Tokyo Electron Limited

Justin Moses

Merritt Funk

Chelsea Dubose

Barton Lane

Yohei Yamazawa

Kazuki Moyama

Kazushi Kaneko

Michael Hummel

Alok Ranjan

Peter Ventzek

Megan Doppel

In one exemplary embodiment described herein are innovative plasma processing methods and system that utilize direct measurement of direct current (DC) field or self-bias voltage (Vdc) in a plasma processing chamber. In one embodiment, a non-plasma contact measurement using the electric field effect from Vdc is provided. The Vdc sensing method may be robust to a variety of process conditions. In one embodiment, the sensor is integrated with any focus ring material (for example, quartz or doped-undoped silicon). Robust extraction of the Vdc measurement signal may be used for process control. In one embodiment, the sensor may be integrated, at least in part, with the substrate being processed in the chamber.

Process control enabled VDC sensor for plasma process

A radio frequency (RF) system including: a first conductive covering surface, a portion of the first conductive covering surface including a portion of the first outer wall of a first RF device; a second conductive covering surface aligned to the first conductive covering surface, the second conductive covering surface being disposed around the insulating hole; an insulating hole for an RF center conductor extending through the first conductive covering surface and the second conductive covering surface, the first conductive covering surface and the second conductive covering surface being disposed around the insulating hole; a cavity bounded by the first conductive covering surface and the second conductive covering surface, the cavity being an insulating region; and an RF signal pickup disposed within the cavity.

Radio frequency (RF) system with embedded RF signal pickups

A radio frequency sensor assembly includes a sensor casing disposed around a central hole, the sensor casing including a first conductive cover and a second conductive cover. The assembly includes a cavity disposed around the central hole and includes a dielectric material, the cavity being bounded by a first major outer surface and a second major outer surface along a radial direction from a center of the central hole, where the first conductive cover is electrically coupled to the second conductive cover through a coupling region beyond the second major outer surface of the cavity, and electrically insulated from the second conductive cover by the cavity and the central hole. The assembly includes a current sensor electrically insulated from the sensor casing and including a current pickup disposed symmetrically around the central hole, the current pickup being disposed within the cavity and being insulated from the sensor casing.

RF voltage and current (V-I) sensors and measurement methods

According to an embodiment, a radiating structure of a resonating structure used for plasma processing is disclosed. The radiating structure includes a set of first arms and a set of second arms. Each first arm has a first inductance and is coupled to a respective first capacitor and a respective second capacitor of the resonating structure to form a corresponding first resonant circuit operating at a first resonance frequency. Each second arm has a second inductance and is coupled to a respective third capacitor and a respective fourth capacitor of the resonating structure to form a corresponding second resonant circuit operating at a second resonance frequency. In a first mode of operation, the resonating structure operates as a single resonance antenna. In a second mode of operation, the resonating structure operates as a parallel resonance antenna.

Parallel resonance antenna for radial plasma control

Embodiments are described herein for power generation systems and methods that use quadrature splitters and combiners to facilitate plasma stability and control. For one embodiment, a quadrature splitter receives an input signal and generates a first and second signals as outputs with the second signal being ninety degrees out of phase with respect to the first signal. Two amplifiers then generate a first and second amplified signals. A quadrature combiner receives the first and second amplified signals and generates a combined amplified signal that represents re-aligned versions of the first and second amplified signals. The power amplifiers can be combined into a system to generate a high power output to a processing chamber. Further, detectors can generate measurements used to monitor and control power generation. The power amplifiers, system, and methods provide significant advantages for high-power generation delivered to process chambers for plasma generation during plasma processing.

Power generation systems and methods for plasma stability and control

A radio frequency (RF) system includes a RF power source configured to power a load with an RF signal; an RF pipe including an inner conductor and an outer conductor connected to ground coupling the RF power source to the load; and a current sensor aligned to a central axis of the RF pipe carrying the RF signal. A sensor casing is disposed around the RF pipe, where the sensor casing includes a conductive material connected to the outer conductor of the RF pipe. A gallery is disposed within the sensor casing and outside the outer conductor of the RF pipe, where the current sensor is disposed in the gallery. A slit in the outer conductor of the RF pipe exposes the current sensor to a magnetic field due to the current of the RF signal in the inner conductor of the RF pipe.

Methods and systems are disclosed for focus ring thickness measurement and feedback control within process chambers. For disclosed embodiments, in-chamber sensors measure physical parameters associated with focus rings, and these measurements are used to determine thickness for the focus rings. The thickness determinations can be used to detect when a focus ring should be replaced and can also be used as feedback to adjust the position of the focus rings within the chamber. For one embodiment, measurements from ultrasonic sensors are used to make thickness determinations for focus rings. For further embodiments, these ultrasonic sensors are positioned at end portions of focus ring lift pins. Other sensors can also be used such as capacitive sensors, resistive sensors, and/or other desired sensors. Further variations and implementations can also be achieved using in-chambers sensors to facilitate focus ring thickness determinations.

Methods and systems for focus ring thickness determinations and feedback control

Embodiments are described for modules, multi-stage systems, and related methods for radio frequency (RF) power amplifiers with reduced size and weight requirements. Fluid cooling is incorporated directly into the power amplifier (PA) module design rather than requiring PA modules to be mounted on separate cooling devices. For one embodiment, a PA module includes a circuit board, RF circuit components, a ground plane, and a cooling plate having one or more cooling channels to receive a cooling fluid. The cooling channels are positioned to dissipate heat from the RF circuit components through the ground plane. For a further embodiment, the PA module also includes RF bias and power electronics within a housing for the PA module without requiring an external control board or power conversion electronics. Also disclosed are multi-stage PA systems having a plurality of PA modules that are similarly cooled using cooling channels.

Modules, multi-stage systems, and related methods for radio frequency power amplifiers

Embodiments of method and system for controlling plasma performance are described. In an embodiment a method may include supplying power at a first set of power parameters to a plasma chamber. Additionally, the method may include forming plasma within the plasma chamber using the first set of power parameters. The method may also include measuring power coupling to the plasma at the first set of power parameters. Also, the method may include supplying power at a second set of power parameters to the plasma chamber. The method may additionally include measuring power coupling to the plasma at the second set of power parameters to the plasma. The method may also include adjusting the first set of power parameters based, at least in part, on the measuring of the power coupling at the second set of power parameters.

Growing community of inventors

Austin, TX, United States of America

Justin Moses