Journal of Photopolymer Volume 7, Number Communication Synchrotron of Plasma Radiation Polymerized in Oxygen G.K. Vinogradov, 3(1994) Science and 615-618 Technology ©1994TAPJ Patterning Organo Silicons Atmosphere C. Shao, K. Sends, and S. Morita Center for Cooperative Research in Advanced Science and Technology, Nagoya University, Nagoya 464-OY, Japan. 1. Introduction Recently some reports have been published on the development of new approaches for all dry photo lithographic processing based on silicon containing plasma polymerized resists [1,2]. Silylation technology is well known and widely used in micro lithography [3,4]. Silicon containing crosslinked thin films, on the other hand, were plasma polymerized for different purposes of surface coating such as optical, mechanical, and electrical [5,6]. It was also shown, that Si-Si network can be plasma polymerized from, for example, aromatic silanes undergoing particularly scission of Si-CH3 and Si-H bonds [7]. Silylated resists have been patterned by UV irradiation in an oxygen atmosphere as well. However, only the combination of plasma polymerization of silicon containing networks with their UV irradiation in the presence of oxygen gives a breakthrough for all dry photo lithographic processing [1,2]. Uv lithography being the only candidate for a recent mass production will be probably replaced in the future with X-ray processing having much lower critical dimension. All the merits of X-ray lithography can be revealed with ultra thin perfect resist layers, which can be deposited and processed exclusively in dry technology cycles. The present paper describes our preliminary results on plasma polymerization containing organic films in an oxygen ambient. and synchrotron X-ray patterning of silicon 2. Experimental Plasma Polymerization. Silicon organic films were deposited in RE capacitively coupled plug flow box-type reactor [S]. The reactor represents a rectangular prism with a well shaped uniform gas flow and a plasma volume, strictly limited with the rectangular copper thermal stabilized Received April 4 , 1994 Accepted May 9, 1994 615 I Photopolym. Sci. Technol., Vol. 7, No.3, 1994 electrodes, teflon stainless chamber. Two walls, sets and a copper of discharge hexamethyldisilazane/Ar mixture mesh. condition have The last was applied of polymer Film thickness The distributions deposition of film thickness with an automatic Patterned been and low frequency hexamethyldisilazane. structure. The reactor used: pulse to suppress was monitored was mounted discharge of time modulated discharge of pure features. Synchrotron X-ray patterning. 15 microns beryllium foil. Deposited and cross linking crystal microbalance. along the gas flow were measured The facility of UVSDR Japan., was used. The wavelength 0.8 nm. A stainless diaphragm supplied sample chamber a differential after was connected pumping resists copper mesh (100 lines/inch, deposited system ring in for about through a possibility the to irradiate Ton. on silicon samples were covered as a mask, irradiated and then removed Science corresponds synchrotron providing of about 0.3-0.5 50% transparent) of oxygen, of Molecular X-ray intensity to the to reveal their self with an X-ray beam through at the Institute of maximum high oxygen pressure Plasma polymerized profilometer films have been irradiated Okazaki, time in the presence 20% ellipsometer. development samples under relatively formation in situ with a quartz samples have been scanned with a mechanical with the cylindrical continuous particulate on silicon substrates inside with a microscope for a prescribed period of to the ambient atmosphere. 3. Results and Discussion All irradiated samples being negative type resists demonstrate however well distinguished self development features (Fig. 1). Irradiated areas become harder and thinner. The minimum X-ray dose in our experiments was about 0.2 Jlcm2 , which is essentially low. The irradiated area can be easily distinguished from non-irradiated by colors for all irradiated samples. Initial steep low dose part of the curve corresponds for initial high rate oxidation reactions. Under the higher doses the rate of thickness decrease is probably dealt with increasing of the degree of oxidation and less probably with a partial polymer ablation. The data known from literature suggest, that the level of sensitivity of best silicon organic polymer resists to oxidation under UV 193 nm irradiation and adjacent wet development is about 35-60 mJlcm2 [9] and can be even improved with chemical sensitizers. Total dose of about 1.2 JIcm2 transferred silicon containing plasma deposited polymers to the level eharacteri- stir of stochiometric Si0 2 [1]. The efficiency of X-ray synchrotron oxidation, and especially Be filtered radiation, must be essentially lower in compare with UV processing, taking into consideration lower absorption and mechanisms of energy transfer from high energy penetrating X-ray photons to low energy chemical bonds accompanied with several energy dissipating processes. 616 J. Photopolym. Sci. Technol., Vol. 7, No.3, Color exhibit microphotographs also some interferometric colors films. Bright areas corresponding as the the changing gray. under to dark is increasing, from dark to phenomenon X-ray beam mesh mask. reddish definitely the mesh difficult oxygen. X-rays gas Secondary can be a excited metastable can promote of the X-ray molecules. species, component oxygen, and states. Every 2 rough in thus these distributed decreasing the exposure. shows a profilometer sample. thus radiative of appropriately of the films Fig. of the film deposited by dissipation excited mechanical absorbed energy electronically contrast Fig. I. Self-development in a pulsed discharge. activated of atomic oxidation the areas oxygen surface of origin processes molecules, part probable are partly ionized explain below with phase produce to some of masked interaction film as well. most direct bright polymer with The is oxidation redistributed of oxidation signal from the for high dose The typical surface compare of masked with exhibiting some reactions. Similar noisy areas be found on can blue areas such squares minimum of unexposed the copper very a color modifying irradiated intact self developed dose It is rather the the are changing It manifests reactions of for irradiation while change of yellowish of 0.2 JIcm2 1994 profile low the areas irradiated surface of etching samples increased load on the profilometer's stylus. hardness of irradiated non-irradiated Fig. 2. Mechanical prlofile of the patterned resist. Initial thickness 200 nm, continuous discharge. unexposed dose and is under In that case areas the effect and indentation is caused of the stylus by the difference inside the of polymer film. 617 J. Photopolym. Sci. Technol., Vol.7, No. 3, 1994 Further now experiments on X-ray oxidative patterning and vet and plasma development are in progress. Conclusion X-ray Silicon containing exposure in irradiated Clear areas optical images phenomena gas phase oxidative have resist Typical been been developed of the resists films have X-ray patterning observed under in all samples have been been patterned by by synchrotron self development any doses from including those with the lowest modified to the secondary processes silicon films be under the high of energy about X-ray dissipation 0.2 doses of JIcm2. dose. as well. through the candidates for oxygen. deposited X-ray ambient. films can be assigned activated Plasma have areas polymerized oxygen of polymer Unexposed This an plasma photo organo lithography can considered in all dry microelectronics as promising technology cycles. References 1. M.W. Horn, S.W. Pang, and M.Rothschild, J. Vac. Sci. Technol., BS 1493 (1990). 2. T.W. Weidman, A.M. Joshi, Appl. Phys. Left. 62 (1993) 374. 3. D.W. Johnston, R.R. Kunz, M.W. Horn, J. Photopolym. Sci. Technol., 6 (1993) 593. 4. M. Morita, A. 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