Method of etching an anisotropic profile in platinum

Details Method of etching an anisotropic profile in platinum Method of etching an anisotropic profile in platinum

2001-09-05

2004-06-15

Norton, Nadine G. (Department: 1765)

Compositions

Etching or brightening compositions

C252S079300, C216S068000, C216S079000

Reexamination Certificate

active

06749770

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
This invention relates to plasma etching of platinum. More specifically, this invention provides an improved method for plasma etching of platinum for producing semiconductor integrated circuits containing platinum electrodes.
2. Description of the Prior Art
The implementation of digital information storage and retrieval is a common application of modern digital electronics. Memory size and access time serve as a measure of progress in computer technology. Quite often storage capacitors are employed as memory array elements. As the state of the art has advanced, small-feature-size high density dynamic random access memory (DRAM) devices require storage capacitors of larger capacitance having high dielectric constant materials. The high dielectric constant materials or ferroelectric materials are made primarily of sintered metal oxide and contain a substantial amount of very reactive oxygen. In the formation of capacitors with such ferroelectric materials or films, the electrodes must be composed of materials with least reactivity to prevent oxidation of the electrodes which would decrease the capacitance of storage capacitors. Therefore, precious metals, such as platinum (Pt), palladium (Pd), etc., are preferred metals used in the manufacture of capacitors for high density DRAM.
Among the possible precious metals for capacitor electrodes, platinum has emerged as an attractive candidate because it is inert to oxidation and is known to have a leakage current (<10
−9
amps/cm
2
) lower than other electrodes such as RuO
2
and Pd. Platinum also is a good conductor.
In the prior art, platinum etching has been conducted by means of isotropic etching, such as wet etching with aqua regia, or by anisotropic etching, such as ion milling with Ar gas or by other means. Because of the nature of isotropic etching, using wet etching with aqua regia causes deteriorated processing accuracy. The grade of precision in isotropic etching is not high enough for fine pattern processing. Therefore, it is difficult to perform submicron patterning of platinum electrodes due to its isotropic property. Furthermore, a problem with ion milling (i.e. anisotropic etching) occurs because the etching speed on platinum, which is to form the electrode, is too slow for mass production.
In order to increase processing accuracy in etching platinum, research and development has been quite active, particularly in the area of etching platinum by means of a dry etching process where etchant gases (e.g., Cl
2
, HBr, O
2
, etc.) are used. The following prior art is representative of the state of art with respect to etching platinum with a plasma of etching gases.
U.S. Pat. No. 5,492,855 to Matsumoto et al. discloses a semiconductor device manufacturing method, wherein an insulation layer, a bottom electrode Pt layer, a dielectric film and a top electrode Pt layer are provided on top of a substrate having already-completed circuit elements and wiring, and then, a capacitor is formed by selectively dry etching the bottom electrode Pt layer after selectively dry etching the top electrode Pt layer and the dielectric film. The manufacturing method uses a gas containing an S component as etching gas for Pt etching, or an etching gas containing S component as an additive gas; and also it implants S into the Pt layer before the Pt dry etching process by means of ion implantation to compose a S and Pt compound, and then dry etches the Pt compound thus composed.
U.S. Pat. No. 5,527,729 to Matsumoto et al. discloses process steps to form on a substrate in which circuit elements and wirings, etc., are already shaped, an insulation layer, a first metal layer, a dielectric film and a second metal layer. A top electrode and a capacitance film are formed by dry etching the second metal layer and the dielectric film. A bottom electrode is formed by dry etching the first metal layer. The etching gas for dry etching the second metal layer is a mixed gas containing hydrogen halide (e.g. HBr) and oxygen, having a ratio of oxygen against the total of hydrogen halide and oxygen set at about 10%-35%. The etching gas is also taught as a gas containing hydrocarbon, such as chloroform. Matsumoto et al. employs a silicon oxide layer as the insulation layer on the substrate, and a platinum layer or palladium layer as the first and second metal layers. Dry etching of the second metal layer and dielectric film is conducted in a low pressure region not higher than about 5 Pa, where the etching speed is high. Matsumoto et al. further teaches that where a mixed gas of hydrogen halide and oxygen is used as the etching gas, the etching speed on the silicon oxide layer can be made sufficiently low relative to that on the second metal layer made of a platinum layer or a palladium layer; in this way, the excessive etching of the silicon oxide layer underlying the first metal layer is avoided, and damage to the circuit elements and wiring, etc. underneath the silicon oxide layer can be prevented. Furthermore according to Matsumoto et al, the ratio of etching speed of the platinum and dielectric material to the resist can be increased by lowering the etching speed on the resist. Therefore, etching of the platinum and dielectric material may be conducted by using a mask of normal lay-thickness resist (generally speaking, about 1.2 &mgr;m to about 2.0 &mgr;m thick), instead of using a conventional thick-layer resist (about 3 &mgr;m and thicker).
Chou et al. in an article entitled “Platinum Metal Etching in a Microwave Oxygen Plasma”, J. Appl. Phys. 68 (5), Sep. 1, 1990, pages 2415-2423, discloses a study to understand the etching of metals in both plasma and chemical systems. The study found that the etching of platinum foils in an oxygen plasma generated in a flow-type microwave system and that very rapid etching (~6 Å/s) took place even at low power inputs (200 W). The principal plasma parameters, including oxygen atom concentration, ion concentration, and electron temperature, were measured by Chou et al. as a function of distance below the microwave coupler. These were correlated to the rate of foil etching, which decreased with increasing distance from the coupler. On the basis of these correlations Chou et al. formulated a simple mechanistic model. The study by Chou et al. further found that the etching of platinum in an oxygen plasma jet results from the concomitant action of oxygen atoms and high energy electrons.
Nishikawa et al. in an article entitled “Platinum Etching and Plasma Characteristics in RF Magnetron and Electron Cyclotron Resonance Plasmas”, Jpn. J. Appl. Phys., Vol. 34 (1995), pages 767-770, discloses a study wherein the properties of platinum etching were investigated using both rf magnetron and electron cyclotron resonance (ECR) plasmas, together with measurement of the plasma parameters (neutral concentration, plasma density, etc.). Nishikawa et al. performed experiments in Cl
2
plasmas over a pressure ranging from 0.4 to 50 mTorr. In rf magnetron plasmas, the etch rate of Pt was constant at the substrate temperature of from 20 to 160° C. The etch rate and the plasma electron density increased with gas pressure decreasing from 50 to 5 mTorr. In ECR plasmas for rf power of 300 W, Nishikawa et al. found that the etch rate of Pt was almost constant (~100 nm/min) with gas pressure decreasing from 5 to 0.4 mTorr, while the plasma electron density gradually increased with decreasing gas pressure. The study by Nishikawa et al. discusses these experimental results with respect to the relationship between the etch yield and the ratio of neutral Cl
2
flux and ion flux incident on the substrate.
Yokoyama et al. in an article entitled “High-Temperature Etching of PZT/Pt/TiN Structure by High-Density ECR Plasma”, Jpn. J. Appl. Phys., Vol. 34 (1995), pages 767-770, discloses a study wherein micron patterning technologies for the PZT/Pt/TiN/Ti structure with a spin on glass (SOG) mask are demonstrated using a high-density electron cyclotron resonance (ECR) plasma and a high substra

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