The features, aspects and embodiments disclosed herein relate to the manufacture of semiconductor devices, such as semiconductor-on-insulator (SOI) structures, using an improved ion implantation process.
To date, the semiconductor material most commonly used in semiconductor-on-insulator structures has been silicon. Such structures have been referred to in the literature as silicon-on-insulator structures and the abbreviation “SOI” has been applied to such structures. SOI technology is becoming increasingly important for high performance thin film transistors, solar cells, and displays, such as active matrix displays. SOI structures may include a thin layer of substantially single crystal silicon on an insulating material.
Various ways of obtaining SOI structures include epitaxial growth of silicon (Si) on lattice matched substrates. An alternative process includes the bonding of a single crystal silicon wafer to another silicon wafer on which an oxide layer of SiO2 has been grown, followed by polishing or etching of the top wafer down to, for example, a 0.05 to 0.3 micron layer of single crystal silicon. Further methods include ion-implantation methods in which either hydrogen or oxygen ions are implanted either to form a buried oxide layer in the silicon wafer topped by Si in the case of oxygen ion implantation or to separate (exfoliate) a thin Si layer to bond to another Si wafer with an oxide layer as in the case of hydrogen ion implantation.
Manufacture of SOI structures by these methods is costly. The latter method involving hydrogen ion implantation has received some attention and has been considered advantageous over the former methods because the implantation energies required are less than 50% of that of oxygen ion implants and the dosage required is two orders of magnitude lower.
U.S. Pat. No. 7,176,528 discloses a process that produces silicon on glass (SiOG) structure. The steps include: (i) exposing a silicon wafer surface to hydrogen ion implantation to create a bonding surface; (ii) bringing the bonding surface of the wafer into contact with a glass substrate; (iii) applying pressure, temperature and voltage to the wafer and the glass substrate to facilitate bonding therebetween; (iv) cooling the structure to a common temperature; and (v) separating the glass substrate and a thin layer of silicon from the silicon wafer.
Although the manufacturing processes for making SOI structures is maturing, the commercial viability and/or application of final products employing them is limited by cost concerns. A significant cost in producing an SOI structure using the process disclosed in U.S. Pat. No. 7,176,528 is incurred during the ion implantation step. It is believed that reductions in the cost of carrying out the ion implantation process would improve the commercial application of SOI structures. Accordingly, it is desirable to continue to advance the efficiency of producing SOI structures.
Although the features, aspects and embodiments disclosed herein may be discussed in relation to the manufacture of semiconductor-on-insulator (SOI) structures, skilled artisans will understand that such disclosure need not be limited to SOI manufacturing. Indeed, the broadest protectable features, aspects, etc. disclosed herein are applicable to any process in which ion implantation into (or onto) semiconductor material is required, whether such semiconductor material is used in conjunction with an insulator or otherwise.
For ease of presentation, however, the disclosure herein may be made in relation to the manufacture of SOI structures. The specific references made herein to SOI structures are to facilitate the explanation of the disclosed embodiments and are not intended to, and should not be interpreted as, limiting the scope of the claims in any way. The SOI abbreviation is used herein to refer to semiconductor-on-insulator structures in general, including, but not limited to, semiconductor-on-glass (SOG) structures, silicon-on-insulator (SOI) structures, and silicon-on-glass (SiOG) structures, which also encompasses silicon-on-glass-ceramic structures. In the context of this description, SOI may also refer to semiconductor-on-semiconductor structures, such as silicon-on-silicon structures, etc.
In accordance with one or more embodiments herein, methods and apparatus of forming a semiconductor structure, include: subjecting an implantation surface of a semiconductor wafer to an ion implantation process to create an exfoliation layer therein, wherein the ion implantation process includes simultaneously implanting two different species of ions into the implantation surface of the semiconductor wafer.
The two different species of ions may be taken from the group consisting of: boron, hydrogen, and helium, or any other suitable element.
Heat treating the semiconductor wafer may be carried out such that, in the case of H and He implantation, the He ions migrate towards the area of weakening created by the H ions below the implantation surface of the semiconductor wafer.
Other aspects, features, advantages, etc. will become apparent to one skilled in the art when the description of the embodiments herein is taken in conjunction with the accompanying drawings.
For the purposes of illustrating the various aspects and features disclosed herein, there are shown in the drawings forms that are presently preferred, it being understood, however, that the covered embodiments are not limited to the precise arrangements and instrumentalities shown.
With reference to the drawings, wherein like numerals indicate like elements, there is shown in
The SOI structure 100 may include a substrate 102, and a semiconductor layer 104. Such an SOI structure 100 may have suitable uses in connection with fabricating thin film transistors (TFTs), e.g., for display applications, including organic light-emitting diode (OLED) displays and liquid crystal displays (LCDs), integrated circuits, photovoltaic devices, etc. Although not required, the semiconductor material of the layer 104 may be in the form of a substantially single-crystal material. The word “substantially” is used in describing the layer 104 to take into account the fact that semiconductor materials normally contain at least some internal or surface defects either inherently or purposely added, such as lattice defects or a few grain boundaries. The word “substantially” also reflects the fact that certain dopants may distort or otherwise affect the crystal structure of the bulk semiconductor.
For the purposes of discussion, it is assumed that the semiconductor layer 104 is formed from silicon. It is understood, however, that the semiconductor material may be a silicon-based semiconductor or any other type of semiconductor, such as, the III-V, II-IV, II-IV-V, etc. classes of semiconductors. Examples of these materials include: silicon (Si), germanium-doped silicon (SiGe), silicon carbide (SiC), germanium (Ge), gallium arsenide (GaAs), GaP, and InP.
The substrate 102, may be any desirable material exhibiting any desirable characteristics. For example, in some embodiments, the substrate 102 may be formed from a semiconductor material, such as the above-listed varieties.
In accordance with alternative embodiments, the substrate 102 may be an insulator, such as glass, an oxide glass, or an oxide glass-ceramic. As between oxide glasses and oxide glass-ceramics, the glass may have the advantage of being simpler to manufacture, thus making them more widely available and less expensive. By way of example, a glass substrate 102 may be formed from glass containing alkaline-earth ions, such as, substrates made of CORNING INCORPORATED GLASS COMPOSITION NO. 1737 or CORNING INCORPORATED GLASS COMPOSITION NO. EAGLE 2000™. These glass materials have particular use in, for example, the production of liquid crystal displays.
While the subject matter of particular interest herein involves ion implantation into semiconductor material, it is believed that providing some additional context in terms of a specific process for manufacturing the SOI 100 is beneficial. Thus, reference is now made to
Turning first to
An exfoliation layer 122 is created by subjecting the implantation surface 121 to an ion implantation process to create a weakened region 123 below the implantation surface 121 of the donor semiconductor wafer 120. Although it is this ion implantation process that is the focus of the disclosure herein, at this point only general reference will be made to the process for creating the weakened region 123. Later in this description, however, a more detailed discussion of one or more ion implantation processes of specific interest will be provided. The ion implantation energy may be adjusted using to achieve a general thickness of the exfoliation layer 122, such as between about 300-500 nm, although any reasonable thickness may be achieved. The effect of ion implantation into the donor semiconductor wafer 120 is the displacement of atoms in the crystal lattice from their regular locations. When the atom in the lattice is hit by an ion, the atom is forced out of position and a primary defect, a vacancy and an interstitial atom, is created, which is called a Frenkel pair. If the implantation is performed near room temperature, the components of the primary defect move and create many types of secondary defects, such as vacancy clusters, etc.
With reference to
In the bonding process, appropriate surface cleaning of the substrate 102 (and the exfoliation layer 122 if not done already) may be carried out. Thereafter, the intermediate structures are brought into direct or indirect contact. The resulting intermediate structure is thus a stack, including the bulk material layer of the donor semiconductor wafer 120, the exfoliation layer 122, and the glass substrate 102.
Prior to or after the contact, the stack of the donor semiconductor wafer 120, the exfoliation layer 122, and the glass substrate 102 is heated (indicated by the arrows in
In addition to the above-discussed temperature characteristics, mechanical pressure (indicated by the arrows in
A voltage (indicated by the arrows in
With reference to
The cleaved surface 125 of the SOI structure 100, just after exfoliation, may exhibit surface roughness, excessive silicon layer thickness, and/or implantation damage of the silicon layer (e.g., due to the formation of an amorphized silicon layer). Depending on the implantation energy and implantation time, the thickness of the exfoliation layer 122 may be on the order of about 300-500 nm, although other thicknesses may also be suitable. These characteristics may be altered using post bonding processes in order to advance from the exfoliation layer 122 and produce the desirable characteristics of the semiconductor layer 104 (
Reference is now made to
With reference to
The ion shower tool 200 of
Conditions are established within the plasma chamber 206 to ensure that desirable ion acceleration and energy levels are achieved to produce plasma of each gas. For example, a gas within the chamber 206 is excited to form plasma, which may be achieved via an RF antenna (not shown). The positively charged first and second gas ions are accelerated towards the donor semiconductor wafer 120 by way of an electric field between the first and second electrodes 208, 210. (It is noted that in a practical piece of equipment, there may be one or more additional electrodes, not shown, which contribute to and/or produce the required plasma and acceleration.) The field may be of sufficient magnitude to accelerate the first and second ions to an energy of between about 25-150 KeV, such as about 80 KeV. As the second electrode 210 is in the form of a grid, the ions may pass therethrough and strike the implantation surface 121 of the donor semiconductor wafer 120 and become implanted in the donor semiconductor. The energy to which the first and second ions are accelerated is selected such that the ions are implanted in the donor semiconductor wafer to the desired depth, e.g. approximately along the desired weakened region 123 below the implantation surface 121 of the donor semiconductor wafer 120. Mass flow control valves or needle valves 205A, 205B may be located in the gas feed lines between the first and second tanks 202, 204 in order to control the ratio of the first gas to the second gas in the plasma chamber 206 and thereby control the ratio of first ions to second ions implanted into the semiconductor donor wafer 120. The ratio of the first ions to the second ions being implanted may also be controlled by adjusting the distribution of the plasma in the plasma chamber 206 by controlling one or more of the arc voltage, arc current, and the biasing platen.
The specific type of implantation technique carried out within the ion implant tool 200 is not limited to ion shower type implant tools. Other suitable ion implantation techniques include plasma immersion ion implantation techniques. With reference to
A donor silicon wafer of was implanted with both hydrogen and helium ions at an implantation energy of 80 KeV, a scan speed of 100 mm/s, an ion beam current density of 500 uA/cm, and gas flow ratios of hydrogen to helium of 8/32 ccm. The ion beam current was measured prior to implantation and efforts were made to ensure that the beam current was uniform. It is contemplated to outfit the tool 200 with a beam current detector and mass separation function in order to provide monitoring of, and control over, the hydrogen/helium ion ratio. The transport mechanism 212 of the tool 200 was used to scan the donor silicon wafer 120 back and forth a suitable number of times in order to achieve a target dose.
After the simultaneous implantation of hydrogen and helium ions into the donor silicon wafer 120, the sample was separated into five pieces. Each sample was heat treated for about four hours at different temperatures: 20° C., 250° C., 300° C., 350° C., and 425° C. The samples were then measured for hydrogen and helium depth profile via TOF-SIMS analysis. The results of the TOF-SIMS analysis are shown in
It is noted that the peak concentration of hydrogen occurs at a depth that remains substantially stable at about 400 nm. The room temperature (20° C.) peak concentration of helium, however, lies at a depth of about 600 nm. With heat treatment, the peak concentration of helium migrates to about 400 nm.
Although the aspects, features, and embodiments disclosed herein have been described with reference to particular details, it is to be understood that these details are merely illustrative of broader principles and applications. It is therefore to be understood that numerous modifications may be made to the illustrative embodiments and that other arrangements may be devised without departing from the spirit and scope of the appended claims.