Abstract:
Embodiments of the present invention generally relate to an optical valve that modifies a laser beam to allow more energy to be irradiated onto less absorbing areas on a substrate and less energy to be irradiated onto more absorbing areas on the substrate, thus creating a more uniform heating field. The optical valve is a layered structure comprising a reflective switch layer, an absorbing layer, a thermal resistor and a thermal bath.
Abstract:
A method and apparatus for determining the temperature of a substrate within a processing chamber are described herein. The methods and apparatus described herein utilize an etalon assembly and a heterodyning effect to determine a first temperature of a substrate. The first temperature of the substrate is determined without physically contacting the substrate. A separate temperature sensor also measures a second temperature of the substrate and/or the substrate support at a similar location. The first temperature and the second temperature are utilized to calibrate one of the temperature sensors disposed within the substrate support, a model of the processes performed within the processing chamber, or to adjust a process parameter of the process performed within the processing chamber.
Abstract:
A thermal processing apparatus and method in which a first laser source, for example, a CO2 emitting at 10.6 μm is focused onto a silicon wafer as a line beam and a second laser source, for example, a GaAs laser bar emitting at 808 nm is focused onto the wafer as a larger beam surrounding the line beam. The two beams are scanned in synchronism in the direction of the narrow dimension of the line beam to create a narrow heating pulse from the line beam when activated by the larger beam. The energy of GaAs radiation is greater than the silicon bandgap energy and creates free carriers. The energy of the CO2 radiation is less than the silicon bandgap energy so silicon is otherwise transparent to it, but the long wavelength radiation is absorbed by the free carriers.
Abstract:
Apparatus and methods of treating a substrate with an amorphous semiconductor layer, or a semiconductor layer having small crystals, to form large crystals in the substrate are described. A treatment area of the substrate is identified and melted using a progressive melting process of delivering pulsed energy to the treatment area. The treatment area is then recrystallized using a progressive crystallization process of delivering pulsed energy to the area. The pulsed energy delivered during the progressive crystallization process is selected to convert the small crystals into large crystals as the melted material freezes.
Abstract:
A method and apparatus for decorrelating coherent light from a light source, such as a pulsed laser, in both time and space in an effort to provide intense and uniform illumination are provided. For some embodiments employing a pulsed light source, the output pulse may be stretched relative to the input pulse width. The methods and apparatus described herein may be incorporated into any application where intense, uniform illumination is desired, such as pulsed laser annealing, welding, ablating, and wafer stepper illuminating.
Abstract:
A method includes exposing a sample etalon-object to sample incident radiation, resulting in a sample transmitted radiation and sample reflected radiation; exposing a reference etalon-object to reference incident radiation, resulting in a reference transmitted radiation and reference reflected radiation; and analyzing resultant radiation for a heterodyned spectrum. The sample transmitted radiation may become the reference incident radiation, and the reference transmitted radiation may become the resultant radiation. The reference transmitted radiation may become the sample incident radiation, and the sample transmitted radiation may become the resultant radiation. The sample transmitted radiation may become the reference incident radiation, and the reference reflected radiation may become the resultant radiation. The reference transmitted radiation may become the sample incident radiation, and the sample reflected radiation may become the resultant radiation.
Abstract:
A calibration curve for a wafer comprising a layer on a substrate is determined. The calibration curve represents a local parameter change as a function of a treatment parameter associated with a wafer exposure to a light. The local parameter of the wafer is measured. An overlay error is determined based on the local parameter of the wafer. A treatment map is computed based on the calibration curve to correct the overlay error for the wafer. The treatment map represents the treatment parameter as a function of a location on the wafer.
Abstract:
A semiconductor processing method and semiconductor device are described. The processing method includes forming a p-doped germanium structure on a substrate, annealing the p-doped germanium structure using pulses of laser radiation, and forming a titanium structure in direct contact with the p-doped germanium structure.
Abstract:
A thermal processing apparatus and method in which a first laser source, for example, a CO2 emitting at 10.6 μm is focused onto a silicon wafer as a line beam and a second laser source, for example, a GaAs laser bar emitting at 808 nm is focused onto the wafer as a larger beam surrounding the line beam. The two beams are scanned in synchronism in the direction of the narrow dimension of the line beam to create a narrow heating pulse from the line beam when activated by the larger beam. The energy of GaAs radiation is greater than the silicon bandgap energy and creates free carriers. The energy of the CO2 radiation is less than the silicon bandgap energy so silicon is otherwise transparent to it, but the long wavelength radiation is absorbed by the free carriers.
Abstract:
Embodiments of the invention generally relate to pyrometry during thermal processing of semiconductor substrates. More specifically, embodiments of the invention relate to a pyrometry filter for a thermal process chamber. In certain embodiments, the pyrometry filter selectively filters selected wavelengths of energy to improve a pyrometer measurement. The pyrometry filter may have various geometries which may affect the functionality of the pyrometry filter.