JP2013120935A - Method of characterizing semiconductor light-emitting device on the basis of features of product wafer - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide a method of characterizing a semiconductor light-emitting device (LED) on the basis of the characteristics of a product wafer.SOLUTION: The method of characterizing a semiconductor light-emitting device includes a step for measuring at least one characteristic, such as the curvature or the device layer stress, of a product wafer. The relationship of at least one characteristic and the emission wavelength of an LED die formed of a product wafer is established. According to the relationship, emission wavelength from an LED structure formed on the device layer of a product wafer formed similarly is predicted. This method may also be used for characterizing a product wafer, more specifically an LED structure formed on the product wafer, and may be used for process control when manufacturing a large capacity LED.

Description

Priority claim

  This application claims the priority based on the US provisional application (No. 61 / 567,820) for which it applied on December 7, 2012, and uses the provisional application.

  The present invention relates primarily to the manufacture of semiconductor light emitting devices (LEDs) such as light emitting diodes and laser diodes, and specifically to a method for characterizing semiconductor LEDs based on product wafer characteristics.

  Semiconductor LEDs, such as light emitting diodes and laser diodes, are rapidly spreading as an alternative to conventional light sources in almost all areas of light and lighting applications. As a result, semiconductor LEDs have been adapted to emission wavelengths in a very wide range while increasing the number of manufacturing.

  Examples of semiconductor LEDs used for general illumination include light emitting diodes (also called “LEDs”) and diode lasers. A phosphor coating can be used to form a “white” light spectrum. This phosphor responds to a specific emission wavelength (eg, blue wavelength) of the device, causing a portion of the emitted light to Stokes shift from a shorter wavelength to a longer wavelength, and the output light into a white spectrum. The white spectrum is characterized by an equivalent color temperature associated with the emission spectrum of the corresponding blackbody radiation. The “warm” white light spectrum is characterized by a color temperature of about 2800 ° K, while the color temperature of the “cold” white light spectrum is about 5000 ° K. For many applications, the warm white light spectrum is preferred.

US Pat. No. 6,031,611

In order to obtain an appropriate color temperature, the emission wavelength λ _E of the semiconductor light-emitting device needs to match the absorption / emission spectrum Δλ of the fluorescent material. Typically, the actual emission wavelength λ _E needs to be within plus or minus 2 nm from the intended (selected) emission wavelength λ _ED in order to properly match the absorption and emission properties of the phosphor. is there. When properly adapted, LED luminaires emit “white light” with a color temperature on the order of 2800 ° K. The value of a device that deviates from a specific wavelength specification is greatly reduced. This is because such devices emit "off-color" light and do not meet consumer demand. LED manufacturers often sell such “off-color” LEDs for applications where color is not important, such as flashlights and outdoor parking facilities. However, the value of such LEDs is much lower than those sold in the general home lighting market where color temperature is important. For this reason, LED manufacturers strive to produce more LEDs in a more valuable spectral region from a single wafer.

  For optimum production, and associated value and benefit, there is a need for the manufacture of semiconductor light emitting devices having precise emission wavelengths that fall within specified tolerances. There is also a need to be able to know the emission wavelength of a light emitting chip (die) that will eventually become a semiconductor light emitting device through a manufacturing process in advance.

  A method for characterizing a semiconductor light emitting device (LED) based on product wafer characteristics is disclosed. This method includes the step of measuring at least one of the characteristics of the product wafer, such as curvature and device layer stress. The method also includes the step of clarifying the relationship between the at least one feature and the emission wavelength of the LED die formed from the product wafer. This relationship makes it possible to predict the emission wavelength of the LED structure formed in the device layer of the product wafer formed in the same manner. This can also be used to characterize product wafers and perform process control of large scale LEDs.

In one aspect of the invention, the method measures device layer stress S (x, y) in a test product wafer, cuts the test product wafer to form a die, and the device layer stress and the corresponding device. By measuring the emission wavelength of the die according to the position (x, y), the device layer stress S (x, y) and the emission wavelength λ _E (x, y) in the device structure formed on the product wafer It has the process of clarifying the relationship. This method further includes a step of measuring a curvature change ΔC (x, y) of the test product wafer based on the measurement of the curvature of the substrate before and after the processing of the substrate forming the device. This method also includes a step of calculating a device layer stress S (x, y) in the test product wafer based on the measured curvature change ΔC. Also, the method further corresponds to the emission wavelength lambda _E, in order to make predictions of the emission wavelength in the device structure, the actual emission wavelength lambda _E, device layer stress on the product wafer for testing S (x , y) and a step of associating with the device structure based on the relationship between its position (x, y).

This method preferably further includes a step of calculating a stress S (x, y) in the test product wafer based on the measured curvature change ΔC using the following relational expression.
S (x, y) = {M _s h _s ² / 6h _F } ΔC (x, y) (Formula 1)
Here, M _s is the biaxial coefficient of the substrate 20, h _s is the height of the substrate, and h _F is the thickness of the device structure.

  In this method, the device structure can include either a light emitting diode or a laser diode structure.

  Preferably, the method further comprises the steps of determining a target emission wavelength, cutting a product wafer from the device structure to form a die, and selecting a die based on the predicted emission wavelength. It is.

  The method further includes a step of defining an allowable range of a change amount of the emission wavelength, a step of comparing the predicted emission wavelength with the allowable range, and discarding the product wafer based on the comparison, It is preferable to have a step of determining a procedure including whether to rework the product wafer or selectively use a part of the product wafer.

  In this method, metal organic chemical vapor deposition (MOCVD) can be used for processing the substrate.

  Another aspect of the present invention is a method for characterizing an emission wavelength in a semiconductor light emitting device (LED) structure of a product wafer having a substrate and a device layer. The method includes measuring at least one feature in a test product wafer formed in substantially the same manner as the product wafer, wherein the “at least one feature” includes device layer stress and product wafer curvature. Is selected from the feature group including The method also includes cutting at least one test product wafer to form an LED die associated with a predetermined location on the test product wafer. The method also includes measuring the LED emission wavelengths of individual LED dies in order to clarify a series of LED emission wavelengths that vary depending on the location on the product wafer. The method further includes defining a relationship between at least one product wafer feature for testing, a series of LED emission wavelengths, and LED die positions, and a relationship defined by defining the relationship. Is used to predict the LED emission wavelength in the LED structure formed on the product wafer.

  The method preferably includes the step of binning the LED structure of the product wafer based on the relationship obtained by “defining the relationship”.

  In this method, the product wafer preferably includes a substrate. In addition, the method preferably further includes a step of measuring the curvature of the substrate prior to forming the product wafer.

  Preferably, the method further comprises the step of measuring at least one of a substrate curvature and a product wafer curvature using coherent gradient sensing (CGS).

  In this method, the device structure has a predetermined dimension, and in this method, at least one product wafer for testing is provided so that the device structure has a dimension substantially equal to or smaller than the dimension of the device structure. It is preferable to have a step of defining the characteristics of

Another aspect of the present invention is a method of forming a semiconductor light emitting device (LED). The method includes the step of forming a product wafer including an LED structure formed on a substrate by a process including one or more process variables, the LED structure being formed on the substrate. Has a known initial curvature C ₀ (x, y). This method further includes the step of measuring the curvature C (x, y) of the product wafer after forming the light emitting device structure, and the change in curvature ΔC (x, y) = C (x, y) −C _0. a step of defining (x, y). This method further includes a step of calculating a stress S (x, y) in the product wafer based on the measured change in curvature ΔC (x, y). This method further calculates the calculated stress S (x, y) based on the relationship between the calculated stress S (x, y) and the (x, y) position of the light emitting device structure on the product wafer. A step of associating with the emission wavelength λ _E of the structure. The method also includes the steps of comparing the emission wavelength λ _E with the emission wavelength variation tolerance and binning the LED structure into one or more bins based on the tolerance.

  The method preferably further comprises using only the LED structures in the selected one or more bins to form the LED device.

  The method further reduces at least one of the one or more process variables to reduce the amount of variation in emission wavelength in the light emitting device structure as a function of the (x, y) position of the light emitting device structure on the product wafer. It is preferable to have a step of adjusting the.

  In this method, the process variables are preferably selected from a series of process variables including time, temperature, temperature uniformity, gas partial pressure, gas partial pressure uniformity, gas flow rate, and gas flow rate uniformity. It is.

  This method further measures the curvature of one or more test product wafers formed in the same manner as the product wafer, cuts the one or more test product wafers to form LED dies, It is preferable to have a step of measuring the emission wavelength of the LED die using a function of the (x, y) position on the test product wafer, the measured product wafer curvature, and the emission wavelength. It is.

  The method further includes the steps of forming a new product wafer, measuring the curvature of the new product wafer, and further, the LED emission wavelength of the LED structure on the new product wafer based on the measured curvature of the new product wafer. It is preferable to have a step of defining

  Another aspect of the present invention is a method of forming a semiconductor light emitting device (LED). The method includes a step of forming a product wafer having an LED structure formed on a semiconductor substrate by a process having one or more process variables, and a step of measuring the curvature uniformity of the product wafer after forming the LED structure. And adjusting at least one of the one or more process variables to satisfy at least one of a curvature uniformity condition and a stress uniformity condition.

Another aspect of the present invention is a method of forming a semiconductor light emitting device (LED). The method includes forming a product wafer that includes LED structures formed on a substrate by a process having one or more process variables. The substrate has a known initial curvature C ₀ (x, y) prior to the formation of the light emitting device structure thereon. The method is also based on measuring the curvature C (x, y) of the product wafer after forming the light emitting device structure, and C ₀ (x, y) and C (x, y). A step of defining curvature uniformity; The method also includes defining a first number of dies that are included in the first range of curvature uniformity. The method also includes defining a second number of dies that are included in the second range of curvature uniformity. The method also includes the step of providing a quality value to the product wafer based on the first number and the second number.

  The method preferably further comprises the step of obtaining the properties of the product wafer based on the given quality value.

  The method further preferably includes the step of cutting the product wafer to form LED dies associated with the first number and the second number. The method further uses the LED die associated with the first number used in the first application and the LED die associated with the second number used in the second application. It is preferable to have a process.

Another aspect of the present invention is a method of forming a semiconductor light emitting device. The method includes forming a product wafer including a light emitting device structure formed on a substrate by a process having one or more process variables, the light emitting device structure being formed on the substrate. Has a known initial curvature C ₀ (x, y). This method also includes the step of measuring the curvature C (x, y) of the product wafer after forming the light emitting device structure, and the change in curvature ΔC (x, y) = C (x, y) −C _0. a step of defining (x, y). This method also calculates the emission wavelength λ _E of the light emitting device structure based on the calculated curvature C (x, y) and (x, y) position relationship in the light emitting device structure on the product wafer. A step of associating with the wafer curvature C (x, y,). The method also includes a step of comparing the emission wavelength λ _E and the emission wavelength variation allowable range in order to define which light emitting structure can be used to form a light emitting device.

  Additional features and advantages of the invention will be set forth in the detailed description which follows. Some of them will be readily apparent to those skilled in the art from the detailed description, or by practicing the invention described herein, including the following detailed description, the claims, and the accompanying drawings. Be recognized.

  It should be understood that the above description relating to the background art and the following detailed description provide an outline or framework for understanding the nature and characteristics of the present invention described in the claims. Should. The accompanying drawings are included to provide a further understanding of the invention, and are incorporated in and constitute a part of this specification. The drawings illustrate various embodiments of the invention and together with the description serve to explain the principles and practice of the invention.

It is a top view which shows an example of the product wafer used for formation of a semiconductor light-emitting device. It is sectional drawing which shows an example of the product wafer used for formation of a semiconductor light-emitting device. FIG. 2 is a perspective view of an example LED device showing how a die from a product wafer is incorporated into the LED device structure. It is a figure which shows the aggregate | assembly of the sapphire substrate supported by the susceptor. FIG. 6 is an enlarged cross-sectional view of a portion of the susceptor showing how the substrate is supported by the susceptor. FIG. 3 is a schematic diagram of a MOCVD reactor system used to form a device layer on a substrate to form the product wafer shown in FIG. FIGS. 7A to 7D are plan views of product wafers on which curves indicating variations in the product wafer temperature T, device dimensions D, device layer stress S, and emission wavelength λ _E are drawn. FIGS. 8A to 8C are plan views of product wafers on which curves indicating variations in product wafer curvature C, device layer stress S, and emission wavelength λ _E are drawn. It is a top view about an example of the product wafer in which the predicted light emission wavelength was shown similarly to FIG. 8C. The 457 nm and 455 nm curves are shown in bold lines to show the limitations of the required device structure with a wavelength of 456 nm plus or minus 1 nm. 1 is a schematic diagram of an example of a coherent gradient sensing (CGS) system used in one example to measure substrate and product wafer curvature. FIG. It is a flowchart about an example of the method of estimating the light emission wavelength of the die cut out from the said product wafer based on the curvature measurement of a product wafer. Note that some of the above drawings show orthogonal coordinate systems for reference, but these are not intended to limit the direction and configuration.

  Reference will now be made in detail to embodiments of the invention. An example of the embodiment is illustrated in the accompanying drawings. In the drawings, the same or similar reference numerals and symbols are used as much as possible to refer to the same or similar parts. The description of the claims is incorporated herein and forms part of the Detailed Description.

As described in detail below, the device layer stress is the stress in the device layer 30 that defines the device 50. The device layer stress is expressed as S (x, y) or simply S. S is a simplified notation of S (x, y; σi, j), and σi, j is a stress tensor. The stress tensor σi, j defines the stress at all positions of the device layer on the substrate. The coordinates (x, y) represent orthogonal coordinates on the wafer of points in the device layer 30 where the stress is defined. The stress tensor σi, j has three orthogonal normal stress elements (σ ₁₁ , σ ₂₂ , σ ₃₃ ) and six orthogonal shear stresses (σ ₁₂ , σ ₁₃ , σ ₂₁ , σ ₂₃ , σ ₃₁ , σ ₃₂ ) is specified. If the coordinate system used for measuring stress is oriented in the basic direction, the stress tensor is composed of only three orthogonal normal stress elements. In one example, S (x, y) has a single value representing stress, which may be, for example, a maximum stress element, a sum of stress elements, an average of stress elements, or several stresses. Can be a value of a combination of elements. In another example where the rate of change of the stress at a given (x, y) position is used, the notation S ′ (x, y) is used.

Furthermore, in the following description, the surface curvature C (x, y) is expressed as C (x, y; n). Here, n is a normal vector in a given direction in the XY plane, and defines a plane that intersects at right angles to the XY plane. C (x, y) is the curvature of a curve formed on the surface when the plane intersects the surface. In general, this curvature is defined as 1 / R. Here, R is the local radius of the curvature of the surface at the point (x, y) on the plane defined by the normal vector n. When C (x, y) is a scalar function, in one example, n is along one direction. In general, C (x, y) is a tensor because it can take a plurality of related curvatures, and is one in each direction for the unit vector n. In one example, the curvature C (x, y) is a function H (x, y) that defines the height of each surface point (x, y) as if measured at a reference plane (eg, a perfectly flat wafer). Can be determined from Specifically, C (x, y) is obtained by aligning an arc with a plurality of points surrounding a point (x, y) in a given plane in order to obtain an optimal radius R, so that H (x, y) Obtained from. This also determines the curvature as 1 / R. C (x, y) can also be obtained from the second derivative of H (x, y) using standard mathematical techniques. The notation C ₀ is used to represent the curvature of the substrate used for forming the product wafer.

  In the discussion herein, the acronym “LED” is generally understood as meaning “light emitting device” but also means “light emitting diode”. Moreover, those skilled in the art will understand the difference between the two based on the context in which this initial is used.

  FIG. 1 is a plan view showing an example of a product wafer 10 used for forming a semiconductor LED such as a light emitting diode and a laser diode, and FIG. 2 is a sectional view thereof. Here, the term “product wafer” generally means a wafer or a substrate having a device structure formed on the surface thereof, and the device structure is used to form, for example, an LED product or a device. It is used for manufacture of the light emitting device which can be used.

The product wafer 10 includes an edge 21, a top surface 22, and a bottom surface 24, and includes a semiconductor substrate 20 having a device layer 30 formed on the surface 22. An example semiconductor substrate 20 is made of sapphire or silicon. The device layer 30 includes an array 32 of semiconductor light emitting device structures (device structures) 40. In one example, the product wafer 10 has thousands of device structures 40 approximately 1 mm in size. The diameter of the sapphire substrate 20 in the example product wafer 10 is 2 to 6 inches, and that of a silicon substrate is 6 to 12 inches. The device structure 40 is related to the actual emission wavelength λ _E and the output spectrum Δλ related to the color temperature described above. The emission wavelength required or selected for the device structure 40 is denoted as λ _ED .

When processing of the product wafer 10 is completed so that the device structure 40 is functional, the product wafer 10 is cut (“die” to separate the individual device structures in the array 32 to form individual dies 42. "). The die 42 is incorporated into a semiconductor light emitting device structure to form a light emitting device 50, as shown in FIG. 3 as a perspective view according to an example of an LED device. The LED device 50 of FIG. 3 has an anode 52A and a cathode 52C that extend to the inside 54 of the epoxy lens casing 56. The cathode 52C has a reflective recess 58 in which the die 42 is disposed. The wire bond 60 electrically connects the anode 52A and the cathode 52C to the LED. A power source (not shown) is connected to the anode 52A and the cathode 52C in order to power the LED and emit light 62 of the actual wavelength λ _E. If the die 42 is a known die, the LED device 50 of FIG. 3 is a known device, but if the die 42 is formed using the method according to the present invention, the LED device 50 is a known device. is not.

  An example of the device structure 40 is in the form of an LED manufactured by growing GaN on the sapphire substrate 20. Metal organic chemical vapor deposition (MOCVD) is used for the growth of GaN. MOCVD is performed in a MOCVD reactor, and a multi-quantum well structure (not shown) is formed by MOCVD.

  FIG. 4 shows an assembly of sapphire substrates 20 supported on a substrate holding member or susceptor 70 having a surface 72. FIG. 5 is an enlarged sectional view of the susceptor 70 and shows an example of how the substrate 20 is supported by the susceptor 70. The susceptor 70 has an opening 76 formed in the top surface 72. The opening defines a lip 78 that supports the substrate 20 on the bottom surface 24 in the vicinity of the edge 21.

  FIG. 6 shows a MOCVD reactor system 90 having a reaction chamber 100 operably connected to the MOCVD subsystem 96. The MOCVD subsystem 96 includes various MOCVD system elements (not shown) such as a vacuum pump, a gas source, a ventilation system, and a diaphragm vacuum gauge. The MOCVD chamber 100 has an internal space 104 in which the susceptor 70 and the substrate 20 are provided when the MOCVD is operated. After the MOCVD process is performed, the substrate 20 becomes the product wafer 10. The MOCVD reaction system 90 has a controller 110 operably connected to the MOCVD subsystem 96. The controller 110 controls the MOCVD process (indicated by arrow 105) that occurs in the reactor interior space 104.

In particular, since the actual emission wavelength λ _E greatly varies depending on the growth conditions of MOCVD, the controller 110 is used to carefully control the temperature T of the product wafer 10. 7A to 7D are plan views of an example of the product wafer 10, where the temperature T (x, y), the device dimension T (x, y), the device layer stress S (x, y), and (actual ) Schematically shows an example of a contour line of the emission wavelength λ _E (x, y). Here, since the substrate 20 is subjected to a process for forming the product wafer 10, the temperature T means either the substrate temperature or the product wafer temperature. Hereinafter, in order to facilitate the discussion, “product wafer temperature” is described.

When the product wafer temperature T (x, y) changes (FIG. 7A), for example, the device dimension D (x, y) such as the thickness of a multiple quantum well structure (not shown) formed during the MOCVD process becomes It varies depending on the corresponding method (FIG. 7B). In other words, the device layer stress S (x, y) on the product wafer 10 (FIG. 7C) also varies correspondingly. Variations in device layer stress S (x, y) also cause variations in the actual emission wavelength λ _E (FIG. 7D).

In some cases, a 1 ° K temperature change in the product wafer temperature T may cause a shift δλ _E of about 1 nm in the emission wavelength λ _E. Therefore, in order to ensure proper control of the product wafer temperature T, it is required to first detect and ultimately control temperature non-uniformity and temperature reproducibility in the MOCVD reaction system 90. Become. Product wafer temperature non-uniformity can lead to local variations in growth conditions that cause variations in LED emission wavelengths.

Currently, in the manufacture of the device structure 40 by MOCVD, the actual emission wavelength λ _E and the corresponding emission uniformity are not known until the device structure 40 is cut from the product wafer 10 to form the die 42. The die is incorporated into a light emitting device such as LED device 50 of FIG. 3 or an equivalent test structure.

So far, in order to estimate or predict the LED emission wavelength λ _E , the substrate is inspected using glitter technology. In this inspection, a short wavelength source (especially 248 nm) irradiates the multiple quantum well region to emit light. However, a major limitation of this technique is that it is a point-by-point inspection technique. To accurately map the entire product wafer with a high spatial resolution (eg, a spatial resolution smaller than the die size), a time of 30 minutes to 240 minutes, depending on the size of the substrate used to form the product wafer. It takes.

  A further limitation of this technology is that in general the emission wavelength from photoluminescence is not the same as the emission wavelength emitted from the LED during electrical stimulation. The cause of this difference is believed to be due to the additional manufacturing process that the LED undergoes between the photoluminescence test and the final product. In particular, there is a “deviation” between the photoluminescence emission wavelength and the LED emission wavelength due to electrical stimulation pre-measured during manufacture. This is therefore used as a process monitor.

The amount of the device layer stress S (x, y) in the device structure 40 formed on the product wafer 10 is directly related to the history of the product wafer temperature T (x, y), that is, T (x, y, t). Related. Here, t is time. Basically, product wafer temperature differences (ie, non-uniform heating) during the deposition process cause variations in the thickness of the stacked GaN layers (specifically, multiple quantum well layers). . After the deposition process and when the substrate returns to room temperature, the difference in thermal expansion ratio of the constituent materials forming the device structure 40 is the relative expansion of the device structure relative to the substrate 20 in the thermal cycle. Causes contraction. Non-uniform heating causes non-uniform device layer stress and non-uniform emission wavelength (λ _E ).

  This relative expansion / contraction causes stress in the device structure 40 formed on the product wafer 10. A part of the thermal energy given to the product wafer is stored in the device layer 30 as mechanical energy. Product wafer temperature T (x, y) non-uniformity (eg, variation) during deposition is due to layer thickness non-uniformity (variation) and ultimately device layer stress S (x, y) non-uniformity Leads to sex (variation). Product wafers 10 that differ only in temperature T (x, y) differ only in device layer stress S (x, y).

The device layer stress S (x, y) can be monitored through a change in substrate curvature ΔC (x, y). The most common stress measurement system relies on measurement of product wafer shape changes to calculate device layer stress. The device stress S (x, y) in the device structure 40 supported by the product wafer 10 is calculated from the change in curvature ΔC (x, y) using the Stoney equation (Equation 1).
S (x, y) = {M _s h _s ² / 6h _F } ΔC (x, y) (Formula 1)
Where M is the biaxial modulus, h is the thickness, the subscript “F” represents the laminated film (eg GaN), and the subscript “s” is the substrate (eg , Sapphire or silicon). A change in C (x, y) on the wafer indicates a non-uniform device layer stress S.

It is known that the device layer stress S can occur due to temperature and non-uniformity of the coefficient of thermal expansion (α) between the film (ie, device layer 30) and the underlying substrate 20 The device layer stress S is given by the following equation representing the device layer stress S and the curvature C.
S (x, y) = M _f ε _m (T) = M _f (α _f -α _s ) ΔT (Formula 2)
C (x, y) = {6M _f h _f / M _s h _s ² } (α _f -α _s ) ΔT (Formula 3)
Here, ε _m is a distortion due to non-uniformity or mismatch between the film and the substrate, and ΔT is a difference from the stress-free temperature T ₀ (that is, the temperature at which the film and the substrate are aligned).

The above equation shows how the change in curvature ΔC (x, y) is related to the change in stacking temperature. Therefore, from these equations, the product wafer curvature can be related to the “temperature” directly related to the emission wavelength λ _{E of the} LED.

  The above equations are based on specific conditions related to stress and deformation states, device structure geometry, and thermomechanical properties of the constituent materials. More complex types or variations of this formula can be created for film / substrate systems with irregular properties. However, for any particular device / substrate system, an appropriate relationship may be created along a straight line that correlates changes in substrate curvature to temperature changes related to changes in emission wavelength.

  One aspect of the present disclosure provides at least one product wafer characteristic, such as product wafer stress (ie, one or more elements in the stress tensor) and curvature, and at least one product output, efficiency, wavelength, spectral bandwidth, etc. Associate with LED performance characteristics. In one example, this is accomplished by empirically establishing a relationship between at least one measured performance characteristic in the LED and at least one product wafer characteristic. In one example, this is accomplished by evaluating at least one performance characteristic in the LED obtained from the product wafer against the individual processing steps used to form the product wafer. This is also achieved by evaluating at least one LED performance characteristic for a plurality of processing steps used to form a product wafer.

  Thus, one aspect of the present disclosure includes a method of using at least one of product wafer stress and product wafer curvature as a process monitor for performing quality control that aggregates and selects the performance of individual dies on a product wafer. . This method includes a method of monitoring the deposition characteristics during product wafer formation and performing process optimization. The method may further include adapting the performance of a set of two or more same type process tools to match the product wafer and LED die when formed on different process tools. In other words, product wafers formed by different process tools in a matched set are more similar than if the process tools are not matched.

FIGS. 8A to 8C schematically illustrate, for example, contour lines of curvature C (x, y), device layer stress S (x, y), and actual emission wavelength λ _E (x, y). It is a top view regarding an example. One aspect of the present disclosure is to determine the device layer stress S (x, y) by measuring the curvature C (x, y) of the product wafer, and then the corresponding device structure 40 on the product wafer 10. Using the determined device layer stress S (x, y) to predict the actual emission wavelength λ _E of the processed (separated) die 42 as a function of the position (x, y) of Including.

In FIG. 8C, one particular device structure 40 is shown having a position (xi, yj) measured relative to a reference position (eg, the center of the product wafer). The enlarged inset of the array 32 of device structures 40 shows more detailed (ie, dense) contour lines λ _E at the actual emission wavelength λ _E in 1 nm increments. In one example, a change (shift) in emission wavelength at 1 nm δλ _E can be predicted.

Figure 9 is a plan view of a virtual product wafer 10, it shows an example of a 2nm increments contour of the light-emitting wavelength lambda _EP predicted. The product wafer 10 has a concave or bowl-shaped curvature C (x, y). Assuming that the required emission wavelength is a fluctuation allowance δλ of plus or minus 1 nm and the emission wavelength λ _ED is 456 nm, the product wafer 10 is cut and shown in bold lines according to the predicted wavelength contour in FIG. Only the die 42 from the device structure 40 that is located (x, y) between the expected wavelength contours at 455 nm and 457 nm (ie within the optical wavelength variation tolerance δλ) may be used in the final light emitting device 50. It becomes possible. For this reason, in one example, the first group of LED structures 40 falls within the range of contour lines from 455 nm to 457 nm, and the second group of LED structures 40 falls outside the range of these contour lines. The sorting of this type of LED structure 40 based on the selected specifications (here the emission wavelength) can be used to determine the resulting LED die 42 for the first and second applications, or the first type of LED device and the first type. Used for placement in two types of LED devices.

  Currently, the number of dies 42 within an acceptable wavelength variation range (ie, δλ = + / − 1 nm as an example) can be estimated. In addition, it is possible to estimate the number of dies 42 that deviate slightly from this frame, but are still useful for use in “off color”. Furthermore, the number of dies 42 that are out of the usable range and therefore have no intrinsic value can be estimated. The essential value of the product wafer 10 can be determined from the number of dies 42 in each wavelength variation range and knowing the value of the die 42 in each wavelength variation range. This allows the LED manufacturer to determine whether there is sufficient reason to continue processing a particular product wafer 10. For example, if an array of dies does not fall within the useful wavelength range, there is little reason to continue manufacturing the wafer 10 and add extra expense.

In short, a wavelength shift in the light emission wavelength λ _E of the LED occurs due to a change in deposition temperature in LED manufacturing. These same temperature changes cause a stress change in the deposited film that causes a change in wafer curvature. Therefore, the change in the wafer curvature C is related to the wavelength shift through the above formula.

  In practice, it may be difficult to know the exact values of the material constants (such as coefficient of thermal expansion α and biaxial coefficient M) of various materials used during MOCVD processing at elevated temperatures. For example, a typical temperature in a MOCVD process is usually about 1000 ° C. In order to analytically link the above formula with the actual LED wavelength shift, accurate knowledge of these material constants and the temperature history of the substrate 20 is required. This information may not be available.

Therefore, it is necessary experimentally by accurately measuring the curvature C at all points on one or more test product wafers 10 and measuring the LED emission wavelength λ _E of the LED die 1042 obtained from the product wafer 10. While acquiring data, it may be more convenient to create an actual wavelength shift lookup table or correlation curve for the actual wavelength shift. According to this approach, the measured substrate curvature C can be associated with actual device data, and the actual device data and subsequent substrate curvature can be used as a process control and inspection monitor for high capacity LED manufacturing. it can.

The main advantage of using wafer curvature C to measure emission wavelength λ _E and emission uniformity using currently used photoluminescence technology is that the wafer curvature is very high in a very short time. It can be measured with. A coherent gradient sensing system (described below) can easily spatially sample a substrate at hundreds of microns smaller than the typical die size of 1 mm and can inspect (measure) a 200 mm wafer in about 1 minute. . In contrast, it would take several hours to obtain similar spatial information on a 200 mm wafer using a photoluminescence system.

  FIG. 10 is a schematic diagram illustrating an example of a coherent gradient sensing (CGS) system 200 that can be used to measure the curvature C (x, y) of the product wafer 10. Details on how the CGS moves are described in US Pat. No. 6,031,611 (the '611 patent), which is incorporated herein. FIG. 10 is based on FIG. 1 of the '611 patent.

  The CGS system 200 includes a digital camera 210, a filtering lens 224 (eg, a filter in combination with the lens shown in the '611 patent and its FIG. 1), first and second axially spaced along an axis A1. It has diffraction gratings G1 and G2, a beam splitter 230, and a wafer stage 240. The CGS system 200 also includes a laser 250 disposed along an optical axis A2 that intersects the axis A1 at the beam splitter 230. The CGS system 200 also includes a controller or signal processing device 260 operatively connected to the digital camera 210 and the laser 250. An example of the signal processing device 260 is a computer having a processor 262 and a computer readable medium (memory) 264, or an apparatus including such a computer and medium. The medium (memory) 264 controls the movement of the CGS system 200 to measure the product wafer curvature C (x, y) in the manner described in the '611 patent through instructions recorded on itself. It is like that.

  In operation, the laser 250 generates a parallel laser beam 252 that is directed to the product wafer 10 by the beam splitter 230. This parallel laser beam is reflected on the product wafer 10 (specifically, the device layer 30) as reflected light 252R that penetrates the beam splitter 230 and the diffraction gratings G1 and G2 and travels upward. The two diffraction gratings G1 and G2 are separated from each other or are adapted to shear a parallel laser beam. The light passing through the diffraction gratings G 1 and G 2 is focused on the digital camera 210 using the filtering lens 224.

  The shearing and filtering process causes a stripe pattern that is a contour line of the surface gradient on the product wafer 10 in the digital camera 210. Thus, two orthogonal interferogram sets can be numerically integrated to reconstruct the substrate topography, or numerically separated to obtain the product wafer curvature C (x, y). Used to characterize the surface gradient. A two-camera configuration for the CGS system, as shown in FIG. 6 of the '611 patent, is also used to help capture two orthogonal sets of interferograms.

  The curvature map, that is, the curvature C (x, y) of the product wafer is generated from the interference fringes using, for example, the method described in the '611 patent implemented by the controller 260. In one example, the measured curvature C (x, y) of the product wafer 10 has a spatial resolution on the order of about 100 microns to 300 microns. Thus, in a device structure 40 having a dimension d on the order of about 1 mm (see FIG. 3), there is at least one curvature data point for each device, and in some cases, multiple for each device (die). There may be data points. In one example, the method disclosed herein includes defining a spatial stress variation S (x, y) in the product wafer to a dimension that is substantially the same as or smaller than the dimension d of the device structure 40. Yes.

In one example, the curvature C ₀ (x, y) of the substrate 20 is measured prior to processing the substrate to form the product wafer 10. Thereby, a change in curvature ΔC (x, y) = C (x, y) −C ₀ (x, y) is calculated.

When the curvature C ₀ (x, y) and C (x, y) of the product wafer are measured and the change in curvature ΔC (x, y) is calculated, the device layer stress S (x, y) is It becomes possible to specify. In one example, this can be accomplished by using the Stoney equation (Equation 1 above) that relates the device layer stress S to the change in curvature ΔC.

  In most product wafers 10, the change in curvature ΔC (x, y) varies from wafer to wafer and also from the orientation, which implies the presence of non-uniform device layer stress S (x, y). Alternatively, if the material characteristics at each temperature are unknown, the wavelength shift δλ with respect to the measured curvature C on the sample substrate (wafer) is measured and these measured values are related for future measurements of the product wafer 10. It is possible.

  Other methods can be used to perform measurements that can define C (x, y). Examples of such methods include profilometry (shape measurement), interference measurement, capacitance measurement, and laser beam deviation. Similarly, the device layer stress S (x, y) can be defined by measuring the strain of the crystal lattice using, for example, X-ray diffraction or Raman spectroscopy.

Accordingly, one aspect of the method in the present disclosure includes the following steps.
1. A step of measuring the shape (curvature) C ₀ (x, y) of the substrate 20 prior to performing processing (for example, MOCVD).
2. A step of measuring the shape C (x, y) of the product wafer 10 after the processing.
3. To define the change in curvature ΔC associated with the product wafer 10 induced by processing the substrate 20 to form the product wafer, ΔC (x, y) = C (x, y) −C ₀ calculating (x, y).
4). In order to calculate the device layer stress S (x, y) of the product wafer induced by the above process based on ΔC (x, y), the Stoney formula or related formula (for example, Blake formula) is calculated. And calculating the device layer stress S (x, y) of the product wafer.
5. Associating the device structure 40 at the position (xi, yj) with the device layer stress S (xi, yj).
6). The emission wavelength λ _E (xi, yj) that enables measurement of the curvature of the product wafer to predict the emission wavelength of the LED structure 40 that forms the LED die when the product wafer is cut out, and the device layer stress The step of associating the value S (xi, yj).

Step 6 above. Then, it is necessary to correlate the actual emission wavelength λ _E , the change in curvature ΔC, and the change in device layer stress S (x, y) depending on the type of processing and the type of device structure 40 to be manufactured. This can be done if all material properties are well known and the relationship between temperature and deposition rate is well known. As described above, since these relationships are not well known, it is necessary to experimentally generate data for associating the measured curvature variation with the emission wavelength variation.

In one example, an experimental “fingerprinting” process can be performed as follows.
1. A step of completing steps 1 to 4 for one or more product wafers 10 to perform a specific process for forming a device structure.
2. 2. measuring the actual emission wavelength λ _E of the LED die obtained from the test product wafer 10 as a function of the position (x, y) of the device structure to determine λ _E (x, y); A step of determining a relationship between the device layer stress S (x, y) and the actual emission wavelength λ _E (x, y).

The method according to the present invention also includes performing product wafer process monitoring and process control to determine (predict) the actual emission wavelength λ _E resulting from the LED die 42 when the product wafer is cut out. Contains. This can be done between a given product wafer and multiple different product wafers that are subjected to the same process (ie, the same device structure). The selected LED die 42 characterized using the method of the present disclosure can be used to select the type of LED device 50 as shown in FIG.

The method according to the present invention also includes performing a process optimization to form the device structure 40 by adjusting at least one process variable used to form the product wafer 10.
For example, this includes the following steps.
1. Relationship between process variables (eg, temperature, temperature uniformity, gas partial pressure, gas partial pressure uniformity, flow rate, flow rate uniformity, time) and process induced stress properties (eg, average stress and stress uniformity) Establishing the process,
2. Modifying at least one process variable in order to optimize the stress characteristics of the process to obtain the required device characteristics such that the emission wavelength is as close as possible to the required emission wavelength.

The method of the present invention aiming at process optimization also includes the following steps.
1. Establishing stress properties associated with different process tools (eg, different MOCVD reaction systems) used to perform the same process;
2. Identifying a specific process tool that can provide the minimum required stress characteristics, that is, the maximum device performance change (eg, maximum change in actual emission wavelength),
3. Processes that affect the stress characteristics (ie, wafer temperature, wafer temperature uniformity, gas partial pressure, gas partial pressure uniformity, gas flow rate, gas flow rate uniformity, etc.), hardware or control settings, adjustments, etc. The process of checking tool variables,
4). Reduced changed, and the step of adjusting the process tool variables to obtain a specific example to minimize the change in the emission wavelength lambda _E of the LED die emission wavelength lambda _E.

FIG. 11 is a flowchart 300 showing an example of a method for predicting the actual emission wavelength λ _E of the LED die 42 formed from the product wafer 10 based on the measurement of the curvature of the product wafer and the substrate used to form the product wafer. It is.

The flow diagram 300 establishes a relationship between the device layer stress S (x, y) and the actual emission wavelength λ _E (x, y) of the die 42 formed from the device structure 40 on the product wafer 10. Step 302 is included.

The flow diagram 300 includes a second step 304 for measuring the change in curvature ΔC (x, y) of the product wafer 10 based on the substrate locality measurement C ₀ (x, y) described above.

  The flow diagram 300 includes a third step 306 of calculating the device layer stress S (x, y) of the product wafer 10 based on, for example, the change in curvature ΔC measured using the Stoney equation.

  The flow diagram 300 includes a fourth step 308 relating the (x, y) device structure 40 in the die 42 formed on the product wafer 10 to the calculated device layer stress S (x, y). Yes.

The flow diagram 300 includes a fifth step 310 relating the actual emission wavelength λ _E to the various dies 42 based on the device layer stress values S (x, y) established in step 302.

The flow diagram 300 includes a sixth step 312 that adjusts at least one process variable to reduce the range of changes in the emission wavelength λ _E of the die 42.

In other examples of the methods disclosed herein, product wafer curvature measurements can be performed at different stages in the completion of the product wafer process.
This gives insight into how the product wafer curvature changes with each process step.

Also, as described above, the flow diagram 300 can be used to obtain a look-up table or correlation curve for the actual wavelength shift by precisely measuring the curvature C of one (a set of) sample wafers. As part of the sub-step of experimentally obtaining the necessary data from the test product wafer 10 and subsequently measuring the LED emission wavelength λ _E to correlate the measured substrate curvature C with the actual device data You may have a process. This allows the product wafer fraction measurement to be used as a process control and inspection monitor for subsequent high capacity LED device manufacturing.

  It will be apparent to those skilled in the art that various modifications and variations can be made to the present invention without departing from the spirit and scope of the invention. Accordingly, the present invention includes modifications and variations of this invention within the scope of the appended claims and their equivalents.

This application claims the 201 priority based on the filed US provisional application (No.61 / 567,820) to 1 December 7, is intended to incorporate the same provisional application.

Claims (22)

A method for characterizing the emission wavelength of a semiconductor light emitting device structure of a product wafer having a substrate, comprising:
Measure device layer stress S (x, y) in the test product wafer, cut the test product wafer to form a die, and respond to the device layer stress and the corresponding device position (x, y) By measuring the emission wavelength of the die, the relationship between the device layer stress S (x, y) and the emission wavelength λ _E (x, y) in the device structure formed on the product wafer is clarified. And a process of
Measuring a change ΔC (x, y) in curvature of the test product wafer based on measurement of curvature of the substrate before and after the substrate process for forming the device structure; and
Calculating the device layer stress S (x, y) in the test product wafer based on the measured change in curvature ΔC;
Corresponding to the emission wavelength lambda _E, the order of performing the prediction of the emission wavelength in the device structure, the actual emission wavelength lambda _E, the device layer stress S (x, y) and the product wafer for the test Associating with the device structure based on its relationship to its position (x, y) in The method according to claim 1, further comprising: calculating the stress S (x, y) in the test product wafer based on the measured change in curvature ΔC using the following relational expression.
S (x, y) = (M _s h _s ² / 6h _F } ΔC (x, y)
Here, M _s is the biaxial coefficient of the substrate, h _s is the height of the substrate, and h _F is the thickness of the device structure.   The method of claim 1, wherein the device structure comprises one of a light emitting diode and a laser diode structure. Determining a desired emission wavelength;
Cutting the product wafer from the device structure to form the die; and
The method of claim 1, further comprising selecting the die based on the predicted emission wavelength. The step of defining an allowable range of the change amount of the emission wavelength, the step of comparing the predicted emission wavelength with the allowable range, and based on the comparison, discarding the product wafer or recycling the product wafer. The method of claim 1, further comprising the step of determining a procedure that includes either processing or selectively using a portion of the product wafer.   2. The method according to claim 1, wherein the substrate is processed by metal organic chemical vapor deposition (MOCVD). A method for characterizing an emission wavelength in a semiconductor light emitting device (LED) structure of a product wafer having a substrate and a device layer, comprising:
a) measuring at least one feature in a test product wafer formed in substantially the same manner as the product wafer, wherein “at least one feature” includes device layer stress and product wafer curvature; Selected from a feature group,
b) cutting the at least one test product wafer to form an LED die associated with a predetermined position on the test product wafer;
c) measuring the LED emission wavelength of each of the LED dies in order to clarify a series of LED emission wavelengths that vary depending on the position on the product wafer;
d) defining the relationship between the characteristics of the at least one product wafer for testing, the series of LED emission wavelengths, and the position of the LED die; and
e) A method comprising predicting the LED emission wavelength in the LED structure formed on the product wafer using the relationship defined in step d).   8. The method of claim 7, comprising binning the LED structure of the product wafer based on the relationship obtained by step d). The product wafer includes a substrate,
The method of claim 7, further comprising measuring a curvature of the substrate prior to forming the product wafer.   The method of claim 9, further comprising measuring at least one of a curvature of the substrate and a curvature of a product wafer using coherent gradient sensing (CGS). The device structure has predetermined dimensions;
10. The method of claim 9, comprising defining the characteristics of the at least one test product wafer to be substantially equal to or smaller than the dimensions of the device structure. A method of forming a semiconductor light emitting device (LED) comprising:
Forming a product wafer that includes an LED structure formed on a substrate by a process that includes one or more process variables, wherein the substrate has a known initial state prior to the formation of the LED structure; Has a curvature C ₀ (x, y),
Measuring the curvature C (x, y) of the product wafer after forming the light emitting device structure, and the change in curvature ΔC (x, y) = C (x, y) −C ₀ (x, y) The process of defining,
Calculating a stress S (x, y) in the product wafer based on the measured curvature change ΔC (x, y);
Calculate the stress S (x, y) calculated based on the relationship between the calculated stress S (x, y) and (x, y) position in the light emitting device structure on the product wafer. Correlating with the emission wavelength λ _E of
A method comprising comparing the emission wavelength λ _E with an emission wavelength variation tolerance and binning the LED structure into one or more bins based on the tolerance.   The method of claim 12, further comprising using only LED structures in one or more selected bins to form an LED device.   Adjusting at least one of the one or more process variables as a function of the (x, y) position of the light emitting device structure on the product wafer to reduce variations in light emission wavelength in the light emitting device structure The method according to claim 12, further comprising the step of:   15. The process variable of claim 14, wherein the process variable is selected from a series of process variables including time, temperature, temperature uniformity, gas partial pressure, gas partial pressure uniformity, gas flow rate, and gas flow rate uniformity. Method. Measuring the curvature of one or more test product wafers formed by the same method as the product wafer;
Cutting the one or more test product wafers to form LED dies;
Measuring the emission wavelength of the LED die using a function of the (x, y) position on the one or more test product wafers, the measured product wafer curvature, and the emission wavelength; 15. The method of claim 14, further comprising: Forming a new product wafer,
Measuring the curvature of the new product wafer; and
The method of claim 16, further comprising defining an LED emission wavelength of an LED structure on the new product wafer based on the measured curvature of the new product wafer. A method of forming a semiconductor light emitting device (LED) comprising:
Forming a product wafer having an LED structure formed on a semiconductor substrate by a process having one or more process variables;
After forming the LED structure, in order to satisfy at least one of a curvature uniformity condition and a stress uniformity condition, and a step of measuring a curvature uniformity of the product wafer, at least one of the one or more process variables A method comprising the step of adjusting one. A method of forming a semiconductor light emitting device (LED) comprising:
Forming a product wafer including an LED structure formed on a substrate by a process having one or more process variables, wherein the substrate is prior to forming the light emitting device structure thereon; Has a known initial curvature C ₀ (x, y),
A step of measuring the curvature C (x, y) of the product wafer after forming the light emitting device structure, and defining the curvature uniformity based on C ₀ (x, y) and C (x, y) The process of
Defining a first number of dies included in a first range of curvature uniformity;
Defining a second number of dies included in a second range of curvature uniformity;
Providing a quality value to the product wafer based on the first number and the second number.   The method of claim 19, further comprising positioning the product wafer on the basis of the given quality value. Cutting the product wafer to form LED dies associated with the first number and the second number;
Using the LED die associated with the first number for use in a first application, and using the LED die associated with the second number for use in a second application. 20. The method of claim 19, further comprising: A method of forming a semiconductor light emitting device comprising:
Forming a product wafer comprising a light emitting device structure formed on a substrate by a process having one or more process variables, wherein the substrate is known prior to the light emitting device structure being formed; Has an initial curvature C ₀ (x, y),
After forming the light emitting device structure, a step of measuring the curvature C (x, y) of the product wafer, and a change in curvature ΔC (x, y) = C (x, y) −C ₀ (x, y) The process of defining,
The emission wavelength λ _E of the light emitting device structure is calculated based on the calculated curvature C (x, y) and (x, y) position relationship in the light emitting device structure on the product wafer. Correlating with wafer curvature C (x, y,),
A method comprising the step of comparing the emission wavelength λ _E and the emission wavelength variation tolerance to determine which light emitting structure can be used to form a light emitting device.

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