1. Field of the Invention
The invention relates to a gas flow device and, more particularly, to a gas flow device for controlling the flow of gases from a gas source into a process chamber.
2. Description of the Related Art
Many of the processes used in the manufacturing of integrated circuits are performed at sub-atmospheric pressures in dedicated systems called process chambers. These systems typically incorporate vacuum pumps to maintain a desired process pressure range, and are coupled to a gas distribution system which supplies the gaseous chemicals required for specific processes. Such processes include deposition (CVD, PECVD, LPCVD, ALD, or PVD, for example) or ion implantation (beam line ion implantation, plasma doping ion implantation, or plasma immersion ion implantation). Gaseous chemicals are typically stored in superatmospheric pressure cylinders, each having a dedicated pressure regulator. In certain cases, cylinders may be at sub-atmospheric pressure (as in so-called Safe Delivery System® products). Additionally, certain materials, such as organo-metallic compounds, may be sublimated or otherwise gasified from either solid or liquid materials.
Gases are typically fed into a gas distribution manifold for communication to a specific process chamber or chambers on demand. This manifold is connected to one or more outlets which contain metering valves to control the flow of gaseous material to its point of use. The characteristics of this metering valve largely determines the instantaneous downstream pressure of the process chamber. An ideal gas metering technology would enable process pressure accuracy (match of actual process pressure to user set point value), repeatability, stability, and fast response to fluctuations in upstream pressure, also an important aspect of stability.
The most common type of metering valve for many applications is the mass flow controller (MFC). MFC's are readily available in multiple flow ranges, are relatively inexpensive, and have a small footprint. Conventional MFC's regulate flow by measuring the heat transferred to a volume of gas by a heater element; they are therefore calibrated for the heat capacity of a specific gas. This technology has certain inherent limitations, particularly for low flow (e.g., 0.2 sccm to 10 sccm) and low process pressure (e.g., 0.1 milliTorr to 100 milliTorr) applications, in that it is subject to drift, and is inherently slow, so that thermally-based MFC's cannot properly adapt to fast transients in inlet pressure. Therefore, a need exists for an improved gas flow device with fast transient response and improved stability.
U.S. Pat. No. 7,723,700 to Horsky et al., (“the '700 patent”) discloses a vapor delivery system for delivering a steady flow of sublimated vapor to a vacuum chamber. The vapor delivery system of the '700 patent includes a vaporizer of solid material, a mechanical throttling valve and a pressure gauge followed by a vapor conduit to the vacuum chamber. The vapor flow rate is determined by both the temperature of the vaporizer and the setting of the conductance of the mechanical throttle valve located between the vaporizer and the vacuum chamber. The temperature of the vaporizer in the '700 patent is determined by closed-loop control to a set-point temperature and the mechanical throttle valve is electrically controlled, e.g., the valve position is under closed-loop control (i.e., a feedback loop) based on the output of the pressure gauge. Additionally, according to col. 12 of the '700 patent, lines 59-63 states that the pressure at the outlet of the vaporizer (i.e., upstream of the throttle valve) is about 65 milliTorr. Thus, the pressure at the inlet of the control device of the '700 patent is much lower than is found at the outlet of a typical gas source or tank.
What is needed is a system device and method that can deliver a steady gas flow with gas received from a tank or a gas source at a typical or standard tank pressure. What is additionally needed is a system, device and method for delivering a steady gas flow that does not require closed-loop control of a temperature of the device to regulate gas flow. What is further needed is a gas flow device that can be easily interposed into the gas flow path between the gas source and a process chamber to improve stability of the gas flow.
In order to overcome the above-mentioned disadvantages of the heretofore-known devices of this general type, it is accordingly an object of the invention to provide a system for controlling the flow of gas from a gas source to a process chamber. A gas flow device is interposed into the gas flow between the gas source and the process chamber. In accordance with one particular embodiment of the invention, the gas flow device includes one or more pressure reduction devices, a controllable valve, a pressure gauge, and a control system that controls the valve in response to information received from the pressure gauge. The gas flow device provides a stable inlet pressure to the process chamber, thus minimizing pressure instabilities in the process chamber.
Additionally, a method is provided for producing a stable and well-defined pressure through closed-loop control of an adjustable valve or throttle valve using data obtained from a downstream pressure gauge. In one particular embodiment of the invention, a set point for a desired pressure, as measured at the downstream pressure gauge is selected. The measured pressure signal from the downstream pressure gauge is fed to the input of a control system, which compares the measured pressure signal with the set point value. Depending on the difference between the measured pressure signal and the set point value, the control system produces an error signal, which is used to generate an output or control signal to the adjustable value, to adjust the position of a throttling element of the valve in order to minimize the magnitude of the error signal.
Although the invention is illustrated and described herein as embodied in a gas flow system, device and method, it is nevertheless not intended to be limited to the details shown, since various modifications and structural changes may be made therein without departing from the spirit of the invention and within the scope and range of equivalents of the claims.
The construction of the invention, however, together with the additional objects and advantages thereof will be best understood from the following description of the specific embodiments when read in connection with the accompanying drawings.
Referring now to
In accordance with the present invention, a gas flow device 112 is disposed in the flow path between the gas source 110 and the process chamber 114. In one particular embodiment of the invention, the gas flow device 112 can be provided as a single or stand-alone unit encompassed in a housing 112a. Pressurized gas is received into the gas flow device 112 from the outlet of gas source 110, via a standard gas line connector 111. In one particular embodiment of the invention, the pressure P1 at the outlet of the gas source 110 is a standard or typical tank pressure, such as, but not limited to, 5 PSIG. The gas flow device 112 reduces the gas pressure such that gas exits a gas line connector 113, connected to an inlet of the process chamber 114, at a reduced pressure P4.
Referring now to
In the particular embodiment of
Downstream of the pressure regulator 107 of the gas source 110, the pressure is further reduced to a pressure P2 by pressure reduction device 116, which is a conductance limitation having a conductance C1. For example, the pressure reduction device 116 is configured in one embodiment of the invention to have a conductance C1, such that the pressure P2 may be between 1 Torr and 100 Torr. In one embodiment of the invention, the pressure reduction device 116 may be a long, narrow pipe (illustrated as a ‘loop’ in
An electrically-adjustable or controllable metering or throttle valve (V2) 118 is disposed downstream of the pressure reduction device 116. The valve 118 is selected to be a high-conductance valve having a dynamic range of between 3 and 100, for example. That is, when in a flow condition, valve 118 will reduce the pressure P2 by between 3 and 100 times, to a pressure P3. The pressure P3 downstream of the valve 118 is measured by the pressure gauge (G3) 120. pressure gauge 120 is, preferably, selected to measure the pressure P3 with excellent reproducibility and low signal-to-noise ratio. Pressure gauge 120 can be selected to provide optimized performance in the useful pressure range P3. This is of note since gauges are typically configured to operate best within a given pressure range. The output signal from the pressure gauge 120 is interpreted by a control system 124 to adjust the conductance of the adjustable valve 118. In one particular embodiment of the invention, the valve 118 is electrically adjustable, for example by an electric motor which moves a throttling element of the valve 118 to set a particular conductance of the valve 118.
The control system 124 can include a computer, microprocessor and/or microcontroller configured by software stored in memory and executable by the computer, microprocessor and/or microcontroller to execute the steps of the method discussed herein. Alternately, the control system 124 can include hardware hardwired to perform the steps of the method of the invention. In one particular embodiment of the invention, the control system 124 is configured by software and/or hardware to receive a pressure value for the pressure P3 from the pressure gauge 120 at an input 126 to the control system 124 and process the pressure value to control the state of, and correspondingly the conductance of, the adjustable valve 118, based on an output 128 from the control system 124.
Downstream of the pressure gauge 120 is another pressure reduction device 122 having a conductance C2. In the present preferred embodiment, the conductance C2 is a fixed conductance C2, although a variable conductance device could be used, if desired. As can be seen from
By selecting appropriate conductance values C1 and C2, a broad range of process chamber pressures can be produced. The values for C1 and C2 can be optimized to deliver a desired range of pressures P4 to the process chamber 114. Additionally, the conductance values C1 and C2 can be selected before assembly of the gas flow device unit, so as to permit operation in a pre-selected range of gas pressures. If desired, the gas flow device 112 can be configured to permit the pressure reduction elements 116, 122 to be demountable from the gas flow device assembly, and replaced by different fixed or variable pressure reduction elements having different conductance values or ranges.
According to the present invention, four distinct pressure values can be defined in connection with the gas flow device 112:
A fifth pressure, P5, can be found in the process chamber 114. The purpose of gas flow device 112 is to provide a variable, but stable, pressure P4 at its outlet, which is the inlet of the process chamber 114. One exemplary configuration of a process chamber 114 will be described in connection with
Although
Referring now to
Typically, transport magnet 213 disperses ion beam 219 according to the mass-to-charge ratio of the ions, such that unwanted ions can be prevented from reaching the wafer or substrate 215 by a simple aperture plate located between transport magnet 213 and wafer or substrate 215. The gas pressure within ionization chamber 205 is typically between 0.1 mTorr and 10 mTorr, depending on the type of ion source used by the ion implanter. In certain cases, however, the pressure may be substantially higher or lower. Although the pressure within the ionization chamber 205 of the ion source is in the milliTorr range, the pressure within the surrounding vacuum chamber 217 is typically at least an order of magnitude lower. This reduced pressure is meant to preserve the ion beam during transport, and also to maintain high electric fields without unwanted electrical discharges.
Referring now to
One goal of this invention is to produce a stable and well-defined pressure P3. This is accomplished through closed-loop control of throttle valve 118 using data obtained from the downstream pressure gauge 120. One particular method 200 for setting the pressure P3 will now be described in connection with
Referring now to
The following examples serve to illustrate the utility of the invention only, and are not meant to limit the invention to only the values given in the examples. The effects of turbulence, viscous versus molecular flow, and transitions between flow regimes will depend on the properties and geometries of the components which are selected to provide the desired characteristics of C1, C2 and V2, as described herein, and indeed how they are physically coupled.
An implanter ion source receiving a volumetric flow of process gas of 2 sccm at an ion source pressure of 1 mTorr. The gas inlet to the ion source is a long thin pipe with a conductance C of 5×10−2 L/s. The gas source is a high-pressure cylinder regulated down to 5 psig.
P1: 5 psig
P5: 1 mTorr
C: 5×10−2 L/s
Q: 2 sccm=2.5×10−2 Torr-L/s.
We use the relation
C=Q/(P4−P5) (1)
to determine P4 from a known C and Q. Thus,
P4=Q/C+P5. (2)
For such a small conductance C, the pressure drop is substantial, so that P5<<P4. Thus,
P4˜Q/C. (3)
Therefore, P4 is about 0.5 Torr. Choosing a finite value of C2 will only serve to increase the operating pressure of V2. For this example, assume that C2 is large, so that P3˜P4. This embodiment is shown in
If V2 is a throttle valve with a useful dynamic range of 20, then P2 (the inlet pressure to V2) can be between about 10 Torr and 0.5 Torr. This range is somewhat dependent on the finite conductance of V2 in its fully open position, but we note that in practice, the conductance dynamic range of V2 can be accurately measured.
With the range of P2 thus defined, C1 is required to reduce the pressure from 5 psig (approximately 1000 Torr) to approximately 5 Torr (the middle of V2's useful control range for P2). This factor of 200 in pressure reduction can be accomplished by either a variable-conductance valve, for example if adjustability is required, or a fixed pressure reducer, such as a long thin pipe as shown in
Using the form of Equation (1), we find that the required conductance for C1 is:
C1=Q/(P1−P2). (4)
Inserting the values Q=2.5×10−2 Torr-L/s, P1=1000 Torr, and P2=5 Torr, we have
C1˜2.5×10−5 L/s. (5)
Implanter ion source receiving a volumetric flow of process gas of 0.2 sccm with ion source pressure of 1 mTorr. The gas inlet to the source is a long thin pipe with a conductance of 5×10−2 L/s. The gas source is sub-atmospheric gas cylinder providing a delivery pressure of 500 Torr.
P1: 500 Torr
P5: 1 mTorr
C: 5×10−2 L/s
Q: 0.2 sccm=2.5×10−3 Torr-L/s.
This example is similar to Example 1 except for the sub-atmospheric delivery pressure of the gas source and the volumetric flow, so we will use the embodiment of
P4=P3˜Q/C (6)
P3=50 mTorr. (7)
If V2 is a throttle valve with a useful dynamic range of 20, then P2 can be between about 1 Torr and 50 mTorr. Thus, we choose P2 to be centered about the useful range of V2:
P2=0.5 Torr. (8)
Again using Equation (1), we find that the required conductance for C1 is:
C1=Q/(P1−P2). (9)
Inserting the values Q=2.5×10−3 Torr-L/s, P1=500 Torr, and P2=0.5 Torr, we have
C1˜5×10−6 L/s.
An alternative solution to example 2 can be realized by using the embodiment of
P1: 500 Torr
P4: 50 mTorr
P5: 1 mTorr
C: 5×10−2 L/s
Q: 0.2 sccm=2.5×10−3 Torr-L/s.
For example, we can choose
C2=1×10−4 L/s,
yielding
P3=25 Torr.
Thus, V2 can operate from about 25 Torr to about 500 Torr. Selecting the approximate midpoint of this pressure range,
P2=250 Torr.
To calculate the required conductance C1 between the gas source and V2,
C1=Q/(P1−P2).
Inserting these values yields
C1=1×10−5 L/s.
Thus, we see that in this example, incorporating a finite conductance C2<C increases the required conductance of C1.
Process chamber receiving a volumetric flow of process gas of 100 sccm at a process pressure of 100 mTorr. The process chamber gas inlet has a conductance of 0.5 L/s.
P1: 5 psig
P5: 100 mTorr
C: 0.5 L/s
Q: 100 sccm=1.3 Torr-L/s
Using the same approach as used in example 1, we use embodiment 2; that is, we set
P3=P4. (16)
We calculate the expected values of P3, P2, and C1:
P3=Q/C+P5. From Eq. (2),
Substituting the values above,
P3=2.7 Torr.
If we select a throttle valve V2 with a dynamic range of at least 20, then P2 should be in the approximate range 2 Torr to 40 Torr. With the range of P2 thus defined, V1 is required to reduce the pressure from 5 psig (approximately 1000 Torr) to approximately 20 Torr (in the middle of the useful control range for P2). This factor of 50 in pressure reduction can be accomplished by either a variable-conductance valve, for example if adjustability is required, or a fixed pressure reducer, such as a round pipe with entrance and exit apertures, as shown in
Again using Equation (1), we find that the required conductance for V1 is:
C1=Q/(P1−P2). (18)
Inserting the values Q=1.3 Torr-L/s, P2=20 Torr, and P1=1000 Torr, we have
C1˜1.3×10−3 L/s. (19)
Accordingly, while a preferred embodiment of the present invention is shown and described herein, it will be understood that the invention may be embodied otherwise than as herein specifically illustrated or described, and that within the embodiments certain changes in the detail and construction, as well as the arrangement of the parts, may be made without departing from the principles of the present invention as defined by the appended claims.
The present application claims priority to co-pending Provisional Patent Application No. 61/629,058 filed on Nov. 12, 2011, entitled “Gas Flow Device”; that application being incorporated herein, by reference, in its entirety.
Number | Date | Country | |
---|---|---|---|
61629058 | Nov 2011 | US |