Semiconductor device manufacturing: process – Making device or circuit emissive of nonelectrical signal
Reexamination Certificate
1998-12-16
2001-02-27
Nelms, David (Department: 2818)
Semiconductor device manufacturing: process
Making device or circuit emissive of nonelectrical signal
C438S201000, C438S257000, C257S321000
Reexamination Certificate
active
06194237
ABSTRACT:
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a method for forming quantum dots in a semiconductor device and a semiconductor device resulting therefrom, and more particularly, to a method for forming quantum dots in a semiconductor device by utilizing agglomeration of a conductive layer or by utilizing simultaneous agglomeration and selective oxidation of the conductive layer and a semiconductor device resulting therefrom.
2. Discussion of the Related Art
The MOS structure is a basic structure of a semiconductor memory device. As limitations to this structure are detected with regard to device integration, development of a new semiconductor fabrication technology is needed for increasing a semiconductor memory device integration.
Specifically, when the semiconductor memory device has the MOS structure, the conventional method of switching based on variations of gate voltage may not be available, particularly when a semiconductor memory device has a device packing density within a 4 giga DRAM range because a distance between a source and a drain is reduced to about 0.13 &mgr;m (S. Wolf, “Silicon Processing; for the VLSI Era”, V2, chap.8). In other words, integration of the MOS structure is typically limited to about 4 giga DRAM because, if the distance between the source and drain becomes closer, malfunctions of the device may occur due to tunneling between the source and the drain and through a gate oxide film, even in the absence of a gate voltage. Therefore, in order to fabricate a device of giga or tera class, a form of device other than the current MOS structure should be employed, a form of device that many research groups currently suggest is the SET(Single Electron Transistor)[see K. K. Likharev, IBM J. Res. Develop. 32(1) p144(1988)].
However, the following problems must be resolved for fabrication of the SET before it is used in place of a switching device such as a DRAM. First, in view of physical performance of the SET, a size of a quantum dot required for an SET cell should be below 10 nm or smaller to prevent errors caused by thermal vibration during operation of the cell. Therefore, at least a few nanometer quantum dot is required for allowing a room temperature operation of the SET.
Second, in addition to the above-described SET cell operation requirement, development of a process for forming quantum dots is required which allows an integration on a wafer of a size greater than 8 to 12 inches. Based on the results of current research, it can be known that the development is still at a stage at which the operation principle of the SET device is recognized. In other words, the development is still at a stage in which EBL(Electron Beam Lithography) and RIE(Reactive Ion Etching) are being used to form quantum dots. [K. Nakazato, T. J. Thornton, J. White, and H. Ahmed, Appl. Phys. Lett. 61(26), 3145(1992)], [D. J. Paul, J. R. A. Cleaver, H. Ahmed, and T. E. Whall, Appl. Phys. Lett. 63(5), 631(1993)], [D. Ali and H. Ahmed, Appl. Phys. Lett. 64(16) 2119(1994)], [E. Leobandung, L. Guo, Y, Wang, and S. Y. Chou, Appl. Phys. Lett. 67(7), 938(1995)], [K. Nakazato, R. J. Blankie, and H. Ahmed, J. Appl. Phys. 75(10), 5123(1992)], [Y. Takahashi, M. Nagase, H. Namatus, K. Kurihara, K. Iwadate, Y. Nakajima, S. Horiguchi, K. Murase, and M. Tabe, IEDM 1994, p936], and [E. Leobandung, L. Guo, and S. Y. Chou, IEDM 1995, p365].
Such a quantum dot may be applied in a memory device of the SET as well as in a light emitting device. The application in a light emitting device is made possible based on the principle that an energy band gap increases as a dimension of a material decreases, with subsequent decrease of a wave length of an emitted light. That is, if the same material is reduced to a nano-scale, the material emits light of a wave length different from a wave length of bulk. Utilizing the dependence of wave length of emitted light on the size of the material, a size of a quantum dot may be controlled to obtain light of a desired wave length. Such research is actively underway in III-V semiconductor fields, which are typical light emitting materials. [D. Leonard, M. Krishnamurthy, C. M. Reaves, and S. P. Denbaars, and P. M. Petroff, Appl. Phys. Lett. 63(23), 3203(1993)] and [O. I. Micic, J. Sprague, Z. Lu, and A. J. Nozik, Appl. Phys. Lett. 68(22), 3150(1996)]. For instance, there are reports that silicon Si or germanium Ge, which has an indirect gap, also emits a blue light when their size is reduced. By forming a quantum dot of such a silicon or germanium, application in a light emitting device is also possible. [Y. Kanemitsu, H. Uto, and Y. Masumoto, Appl. Phys. Lett. 61(18), 2187(1992)] and [H. Morisaki, H. Hashimoto, F. W. Ping, H. Nozawa, and H. Ono, J. Appl. Phys. 74(4), 2977(1993)].
When nano-scale quantum dots are used in the SET, the question of how the quantum dots should be distributed within a cell is basically dependent on a form of an SET structure to be used. Different forms of SET structures suggested until now may be sorted into two categories. In a first of these categories, SET structures are similar to the MOS structures in that they include a source, a drain and a gate formed together with a channel having the quantum dots which allow discrete flow of electrons. However, in this category of SET structure, the channel has an insulator and an array of multi-channel conductors(quantum dots), allowing discrete tunneling of electrons through the quantum dots, i.e., the channel has a form in which the quantum dots are embedded in the insulator[K. Nakazato, T. J. Thornton, J. White, and H. Ahmed, Appl. Phys. Lett. 61(26), 3145(1992)], [D. J. Paul, J. R. A. Cleaver, H. Ahmed, and T. E. Whall, Appl. Phys. Lett. 63(5), 631(1993)], [D. Ali and H. Ahmed, Appl. Phys. Lett. 67(7), 938(1995)], [K. Nakazato, R. J. Blankie, and H. Ahmed, J. Appl. Phys. 75(10), 5123(1992)], [Y. Takahashi, M. Nagase, H. Namatsu, K. Kurihara, K. Iwadate, Y. Nakajima, S. Horiguchi, K. Murase, and M. Tabe, IEDM 1994, p938], [E. Leobandung, L. Guo, and S. Y. Chou, IEDM 1995, p365], [O. I. Micic, H,. Sprague, Z. Lu, and A. J. Nozik, Appl. Phys. Lett. 68(22), 3150(1996)] and [D. V. Averin and K. K. Likaharev, in “Single Charging Tunneling”, edited by H. Grabert and M. H. Devoret (Plenum, N.Y., 1992) p311]. This represents the simplest structure required for transferring electrons by discrete tunneling. Although research verifies that the Coulomb blockade effect required for operating an SET cell is also provided even though the channel is formed with a two dimensional continuous conductive line through which electrons transfer [M. A. Kastner, Rev. Mod. Phys. 64(3), 849(1992)] and [R. A. Smith and H. Ahmed, J. Appl. Phys. 81(6), 2699(1997)], the surest way of inducing the discrete tunneling of electrons is of course providing quantum dots in an insulator.
The other category of SET structures also has a structure similar to the MOS structure, with a floating point quantum dot for charging electrons in the channel thereto for reducing a current flowing through the channel [S. Tiwari, F. Rana, H. Hanafi, A. Hartstein, E. F. Crabbe, and K. Chan, Appl. Phys. Lett. 68(10), 1377(1994)], [K. Yano, T, Ishii, T. Hashimoto, T. Kobayashi, F. Murai, and K. Seki, IEEE Trans. Electron Devices 41(9), 1628(1994)], and [A. Nakajima, T. Futatsugi, K. Kosemura, T. Fukano, and N. Yokoyama, Appl. Phys. Lett. 70(13), 1742(1997)]. This form of SET structure is similar to an EPROM(Electrically Programmable Read Only Memory) which utilizes a hot carrier effect reversely. Such a reduction of current shows a quantized change resulting from electron charging when a Coulomb blockade effect appears, where electrons that are charged in the quantum dots are used to prevent successive charging of further electrons. For this, a charging energy of
Kim Ki Bum
Kwon Jang Yeon
Yoon Tae Sik
Hyundai Electronics Industries Co,. Ltd.
Le Dung A
Nelms David
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