Tokyo Electron Limited

Other

Zhiying Chen

Lee Chen

Merritt Funk

Peter Ventzek

Alok Ranjan

Jianping Zhao

Joel Blakeney

Toshihisa Nozawa

Kazuya Nagaseki

Radha Sundararajan

Toshihiko Iwao

Peter Lowell George Ventzek

Megan Carruth

Barton Lane

Yun Han

Qiang Wang

A method of characterizing a plasma in a plasma processing chamber that includes: sustaining a plasma generated from a process gas in a plasma processing chamber; flowing a probe gas through the plasma processing chamber; obtaining spatially-resolved OES signals at a wavelength of an optical emission line of the probe gas within the plasma processing chamber, signal intensities of the spatially-resolved OES signals being correlated to a plasma parameter of the plasma, the plasma parameter having a spatial distribution within the plasma processing chamber; and based on the spatially-resolved OES signals, constructing a 3D map of OES signals by data fitting of the spatially-resolved OES signals with a computation model; and converting the 3D map of OES signals into a 3D map of the plasma parameter, the 3D map of the plasma parameter including information about the spatial distribution.

Non-intrusive method for 2D/3D mapping plasma parameters

Embodiments of hybrid electron beam and RF plasma systems and methods are described. In an embodiment a method of using a hybrid electron beam and RF plasma system may include forming a first plasma of a first type in a first region of a wafer processing structure. Additionally, such a method may include forming a second plasma of a second type in a second region of the wafer processing structure, the second region of the wafer processing structure being coupled to the first region of the wafer processing structure, the second plasma being ignited independently of the first plasma, wherein an electron beam formed by the first plasma is configured to modulate one or more characteristics of the second plasma. This hybrid e-beam and RF plasma system provides a source to control electron energy distribution function.

Tailored electron energy distribution function by new plasma source: hybrid electron beam and RF plasma

A method for plasma processing includes: sustaining a plasma in a plasma processing chamber, the plasma processing chamber including a first radio frequency (RF) electrode and a second RF electrode, where sustaining the plasma includes: coupling an RF source signal to the first RF electrode; and coupling a bias signal between the first RF electrode and the second RF electrode, the bias signal having a bipolar DC (B-DC) waveform including a plurality of B-DC pulses, each of the B-DC pulses including: a negative bias duration during which the pulse has negative polarity relative to a reference potential, a positive bias duration during which the pulse has positive polarity relative to the reference potential, and a neutral bias duration during which the pulse has neutral polarity relative to the reference potential.

Plasma processing with radio frequency (RF) source and bias signal waveforms

This disclosure relates to a plasma processing system for controlling plasma density near the edge or perimeter of a substrate that is being processed. The plasma processing system may include a plasma chamber that can receive and process the substrate using plasma for etching the substrate, doping the substrate, or depositing a film on the substrate. This disclosure relates to a plasma processing system for controlling plasma density near the edge or perimeter of a substrate that is being processed. In one embodiment, the plasma density may be controlled by reducing the rate of loss of ions to the chamber wall during processing. This may include biasing a dual electrode ring assembly in the plasma chamber to alter the potential difference between the chamber wall region and the bulk plasma region.

Electric pressure systems for control of plasma properties and uniformity

A method of plasma processing comprises generating electrons in a source chamber, generating an electric potential gradient between the source chamber and a processing chamber by applying a first negative direct current (DC) voltage to the source chamber and a ground voltage to the processing chamber, accelerating the electrons from the source chamber through a dielectric injector and into the processing chamber using the electric potential gradient, and generating an electron-beam sustained plasma (ESP) in the processing chamber using the electrons from the source chamber.

Apparatuses and methods for plasma processing

A measurement system for a plasma processing system includes a detector and an ion current meter coupled to the ion current collector and configured to provide a signal based on the measurements from the ion current collector. The detector includes an insulating substrate including a cavity, an ion angle selection grid configured to be exposed to a bulk plasma disposed in an upper portion of the cavity, and an ion current collector disposed within the cavity at an opposite side of the cavity below the ion angle selection grid. The ion angle selection grid includes an ion angle selection substrate and a plurality of through openings extending through the ion angle selection substrate, where each of the plurality of through openings has a depth into the ion angle selection substrate and a width orthogonal to the depth, where a ratio of the depth to the width is greater than or equal to 40.

Ion angle detector

Embodiments of hybrid electron beam and RF plasma systems and methods are described. In an embodiment a method of using a hybrid electron beam and RF plasma system may include forming a field of electrons a first region of a wafer processing structure. Such a method may also include forming a processing plasma in a second region of the wafer processing structure, the second region of the wafer processing structure being coupled to the first region of the wafer processing structure, the processing plasma being maintained by a combination of energy from a radiant energy source and from an electron beam formed from electrons in the field of electrons. Additionally, the method may include controlling a radical composition and ions of the processing plasma by setting a ratio of the energy supplied to the processing plasma from the electron beam and the energy supplied to the processing plasma from the radiant energy source.

Hybrid electron beam and RF plasma system for controlled content of radicals and ions

A process is provided in which a hard mask material comprising ruthenium is used. Ruthenium provides a hard mask material that is etch resistant to many of the plasma chemistries typically used for processing substrate patterning layers, including layers such as, for example, nitrides, oxides, anti-reflective coating (ARC) materials, etc. Further, ruthenium may be removed by plasma chemistries that do not remove nitrides, oxides, ARC materials, etc. For example, ruthenium may be easily removed through the use of an oxygen (O2) plasma. Further, ruthenium may be deposited as a thin planar 10 nm order film over oxides and nitrides and may be deposited as a planar layer.

Ruthenium hard mask process

An apparatus comprises an electron source chamber, an electron-beam sustained plasma (ESP) processing chamber, and a dielectric injector disposed between the electron source chamber and the ESP processing chamber. The dielectric injector comprises a first flared input region comprising a wide entry opening and a narrow exit opening. The wide entry opening opens into to the electron source chamber. The first flared input region is radially symmetric about a longitudinal axis of the dielectric injector. The dielectric injector further comprises a first parallel region comprising an input opening and an output opening. The input opening is adjacent to the narrow exit opening. The output opening is disposed opposite of the input opening. The first parallel region is cylindrical.

Plasma processing apparatuses having a dielectric injector

A plasma processing apparatus includes a processing chamber, a substrate disposed in the processing chamber, and a plurality of electron sources configured to supply electrons to a plasma generated in the processing chamber. Each of the plurality of electron sources includes a first side facing the plasma in the processing chamber. Each of the plurality of electron sources also includes a resonant structure disposed at the first side and configured to be held at a negative direct current bias voltage.

Plasma processing apparatuses including multiple electron sources

A method of plasma processing includes generating a first sequence of source power pulses, generating a second sequence of bias power pulses, combining the bias power pulses of the second sequence with the source power pulses of the first sequence to form a combined sequence of alternating source power pulses and bias power pulses, and, using the combined sequence, generating a plasma comprising ions and processing a substrate by delivering the ions to a major surface of the substrate.

Systems and methods of control for plasma processing

A processing system is disclosed, having an electron beam source chamber that excites plasma to generate an electron beam, and an ion beam source chamber that houses a substrate and also excites plasma to generate an ion beam. The processing system also includes a dielectric injector coupling the electron beam source chamber to the ion beam source chamber that simultaneously injects the electron beam and the ion beam and propels the electron beam and the ion beam in opposite directions. The voltage potential gradient between the electron beam source chamber and the ion beam source chamber generates an energy field that is sufficient to maintain the electron beam and ion beam as a plasma treats the substrate so that radio frequency (RF) power initially applied to the processing system to generate the electron beam can be terminated thus improving the power efficiency of the processing system.

Self-sustained non-ambipolar direct current (DC) plasma at low power

This disclosure relates to a plasma processing system for controlling plasma density near the edge or perimeter of a substrate that is being processed. The plasma processing system may include a plasma chamber that can receive and process the substrate using plasma for etching the substrate, doping the substrate, or depositing a film on the substrate. This disclosure relates to a plasma processing system that may be configured to enable non-ambipolar diffusion to counter ion loss to the chamber wall. The plasma processing system may include a ring cavity coupled to the plasma processing system that is in fluid communication with plasma generated in the plasma processing system. The ring cavity may be coupled to a power source to form plasma that may diffuse ions into the plasma processing system to minimize the impact of ion loss to the chamber wall.

Non-ambipolar electric pressure plasma uniformity control

This disclosure relates to a plasma processing system for controlling plasma density across a substrate and maintaining a tight ion energy distribution within the plasma. In one embodiment, this may include using a dual plasma chamber system including a non-ambipolar plasma chamber and a DC plasma chamber adjacent to the non-ambipolar system. The DC plasma chamber provide power to generate the plasma by rotating the incoming power between four inputs from a VHF power source. In one instance, the power to each of the four inputs are at least 90 degrees out of phase from each other.

Growing community of inventors

Austin, TX, United States of America

Zhiying Chen