WO1999000641A1 - Procede et appareil ameliores pour mesurer la concentration d'ions implantes dans des materiaux semi-conducteurs - Google Patents

Procede et appareil ameliores pour mesurer la concentration d'ions implantes dans des materiaux semi-conducteurs Download PDF

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Publication number
WO1999000641A1
WO1999000641A1 PCT/US1998/013473 US9813473W WO9900641A1 WO 1999000641 A1 WO1999000641 A1 WO 1999000641A1 US 9813473 W US9813473 W US 9813473W WO 9900641 A1 WO9900641 A1 WO 9900641A1
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Prior art keywords
concentration
signal waveform
ions implanted
pulse
pulses
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PCT/US1998/013473
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English (en)
Inventor
Matthew J. Banet
John A. Rogers
Martin Fuchs
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Koninklijke Philips Electronics N.V.
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
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Publication date
Priority claimed from US08/885,786 external-priority patent/US6052185A/en
Application filed by Koninklijke Philips Electronics N.V. filed Critical Koninklijke Philips Electronics N.V.
Priority to EP98932942A priority Critical patent/EP0944810A4/fr
Priority to JP11505843A priority patent/JP2001500976A/ja
Publication of WO1999000641A1 publication Critical patent/WO1999000641A1/fr

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    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
    • G—PHYSICS
    • G01—MEASURING; TESTING
    • G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
    • G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
    • G01N21/17—Systems in which incident light is modified in accordance with the properties of the material investigated
    • G01N21/1717—Systems in which incident light is modified in accordance with the properties of the material investigated with a modulation of one or more physical properties of the sample during the optical investigation, e.g. electro-reflectance

Definitions

  • microelectronic devices include a series of thin insulating (e.g. oxide) and conducting (e.g., metal and polysilicon) films grown or deposited on a single-crystal silicon wafer. Both silicon wafers and polysilicon films are implanted with ions during fabrication so that they exhibit a specified electrical conductance. For example, the silicon may be implanted to create regions that function as a "p" or "n" type semiconductor. After implantation, both silicon and polysilicon are annealed under high temperatures to heal lattice damage that typically results from the implantation process.
  • thin insulating e.g. oxide
  • conducting e.g., metal and polysilicon
  • silicon and polysilicon are strongly affected by three properties of the implanted ions: (1) atomic composition; (2) implantation energy; and (3) ion concentration or dose. Silicon's electrical conductivity is particularly dependent on the concentration of the implanted ions.
  • silicon wafers are typically implanted with arsenic, argon, phosphorous, oxygen, or boron ions ranging in concentration from 10 12 - 10 16 cm '3 . These ions are typically implanted with energies ranging from a few keV to thousands of keV.
  • the performance of a completed microelectronic device depends critically on the electrical properties of the silicon wafer and the overlying polysilicon films, and thus the properties of ions implanted in these materials are carefully monitored during fabrication.
  • One property, called electrical sheet resistance is measured by contacting a sample's surface with an electrical-testing instrument called a 4-point probe. Electrical current flowing from one probe to another depends on the resistance of the material. Resistance, in turn, varies inversely with the concentration of implanted ions .
  • Ion concentration is also monitored using a non-contact, optical method that excites and detects both a photothermal response and an electron-hole plasma within the silicon.
  • a first laser beam irradiates the silicon and is partially absorbed to generate either (or both) the electron-hole plasma and photothermal response. These responses modify the reflectivity of the sample's surface and are measured with a second laser beam. This is partially reflected by the sample and then analyzed to estimate the concentration of the implanted ions.
  • 4 -point probes and instruments that measure optical reflectivity suffer disadvantages. 4 -point probes necessarily contact the sample, and are therefore destructive.
  • Optical-reflectivity instruments have a limited scope of measurement and generate signals that are often difficult to interpret: they are therefore used primarily to determine whether or not a sample has been ion implanted with ions, rather than the actual concentration of the implanted ions. Summary
  • FWM four-wave mixing
  • FWM is carried out with a single laser. This allows measurement of samples that have been difficult or impossible to measure with the two-laser systems described previously.
  • FWM initiates an optical response in a semiconducting material with two laser beams. These beams, which have wavelengths that are strongly absorbed by the sample, are overlapped in time and space on the sample's surface to form a grating pattern.
  • Each laser beam includes pulses that typically have a duration of less than 1 nanosecond.
  • a third laser beam irradiates the grating pattern and is diffracted to form a fourth signal beam.
  • the amplitude of the signal beam depends on the concentration of the ions implanted in the semiconductor material . This concentration can then be analyzed and used to control fabrication processes used to make microelectronic devices.
  • the invention provides a method that determines a concentration of ions implanted in a material.
  • the method includes the steps of: 1) generating at least two excitation laser sub-pulses and a probe pulse from a single pulse emitted from a laser; 2) irradiating a region of the material with a grating pattern formed by overlapping at least two excitation laser sub-pulses to initiate a time-dependent response in the region; 3) diffracting a probe laser pulse off the region to generate at least one time-dependent signal beam; 4) detecting at least one time-dependent signal beam to generate a signal waveform; and 5) processing the signal waveform to determine the concentration of ions implanted in the material .
  • the method includes the step of generating a single laser pulse, and then passing the laser pulse through a diffracting mask to form at least two excitation sub-pulses and at least one probe pulse. Both excitation and probe pulses then irradiate the sample as described above to measure the concentration of ions implanted in the semiconductor.
  • a single pulse may function as both the excitation sub-pulse and the probe pulse (i.e., self diffraction).
  • the processing step described above includes determining a property of the signal waveform (e.g., an amplitude) and then processing the property to determine the concentration of ions implanted in the sample.
  • the processing step may include comparing the property of the signal waveform to a database, e.g., a database that correlates properties of previously measured signal waveforms to concentrations of implanted ions.
  • the processing step includes analyzing the amplitude with a mathematical algorithm to determine the concentration of ions implanted in the material .
  • the processing step can also, include digitizing the signal waveform to generate a data set, and then determining the amplitude of the signal waveform at a point in time by selecting a value from the data set.
  • the processing step includes determining an area covered by a plot of the signal waveform, and then comparing the area to a database similar to that described above.
  • the above-described method and apparatus determines the concentration of ions implanted in different types of host samples.
  • These samples include semiconducting materials, such as silicon-containing (e.g. polysilicon) films, silicon wafers, and films and wafers containing gallium arsenide, aluminum gallium arsenide, germanium, and derivatives and analogies thereof .
  • Other samples that can be measured include ceramic materials, metals, and any other material that can be implanted with ions.
  • the ion implanted in the material is typically an ion of an atom selected from the group including arsenic, argon, boron, oxygen and phosphorous atoms .
  • the method of the invention is carried out with an apparatus that includes: 1) a single laser that generates an excitation laser pulse and a probe laser pulse; 2) a first beam-delivery system that separates the excitation laser pulse into at least two sub-pulses and then irradiates a region of the material with a grating pattern formed by overlapping at least two sub-pulses; 3) a second beam-delivery system that delivers the probe pulse to the sample such that it diffracts off the region to generate a time-dependent signal beam; 4) a photodetector that detects the time-dependent signal beam to generate a signal waveform; and 5) a processor that processes the signal waveform to determine the concentration of ions implanted in the material .
  • the first beam-delivery system includes a diffracting mask (e.g., a phase or amplitude mask) that separates the excitation laser pulse into at least two sub-pulses.
  • the processor is typically a computer that analyzes an amplitude of the signal waveform and then compares the amplitude to a database to determine the concentration of ions implanted in the material.
  • the computer determines an area covered by the signal waveform, and then compares the area to a database to determine the concentration of ions implanted in the material.
  • the excitation sub-pulses and the probe pulse are overlapped in time in the region, and the photodetector has a bandwidth of less than 1 MHz .
  • Another apparatus that carries out the method of the invention includes a single laser and a beam-delivery system that includes a diffracting mask that separates the laser pulse into at least two excitation sub-pulses and a probe pulse.
  • the system also includes a lens that focuses and overlaps the two excitation sub-pulses and the probe pulse on the sample.
  • the sub-pulses form a grating pattern that initiates a time-dependent response in the region and the probe pulse diffracts off the region to generate a time-dependent signal beam.
  • FWM is an accurate, quantitative method for determining the concentration of ions implanted in both semiconductor substrates and thin films.
  • the method is all -optical, non-contact, and non-destructive, and can therefore measure semiconductor materials used in actual devices (i.e., production samples), rather than monitor samples. This information can then be used by manufacturers to improve both the yield and performance characteristics of microelectronic devices containing these materials.
  • the single-laser apparatus for making FWM measurements generates signal waveforms having very high signal-to-noise ratios and the apparatus has a large dynamic range of measurement.
  • This apparatus accurately measures samples, such as silicon wafers implanted with boron ions at low energies and concentrations, that in the past have been difficult to measure with conventional instrumentation, such as those using two lasers. Moreover, this instrument is compact, easily automated, has very few optical elements, and is relatively inexpensive to manufacture. Since the concentration of implanted ions can be measured in this way, it is not necessary to determine the waveform's time dependence. This signal amplitude can be measured with simple optical and electrical components (e.g., low-bandwidth photodetectors and analog-to-digital converters) that are typically low-cost and commercially available.
  • simple optical and electrical components e.g., low-bandwidth photodetectors and analog-to-digital converters
  • phase mask simplifies the alignment of the excitation and probe laser beams and also eliminates the need for additional beam-delivery optics, such as additional lenses and beam splitters, that are normally required for FWM experiments.
  • additional beam-delivery optics such as additional lenses and beam splitters, that are normally required for FWM experiments.
  • the number of required optical elements is even further reduced in embodiments where the phase mask diffracts an incident laser pulse to form both the excitation sub-pulses and the probe pulse.
  • Measurements with the above-mentioned apparatus are made rapidly (typically requiring only a few seconds) and with high spatial resolution (typically using a probe beam having a spot size of about 50 microns or less) .
  • small features of the sample such as a small-scale test site of a microelectronic device or an area near a wafer's edge, can be easily measured.
  • the above-mentioned apparatus can be incorporated into a facile, compact, easy-to-use instrument that can be employed in a microelectronic-device fabrication facility.
  • the instrument for example, can be attached to a production tool and used to make in si tu measurements of an ion-implantation process.
  • Fig. 1 is a schematic drawing of the FWM method
  • Fig. 2 is a graph of a signal measured during FWM with a single-laser optical system
  • Figs. 3A-3B are graphs of the signal waveform amplitude (in mV) vs. the ion implant concentration measured from a set of silicon wafers implanted with different concentrations of boron ions at 3 and 5 keV
  • Fig. 4 is a schematic drawing of a single-laser optical system for measuring the concentration of ions implanted in a sample using FWM
  • Fig. 5 is a drawing of a single laser beam being diffracted to form two excitation sub-pulses and a probe pulse .
  • the concentration of ions implanted in a sample 10 is measured with an optical, laser-based technique called four-wave mixing (FWM) .
  • FWM optical, laser-based technique
  • ISS impulsive stimulated scattering
  • ISTS impulsive stimulated thermal scattering
  • MEASUREMENT OF MATERIAL PROPERTIES WITH OPTICALLY INDUCED PHONONS U.S. Patent 5,633,711
  • SIMPLIFIED DEVICE AND METHOD FOR TIME-RESOLVED OPTICAL MEASUREMENTS U.S.S.N.
  • a pair of optical excitation sub-pulses 12', 12'' from a laser (not shown in the figure) separated by an angle ⁇ are overlapped in time and space in a region on the sample's surf ce. Interference between the overlapped sub-pulses 12', 12'' forms a spatially varying "grating" pattern 15 containing alternating "light” (constructive interference) 17 and “dark” (destructive interference) 19 regions.
  • the sample 10 absorbs radiation in the light regions 17, but not in the dark regions 19 of the grating pattern 15. The absorbed radiation initiates a time-dependent response characterized by an amplitude that depends on the concentration of the ions implanted in the sample 10.
  • This response is measured by irradiating a region near the grating pattern 15 with a probe pulse 20 generated by the same laser that generates the excitation sub-pulses 12' , 12 ' ' .
  • the probe pulse 20 is overlapped in time and space with these sub-pulses on the sample's surface. This means that prior to irradiating the sample, the distance traveled by the excitation sub-pulses and the probe pulse after leaving the single-laser source is roughly equivalent.
  • these three pulses are overlapped in this way, the probe pulse is partially reflected to form a reflected beam 20'', and partially diffracted to form a pair of signal beams 25', 25'' that_ are the +1 and -1 diffracted orders.
  • One or both of the signal beams 25', 25'' is detected with a photodetector (not shown in the figure) to generate a signal waveform.
  • the amplitude of the signal waveform is then analyzed to determine the concentration of the implanted ions.
  • the excitation sub-pulses 12', 12'' typically have a duration of between 0.3 - 0.7 nanoseconds (i.e., 0.3 - 0.7 x 10 's seconds) , an energy of about 2 microjoules/pulse, and a wavelength that is partially absorbed by the sample.
  • the wavelength is typically in the visible spectral region (e.g., 532 nm) . Since it is generated with the same laser, the probe pulse has the same wavelength and duration as the excitation pulse.
  • the energy of the probe pulse is typically between 0.25 and 1.0 microjoules.
  • FWM generates a response in the sample when the excitation radiation has an energy that is above the band gap of the sample (for silicon, this is about 1.1 eV, an energy that corresponds to an optical wavelength of or 900 nm) .
  • the excitation pattern in FWM generates excited-state charge carriers (e.g., electron-hole pairs) in the light regions, but not the dark regions of the grating pattern.
  • the density of charge carriers depends on the concentration of ions implanted in the sample. Once generated, the charge carriers have a finite lifetime and recombine with a time constant on the order of several nanoseconds.
  • the sample's refractive index in the light regions is temporarily changed relative to the refractive index in the dark regions.
  • the diffraction efficiency is highest immediately after the charge carriers are formed, and thus the probe pulse is arranged to impinge on the sample at essentially zero time delay (i.e., the excitation sub-pulses and probe pulse are overlapped in time) .
  • a higher concentration of implanted ions results in a larger number of excited charge carriers and, consequently, a greater difference in refractive index between the light and dark regions of the grating pattern. This, in turn, increases both the diffraction efficiency of the phase grating and the intensity of the diffracted probe beam.
  • Fig. 2 shows a signal waveform 30 measured during FWM from a boron- implanted silicon wafer.
  • the film was implanted with an average concentration of approximately 0.5 x 10 14 cm "3 boron ions at an energy of about 20 keV. Measurements were made with excitation sub-pulses having a wavelength of 532 nm, a duration of about 0.5 nanoseconds, and an energy of about 2.0 microjoules/sub-pulse .
  • the sub-pulses were generated by frequency-doubling the fundamental output from a Nd:YAG laser, and then passing this output through a phase mask (described in more detail with reference to Fig. 4) .
  • the probe pulse was generated by the same laser, and had an energy of about 0.5 microjoules/pulse .
  • the optical path length traveled by the excitation and probe pulses was roughly identical .
  • the signal waveform was measured with a photodetector and analog-to-digital converter that in combination have a bandwidth of about 1 GHz
  • the signal waveform 30 rises rapidly and then decreases in intensity to form a spike having an asymmetric shape.
  • the full -width half-maximum (FWHM) of the spike is roughly equal to the duration of the excitation and probe pulses (about 0.5 ns) .
  • the amplitude of the signal waveform shown as being about 575 mV, depends on the concentration of ions implanted in the silicon sample (0.5 x 10 14 cm '3 in this case) .
  • the signal waveform also includes an oscillatory component 32 that is due to an electronic "ringing" in the photodetector.
  • Figs. 3A and 3B show how the amplitude of the signal waveform varies with the concentration of implanted ions.
  • electronic responses were measured from a set of 100 -mm diameter silicon wafers implanted with boron ions ranging from 1.5 - 3.0 x 10 15 cm "3 .
  • the implant energies for Figs. 3A and 3B were, respectively, 3 and 5 keV.
  • the data were measured from a center point of each wafer using FWM and the same single-laser instrument described above.
  • the data show that the signal waveform amplitude increases systematically with the concentration of implanted ions for each of the implantation energies. Similar dependencies of signal waveform amplitude on ion concentration were observed with boron, arsenic, oxygen, and phosphorous ions implanted in silicon wafers at energies ranging from 1-1000 keV and concentrations ranging from 1.0 x 10 12 to 1.0 x 10 16 cm "3 .
  • silicon wafers with ions implanted at concentrations of 1.0 x 10 12 cm “3 display signal levels of a few hundred mV, while wafers implanted with ions implanted at concentrations of 1.0 x 10 16 cm “3 have signal levels of about 1000 mV.
  • data like that shown in Figs. 3A-3B is measured from a set of samples which vary systematically in one or more properties (e.g., concentration) , and then stored in a database on a computer.
  • concentration e.g., concentration
  • the dependence of signal amplitude on concentration may depend on process conditions such as implant species, temperature, current, and orientation of the wafer relative to the incident ion beam.
  • separate databases each containing a data set similar to that shown in Figs. 3A-3B, is typically generated for each process condition.
  • the data can be measured from a set of test samples having a systematically varying concentration of implanted ions whose concentrations are verified with electrical testing instruments, such as a 4 -point probe.
  • the amplitude of a signal waveform is measured with FWM as described above, and then compared to a value in the appropriate database. This determines the concentration of ions implanted in a sample during an actual fabrication process.
  • FIG. 4 shows an optical system 50 for measuring the properties of an ion-implanted sample 10 using FWM.
  • the system 50 includes a single laser 52, such as a Nd:YAG laser, that generates a pulse 49 having the optical properties described above.
  • the pulse 49 irradiates a beamsplitter 51 that partially reflects a small portion (e.g. typically 5-15%) of the pulse 49 to form a probe pulse 20, and transmits the remainder of the pulse 49 to form the excitation pulse 12.
  • the excitation pulse 12 then irradiates a mirror 53 that reflects it through a first collimating lens 60 and then through a neutral -density filter 61 used for adjusting the pulse energy.
  • the pulse is then focused onto a phase mask 62 with a cylindrical lens 64.
  • the phase mask 62 includes a series of patterns 66, each of which is capable of generating a different grating pattern 15 on the sample 10.
  • the appropriate pattern is selected to produce the desired grating pattern on the sample.
  • the excitation pulse 12 is diffracted into two sub-pulses 12', 12'' that diverge at an angle ⁇ determined by the selected pattern 66.
  • the diverging sub-pulses 12', 12'' are collected with a first imaging lens 70 that focuses and overlaps them onto the surface of the sample 10 to form the grating pattern 15.
  • the first imaging lens 70 is positioned so that the grating pattern 15 has one half of the periodicity of the pattern 66 on the phase mask 62.
  • Different grating patterns can be formed simply by translating the phase mask 62 so that a new pattern is irradiated with the incident excitation pulse 12.
  • the probe pulse 20 is split prior to the collimating lens 60, and thus it spatially diverges over its optical path length, thereby allowing the pulse 20 to be focused to a smaller spot on the sample.
  • a portion 20' of the pulse 20 is reflected by a beam-splitter 65 and detected with a trigger photodetector 67 to generate an electrical pulse for triggering a data-acquisition system.
  • the portion of the probe pulse 20 that passes through the beam-splitter 65 is reflected by a pair of mirrors 21a, 21b and then focused on the grating pattern 15 with a second spherical lens 71 to measure the ion-implanted sample 10.
  • the spacing between the mirrors 21a, 21b is adjusted so that the optical path lengths of the excitation sub-pulses (12' and 12'') and the pulse probe 20 are approximately equal. This overlaps these pulses in time on the sample's surface, thereby ensuring that the maximum signal amplitude (which occurs at zero delay of the probe pulse) will be measured.
  • the sample diffracts a portion of the probe pulse 20 to form a signal beam 25' .
  • a beam-stop 80 blocks a reflected portion of the probe pulse 20''.
  • a second imaging lens 76 collects the signal beam 25' and focuses it into a high-speed (e.g., 1 GHz) photodetector 82. This generates a light-induced electrical signal which is then passes through an analog-to-digital converter 83 to produce a digital signal that is analyzed by a computer 84 which is programmed with an analysis algorithm to determine the concentration of ions implanted in the sample.
  • the analysis algorithm is stored in a computer readable medium from where it is loaded in executable form into RAM memory of the computer.
  • the spatial dimensions of the excitation sub-pulses 12', 12'' and probe pulse 20 focused onto the sample are chosen to maximize the amplitude of the signal waveform.
  • the excitation sub-pulses are typically overlapped to form an elliptical grating pattern with the long and short axes of the ellipse being roughly 150 and 25 microns, respectively.
  • the distance between light and dark regions in the grating pattern is typically between 5 and 15 microns.
  • the probe pulse is typically focused to a round spot that lies completely within the grating pattern. For example, the probe pulse can be focused to a round spot with a diameter of less than 25 microns.
  • Fig. 5 shows another optical configuration 85 for generating both excitation sub-pulses 12', 12'' and a probe pulse 13 from a single laser beam.
  • a single pulse 12 from a laser (not shown in the figure) irradiates a pattern 66 on a phase mask 62 as described above.
  • the pattern is chosen so that a majority (e.g., 85%) of the pulse 12 is diffracted into the +/-1 orders to form the excitation sub-pulses 12', 12''.
  • the portion of the incident pulse 12 diffracted into the +2 (or -2) order forms the probe pulse 13.
  • the excitation sub-pulses 12', 12'' and probe pulse 13 are collected with a single lens (such as lens 70 in Fig. 4) and then focused onto the sample as described above to measure the ion implantation concentration.
  • a mirror may be inserted into the optical system shown in Fig. 5 to reflect the probe pulse through the lens and toward the sample.
  • three sub-pulses are used to excite the sample in a FWM arrangement.
  • the three sub-pulses are equally spaced in a linear fashion (i.e., the center, right, and left beams) prior to being imaged onto the sample.
  • the center beam propagates down a central optical axis of a beam-delivery system, while the right and left beams converge toward the same spot at the same angle but on opposite sides of the center beam.
  • the beams are overlapped on the sample to form the grating pattern that excites charge carriers in the sample.
  • any optical system for performing ISS, ISTS or FWM is suitable to measure the concentration of implanted ions using the method described above.
  • other lasers that have suitable optical properties can be used in place of the Nd:YAG laser described above.
  • FWM measurements can be performed using two synchronized lasers in place of the single laser described above.
  • Each of the synchronized lasers generates a short (e.g., 0.5 ns) optical pulse, one which represents the excitation pulse, and the other laser which represents the probe pulse.
  • the resulting two laser beams are oriented so that pulses are overlapped in time on the sample's surface.
  • the system uses multiple probe pulses, each of which is delayed in of time relative to the others, to measure a decay time constant of the excited charge carriers. For example, the system uses a first probe pulse to irradiate the sample at zero time delay, and then it uses a second pulse, which is mechanically delayed, to irradiate the sample a few nanoseconds later. The first pulse will produce a signal having a given amplitude and the second, later pulse will produce a signal having a lower amplitude. The change in amplitude represents a decay process (e.g. exponential decay process) that can be characterized by a time constant.
  • the computer analyzes the two signal waveforms generated by the two probe pulses and determines the decay time constant for the charge carriers.
  • the computer uses the decay time constant to determine the implantation energy, possibly employing stored tables of empirically derived data to perform a translation from one to the other.
  • a signal waveform is measured as described in the parent patent application (U.S.S.N. 08/885,786), i.e., using two independent lasers.
  • the decay time constant of the waveform can be computed and processed in the manner described above to determine the energy at which the ions were implanted.
  • the apparatus can be modified to additionally measure the thickness of thin oxide (i.e. Si0 2 ) films that are grown on a silicon sample when the sample is subjected to high temperatures.
  • the computer can analyze the reflected probe beam (20" in Fig. 4) in the same way that reflected beams are analyzed in standard ellipsometers or reflectometers .
  • sets of excitation sub-pulses having different wavelengths can be generated and used to simultaneously generate grating patterns in the sample being measured.
  • the intensity of the diffracted signal beams can be analyzed to determine the species of the implanted ions.
  • the apparatus can be modified to simultaneously measure physical processes that result in phase gratings (e.g., excited charge carriers) and surface ripple (e.g., thermal processes) in the sample.
  • thermal processes that generate surface ripple in the sample will have a time dependence and diffraction efficiency that varies with the phase mask pattern (and thus the spatial periodicity of the grating pattern) used during the measurement.
  • time dependance of non-diffusive processes such as charge carrier lifetimes
  • these processes can be determined independently by measuring a sample at a number at different phase mask patters.
  • a probe laser that generates a pulse having a long duration (e.g., several microseconds) relative to the lifetime of the charge carriers can be included in the optical system. This way, measurements can simultaneously be performed with probe pulses having different time durations and peak intensities.
  • the polarization of the diffracted probe pulse can be analyzed to determine certain properties of the sample, such as oxide film thickness and implant species .
  • the signal waveform can be processed by plotting it and then determining the area underneath the plot. This area is then compared to values in a database to determine the ion concentration.
  • the signal waveform is fit to a function to determine its amplitude, which is then processed as described above.
  • mathematical algorithms such as algorithms based on kinetic modeling of a charge-carrier system, can be developed to relate the concentration of implanted ions to an amplitude of the signal waveform. Such algorithms would obviate the need for a database to determine the ion concentration.
  • laser beams that are not pulsed are used in the FWM arrangement to determine the concentration of ions in the sample.
  • the amplitude of the diffracted signal beam correlates to the ion concentration.
  • the signal beam may be detected using standard detection techniques known in the art, such as lock-in detection.

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Abstract

Cette invention se rapporte à un procédé et à un appareil, qui servent à déterminer la concentration d'ions implantés dans un matériau et qui à cet effet consistent: (1) à produire au moins deux sous-impulsions laser d'excitation et une impulsion de sonde à partir d'une seule impulsion émise par un laser; (2) à exposer une région dudit matériau à un rayonnement ayant un réseau de diffraction formé par chevauchement d'au moins deux sous-impulsions laser d'excitation, afin d'initialiser dans la région en question une réponse dépendant du temps; (3) à provoquer la diffraction d'une impulsion laser de sonde dans la direction opposée à la région en question, de façon à produire au moins un faisceau de signal dépendant du temps; (4) à détecter au moins un faisceau de signal dépendant du temps, afin de produire une forme d'onde de signal; et (5) à traiter la forme d'onde de signal pour déterminer la concentration d'ions implantés dans le matériau en question.
PCT/US1998/013473 1997-06-30 1998-06-26 Procede et appareil ameliores pour mesurer la concentration d'ions implantes dans des materiaux semi-conducteurs WO1999000641A1 (fr)

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Application Number Priority Date Filing Date Title
EP98932942A EP0944810A4 (fr) 1997-06-30 1998-06-26 Procede et appareil ameliores pour mesurer la concentration d'ions implantes dans des materiaux semi-conducteurs
JP11505843A JP2001500976A (ja) 1997-06-30 1998-06-26 半導体材料の中に注入されたイオンの濃度を測定するための改善された方法及び装置

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Application Number Priority Date Filing Date Title
US08/885,786 US6052185A (en) 1997-06-30 1997-06-30 Method and apparatus for measuring the concentration of ions implanted in semiconductor materials
US08/885,786 1997-06-30
US08/926,850 US6118533A (en) 1997-06-30 1997-09-10 Method and apparatus for measuring the concentration of ions implanted in semiconductor materials
US08/926,850 1997-09-10

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EP (1) EP0944810A4 (fr)
JP (1) JP2001500976A (fr)
WO (1) WO1999000641A1 (fr)

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WO1999061866A1 (fr) * 1998-05-28 1999-12-02 Koninklijke Philips Electronics N.V. Dispositif et procede permettant de mesurer une caracteristique d'une structure
US6181431B1 (en) * 1997-12-19 2001-01-30 Bernard Siu System and method for laser ultrasonic bond integrity evaluation

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US5734470A (en) * 1995-01-24 1998-03-31 Massachusetts Institute Of Technology Device and method for time-resolved optical measurements

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US5734470A (en) * 1995-01-24 1998-03-31 Massachusetts Institute Of Technology Device and method for time-resolved optical measurements

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Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6181431B1 (en) * 1997-12-19 2001-01-30 Bernard Siu System and method for laser ultrasonic bond integrity evaluation
US6490047B2 (en) 1997-12-19 2002-12-03 Bernard K. Siu System and method for laser ultrasonic bond integrity evaluation
WO1999061866A1 (fr) * 1998-05-28 1999-12-02 Koninklijke Philips Electronics N.V. Dispositif et procede permettant de mesurer une caracteristique d'une structure
US6795198B1 (en) 1998-05-28 2004-09-21 Martin Fuchs Method and device for measuring thin films and semiconductor substrates using reflection mode geometry

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JP2001500976A (ja) 2001-01-23
EP0944810A1 (fr) 1999-09-29
EP0944810A4 (fr) 2007-08-08

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