Patent Description:
Plasma processing tools can be used in the manufacture of devices such as integrated circuits, micromechanical devices, flat panel displays, and other devices. Plasma processing tools used in modern plasma etch applications are required to provide a high plasma uniformity and a plurality of plasma controls, including independent plasma profile, plasma density, and ion energy controls. Plasma processing tools can, in some cases, be required to sustain a stable plasma in a variety of process gases and under a variety of different conditions (e.g., gas flow, gas pressure, etc.).

<CIT> describes a method of improving plasma processing of a semiconductor wafer by exposing the wafer or the plasma to photons while the wafer is being processed. One embodiment of the method comprises the steps of etching an aluminum layer and, during the etching, exposing the semiconductor wafer containing the aluminum layer to photons that photodesorb copper chloride from the surface of the layer thus improving the etch process performance.

<CIT> describes a microwave plasma processing apparatus which enables fast and easy plasma ignition at the pressure for plasma processing. In the microwave plasma processing apparatus, a plasma ignition facilitating unit is provided to facilitate plasma ignition induced by a microwave. The plasma ignition facilitating unit includes a deuterium lamp that emits vacuum ultraviolet rays, and a transmission window that allows the vacuum ultraviolet rays to penetrate and irradiate a plasma excitation space.

<CIT> describes an implantation chamber which defines a chamber interior into which one or more workpieces can be inserted and includes a conductive inner wall portion in proximity to the chamber interior. A conductive workpiece support extends into an interior region of the implantation chamber. A conductive electrode is disposed within said implantation chamber relative to said conductive workpiece support to allow workpieces to be placed on the workpiece support in a region between the support and the conductive electrode. <CIT> relates to plasma enhancement in a plasma glow system by increasing the number of photoelectric electrons in the plasma glow by producing photoelectrons from the surface of a target. This is accomplished by flooding the surface of the target with a UV laser beam during the plasma process where emitted photoelectrons are injected into the plasma to increase the plasma density. <CIT> discloses a CVD apparatus comprising a mechanism for charging particles by means of a photoelectron emitter and an ultraviolet lamp. An ultraviolet ray from the ultraviolet lamp is irradiated onto the photoelectron emitter to emit photoelectrons. <CIT> discloses a plasma processing apparatus comprising a UV generation means that generates UV rays at the time of plasma ignition through a transmission window. UV radiation is introduced into the processing chamber. Therefore, the ionization of the gas in the processing chamber is promoted by the electromagnetic wave, and the plasma is easily and quickly ignited even under a low pressure condition.

One example aspect of the present disclosure is directed to a plasma processing apparatus. The plasma processing apparatus includes a plasma chamber. The plasma processing apparatus includes a dielectric wall forming at least a portion of the plasma chamber. The plasma processing apparatus includes an inductive coupling element located proximate the dielectric wall. The plasma processing apparatus includes an ultraviolet light source configured to emit an ultraviolet light beam onto a metal surface that faces an interior volume of the plasma chamber. The plasma processing apparatus includes a controller configured to control the ultraviolet light source.

Variations and modifications can be made to example embodiments of the present disclosure.

A full and enabling disclosure to one of ordinary skill in the art is set forth more particularly in the remainder of the specification, including reference to the accompanying figures, in which:.

Example aspects of the present disclosure are directed to plasma processing apparatus and associated methods for enhancing ignition of inductively coupled plasmas, and in some embodiments electrostatically shielded inductively coupled plasmas. Ignition of inductively coupled plasma (also referred to as inductively coupled plasma striking) can be improved with an ultraviolet light source that emits an ultraviolet light beam onto a dielectric wall and/or a metal surface at a location proximate the plasma prior to or during ignition of the plasma (e.g., from a location outside of the plasma chamber). As such, less RF power can be used to ignite (also referred to as strike) the plasma in less time, with better igniting repeatability and reducing ion bombardment of a dielectric window.

In some example plasma sources, inductive plasma sources with reduced capacitive coupling (e.g., due to electrostatic shielding) can have substantial advantages over other inductive sources that are common in semiconductor processing. Such plasma sources with reduced capacitive coupling can have: (<NUM>) reduced ion bombardment and sputtering of interior dielectric and metal walls of the plasma source; (<NUM>) reduced plasma potential and improved ion optics for extraction; (<NUM>) increased lifetime of source components and improved cleanliness due to reduced wear and roughening of inner surfaces. Conventional plasma sources with reduced capacitive coupling (due to electrostatic shielding, RF frequency or coil configuration) can have intermittent and/or slow ignition of the plasma due to a reduced electric field in a plasma chamber (also referred to as a plasma vessel). Conventional plasma sources can use much higher radio frequency (RF) power and coil voltage to achieve reliable plasma ignition, particularly when higher gas pressures such as above about <NUM> mTorr are used. However, higher RF power, higher coil voltage and/or higher gas pressures cannot always yield reliable ignition, and can often have detrimental side effects such as arcing and localized sputtering of dielectric walls.

In some example plasma sources, a smaller supplemental electrode can be used in a processing chamber of a conventional plasma processing apparatus providing RF power until ignition is achieved. However, such ignition approaches can cause sputtering of the electrode or wall adjacent the electrode resulting in contamination and/or surface roughening that can lead to particle contamination.

According to example aspects of the present disclosure, an ultraviolet light source can be operated to illuminate an inner wall of a plasma chamber such that a larger number (e.g., greater than about <NUM><NUM>) of free electrons can be ejected from the illuminated wall into a gas in the plasma chamber to substantially enhance a rate of initial exponential growth of the plasma with the substantially inductive coupling of the plasma source. The ultraviolet light source can be used to reduce and make more consistent ignition time of the plasma, even at reduced RF power levels. Thus, for inductively coupled plasma sources (e.g., induction coil or antenna) with reduced capacitive coupling (e.g. due to presence of electrostatic shield or other feature), ignition enhancement can be provided using an ultraviolet light source in a plasma chamber.

In some embodiments, one or more ultraviolet light sources (e.g., a lamp or lamps) can be mounted external to a plasma chamber for an inductively coupled plasma source such that the radiation from the ultraviolet light source(s) can illuminate an inner wall (e.g., dielectric wall and/or metal wall) of the plasma chamber. The wall can have direct line of sight to the plasma chamber. For instance, there are no structures blocking a path (e.g., line of sight path) between the wall and an interior of the plasma chamber where the plasma is generated.

The ultraviolet light source(s) can have substantial portion of its output (e.g., ultraviolet light beam) as electromagnetic radiation (EM) radiation below about <NUM> nanometers (nm) wavelength, down to about <NUM> wavelength.

In some embodiments, an electrostatic shield can be located between a dielectric wall, which forms at least a portion of the plasma chamber and the inductively coupled plasma source. In some embodiments, the ultraviolet light source(s) can be located adjacent a window such that one or more ultraviolet light beams from the ultraviolet light source(s) can pass through the window to reach an inner wall of the plasma chamber. For instance, the window can have at least one of: synthetic quartz, UV-grade sapphire, magnesium fluoride (MgF<NUM>) material, or calcium fluoride (CaF<NUM>) material. A space between the ultraviolet light source(s) and the window can be filled with an inert gas to reduce absorption by atmospheric oxygen. The inert gas can include at least one of: helium, neon, argon and/or nitrogen.

In some embodiments, the ultraviolet light source(s) can be operated in a pulsed mode or turned on just before or during initiation of RF power introduction to an inductively coupled plasma source. Radiation from the ultraviolet light source(s) can be maintained at least until the plasma attains some minimal fraction of its ultimate density. In some embodiments, the radiation can be aimed at one or more interior wall areas that are proximate to an exterior inductively coupling element.

According to example aspects of the present disclosure, an inductive plasma source of the type having superior suitability for ultra-clean semiconductor processing can include low wall sputter and low plasma contamination. The disclosed inductive plasma source can substantially improve reliability and speed of plasma ignition while also having superior cleanliness. For instance, a plasma processing apparatus can include a plasma chamber (e.g., an evacuated vessel), a dielectric wall forming at least a portion of the plasma chamber, and an inductive coupling element (e.g., an inductive coupled plasma source, such as an induction coil or an antenna) located proximate the dielectric wall. The inductive coupling element can be connected to a supply of RF power. The plasma processing apparatus can further include a controllable supply of process gas to the plasma chamber interior, and a separately controllable source of ultraviolet radiation (e.g., one or more ultraviolet light beams).

In some embodiments, a plasma processing apparatus can be configured such that a substantial fraction of an ultraviolet radiation from an ultraviolet source can have a line of sight through an at least partially ultraviolet-transparent window in a plasma chamber. The ultraviolet radiation can intercept at least a portion of an interior surface of the plasma chamber such that the ultraviolet radiation can be absorbed on surfaces adjacent plasma when in operation (e.g., in a plasma region). In some embodiments, the ultraviolet light source can have instantaneous power of several Watts or more of radiation emission during operation of which at least <NUM>% and preferably <NUM>% or more is in a hard-ultraviolet band, e.g., in a wavelength range of about <NUM> nanometers to about <NUM> nanometers, such as a wavelength range of about <NUM> nanometers to about <NUM> nanometers. The ultraviolet light source can be a lamp that is separate and isolated from an inductive coupling element. In some embodiments the ultraviolet light source can employ a gas or gases that produce radiation in the hard-ultraviolet band (Wavelength less than about <NUM>). The ultraviolet light source can be turned on or the ultraviolet light source can start pulsing to illuminate a part of an interior surface of the plasma chamber, prior to or simultaneous with a turning-on of RF power to ignite a plasma in the plasma chamber. As such, reliability of ignition and growth of the plasma can be accelerated and improved.

In some embodiments, the inductive coupling element (e.g., an antenna for inductive coupling of RF power to plasma) can have reduced capacitive coupling to dielectric walls of the plasma chamber, and to plasma during operation. In some embodiments, the inductive coupling element can be separated by a substantial physical gap from a dielectric portion (e.g., a dielectric wall) of the plasma chamber such that capacitive coupling of the inductive coupling element to plasma can be reduced. In some embodiments, the inductive coupling element can be located at a distance greater than a radius of the inductive coil. In some embodiments, those part(s) of the inductive coupling element that are physically closest to the dielectric portion of the plasma chamber can be grounded, or connected through a tunable reactance that can have low impedance (e.g., less than about <NUM> Ohms) to electrical ground.

In some embodiments, the plasma processing apparatus can further include one or more pieces of conducting material that can be interposed partially or fully between the inductive coupling element and the dielectric portion of the plasma chamber. The one or more pieces of conducting material can be connected electrically, either directly or through a tunable circuit, to ground thereby forming electrostatic shielding that mitigates capacitive coupling of the inductive coupling element to the plasma. As such, plasma potential can be reduced and energy of ions bombarding the plasma chamber wall can be reduced.

In some example conventional plasma processing apparatus, capacitive coupling of an inductive coupling element to plasma can be sufficiently weak so that normal plasma ignition can become unreliable or require too much time, e.g., during which electrical stresses are often large in RF power components and electric fields large near the inductive coupling element. This slow ignition can be generally the case because inductive discharges generally start in the "E" mode where capacitive coupling initiates the breakdown and then transitions to the "H" mode wherein the inductive coupling takes over sustaining the plasma as it provides the majority of power for electrons doing ionization. In conventional inductive plasma processing apparatus, capacitive electric fields can be larger but more localized than the inductive electric fields.

According to example aspects of the present disclosure, the plasma processing apparatus can have various features for mitigation of capacitive coupling from the inductive coupling element to the plasma, while successfully igniting plasmas rapidly and consistently without employing much higher RF current and RF power levels to the inductive coupling element than those employed for the conventional plasma processing apparatus in steady state operation. In some embodiments, ultraviolet radiation from the ultraviolet light source can promote plasma ignition and growth by ejecting photo-electrons from an irradiated surface(s) into dilute gas proximate what will be a plasma region (once ignited) as RF power is applied to the inductive coupling element. These electrons can then be accelerated by electrical fields in the plasma region to cause ionization of the gas in the plasma chamber. The ionization can then provide additional electrons that take part in "avalanche" of ionization which forms the plasma. In some embodiments, a plasma-facing surface irradiated with the ultraviolet radiation can be a part of a dielectric or metal wall of the plasma chamber. The dielectric or metal wall can have substantial induction electric fields when RF power is being provided. In some embodiments, the ultraviolet irradiated surface can be a metal surface on an interior of the plasma chamber that has a line of sight to the plasma region.

In some embodiments, metal surfaces that are not electrically floating (e.g., are electrically grounded) are desired since they do not charge up so as to prevent electron emission as electrons are ejected from the surface. Further, the energy required for electron photo-emission is less in conducting materials than in insulating materials since conduction band electrons require less energy to be ejected than valence band electrons from solids. Further, metal walls do not charge-up resulting in trapping of emitted electrons as insulating materials can do.

In some embodiments, ultraviolet light sources for promotion of plasma ignition can have total instantaneous radiation output of about <NUM> Watt or more with output emission spectrum having at least <NUM>% of power in the hard-ultraviolet band (e.g., in a wavelength range less than about <NUM> nanometers). Examples of such ultraviolet light sources can include Xenon flashlamps, Deuterium lamps, excimer lamps or other any suitable light sources that meet the above features. In some embodiments, a window in the plasma chamber can be made of material transmissive of hard-ultraviolet radiation. The window can have at least one of synthetic quartz, UV-grade Sapphire, or more highly UV transmissive materials such as MgF<NUM> or CaF<NUM>. In some embodiments, the window can be a vacuum window with atmospheric pressure gas around the ultraviolet light source. For instance, a space between the ultraviolet light source and the window can be filled with an inert gas (e.g., helium, argon, neon, and/or nitrogen) to reduce absorption by atmospheric oxygen.

In some embodiments, the hard-ultraviolet band of the ultraviolet light source can include a wavelength range that between about <NUM> nanometers and about <NUM>. This band can be referred to as "Vacuum Ultraviolet" (VUV), since these wavelengths are strongly absorbed by oxygen, such as in oxygen in air. In some embodiments, the ultraviolet radiation can have <NUM>% or more its electromagnetic radiation output in a VUV part of a spectrum of the ultraviolet light source. The instantaneous output power in the hard-UV band at the time of plasma ignition can be about <NUM> Watt or more. This photon energy can be helpful because the photo-emission of an electron from an insulator requires such photon energy that it can raise a valence electron past the conduction band and into the free electron energy space. For photoemission from metal, photon energy from the ultraviolet light source can raise an electron from a conduction band to a free state. In some embodiments, the photo-electron emission from the interior surface of the plasma chamber can include at least <NUM> electrons. To reduce heat buildup in an ultraviolet light source(s) (e.g., lamp), the ultraviolet light source can be pulsed with multiple very short pulses at short intervals (e.g., less than about <NUM> milliseconds and preferably less than <NUM> milliseconds). The ultraviolet light source can start pulsing prior to or just following the time of initiation of RF power supplied to the inductive coupling element. In some embodiments, the ultraviolet radiation pulses can have a frequency of at least about <NUM> per second so that a UV radiation pulse will occur within about <NUM> milliseconds after the electric field strength is capable of initiating breakdown thereby reducing the total time at high level RF power for the ignition process.

In some embodiments, the ultraviolet light source can be a xenon arc flashlamp with an ultraviolet window or a VUV window that produces ultraviolet light in the hard-ultraviolet band or in the VUV band. In some embodiments, the xenon arc flashlamp can be small (e.g., less than or about <NUM> inch for all dimensions). In some embodiments, the xenon arc flashlamp can be a high-pressure arc lamp that can pulse up to about <NUM> Hertz (Hz) and operate at an average power level less than about <NUM> Watts. In some embodiments, an arc lamp can produce strong continuum radiation down to about <NUM> nanometers in wavelength. In some embodiments such a small flashlamp might be positioned within the volume where the gas pressure is low and the plasma would otherwise occupy. Such a small flashlamp might be "plugged-in" within the plasma chamber, in some embodiments in a recessed volume embedded into a metal or dielectric structure. The arc lamp can have pulse energy about <NUM> millijoules (mJ) to produce at least about <NUM><NUM> hard-ultraviolet photons per pulse with the photoelectron efficiency of at least about <NUM>% producing orders of magnitude of more photoelectrons than needed.

In some embodiments, the ultraviolet light source can be a deuterium VUV lamp with MgF<NUM> window. The deuterium VUV lamp can be a high-pressure deuterium arc lamp with radiation substantially in a band at about <NUM> nanometers. The high-pressure deuterium arc lamp can be a continuous wave (CW) VUV source, not pulsed. In some embodiments, there is an about <NUM> seconds warm-up time for these lamps, so it is important to turn the deuterium VUV lamp on about <NUM> seconds to <NUM> seconds before ignition is desired and off in synchrony with plasma reaching a full power. Provision should be made for cooling such a lamp since continuous operation produces substantial heat. Life of such lamp can be at least about <NUM> hours, which can be adequate for about <NUM>,<NUM> ignitions, which can be adequate for at least about <NUM> months of <NUM> x <NUM> process operation.

In some embodiments, the ultraviolet light source can be an excimer RF/pulse xenon lamp. For instance, the excimer xenon lamp can be a highly efficient source of about <NUM> nanometers radiation. The excimer xenon lamp can have long lifetime (e.g., longer than about <NUM>,<NUM> hours).

In some embodiments, the ultraviolet light source(s) for acceleration of plasma ignition can illuminate area(s) of the inner wall of the plasma chamber through a vacuum window of the plasma chamber. The vacuum window can be at least partially transparent to ultraviolet radiation. In some embodiments, the vacuum window can be highly transmissive of ultraviolet light such as MgF<NUM>, CaF<NUM> or similar materials. In some embodiments, the vacuum window can have materials such as "synthetic quartz" materials that have better UV transmission than natural or conventional quartz down to wavelengths of about <NUM>. Such window materials can have at least <NUM>% transmission of ultraviolet light in a wavelength range of from about <NUM> nanometers to about <NUM> nanometers. In some embodiments, the ultraviolet light source can be mounted adjacent or near to the vacuum window in a vacuum wall (e.g., a dielectric part of the vacuum wall, and/or a metal part of the vacuum wall) of the plasma chamber. In some embodiments, a space between the ultraviolet light source and the vacuum window can be purged or filled with helium or nitrogen to reduce UV loss due to absorption by atmospheric oxygen.

In some embodiments, ultraviolet radiation from the ultraviolet light source can be incident on a surface on the inside of the plasma chamber. The surface in some embodiments can be adjacent a volume with substantial induction electric field such that photoelectrons can provide a substantial density in the plasma region where the gas breakdown and plasma ignition avalanche occur. In some embodiments, a threshold for plasma ignition can be lowered to about the same power density level as is used for sustaining the plasma, e.g., power density as much as about <NUM>% less than the RF power for a normal plasma ignition threshold.

In some embodiments, the plasma processing chamber can include a smaller adjacent chamber that is separated from a plasma chamber by an ultraviolet transmissive window. For instance, such small adjacent chamber can be a sealed chamber having at least two electrodes and a high-pressure inert gas such as xenon. The window between the smaller adjacent chamber and the main plasma chamber can in part be made of a VUV transmissive material such as synthetic quartz. Ignition of plasma can be then facilitated by supplying appropriate pulsed DC power to the electrodes in the adjacent chamber such that plasma is rapidly struck in the adjacent chamber and produces copious VUV radiation that illuminates dielectric wall(s) and/or metal wall(s) of the plasma chamber through the window.

Example aspects of the present disclosure are directed to a plasma processing apparatus. The plasma processing can include a plasma chamber, a dielectric wall forming at least a portion of the plasma chamber, an inductive coupling element located proximate the dielectric wall, an ultraviolet light source (e.g., CW lamp or pulsed lamp, such as, a xenon arc flashlamp, deuterium lamp, or an excimer RF /pulse xenon lamp) to emit an ultraviolet light beam onto a metal surface or a dielectric surface in the plasma chamber. The metal surface or a dielectric surface can emit one or more electrons into the plasma chamber when the ultraviolet light beam is incident on the metal surface or a dielectric surface. The plasma processing apparatus further includes a controller to control the power to the ultraviolet light source and thereby the emission of ultraviolet light beam upon the metal surface prior to or during ignition of a plasma in a process gas by energizing the inductive coupling element with a radio frequency (RF) energy (e.g., exciting with RF energy).

In some embodiments, the controller (e.g., a computer, microcontroller(s), other control device(s), etc.) can include one or more processors and one or more memory devices. The one or more memory devices can store computer-readable instructions that when executed by the one or more processors cause the one or more processors to perform operations, such as turning on the ultraviolet light source to emit the ultraviolet light beam on the metal surface or the dielectric surface prior to or during ignition of a plasma, or other suitable operation.

In some embodiments, the plasma chamber can further include one or more reflective elements (e.g., mirrors) to reflect the light beam onto the metal surface or the dielectric surface. In some embodiments, the metal surface and/or dielectric surface can be electrically grounded. In some embodiments, the ultraviolet light source can emit the light beam in a wavelength range from about <NUM> nanometers to about <NUM> nanometers. In some embodiments, the plasma processing apparatus can include an electrostatic shield (e.g., a Faraday shield, or other suitable conductive materials) located between the dielectric wall and the inductive coupling element. In some embodiments, the ultraviolet light beam can pass through a vacuum window to reach the metal surface and/or dielectric surface. The vacuum window (e.g., synthetic quartz, UV-grade sapphire, magnesium fluoride (MgF2) material, or calcium fluoride (CaF2) material) can be at least partially transparent to the ultraviolet light beam. In some embodiments, a space between the ultraviolet light source and the window can be filled with a gas (e.g., helium or nitrogen) to reduce absorption by atmospheric oxygen. In some embodiments, the plasma chamber can be separated (e.g., by a separation grid) from a processing chamber having a workpiece support configured to support a workpiece.

Example aspects of the present disclosure are directed to a method for igniting a plasma in a plasma processing apparatus. The method can include admitting a process gas into a plasma chamber. The method can include exciting an inductive coupling element to initiate ignition of the plasma in the process gas. Prior to or during excitation of the inductive coupling element for the purpose of ignition of the plasma in the process gas, the method can include emitting an ultraviolet light, via an ultraviolet light source, onto a metal surface and/or dielectric surface in the plasma chamber. The metal surface and/or dielectric surface can emit one or more electrons into the plasma chamber when the ultraviolet light beam is incident on the metal surface or a dielectric surface. The method can include energizing the inductive coupling element with a radio frequency (RF) energy to sustain the plasma in the process gas.

Aspects of the present disclosure are discussed with reference to a "workpiece" that is a "semiconductor wafer" for purposes of illustration and discussion. Those of ordinary skill in the art, using the disclosures provided herein, will understand that the example aspects of the present disclosure can be used in association with any semiconductor substrate or other suitable substrate. In addition, the use of the term "about" in conjunction with a numerical value is intended to refer to within ten percent (<NUM>%) of the stated numerical value.

Example aspects of the present disclosure can provide a number of technical effects and benefits. For instance, a plasma processing apparatus can include an ultraviolet light source that can be controlled to emit the ultraviolet light beam on a metal surface or on a dielectric surface prior to or during ignition of a plasma in a process gas by energizing the inductive coupling element with a radio frequency (RF) energy. As such, the plasma processing apparatus can improve ignition of plasma with a lower RF power level and can also improve speed and reliability of plasma ignition for semiconductor wafers. The plasma processing apparatus can also reduce sputtering, particle contamination, and roughening of the inner walls of the plasma chamber.

<FIG> depicts an example plasma processing apparatus <NUM> according to example embodiments of the present disclosure. As illustrated, the plasma processing apparatus <NUM> includes a processing chamber <NUM> and a plasma chamber <NUM> that is separated from the processing chamber <NUM>. The processing chamber <NUM> includes a substrate holder or workpiece support <NUM> operable to hold a workpiece <NUM> to be processed, such as a semiconductor wafer. In this example illustration, a plasma is generated in the plasma chamber <NUM> (i.e., plasma generation region <NUM>) by an inductively coupled plasma source <NUM> and desired species are channeled from the plasma chamber <NUM> to the surface of substrate <NUM> through a separation grid assembly <NUM>.

Aspects of the present disclosure are discussed with reference to an inductively coupled plasma source for purposes of illustration and discussion. Those of ordinary skill in the art, using the disclosures provided herein, will understand that any plasma source (e.g., inductively coupled plasma source, capacitively coupled plasma source, etc.) can be used without deviating from the scope of the present disclosure. In particular, in some embodiments there need not be a separation, baffle or grid between plasma generation and substrate support volumes.

The plasma chamber <NUM> includes a dielectric side wall <NUM> and a ceiling <NUM>. The dielectric side wall <NUM>, the ceiling <NUM>, and the separation grid <NUM> define a plasma chamber interior <NUM>. The dielectric side wall <NUM> can be formed from a dielectric material, such as quartz and/or alumina. The inductively coupled plasma source <NUM> can include an induction coil <NUM> disposed adjacent to the dielectric side wall <NUM> above the plasma chamber <NUM>. The induction coil <NUM> is coupled to an RF power generator <NUM> through a suitable matching network <NUM>. Process gases (e.g., reactant and/or carrier gases) can be provided to the chamber interior from a gas supply <NUM> and an annular gas distribution channel <NUM> or other suitable gas introduction mechanism. When the induction coil <NUM> is energized with RF power from the RF power generator <NUM>, a plasma can be generated in the plasma chamber <NUM>. In a particular embodiment, the plasma processing apparatus <NUM> can include an optional grounded Faraday shield <NUM> to reduce capacitive coupling of the induction coil <NUM> to the plasma. In some embodiments the Faraday shield need not be directly grounded but may be grounded through a tunable reactive circuit that may be tuned to a low reactive impedance.

As shown in <FIG>, the separation grid <NUM> separates the plasma chamber <NUM> from the processing chamber <NUM>. The separation grid <NUM> can be used to perform ion filtering from a mixture generated by plasma in the plasma chamber <NUM> to generate a filtered mixture. The filtered mixture can be exposed to the workpiece <NUM> in the processing chamber <NUM>.

According to example aspects of the present disclosure, ignition of inductively coupled plasma can be improved with an ultraviolet light source that emits an ultraviolet light beam onto a dielectric wall and/or a metal surface at a location proximate the volume that will be occupied by plasma following ignition of the plasma. As such, less power can be used to ignite the plasma with better igniting repeatability and to reduce a direct electric field ion bombardment to a dielectric window.

As can be seen in <FIG>, the plasma processing chamber <NUM> further includes an ultraviolet light source <NUM> and an ultraviolet (UV) emission assembly <NUM>.

The ultraviolet light source <NUM> is mounted external to the plasma chamber <NUM> for the inductively coupled plasma source <NUM> such that radiation from the ultraviolet light source <NUM> can illuminate an inner wall of the UV emission assembly <NUM> prior to or during ignition of the plasma. The ultraviolet light source <NUM> emits one or more ultraviolet light beams <NUM> (e.g., in a wavelength range of about <NUM> nanometers to about <NUM> nanometers) into the plasma chamber <NUM> through the UV emission assembly <NUM>. The ultraviolet light source <NUM> can be a CW lamp or a pulsed lamp. Examples of the ultraviolet light source <NUM> can include a xenon arc flashlamp, deuterium lamp, an excimer RF /pulse xenon lamp, or any other suitable light source that emits an ultraviolet light beam. For instance, the ultraviolet light source <NUM> can be turned on or the ultraviolet light source <NUM> can start pulsing to illuminate a part of an interior surface of the UV emission assembly <NUM>, prior to or simultaneous with a turning-on of RF power <NUM> to ignite the plasma in the plasma chamber120. Radiation from the ultraviolet light source <NUM> can be maintained at least until the plasma attains a substantial fraction of its ultimate density. As such, reliability of ignition and growth of the plasma can be accelerated and improved.

In some embodiments, to reduce heat buildup in the ultraviolet light source <NUM>, the ultraviolet light source <NUM> can be pulsed with multiple rapid pulses (e.g., less than about <NUM> millisecond) at very short intervals (e.g., less than about <NUM> milliseconds). The ultraviolet light source <NUM> can start pulsing prior to or just following the time of initiation of RF power <NUM> supplied to the inductively coupled source <NUM>. In some embodiments, the ultraviolet radiation pulses can have a frequency of at least about <NUM> per second and preferably <NUM> per second or more so that multiple pulses can contribute ultraviolet photons to an ignition process. As such, ultraviolet acceleration of plasma ignition can only take about <NUM> milliseconds.

In some embodiments, ultraviolet radiation from the ultraviolet light source <NUM> can promote plasma ignition and growth by ejecting photo-electrons from an irradiated surface(s) proximate the plasma region <NUM> as the RF power <NUM> is applied to the inductively coupled plasma source <NUM>, as further described below. The irradiated surface may be metal or insulator material or metal with a very thin insulator surface layer.

In some embodiments (not shown in <FIG>), the plasma processing apparatus <NUM> includes a controller that controls the ultraviolet light source <NUM> to emit the ultraviolet light beam. The controller (e.g., a computer, microcontroller(s), other control device(s), etc.) can include one or more processors and one or more memory devices. The one or more memory devices can store computer-readable instructions that when executed by the one or more processors cause the one or more processors to perform operations, such as turning on the ultraviolet light source to emit the ultraviolet light beam on a metal surface or a dielectric surface prior to or during ignition of a plasma, or other suitable operation.

The UV emission assembly <NUM> includes one or more walls <NUM>, one or more reflective elements (e.g., mirrors) <NUM> and a vacuum window <NUM>. The structure <NUM> may be electrically grounded so that the surfaces <NUM> and <NUM> are grounded. At least a portion of the wall(s) <NUM> can be metal, and/or dielectric. When the ultraviolet light beam <NUM> is incident on a surface <NUM> (e.g., a metal surface or a dielectric surface) at a location proximate the plasma, the surface <NUM> can emit one or more electrons into the plasma region <NUM>. In some embodiments, an instantaneous output power of the ultraviolet light source <NUM> at the time of plasma ignition can be about <NUM> Watt or more. This can be because the photo-emission of an electron from an insulator requires such photon energy that it can raise a valence electron past the conduction band and into the free electron energy space. For photoemission from metal, photon energy from the ultraviolet light source <NUM> can raise an electron from a conduction band to a free state which typically takes less photon energy. In some embodiments, the photo-electron emission from the surface <NUM> of the UV emission assembly <NUM> can include at least <NUM> electrons in a pulse.

In some embodiments, electrons emitted from the surface <NUM> into the volume <NUM> can then be accelerated by electrical fields in the volume <NUM> to cause ionization of the gas in the plasma chamber <NUM>. Typically, as the plasma develops and shields the plasma nearer the chamber axis of the dielectric vessel <NUM> the induction fields are much stronger near the inner surface of the dielectric vessel <NUM>. The ionization can then provide additional electrons that take part in "avalanche" of ionization which forms the plasma. In some embodiments (not shown in <FIG>), a plasma-facing surface irradiated with ultraviolet radiation can be a part of a dielectric wall of a plasma chamber, as further described in <FIG>. The dielectric wall can have substantial induction electric fields when an RF power is being provided. In some embodiments (not shown in <FIG>), ultraviolet irradiated surface can be a metal surface on an interior of a plasma chamber that has a line of sight to the volume within the vessel <NUM> that is close to the coil <NUM>, as further described in <FIG>.

As can be seen in <FIG>, the ultraviolet light beam <NUM> is reflected onto the surface <NUM> via a reflective element (e.g., a mirror) <NUM>. Electrons <NUM> emitted from the surface <NUM> pass into the plasma region <NUM>.

The vacuum window <NUM> separates the UV source <NUM> from the reflector <NUM>, the surface <NUM> and surface <NUM> that are exposed to the plasma chamber interior <NUM>. The vacuum window <NUM> can be an ultraviolet transmissive window. For instance, the window <NUM> can have at least one of: synthetic quartz, UV-grade sapphire, magnesium fluoride (MgF2) material, or calcium fluoride (CaF2) material. As another example, a space between the ultraviolet light source(s) and the window can be filled with a gas (e.g., helium or nitrogen) to reduce absorption by atmospheric oxygen.

In some embodiments (not shown in <FIG>), the UV emission assembly can be a sealed chamber having at least two electrodes and a high-pressure inert gas such as xenon. The vacuum window can in part be made of a VUV transmissive material such as synthetic quartz. Ignition of plasma can be then facilitated by supplying appropriate pulsed electric power to the electrodes in the UV emission assembly such that that the UV emission assembly experiences electric breakdown and to produce copious VUV radiation that illuminates dielectric wall(s) and/or metal wall(s) of the plasma chamber.

<FIG> depicts a flow diagram of an example method (<NUM>) for accelerating ignition of an inductively coupled plasma according to example aspects of the present disclosure. The method (<NUM>) can be implemented using the plasma processing apparatus <NUM>. However, as will be discussed in detail below, the methods according to example aspects of the present disclosure can be implemented using other approaches without deviating from the scope of the present disclosure. <FIG> depicts steps performed in a particular order for purposes of illustration and discussion. Those of ordinary skill in the art, using the disclosures provided herein, will understand that various steps of any of the methods described herein can be omitted, expanded, performed simultaneously, rearranged, and/or modified in various ways without deviating from the scope of the present disclosure. In addition, various additional steps (not illustrated) can be performed without deviating from the scope of the present disclosure.

At (<NUM>), the method can include placing a workpiece on a workpiece support. For instance, a workpiece <NUM> can be placed on a workpiece support <NUM> in a processing chamber <NUM>.

At (<NUM>), the method can include admitting a process gas into a plasma chamber. For instance, a process gas can be admitted into the plasma chamber interior <NUM> from the gas source <NUM> via the annular gas distribution channel <NUM> or other suitable gas introduction mechanism.

At (<NUM>), prior to or during initiation of providing RF power to the induction coil, the method can include emitting an ultraviolet light beam, via an ultraviolet light source, onto a metal surface and/or dielectric surface in the plasma chamber. The metal surface and/or dielectric surface can emit one or more electrons into the plasma chamber when the ultraviolet light beam is incident on the metal surface and/or dielectric surface. For instance, prior to or during ignition of the plasma in the process gas, an ultraviolet light source <NUM> can emit an ultraviolet light beam <NUM> that passes through a transmissive vacuum window and is reflected onto a surface <NUM> via a reflective element (e.g., a mirror) <NUM>. Electrons <NUM> emitted from the surface <NUM> pass directly into the plasma region <NUM> because the surface <NUM> has direct line of sight to the plasma region <NUM> and plasma chamber interior <NUM>.

At (<NUM>), the method can include energizing or continuing to energize the inductive coupling element with a radio frequency (RF) energy to sustain the plasma in the process gas. For instance, the induction coil <NUM> can be energized with the RF power generator <NUM> to sustain the plasma in the process gas.

At (<NUM>), the method can include exposing the workpiece to one or more species generated by the plasma. For instance, one or species generated by the plasma can be channeled from the plasma chamber <NUM> to surface of the workpiece <NUM> through the separation grid assembly <NUM>.

<FIG> depicts an example plasma processing apparatus <NUM> according to example embodiments of the present disclosure. The plasma processing apparatus <NUM> is similar to the plasma processing apparatus <NUM> of <FIG>.

More particularly, plasma processing apparatus <NUM> includes a processing chamber <NUM> and a plasma chamber <NUM> that is separated from the processing chamber <NUM>. Processing chamber <NUM> includes a substrate holder or workpiece support <NUM> operable to hold a workpiece <NUM> to be processed, such as a semiconductor wafer. In this example illustration, a plasma is generated in plasma chamber <NUM> (i.e., plasma generation region <NUM>) by an inductively coupled plasma source <NUM> and desired species are channeled from the plasma chamber <NUM> to the surface of substrate <NUM> through a separation grid assembly <NUM>. In some embodiments, there is no separation grid or other structure between the plasma chamber <NUM> and the processing chamber <NUM>.

The plasma chamber <NUM> includes a dielectric side wall <NUM> and a ceiling <NUM>. The dielectric side wall <NUM>, ceiling <NUM>, and separation grid <NUM> define a plasma chamber interior <NUM>. Dielectric side wall <NUM> can be formed from a dielectric material, such as quartz and/or alumina. The inductively coupled plasma source <NUM> can include an induction coil <NUM> disposed adjacent to the dielectric side wall <NUM> above the processing chamber <NUM>. The induction coil <NUM> is coupled to an RF power generator <NUM> through a suitable matching network <NUM>. Process gases (e.g., an inert gas) can be provided to the chamber interior from gas supply <NUM> or other suitable gas introduction mechanism. When the induction coil <NUM> is energized with RF power from the RF power generator <NUM>, a plasma can be generated in the plasma chamber <NUM>. In a particular embodiment, the plasma processing apparatus <NUM> can include an optional grounded Faraday shield <NUM> to reduce capacitive coupling of the induction coil <NUM> to the plasma.

According to example aspects of the present disclosure, ultraviolet light source(s) can be located adjacent a window such that one or more ultraviolet light beams from the ultraviolet light source(s) can pass through the window to reach an inner wall of a plasma chamber. For instance, as can be seen in <FIG>, the plasma processing chamber <NUM> further includes an ultraviolet light source <NUM> and a vacuum window <NUM>.

The ultraviolet light source <NUM> is mounted adjacent the vacuum window <NUM> such that an ultraviolet light beam <NUM> from the ultraviolet light source <NUM> passes through the window <NUM> to reach an interior surface <NUM> of the dielectric wall <NUM> of the plasma chamber <NUM>. The interior surface <NUM> is proximate a plasma region <NUM> (or a plasma in the plasma region <NUM>). As can be seen in <FIG>, the ultraviolet light beam <NUM> intercepts a portion of the interior surface <NUM> of the plasma chamber <NUM> such that the ultraviolet light beam <NUM> is incident upon the interior surface <NUM> at a location adjacent plasma in operation.

The ultraviolet light source <NUM> can be a CW lamp or a pulsed lamp. Examples of the ultraviolet light source <NUM> can include a xenon arc flashlamp, deuterium lamp, an excimer RF /pulse xenon lamp, or any other suitable light source that emits an ultraviolet light beam. For instance, the ultraviolet light source <NUM> can be turned on or the ultraviolet light source <NUM> can start pulsing to illuminate a part of the interior surface <NUM> of the dielectric wall <NUM>, prior to or simultaneous with a turning-on of RF power <NUM> to ignite the plasma in the plasma chamber120. Radiation from the ultraviolet light source <NUM> can be maintained at least until the plasma attains a fraction of its ultimate density. As such, reliability of ignition and growth of the plasma can be accelerated and improved.

In some embodiments, to reduce heat buildup in the ultraviolet light source <NUM>, the ultraviolet light source <NUM> can be pulsed with multiple rapid pulses at very short intervals (e.g., less than <NUM> milliseconds). The ultraviolet light source <NUM> can start pulsing prior to or just following the time of initiation of RF power <NUM> supplied to the inductively coupled source <NUM>. In some embodiments, the ultraviolet radiation pulses can have a frequency of at least about <NUM> and in some embodiments <NUM> per second so that multiple pulses can contribute ultraviolet photons to an ignition process. As such, ultraviolet acceleration can only take about <NUM> milliseconds.

In some embodiments, ultraviolet radiation from the ultraviolet light source <NUM> can promote plasma ignition and growth by ejecting electrons from an irradiated surface(s) proximate the plasma as the RF power <NUM> is applied to the inductively coupled plasma source <NUM>. When the ultraviolet light beam <NUM> is incident on the interior surface <NUM> (e.g., a dielectric surface) at a location proximate the plasma, the surface <NUM> can emit one or more electrons into the plasma region <NUM>. In some embodiments, an instantaneous output power of the ultraviolet light source <NUM> at the time of plasma ignition can be about <NUM> Watt or more. This can be because the photo-emission of an electron from an insulator requires such photon energy that it can raise a valence electron past the conduction band and into the free electron energy space. In some embodiments, the photo-electron emission from the surface <NUM> can include at least <NUM> electrons. In some embodiments, electrons emitted from the surface <NUM> can then be accelerated by electrical fields in the plasma region <NUM> to cause ionization of the gas in the plasma chamber <NUM>. The ionization can then provide additional electrons that take part in "avalanche" of ionization which forms the plasma. In some embodiments there may be a thin metal coating on the dielectric wall that may intercept the UV radiation from the source <NUM>.

In some embodiments (not shown in <FIG>), the plasma processing apparatus <NUM> includes a controller that controls the ultraviolet light source <NUM> to emit the ultraviolet light beam <NUM>. The controller (e.g., a computer, microcontroller(s), other control device(s), etc.) can include one or more processors and one or more memory devices. The one or more memory devices can store computer-readable instructions that when executed by the one or more processors cause the one or more processors to perform operations, such as turning on the ultraviolet light source to emit the ultraviolet light beam on a dielectric surface prior to or during ignition of a plasma, or other suitable operation.

The vacuum window <NUM> can be one example embodiment of the vacuum window <NUM>. For instance, the window <NUM> can have at least one of: synthetic quartz, UV-grade sapphire, magnesium fluoride (MgF2) material, or calcium fluoride (CaF2) material. As another example, a space between the ultraviolet light source <NUM> and the window <NUM> can be filled with a gas (e.g., helium, nitrogen, argon, and/or nitrogen) to reduce absorption by atmospheric oxygen.

<FIG> depicts an example plasma processing apparatus <NUM> according to example embodiments of the present disclosure. The plasma processing apparatus <NUM> is similar to the plasma processing apparatus <NUM> of <FIG> and the plasma processing apparatus <NUM> of <FIG>.

More particularly, plasma processing apparatus <NUM> includes a processing chamber <NUM> and a plasma chamber <NUM> that is separated from the processing chamber <NUM>. Processing chamber <NUM> includes a substrate holder or workpiece support <NUM> operable to hold a workpiece <NUM> to be processed, such as a semiconductor wafer. In this example illustration, a plasma is generated in plasma chamber <NUM> (i.e., plasma generation region <NUM>) by an inductively coupled plasma source <NUM> and desired species are channeled from the plasma chamber <NUM> to the surface of substrate <NUM> through a separation grid assembly <NUM>.

The plasma chamber <NUM> includes a dielectric side wall <NUM> and a ceiling <NUM>. The dielectric side wall <NUM>, ceiling <NUM>, and separation grid <NUM> define a plasma chamber interior <NUM>. Dielectric side wall <NUM> can be formed from a dielectric material, such as quartz, glass, alumina, silicon nitride, silicon oxynitride, aluminum nitride, aluminum oxynitride, or other high-temperature capable dielectric or combination thereof. The inductively coupled plasma source <NUM> can include an induction coil <NUM> disposed adjacent to the dielectric side wall <NUM> above the plasma chamber <NUM>. The induction coil <NUM> is coupled to an RF power generator <NUM> through a suitable matching network <NUM>. Process gases (e.g., an inert gas) can be provided to the chamber interior from gas supply <NUM> or other suitable gas introduction mechanism. When the induction coil <NUM> is energized with RF power from the RF power generator <NUM>, a plasma can be generated in the plasma chamber <NUM>. In a particular embodiment, the plasma processing apparatus <NUM> can include an optional grounded Faraday shield <NUM> to reduce capacitive coupling of the induction coil <NUM> to the plasma.

As shown in <FIG>, a separation grid <NUM> separates the plasma chamber <NUM> from the processing chamber <NUM>. The separation grid <NUM> can be used to perform ion filtering from a mixture generated by plasma in the plasma chamber <NUM> to generate a filtered mixture. The filtered mixture can be exposed to the workpiece <NUM> in the processing chamber.

According to example aspects of the present disclosure, ultraviolet light source(s) can be located adjacent a window such that one or more ultraviolet light beams from the ultraviolet light source(s) can pass through the window to impinge on a metal surface <NUM> that is a metal structure <NUM> of a plasma chamber (e.g., a top cap). As can be seen in <FIG>, the plasma processing chamber <NUM> further includes an ultraviolet light source <NUM>, a vacuum window <NUM> and a metal wall <NUM>. The ultraviolet light source <NUM> is mounted adjacent the vacuum window <NUM> such that an ultraviolet light beam <NUM> from the ultraviolet light source <NUM> passes through the window <NUM> to reach an interior surface <NUM> of the metal wall <NUM> of the plasma chamber <NUM>. The interior surface <NUM> is proximate a plasma region <NUM> (or a plasma in the plasma region <NUM>). As can be seen in <FIG>, the ultraviolet light beam <NUM> intercepts a portion of the interior surface <NUM> of the plasma chamber <NUM> such that the ultraviolet light beam <NUM> can pass through some part of the volume that may be occupied by plasma in operation and can also pass through some part of the evacuated volume that may not be occupied by plasma in operation.

The ultraviolet light source <NUM> can be a CW lamp or a pulsed lamp. Examples of the ultraviolet light source <NUM> can include a xenon arc flashlamp, deuterium lamp, an excimer RF /pulse xenon lamp, or any other suitable light source that emits an ultraviolet light beam. For instance, the ultraviolet light source <NUM> can be turned on or the ultraviolet light source <NUM> can start pulsing to illuminate a part of the interior surface <NUM> of the metal wall <NUM>, prior to or simultaneous with a turning-on of RF power <NUM> to ignite the plasma in the plasma chamber120. Radiation from the ultraviolet light source <NUM> can be maintained at least until the plasma attains a fraction of its ultimate density. As such, reliability of ignition and growth of the plasma can be accelerated and improved.

In some embodiments, to reduce heat buildup in the ultraviolet light source <NUM>, the ultraviolet light source <NUM> can be pulsed with multiple rapid pulses at very short intervals (e.g., less than <NUM> milliseconds and more preferably less than <NUM> milliseconds). The ultraviolet light source <NUM> can start pulsing prior to or just following the time of initiation of RF power <NUM> supplied to the inductively coupled source <NUM>. In some embodiments, the ultraviolet radiation pulses can have a frequency of at least about <NUM> per second so that multiple pulses can contribute ultraviolet photons to an ignition process. As such, the total duration of ultraviolet acceleration of plasma ignition can only take about <NUM> milliseconds and preferably less than <NUM> milliseconds.

In some embodiments, ultraviolet radiation from the ultraviolet light source <NUM> can promote plasma ignition and growth by ejecting electrons from an irradiated surface(s) proximate the volume that will be occupied by plasma as the RF power <NUM> is applied to the inductively coupled plasma source <NUM>. When the ultraviolet light beam <NUM> is incident on the interior surface <NUM> (e.g., a metal surface) at a location proximate where the plasma will be, the surface <NUM> can emit one or more electrons into the region <NUM> that the plasma will occupy. In some embodiments, an instantaneous output power of the ultraviolet light source <NUM> at the time of plasma ignition can be about <NUM> Watt or more, preferably a fraction larger than <NUM>% of which is in the hard UV band. This can be because the photo-emission of an electron from an insulator requires such photon energy that it can raise a valence electron past the conduction band and into the free electron energy space. In some embodiments, in one pulse of UV the photo-electron emission from the surface <NUM> can include at least <NUM> electrons.

In some embodiments, electrons emitted from the surface <NUM> can then be accelerated by electrical fields in the region <NUM> induced by the rf current in the induction coil to cause ionization of the gas in the plasma chamber <NUM> to fill the region <NUM> with plasma. The ionization of gas in this region can then provide additional electrons that take part in "avalanche" of ionization which forms the plasma.

In some embodiments (not shown in <FIG>), the plasma processing apparatus <NUM> includes a controller that controls the ultraviolet light source <NUM> to emit the ultraviolet light beam <NUM>. The controller (e.g., a computer, microcontroller(s), other control device(s), etc.) can include one or more processors and one or more memory devices. The one or more memory devices can store computer-readable instructions that when executed by the one or more processors cause the one or more processors to perform operations, such as turning on the ultraviolet light source to emit the ultraviolet light beam on a metal surface prior to or during ignition of a plasma, or other suitable operation.

The vacuum window <NUM> can be one embodiment of the vacuum window <NUM>. For instance, the window <NUM> can have at least one of: synthetic quartz, UV-grade sapphire, magnesium fluoride (MgF2) material, or calcium fluoride (CaF2) material. As another example, a space between the ultraviolet light source <NUM> and the window <NUM> can be filled with a gas (e.g., helium or nitrogen) to reduce absorption by atmospheric oxygen.

More particularly, plasma processing apparatus <NUM> includes a processing chamber <NUM> and a plasma chamber <NUM> that is separated from the processing chamber <NUM>. Processing chamber <NUM> includes a substrate holder or workpiece support <NUM> operable to hold a workpiece <NUM> to be processed, such as a semiconductor wafer. In this example illustration, a plasma is generated in plasma chamber <NUM> (i.e., plasma generation region) by an inductively coupled plasma source <NUM> and desired species are channeled from the plasma chamber <NUM> to the surface of substrate <NUM> through a separation grid assembly <NUM>.

The plasma chamber <NUM> includes a dielectric side wall <NUM> and a ceiling <NUM>. The dielectric side wall <NUM>, ceiling <NUM>, and separation grid <NUM> define a plasma chamber interior <NUM>. Dielectric side wall <NUM> can be formed from a dielectric material, such as quartz and/or alumina or other high temperature resistant dielectrics such as ceramics. The inductively coupled plasma source <NUM> can include an induction coil <NUM> disposed adjacent to the dielectric side wall <NUM> above the plasma chamber <NUM>. The induction coil <NUM> is coupled to an RF power generator <NUM> through a suitable matching network <NUM>. Process gases can be provided to the chamber interior from gas supply <NUM> and annular gas distribution channel <NUM> or other suitable gas introduction mechanism. When the induction coil <NUM> is energized with RF power from the RF power generator <NUM>, a plasma can be generated in the plasma chamber <NUM>. In a particular embodiment, the plasma processing apparatus <NUM> can include an optional grounded Faraday shield <NUM> to reduce capacitive coupling of the induction coil <NUM> to the plasma.

The example plasma processing apparatus <NUM> of <FIG> is operable to generate a first plasma <NUM> (e.g., a remote plasma) in the plasma chamber <NUM> and a second plasma <NUM> (e.g., a direct plasma) in the processing chamber <NUM>. As used herein, a "remote plasma" refers to a plasma generated remotely from a workpiece, such as in a plasma chamber separated from a workpiece by a separation grid. As used herein, a "direct plasma" refers to a plasma that is directly exposed to a workpiece, such as a plasma generated in a processing chamber having a workpiece support operable to support the workpiece.

More particularly, the plasma processing apparatus <NUM> of <FIG> includes a bias source having bias electrode <NUM> in the workpiece support <NUM>. The bias electrode <NUM> can be coupled to an RF power generator <NUM> via a suitable matching network <NUM>. When the bias electrode <NUM> is energized with RF energy, a second plasma <NUM> can be generated from a mixture in the processing chamber <NUM> for direct exposure to the workpiece <NUM>. The processing chamber <NUM> can include a gas exhaust port <NUM> for evacuating a gas from the processing chamber <NUM>.

According to example aspects of the present disclosure, ignition of inductively coupled plasma can be improved with an ultraviolet light source that emits an ultraviolet light beam onto a dielectric wall and/or a metal surface at a location proximate to where the plasma will be, prior to or during ignition of the plasma. As such, less power can be used to ignite either or both of the plasmas with better igniting repeatability and to reduce a direct electric field ion bombardment to a dielectric window.

As can be seen in <FIG>, the plasma processing chamber <NUM> further includes an ultraviolet light source <NUM> and a metal top structure <NUM> containing a UV transmissive window <NUM>. The ultraviolet light source <NUM> is mounted external to the plasma chamber <NUM> for the inductively coupled plasma source <NUM> such that radiation from the ultraviolet light source <NUM> can illuminate an inner wall of the metal top structure <NUM> prior to or during ignition of the plasma. The ultraviolet light source <NUM> emits one or more ultraviolet light beams <NUM> into the plasma chamber <NUM> through the UV transmissive window <NUM>. The ultraviolet light source <NUM> can be a CW lamp or a pulsed lamp. Examples of the ultraviolet light source <NUM> can include a xenon arc flashlamp, deuterium lamp, an excimer RF /pulse xenon lamp, or any other suitable light source that emits an ultraviolet light beam. For instance, the ultraviolet light source <NUM> can be turned on or the ultraviolet light source <NUM> can start pulsing UV energy that is then transmitted through window <NUM> to illuminate a part of an interior surface of the metal top structure <NUM>, that faces the interior of the plasma chamber, prior to or simultaneous with a turning-on of RF power <NUM> to ignite the plasma in the plasma chamber <NUM>. Radiation from the ultraviolet light source <NUM> can be maintained at least until the plasma attains a fraction of its ultimate density or the voltage on the inductive coupling antenna exhibits a substantial and rapid change as the plasma occupies a portion of the interior of the chamber. As such, reliability of ignition and growth of the plasma can be accelerated and improved.

In some embodiments, to reduce heat buildup in the ultraviolet light source <NUM>, the ultraviolet light source <NUM> can be pulsed with multiple rapid pulses at very short intervals (e.g., less than <NUM> milliseconds). The ultraviolet light source <NUM> can start pulsing prior to or just following initiation of RF power <NUM> supplied to the inductively coupled source <NUM>. In some embodiments, the ultraviolet radiation pulses can have a frequency of at least about <NUM> per second so that multiple pulses can contribute ultraviolet photons to an ignition process. As such, ultraviolet-assisted ignition of the plasma can only take about <NUM> milliseconds or less.

In some embodiments, ultraviolet radiation from the ultraviolet light source <NUM> can promote plasma ignition and growth by ejecting photo-electrons from an irradiated surface(s) proximate the region <NUM> that will contain plasma as the RF power <NUM> is applied to the inductively coupled plasma source <NUM>, as further described below.

The metal top structure <NUM> includes one or more walls <NUM>, one or more reflective elements (e.g., mirrors) <NUM> and a vacuum window <NUM>. The structure <NUM> is electrically grounded or may be biased negatively with respect to earth ground, particularly during the plasma ignition phase. At least a portion of the wall(s) <NUM> can be metal, and/or dielectric. When the ultraviolet light beam <NUM> is incident on a surface <NUM> (e.g., a metal surface or a dielectric surface) at a location proximate the volume that will contain the plasma, the surface <NUM> can emit one or more electrons into the region <NUM>. In some embodiments, an instantaneous output power of the ultraviolet (UV) light source <NUM> at the time of plasma ignition can be about <NUM> Watt or more. The wavelength of at least part of the radiation may be less than about <NUM>, being in the hard UV band. This can be because the photo-emission of an electron from an insulator requires such photon energy that it can raise a valence electron past the conduction band and into the free electron energy space. For photoemission from metal, photon energy from the ultraviolet light source <NUM> can raise an electron from a conduction band to a free state. In some embodiments, the photo-electron emission from the surface <NUM> of the UV emission assembly <NUM> can include at least <NUM> electrons.

In some embodiments, electrons emitted from the surface <NUM> can then be accelerated by electrical fields in the plasma region <NUM> to cause ionization of the gas in the plasma chamber <NUM>. The ionization can then provide additional electrons that take part in exponential growth "avalanche" of ionization which forms the plasma. In some embodiments (not shown in <FIG>), an interior volume-facing surface irradiated with ultraviolet radiation can be a part of a dielectric wall of a plasma chamber, as described above in <FIG>. The dielectric wall can have substantial induction electric fields when an RF power is being provided. In some embodiments (not shown in <FIG>), ultraviolet irradiated surface can be a metal surface on an interior wall of a plasma chamber that has a line of sight to a region that will contain plasma after ignition, as described above in <FIG>.

As can be seen in <FIG>, the ultraviolet light beam <NUM> is reflected onto the surface <NUM> via a reflective element (e.g., a mirror) <NUM>. Electrons <NUM> emitted from the surface <NUM> are emitted directly into the region <NUM> that will contain plasma after ignition.

The vacuum window <NUM> separates the lamp <NUM> from the plasma chamber interior <NUM>. The vacuum window <NUM> can be an ultraviolet transmissive window. For instance, the window <NUM> can have at least one of: synthetic quartz, UV-grade sapphire, magnesium fluoride (MgF2) material, or calcium fluoride (CaF2) material. As another example, a space between the ultraviolet light source(s) and the window can be filled with a gas (e.g., helium or nitrogen) to reduce absorption by atmospheric oxygen.

In some embodiments (not shown in <FIG>), the UV emission assembly can be a sealed chamber having at least two electrodes and a high-pressure inert gas such as xenon. The vacuum window can in part be made of a UV transmissive material such as synthetic quartz. Ignition of plasma can be then facilitated by supplying appropriate RF power to the inductive coupling element while there is fast pulsed DC power to the electrodes in the UV emission assembly such that that the UV emission assembly can produce copious UV radiation that illuminates dielectric wall(s) and/or metal wall(s) of the plasma chamber.

<FIG> depicts a plasma processing apparatus <NUM> similar to that of <FIG> and <FIG>. More particularly, plasma processing apparatus <NUM> includes a processing chamber <NUM> and a plasma chamber <NUM> that is separated from the processing chamber <NUM>. Processing chamber <NUM> includes a substrate holder or workpiece support <NUM> operable to hold a workpiece <NUM> to be processed, such as a semiconductor wafer. In this example illustration, a plasma is generated in plasma chamber <NUM> (i.e., plasma generation region) by an inductively coupled plasma source <NUM> and desired gas phase species are channeled from the plasma chamber <NUM> to the surface of substrate <NUM> through a separation grid assembly <NUM>.

The plasma chamber <NUM> includes a dielectric side wall <NUM> and a ceiling <NUM>. The dielectric side wall <NUM>, ceiling <NUM>, and separation grid <NUM> define a plasma chamber interior <NUM>. Dielectric side wall <NUM> can be formed from a dielectric material, such as quartz and/or alumina. The inductively coupled plasma source <NUM> can include an induction coil <NUM> disposed adjacent the dielectric side wall <NUM> about the plasma chamber <NUM>. The induction coil <NUM> is coupled to an RF power generator <NUM> through a suitable matching network <NUM>. Process gas (e.g., an inert gas) can be provided to the chamber interior from gas supply <NUM> and annular gas distribution channel <NUM> or other suitable gas introduction mechanism. When the induction coil <NUM> is energized with RF power from the RF power generator <NUM>, a plasma can be generated in the plasma chamber <NUM>. In a particular embodiment, the plasma processing apparatus <NUM> can include an optional grounded Faraday shield <NUM> to reduce capacitive coupling of the induction coil <NUM> to the plasma.

The example plasma processing apparatus <NUM> of <FIG> is operable to generate a first plasma <NUM> (e.g., a remote plasma) in the plasma chamber <NUM> and a second plasma <NUM> (e.g., a direct plasma) in the processing chamber <NUM>. As shown, the plasma processing apparatus <NUM> can include an angled dielectric sidewall <NUM> that extends from the vertical sidewall <NUM> associated with the remote plasma chamber <NUM>. The angled dielectric sidewall <NUM> can form a part of the processing chamber <NUM>.

A second inductive plasma source <NUM> can be located proximate the dielectric sidewall <NUM>. The second inductive plasma source <NUM> can include an induction coil <NUM> coupled to an RF generator <NUM> via a suitable matching network <NUM>. The induction coil <NUM>, when energized with RF energy, can induce a direct plasma <NUM> from a mixture in the processing chamber <NUM>. A Faraday shield <NUM> can be disposed between the induction coil <NUM> and the sidewall <NUM>.

The workpiece support <NUM> can be movable in a vertical direction noted as "V. " For instance, the workpiece support <NUM> can include a vertical lift <NUM> that can be configured to adjust a distance between the workpiece support <NUM> and the separation grid assembly <NUM>. As one example, the workpiece support <NUM> can be located in a first vertical position for processing using the remote plasma <NUM>. The workpiece support <NUM> can be in a second vertical position for processing using the direct plasma <NUM>. The first vertical position can be closer to the separation grid assembly <NUM> relative to the second vertical position.

The plasma processing apparatus <NUM> of <FIG> includes a bias source having bias electrode <NUM> in the workpiece support <NUM>. The bias electrode <NUM> can be coupled to an RF power generator <NUM> via a suitable matching network <NUM>. The processing chamber <NUM> can include a gas exhaust port <NUM> for evacuating a gas from the processing chamber <NUM>.

According to example aspects of the present disclosure, ignition of inductively coupled plasma can be improved with an ultraviolet light source that emits an ultraviolet light beam onto a dielectric wall and/or a metal surface at a location proximate the region wherein there will be plasma once there is ignition of the plasma. As such, less power can be used to ignite the plasma with better igniting repeatability and to reduce a direct electric field ion bombardment to a dielectric window.

As can be seen in <FIG>, the plasma processing chamber <NUM> further includes an ultraviolet light source <NUM> and a UV emission assembly <NUM>.

The ultraviolet light source <NUM> is mounted external to the plasma chamber <NUM> for the inductively coupled plasma source <NUM> such that radiation from the ultraviolet light source <NUM> can illuminate an inner wall of the metal top structure <NUM> prior to or during ignition of the plasma. The ultraviolet light source <NUM> emits one or more ultraviolet light beams <NUM> (e.g., in a wavelength range of about <NUM> nanometers to about <NUM> nanometers) into the plasma chamber <NUM> through the UV transmissive window <NUM>. The ultraviolet light source <NUM> can be a CW lamp or a pulsed lamp. Examples of the ultraviolet light source <NUM> can include a xenon arc flashlamp, deuterium lamp, an excimer RF /pulse xenon lamp, or any other suitable light source that emits an ultraviolet light beam. For instance, the ultraviolet light source <NUM> can be turned on or the ultraviolet light source <NUM> can start pulsing to illuminate a part of an interior surface of the UV emission assembly <NUM>, prior to or simultaneous with a turning-on of RF power <NUM> to ignite the plasma in the plasma chamber120. Radiation from the ultraviolet light source <NUM> can be maintained at least until the plasma attains a substantial fraction of its ultimate density. As such, reliability of ignition and growth of the plasma can be accelerated and improved.

In some embodiments, to reduce heat buildup in the ultraviolet light source <NUM>, the ultraviolet light source <NUM> can be pulsed with multiple rapid pulses at very short intervals (e.g., less than <NUM> milliseconds). The ultraviolet light source <NUM> can start pulsing prior to or just following the time of initiation of RF power <NUM> supplied to the inductively coupled source <NUM>. In some embodiments, the ultraviolet radiation pulses can have a frequency of at least about <NUM> per second so that multiple pulses can contribute ultraviolet photons to an ignition process. As such, in some embodiments ultraviolet assisted plasma ignition can only take about <NUM> milliseconds or less.

In some embodiments, ultraviolet radiation from the ultraviolet light source <NUM> can promote plasma ignition and growth by ejecting photo-electrons from an irradiated surface(s) <NUM> proximate the chamber interior that can include the plasma region <NUM> as the RF power <NUM> is applied to the inductively coupled plasma source <NUM>, as further described below.

In some embodiments (not shown in <FIG>), the plasma processing apparatus <NUM> includes a controller that controls the ultraviolet light source <NUM> to emit the ultraviolet light beam. The controller (e.g., a computer, microcontroller(s), other control device(s), etc.) can include one or more processors and one or more memory devices. The one or more memory devices can store computer-readable instructions that when executed by the one or more processors cause the one or more processors to perform operations, such as turning on the ultraviolet light source to emit the ultraviolet light beam to impinge on a metal surface or a dielectric surface prior to or during ignition of a plasma, or other suitable operation.

The UV emission assembly <NUM> includes one or more walls <NUM>, one or more reflective elements (e.g., mirrors) <NUM> and a vacuum window <NUM>. The wall(s) <NUM> is grounded. At least a portion of the top structure <NUM> can be metal, and/or dielectric. When the ultraviolet light beam <NUM> is incident on a surface <NUM> (e.g., a metal surface or a dielectric surface) at a location proximate the volume that will contain plasma, the surface <NUM> can emit one or more electrons into that region <NUM>. In some embodiments, an instantaneous output power of ultraviolet radiation from the light source <NUM> at the time of plasma ignition can be about <NUM> milliwatts and more preferably <NUM> Watt or more. UV radiation is employed because the photo-emission of an electron from an insulator requires such photon energy that it can raise a valence electron past the conduction band and into the free electron energy space. For photoemission from metal, photon energy from the ultraviolet light source <NUM> can raise an electron from a conduction band to a free state. In some embodiments, the photo-electron emission from the surface <NUM> of the UV emission assembly <NUM> can include at least <NUM> electrons.

In some embodiments, electrons emitted from the surface <NUM> can then be accelerated by electrical fields in the plasma region <NUM> to cause ionization of the gas in the interior of the chamber <NUM> where plasma will be located. The ionization can then provide additional electrons that take part in exponential growth "avalanche" of ionization and resultant electron density, which forms the plasma. In some embodiments (not shown in <FIG>), a plasma-facing surface irradiated with ultraviolet radiation can be a part of a dielectric wall of a plasma chamber, as further described in <FIG>. The dielectric wall can have substantial electric fields when an RF power is being provided to an inductive coupling antenna. In some embodiments (not shown in <FIG>), ultraviolet irradiated surface can be a metal surface on an interior of a plasma chamber that has a line of sight to a region of the chamber interior that will contain plasma, as further described in <FIG>.

As can be seen in <FIG>, the ultraviolet light beam <NUM> is reflected onto the surface <NUM> via a reflective element (e.g., a mirror) <NUM>. Electrons <NUM> emitted from the surface <NUM> directly into the region <NUM> that will contain plasma.

The vacuum window <NUM> separates the UV source <NUM> from the plasma chamber interior <NUM>. The vacuum window <NUM> can be an ultraviolet transmissive window. For instance, the window <NUM> can have at least one of: synthetic quartz, UV-grade sapphire, magnesium fluoride (MgF2) material, or calcium fluoride (CaF2) material. As another example, a space between the ultraviolet light source(s) and the window can be filled with a gas (e.g., helium or nitrogen) to reduce UV absorption by atmospheric oxygen.

Claim 1:
A plasma processing apparatus (<NUM>), comprising:
a plasma chamber (<NUM>);
a dielectric wall (<NUM>) forming at least a portion of the plasma chamber (<NUM>);
an inductive coupling element (<NUM>) located proximate the dielectric wall (<NUM>);
an ultraviolet light source (<NUM>) configured to emit an ultraviolet light beam (<NUM>) onto a metal surface (<NUM>) that faces an interior volume of the plasma chamber (<NUM>), the metal surface (<NUM>) being a metal structure of the plasma chamber (<NUM>); and
a controller configured to control the ultraviolet light source (<NUM>) such that it emits the ultraviolet light beam (<NUM>) on the metal surface (<NUM>) prior to or at the same time as the inductive coupling element (<NUM>) being energized with radio frequency, RF, energy.