Method of etching metallic film for semiconductor devices

There is provided a method of etching metallic film for a semiconductor device, in which a semiconductor substrate with a metallic film exposed in a film pattern is inserted onto a chuck in a chamber of an electrostatic shielded radio frequency (ESRF) inductive-coupled plasma source, the ESRF inductive-coupled plasma source also including a coil connected to an upper electrode, a lower electrode connected to the chuck, a gas supply assembly, a pressure control assembly and a temperature control assembly. An etching gas is supplied to the chamber at a predetermined etch gas supply rate. Pressure inside the chamber is maintained at a predetermined pressure level. The upper and lower electrodes are powered with predetermined upper and lower powers, respectively, at predetermined upper and lower RFs, respectively. The chamber walls are cooled to a predetermined temperature. The metallic film is etched such that trenches in the metallic film are formed with predetermined trench qualities including a predetermined trench critical dimension no greater than a critical dimension associated with large scale integration.

BACKGROUND 
1. Field of the Invention 
The present invention relates to a method of etching metallic films for 
semiconductor devices, and more particularly, to a method of etching 
metallic films using plasma formed by electrostatic shielded radio 
frequency (ESRF) inductive-coupled plasma sources. 
2. Description of the Related Art 
Generally, during the fabrication of semiconductor devices, an etching 
process is performed in order to form patterns on a film deposited on a 
semiconductor substrate. The parameters of the etching process depend on 
the characteristics of the materials and structures designed for the 
semiconductor device. With more highly integrated semiconductor devices, 
the pitch, i.e., the horizontal spacing, of structures has become smaller, 
while the number of layers has increased, leading to the need for creating 
trenches through more layers. That is, there is a need for a decreased 
minimum pitch (critical dimension) and an increased aspect ratio (i.e., 
the ratio of depth of a trench to width of the trench) of the patterns 
formed in the films for integration scales beyond large scale integration 
(LSI). Productivity of the fabrication process also depends on etching 
rate, i.e., the depth of a film that can be etched in a unit of time. 
To date, a variety of etching methods have evolved--from wet etching using 
chemicals, to several dry etching methods including using pure plasmas, 
reactive ion etching (RIE), magnetically enhanced reactive ion etching 
(MERIE), electron cyclotron resonance (ECR) plasmas, and electrostatic 
shielded radio frequency (ESRF) inductive coupled plasma sources. 
The etching rates of most of these methods are limited by the depletion of 
etching agents in the vicinity of a film being etched as the etching 
progresses, a phenomenon called micro-loading. Micro-loading can be 
greatly affected by the rate at which reactive etching agents are supplied 
to the vicinity of the film and the rate at which products of the reaction 
are carried away. 
Plasmas are generated in plasma chambers in which electrons of a source 
gas, such as air at normal pressure, are excited by radio frequency (RF) 
high voltages applied across two electrodes or induced by RF electric 
current flow in a coil. The excited electrons then collide with the 
molecules of an etching gas, i.e., a process gas, to produce ions and 
radicals. The ions and radicals then etch the film deposited on the 
substrate. 
Pure plasma etching generates chemical agents including ions and radicals 
from a plasma of excited electrons so that the ions and radicals can react 
chemically with the film deposited on the substrate. The effectiveness of 
this type of etching depends greatly on the material being etched and so 
provides a high degree of selectivity, like chemical etching. For many 
materials this pure plasma etching proceeds in all directions, i.e., the 
etching is isotropic. 
Reactive ion etching (RIE) further accelerates the ions and radicals toward 
the film to increase the kinetic energy of collisions between the reactive 
ions and radicals and the molecules of the film. This ionic bombardment 
increases the effectiveness of etching, especially in the direction of 
bombardment, generally perpendicular to the film. Therefore more 
directional, i.e. more anisotropic, etching occurs than with pure plasma 
etching. RIE also tends to depend less on the material of the film, i.e., 
RIE provides less selectivity than pure plasma etching. In a typical RIE 
device the RF is at 13.56 MegaHertz (MHz), and a capacitor in the 
grounding line allows a negative charge to accumulate on the walls of the 
chamber and the on the wafer. The negative charge repels electrons in an 
adjacent region called a sheath, and accelerates positive ions and 
radicals toward the walls and wafer. 
Electron densities sufficient to produce ions and radicals can be achieved 
at low pressures by introducing a magnetic field that constrain the 
electrons to move in circular or helical trajectories as in MERIE. In ECR 
plasmas, the magnetic field strength is selected to produce a Lorenz force 
that causes circular or helical electron trajectories with a cyclotron 
frequency that matches the RF applied to the electrodes. In ECR plasmas, 
efficient coupling is obtained between the power applied to the electrodes 
and the energy given to the electrons. This is called resonant energy 
coupling, and usually uses a RF at 2.45 GigaHertz (GHz). 
Independent plasma generation and ion acceleration is achieved in the 
inductive coupled plasma sources. In these devices, electrons are excited 
to form a plasma by an RF magnetic field induced by applying RF power to a 
helical coil. The plasma is constrained in a plasma region by the RF 
magnetic filed. A process gas is introduced into the chamber and is 
ionized by the plasma. A separate bias voltage is applied to the wafer to 
accelerate the ions and radicals into the wafer at steep angles. To reduce 
acceleration of plasma and ions and radicals into the walls of the chamber 
by secondary electric fields produced by the coil as a byproduct of the RF 
magnetic field, an ESRF inductive coupled plasma source provides a slotted 
cylindrical conductor around the wall of the chamber as an electrostatic 
shield. The electrostatic shield prevents the accumulation of charge on 
the chamber walls by shorting the fields directed perpendicular to the 
wall, which cause a capacitive coupling, to ground. A solid electrostatic 
shield would also block the propagation of RF electromagnetic waves into 
the chamber. However those waves are needed to establish the axial RF 
magnetic field. Therefore the shield is slotted to allow the RF electric 
fields to propagate that support the axial RF magnetic field desired, and 
that block the waves that provide perpendicular RF magnetic fields. In 
this arrangement ions and radicals can be accelerated into the wafer with 
less acceleration into the walls of the chamber, and the ions and radicals 
can be accelerated with a power independent of the plasma generating RF 
power. As a result low energy ion bombardment and high pressure operations 
are possible. 
The desirability and efficiency of the plasma processes depend on many 
parameters such as the efficiency of electron excitation, the temperature, 
pressure and mix of gases that react with the electrons of the plasma to 
produce ions and radicals, the bias in the electric and magnetic fields 
that accelerate the ions and radicals onto the film, and the contaminating 
effects of plasma interactions with other surfaces in the plasma chamber 
such as the side walls of the plasma chamber. All these parameters can be 
varied almost continuously, so that extensive experimentation is required 
to determine what new combinations of parameters produce results that meet 
particular manufacturing design specifications. Such specifications 
include the selectivity for one film over another, the critical dimension, 
the aspect ratio of the resulting structures, the depth and steepness of 
the trench sides, i.e. the trench profile, and the etching rate. 
As the complexity and integration of semiconductor devices continue to 
increase beyond LSI, limitations in the existing etching methods, such as 
low selectivity, poor anisotropy, micro-loading, and the difficulty in 
identifying new combinations of parameters with desirable results, inhibit 
the productivity of a fabrication facility. These problems are especially 
severe in the etching of metallic films for forming fine contact holes. 
The problems become worse as the number of different metallic layers in a 
metallic film increases. 
The conventional processes for established semiconductor devices typically 
are not applicable to the new devices being designed and manufactured. As 
a result, the conventional etching processes cannot satisfy the modem 
trend toward highly-integrated semiconductor devices beyond LSI devices, 
and so these conventional etching processes limit the utility and 
reliability of fabrication facilities. 
SUMMARY OF THE INVENTION 
The present invention is directed to provide a method of etching metallic 
film on a semiconductor substrate in order to satisfy the manufacturing 
specifications for the modem, highly integrated semiconductor devices 
beyond large scale integration (LSI) devices. 
To achieve these and other advantages, there is provided a method of 
etching metallic film for a semiconductor device in which a semiconductor 
substrate with a metallic film exposed in a film pattern is inserted onto 
a chuck in a chamber of an electrostatic shielded radio frequency (ESRF) 
inductive-coupled plasma source, the ESRF inductive-coupled plasma source 
also including a coil connected to an upper electrode, a lower electrode 
connected to the chuck, a gas supply assembly, a pressure control assembly 
and a temperature control assembly. An etching gas is supplied to the 
chamber at a predetermined etch gas supply rate. Pressure inside the 
chamber is maintained at a predetermined pressure level. The upper and 
lower electrodes are powered with predetermined upper and lower powers, 
respectively, at predetermined upper and lower RFs, respectively. The 
chamber walls are cooled to a predetermined temperature. The metallic film 
is etched such that trenches in the metallic film are formed with 
predetermined trench qualities including a predetermined trench critical 
dimension no greater than a critical dimension associated with large scale 
integration. 
In other aspects of the method, the metallic film includes aluminum, and 
the etching gas includes chlorine supplied at a rate in a range from about 
30 cc/min to about 100 cc/min mixed with boron trichloride supplied at a 
rate less than about 100 cc/min. In still other aspects, a pressure is 
maintained at a predetermined pressure in the range from about 3 milliTorr 
(mTorr) to about 15 mTorr, and a temperature is maintained at a 
predetermined temperature in the range from about 30.degree. C. to about 
50.degree. C.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS 
The invention is here described in terms of examples including the 
preferred embodiment with reference to FIG. 1 and FIG. 2. 
FIG. 1 shows a chamber 1 of an electrostatically shielded radio frequency 
(ESRF) inductive-coupled plasma source. The source has a chuck 12 placed 
inside the chamber 1 for mounting a semiconductor substrate such as a 
wafer 10 in the chamber 1. The chuck 12 is electrically powered through a 
lower electrode (not shown). The chamber 1 has substantially concentric 
cylindrical inner wall 14 and outer wall 16. The chamber 1 has a gas 
supply assembly including a cover 18 attached to the top of the inner wall 
with holes a certain distance apart from each other to supply gases into 
the chamber 1. The chamber 1 also includes a floor (not shown) which is 
connected to the bottom of the inner wall 14. The cover 18, inner wall 14, 
and floor are connected so that a predetermined pressure can be maintained 
between them in a plasma region as part of a pressure control assembly. 
The inner wall 14 is formed with non-conductive material such as quartz or 
ceramic, or other insulating material; and the outer wall 16 is formed 
with conductive material. 
The chamber 1 also includes a helical coil 20 powered through an upper 
electrode (not shown). The helical coil is disposed in the space between 
the inner wall 14 and the outer wall 16 so that the central axis of the 
coil is substantially concentric with the central axis of the inner wall 
14 and the outer wall 16. 
An electrostatic shield 22 is installed in the inner wall 14. Also 
installed between the inner wall 14 and the outer wall 16, below the coil 
20, is a cooler 24 in contact with the inner wall 14 to cool the inner 
wall 14, as part of a temperature control assembly. 
The plasma is formed in the plasma region of the chamber of the ESRF 
inductive-coupled plasma source. Gas, such as etching gas and supplemental 
gas, is supplied through the holes of the cover 18 to provide both 
electrons for the plasma and ions and radicals for etching the film on the 
wafer 10. The upper electrode and the lower electrode 26 are driven at 
specified RFs, for example, both at 13.56 Mega Hertz (MHz). The coil RF 
power supplied to the upper electrode excites the electrons to escape the 
molecules of at least one species of the gases (either one species of the 
etching gas or one of the supplemental gas) thus forming the plasma. The 
coil RF power also constrains the electrons to orbit in a plasma region 
away from the chuck 12. The electrons of the plasma then interact with 
other species of the etching gas to form ions and radicals. The chuck RF 
power supplied to the lower electrode then accelerates the ions and 
radicals onto the semiconductor substrate such as the wafer 10 to etch 
trenches into the exposed metal film. 
The ESRF inductive-coupled plasma source allows the user to establish 
predetermined pressures and temperatures of operation that can 
significantly affect etching rates and selectivity. Predetermined 
temperatures are attained by cooling using the cooler 24 disposed between 
the inner wall 14 and the outer wall 16. The cooler 24 passes a cooling 
fluid such as liquid helium to absorb heat from the plasma region of the 
chamber 1 through the inner wall 14. 
The method of etching metallic film according to the present invention uses 
plasma formed by the ESRF inductive-coupled plasma source of FIG. 1 to 
etch a metallic film. Referring to FIG. 2, a metallic film may include 
several layers 34, 36 and 38 of different metals. A photoresist 40 is 
formed as an etching mask pattern on the metallic film layers 34, 36, 38, 
which themselves are deposited on an oxide film 32 on the semiconductor 
substrate 30. By properly choosing the etching gas, pressure, and 
temperature, the selectivity can be varied so that the various metallic 
layers are completely etched away while the photresist is not completely 
etched and the underlying oxide film is not substantially etched. The 
anistropy supplied by the ESRF inductive-coupled plasma source can be 
tuned by varying power to the upper and lower electrodes to allow one 
etching process to form deep trenches in several metallic layers of the 
metallic film with reduced undercutting so that steep sided profiles can 
be obtained. 
In example embodiments of the method of the present invention, the metallic 
film is an aluminum (Al) film. In the preferred embodiment, the metallic 
film is multi-layered with a layer of titanium (Ti) 34 underlying a layer 
of aluminum (Al) 36, itself underlying a layer of titanium nitride (TiN) 
38. In the example embodiments, the Al film 36 includes about 0.8% to 1.2% 
of silicon (Si) and may also include about 0.4% to 0.6% of copper (Cu). In 
the preferred embodiment, the Al layer 36 has 0.8 to 1.2% of Si but 
substantially no copper. 
In the preferred embodiment, the main etching gas is a mixture of boron 
trichloride (BCl.sub.3) gas and chlorine (Cl.sub.2) gas; but, Cl.sub.2 gas 
could be used alone. According to an embodiment of the present invention, 
the BCl.sub.3 gas is supplied at a rate less than about 100 cubic 
centimeters per minute (cc/min), and the Cl.sub.2 gas is supplied at a 
rate of about 30 to 100 cc/min. In the preferred embodiment, BCl.sub.3 gas 
and Cl.sub.2 gas are supplied at the rate of 80 cc/min each. These etching 
gases become electrolytic dissociated in the plasma and the electrolytic 
ions and radicals react chemically with the metallic film. 
Nitrogen (N.sub.2) gas can be supplied as a supplementary gas, besides the 
main etching gas, and at a rate of about 5 to 30 cc/min. It is supplied at 
the rate of 10 cc/min in the preferred embodiment. The role of the 
supplementary gas is to provide electrons for the plasma or to bind with 
the chemical products of etching to form chemical species that can be more 
easily removed from the wafer than the chemical products of etching 
themselves. The supplementary gas can reduce the effects of microloading. 
According to another embodiment of the present invention, the etching 
process is carried out at low pressures with the pressure maintained at a 
predetermined level in the range from about 3 to 15 milliTorr (mTorr). In 
the preferred embodiment, the predetermined pressure is maintained at 
about 5 mTorr. The low pressure is maintained to prevent loss of 
bombarding energies of the ions and radicals by reducing interactions 
between gas molecules and to evacuate products of the reactive etching. 
According to another embodiment of the present invention, the etching 
process is performed at a temperature in the range from about 30 to 
50.degree. C., by cooling. In the preferred embodiment, the temperature is 
cooled to about 40.degree. C. by passing liquid helium through the cooler 
24. 
In another embodiment of the present invention, the power applied to the 
upper electrode can be greater than the power applied to the lower 
electrode. The source power applied to the upper electrode should be in 
the range from about 700 to 3500 W, and the bottom power applied to the 
lower electrode should be less than 500 W. In the preferred embodiment, 
the source power is about 800 W, and the bottom power is about 120 W. 
The present invention provides the conditions for forming trenches in all 
layers 34, 36, 38 of the multi-layered metallic film including aluminum, 
without etching away the photoresist, without too much diluting of the 
reactive agents, and without contamination from the inner wall 14. That 
is, trenches can be formed that meet the design specifications for 
critical dimension, anisotropy, trench profile, selectivity, and 
micro-loading. Thus the etching process of the present invention satisfies 
the design specifications to fabricate the fine patterns of modern, highly 
integrated, complex semiconductor devices. 
Now the functions and effects of a concrete embodiment of the present 
invention are illustrated in detail with reference to FIG. 2. First, the 
oxide film 32 is deposited on the semiconductor substrate 30 of a wafer 
10, and then the Ti layer 34, the Al layer 36, and the TiN layer 38 of the 
metallic film are successively deposited. In order to form a designed 
pattern of trenches in the metallic film, a photoresist 40 layer is formed 
on the TiN layer 38, the uppermost metallic layer, and then 
photolithography is carried out on the photoresist to form an etching mask 
that exposes the metallic film in the designed pattern. 
Then the metallic film etching process operates on the exposed metallic 
film 34, 36, 38 as patterned. The wafer 10 with the semiconductor 
substrate 30, oxide layer 32, and metallic film 34, 36, 38 is mounted in 
the chamber 1 on the chuck 12. A plasma is formed in the chamber of an 
ESRF inductive-coupled plasma source with the source power (i.e. an upper 
power) of the upper electrode at 800 W, and the lower power of the lower 
electrode at 120 W. Then the main etching gas, a mixture of BCl.sub.3 gas 
and Cl.sub.2 gas each supplied at the rate of 80 cc/min, is introduced 
into the chamber 1. At the same time, supplementary N.sub.2 gas is 
supplied at the rate of 10 cc/min. The chamber is maintained at a pressure 
of 5 mTorr and cooled to a temperature of 40.degree. C. In order to 
maintain 40.degree. C. of temperature, the chamber 1 uses a cooler 24 with 
liquid helium (He) supplied with 12 Torr of pressure. 
Accordingly, Cl ion and Cl radical are generated from the ionized chlorine 
gas by the plasma. The Cl radical reacts with the layers 34, 36, 38 of the 
metallic film in order to etch through all three layers. In addition, the 
BCl.sub.3 gas is also ionized by the plasma and reacts with the layers 34, 
36, 38 of the metallic film in order. The N.sub.2 gas controls the etching 
rate during the etching process and improves the profiles of the pattern 
formed by the etching process. 
The specific conditions described for the concrete example are considered 
optimum for the anisotropic etching of a metallic film having layers of 
titanium, aluminum, and titanium nitride using a patterned photoresist as 
a mask. If the etching process is carried out within the wider ranges of 
the processing conditions for the present invention, as described 
preceding the concrete example, the present invention should satisfy 
modern specifications of an etching process for a multi-layered metallic 
film, including selectivity and anisotropy, at critical dimensions smaller 
than those associated with LSI devices. 
Therefore, the present invention can be effectively applied during modern, 
more highly integrated semiconductor device fabrication that is more 
demanding in terms of the critical dimension of fine patterns formed, and 
more complex in terms of design specifications. Thus the present invention 
provides increased reliability for modern semiconductor device 
fabrication. 
While the present invention has been described in detail, it should be 
understood that one of ordinary skill in the art can make various changes, 
substitutions and alterations without departing from the spirit and scope 
of the invention as defined by the appended claims and their equivalents.