of a gate electrode. In a narrow width device, where edge regions represent a large percentage (approximately 10-40 percent (%)) of the entire width amount, this results in overall higher device VT. In the wide devices instead, where edge regions represent a small percentage (approximately 1-5%) of the entire width amount, this results in unchanged device VT.
Thus, where a lower threshold voltage is desired, a uniform boron concentration along the surface of well 110 may be targeted. To achieve such a distribution, dopants having an opposite charge of P-type well 110 are introduced into corners of the active region. For example, where well 110 is doped with boron (P-type), dopants 810 may be, but are not limited to arsenic, phosphorous or antimony. Dopants 810 may be introduced in any amount suitable for achieving the desired change in threshold voltage. For example, where an even lower threshold voltage is desirable, a higher concentration of arsenic may be implanted.
As shown in
It should be recognized that changing of the device performance as described above may alternatively include increasing the threshold voltage. This can be useful for narrow devices used in circuits where low leakage (high VT) operation is important. This may, for example, be achieved by doping corners of P-type well 110 with a boron species instead of arsenic. As a result of the further increase in boron concentration near gate electrode 1020 edges (see
It should also be recognized that by use of dopants 810, an STI structure step height may be reduced (due to increased etch rate of implant damaged oxide) while an STI oxide divot remains unchanged. This additional effect results in improved topography and hence poly patterning uniformity and reduced gate leakage tails. Ultimately resulting in better product frequency (Fmax) vs. leakage (ISB) due to the abundance of narrow width devices used in product.
The different material density between, for example, the silicon nitride of mask layer 120 and the silicon dioxide in trenches 210, in one embodiment, is sufficient to allow penetration of dopants 810 to stop within active corner regions 820 of well 110 without penetration into the device channel region (under mask layer 120). Recess 710 in dielectric material 510 facilitates (and could be increased if necessary) the penetration of dopants 810 in the device width direction. After corners 820 are doped as shown in
In one embodiment, where changing the device performance includes decreasing the threshold voltage of a narrow width transistor having a well 110 doped with boron, arsenic may be introduced into an active region at a concentration of about 1E-18/cm3, this concentration is similar to a halo so that it effectively compensates the halo. The arsenic may be introduced at an angle of 10 to 40 degrees. In this aspect, it is to be recognized that the larger the angle of introduction, the wider the transistors that starts to respond to this process. The arsenic may be introduced at an implant energy of 40 to 60 kilo electron volts (keV), the upper energy depending on the thickness of the mask layer 120 over the silicon (in our case about 700 Å) which we don't want penetrate and the lower energy depending on the STI recess 710 we want to penetrate. The implant is introduced at a depth of 100-300 Å, similar to the depth of a halo implant, from the substrate surface.
In one embodiment, once dopants 810 are introduced, mask layer 120 and photoresist layer 830 are etched as shown in
In the preceding detailed description, specific embodiments are illustrated, including a device having implants for changing device performance. It will, however, be evident that various modifications and changes may be made thereto without departing from the broader spirit and scope of the invention as set forth in the claims. For example, N-type devices have been described. It is contemplated that, the apparatus and method is suitable for P-type devices. Still further, changing of VT is described, however, it is further contemplated that performance characteristics may further include, for example, Ioff and ID. The specification and drawings are, accordingly, to be regarded in an illustrative rather than a restrictive sense.