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518 IEEE TRANSACTIONS ON SEMICONDUCTOR MANUFACTURING, VOL. 32, NO. 4, NOVEMBER 2019 Gross Die Per Wafer and Yield Optimization for GaAs ICs With Sub-Micron Features Robbie M. Best and Shiban K. Tiku Abstract—In an effort to maximize gross die per wafer (GDPW) while improving yield, various steps were taken to implement changes in the reticle layout and stepper exposure conditions across multiple designs. This allowed us to satisfy high yield goals for the BiHEMT process in a high volume manufacturing environment. Index Terms—Algorithms, BiHEMT, GaAs ICs, high volume manufacturing, lithography, MIM devices, reticle size, semi- conductor defects, semiconductor device measurements, canon stepper, yield optimization. I. I NTRODUCTION I N IC processing that utilizes 5x lithography tools, reti- cle sizes of 20 to 25 mm are commonly used. A reticle size of 22 mm has been used in the past at Skyworks with Canon FPA-3000 i5+ exposure systems for many GaAs IC technologies that use field-effect transistors (FET) as well as Bipolar transistors. Past technologies involved minimal wafer topography, and thus focus issues were not prevalent. However, with the introduction of the BiHEMT process, involving the fabrication of both Bipolar and HEMT devices on the same epitaxial substrate, challenges surfaced with regards to focus at various layers. These challenges were due to the fact that sub-micron features needed to be printed at both the highest and lowest portions of the BiHEMT topography, which can span a few microns in z-height. Fig. 1 shows a schematic of the typical topography involved in the BiHEMT process. Edge-field focus defects were observed, particularly on layers that use sub-micron features patterned at extreme points in the topography. For example, the base contact layer needs to be resolved not only at the top of the base pedestal (at the top of the topography), but also at the lower portion of the topog- raphy to form the bottom capacitor plate. On the other hand, the gate layer needs to be resolved at the lower portion of the topography only, but requires much finer resolution. This paper explores the steps taken in light of these challenges to successfully maximize gross die per wafer while improving the end-to-end yield. Manuscript received August 14, 2019; revised September 12, 2019; accepted September 13, 2019. Date of publication September 24, 2019; date of current version October 29, 2019. This work was supported by Skyworks Solutions, Inc. (Corresponding author: Robbie M. Best.) The authors are with Skyworks Solutions, Inc., Newbury Park, CA 91320 USA (e-mail: [email protected]; [email protected]). Color versions of one or more of the figures in this article are available online at http://ieeexplore.ieee.org. Digital Object Identifier 10.1109/TSM.2019.2943399 Fig. 1. BiHEMT topography. II. CHALLENGES The primary challenge in the BiHEMT process involves imaging across numerous focal planes. This problem is exacerbated by extreme topography in the BiHEMT design (Fig. 1) that utilizes both Bipolar (at the top of the topogra- phy) and HEMT devices (at the bottom of the topography) on the same epitaxial substrate. Additionally, the BiHEMT process takes advantage of negative-tone photoresist in order to achieve a retrograde resist sidewall profile by exposing the photoresist purposefully out of focus. Unfortunately, this makes establishing adequate depth of focus across multiple levels of the topography even more difficult. Further, the more out of focus a feature is exposed, the more its final dimensions can vary, thereby demanding tighter overlay control between layers. Finally, this tolerance is stressed by lens aberrations such as lens curvature, distortion and astigmatism that worsen as the distance from field center to field corner increases. III. APPROACH In order to safely increase BiHEMT field size from 20 mm × 20 mm in consideration of these process challenges, we developed multiple solutions. To begin, an in-house algorithm was developed to minimize the number of partial field die based upon photolithography tool capability. In parallel, an overlay measurement methodology was developed to ensure appropriate field corner overlay control of critical features as the field size increased. Finally, a “focus invalid area” (FIA) parameter within the exposure recipe was optimized to mit- igate risk of marginal focus on remaining partial fields of a wafer exposure sequence. These three solutions were imple- mented to minimize partial field die, mitigate risk of edge-field focus failures, and improve detection of overlay error. 0894-6507 c 2019 IEEE. Personal use is permitted, but republication/redistribution requires IEEE permission. See http://www.ieee.org/publications_standards/publications/rights/index.html for more information.

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  • 518 IEEE TRANSACTIONS ON SEMICONDUCTOR MANUFACTURING, VOL. 32, NO. 4, NOVEMBER 2019

    Gross Die Per Wafer and Yield Optimization forGaAs ICs With Sub-Micron Features

    Robbie M. Best and Shiban K. Tiku

    Abstract—In an effort to maximize gross die perwafer (GDPW) while improving yield, various steps weretaken to implement changes in the reticle layout and stepperexposure conditions across multiple designs. This allowed usto satisfy high yield goals for the BiHEMT process in a highvolume manufacturing environment.

    Index Terms—Algorithms, BiHEMT, GaAs ICs, high volumemanufacturing, lithography, MIM devices, reticle size, semi-conductor defects, semiconductor device measurements, canonstepper, yield optimization.

    I. INTRODUCTION

    IN IC processing that utilizes 5x lithography tools, reti-cle sizes of 20 to 25 mm are commonly used. A reticlesize of 22 mm has been used in the past at Skyworks withCanon FPA-3000 i5+ exposure systems for many GaAs ICtechnologies that use field-effect transistors (FET) as well asBipolar transistors. Past technologies involved minimal wafertopography, and thus focus issues were not prevalent. However,with the introduction of the BiHEMT process, involving thefabrication of both Bipolar and HEMT devices on the sameepitaxial substrate, challenges surfaced with regards to focusat various layers. These challenges were due to the fact thatsub-micron features needed to be printed at both the highestand lowest portions of the BiHEMT topography, which canspan a few microns in z-height. Fig. 1 shows a schematicof the typical topography involved in the BiHEMT process.Edge-field focus defects were observed, particularly on layersthat use sub-micron features patterned at extreme points in thetopography. For example, the base contact layer needs to beresolved not only at the top of the base pedestal (at the topof the topography), but also at the lower portion of the topog-raphy to form the bottom capacitor plate. On the other hand,the gate layer needs to be resolved at the lower portion ofthe topography only, but requires much finer resolution. Thispaper explores the steps taken in light of these challenges tosuccessfully maximize gross die per wafer while improvingthe end-to-end yield.

    Manuscript received August 14, 2019; revised September 12, 2019;accepted September 13, 2019. Date of publication September 24, 2019; dateof current version October 29, 2019. This work was supported by SkyworksSolutions, Inc. (Corresponding author: Robbie M. Best.)

    The authors are with Skyworks Solutions, Inc., Newbury Park, CA 91320USA (e-mail: [email protected]; [email protected]).

    Color versions of one or more of the figures in this article are availableonline at http://ieeexplore.ieee.org.

    Digital Object Identifier 10.1109/TSM.2019.2943399

    Fig. 1. BiHEMT topography.

    II. CHALLENGES

    The primary challenge in the BiHEMT process involvesimaging across numerous focal planes. This problem isexacerbated by extreme topography in the BiHEMT design(Fig. 1) that utilizes both Bipolar (at the top of the topogra-phy) and HEMT devices (at the bottom of the topography) onthe same epitaxial substrate.

    Additionally, the BiHEMT process takes advantage ofnegative-tone photoresist in order to achieve a retrograde resistsidewall profile by exposing the photoresist purposefully out offocus. Unfortunately, this makes establishing adequate depthof focus across multiple levels of the topography even moredifficult. Further, the more out of focus a feature is exposed,the more its final dimensions can vary, thereby demandingtighter overlay control between layers.

    Finally, this tolerance is stressed by lens aberrations suchas lens curvature, distortion and astigmatism that worsen asthe distance from field center to field corner increases.

    III. APPROACH

    In order to safely increase BiHEMT field size from 20 mm× 20 mm in consideration of these process challenges, wedeveloped multiple solutions. To begin, an in-house algorithmwas developed to minimize the number of partial field diebased upon photolithography tool capability. In parallel, anoverlay measurement methodology was developed to ensureappropriate field corner overlay control of critical features asthe field size increased. Finally, a “focus invalid area” (FIA)parameter within the exposure recipe was optimized to mit-igate risk of marginal focus on remaining partial fields ofa wafer exposure sequence. These three solutions were imple-mented to minimize partial field die, mitigate risk of edge-fieldfocus failures, and improve detection of overlay error.

    0894-6507 c© 2019 IEEE. Personal use is permitted, but republication/redistribution requires IEEE permission.See http://www.ieee.org/publications_standards/publications/rights/index.html for more information.

    https://orcid.org/0000-0002-6170-4437

  • BEST AND TIKU: GDPW AND YIELD OPTIMIZATION FOR GaAs ICs WITH SUB-MICRON FEATURES 519

    Fig. 2. Screenshot of algorithm input variables.

    Fig. 3. This exposure shot map is set to minimize partial field dies.

    A. Minimizing Partial Field Die

    As field size changes, the wafer layout changes in termsof the number of rows and columns that are exposed. Thisdetermines the wafer exposure sequence and the number ofexposed fields, including partial fields, along the edge of thewafer. By inputting various X and Y field dimensions and set-ting a threshold limit for the percentage of partial die allowed(Fig. 2), our wafer exposure algorithm can reduce the num-ber of partial field die exposed (Fig. 3), maximize gross dieper wafer, and reduce the number of total exposure fields toimprove stepper throughput (Fig. 4). The relationship betweenthese parameters is exemplified in Fig. 5.

    The algorithm optimized these conditions in a particularorder that can be modified by the user. First, the percent-age of partial field die was minimized, and then GDPW wasmaximized. Lastly, the total number of exposure shots wasminimized to improve stepper throughput. For this case, thedata point highlighted in shaded green in Fig. 5 represents theoptimal condition.

    B. Mitigating Risk of Edge-Field Focus Failures

    An exposure parameter known as focus invalid area wasoptimized in order to improve partial field focus conditions.The focus invalid area parameter represents the area of thewafer in which the stepper cannot accurately measure focusand tilt. For any given field outside the focus invalid area, fivefocus detectors can be activated, landing on the center and

    Fig. 4. This exposure shot is optimized for stepper throughput. In otherwords, the total number of exposure fields is minimized.

    Fig. 5. Various field size conditions were plotted, showing the relationshipbetween the number of GDPW and the percentage of partial field die, asa function of X/Y field size (secondary X/Y axes) and the number of totalexposure shots.

    corner of each field to establish the focal plane at which thatfield is to be exposed (Fig. 6).

    When all channels are active, the focusing system can mostaccurately and precisely compensate field-by-field for the vari-ability in wafer topography. However, when one or morechannels lie on a portion of a given field that is inside thefocus invalid area, the system relies on the remaining activechannels to determine the focal plane of that field. As a result,both average focus (between the active channels) and die-by-die tilt become less repeatable across the wafer. As thefocus invalid area is reduced, the edge of the focus invalidarea moves towards the wafer edge (Fig. 6). As a result, morefocus channels lie on any wafer edge-fields that are present.After the reticle field size was optimized, the focus invalidarea was reduced from 7 mm to 3 mm. This led to the use ofas many focus channels as possible for a given exposure shot

  • 520 IEEE TRANSACTIONS ON SEMICONDUCTOR MANUFACTURING, VOL. 32, NO. 4, NOVEMBER 2019

    Fig. 6. A partial field is shown with one channel (shown in red) inactive asit is inside the “focus invalid area.”

    Fig. 7. Optical image shows missing base contact due to poor focus.

    map, improving partial field focus conditions for each waferexposed. Examples of some of these focus improvements aredescribed below.

    In our BiHEMT technology, the base contact (BC) of thetransistor is susceptible to focus perturbations on portions ofthe structure closest to the wafer edge (Fig. 7).

    In-line inspection (Fig. 8) of a susceptible BC feature showsthe improvements in focus as the focus invalid area wasreduced.

    Heightened in-line inspection was performed using top-down scanning electron microscopy to gain confidence in theeffectiveness of a reduced focus invalid area at the BC layer.Additionally, electrical parameters and probe yield signatureswere continuously monitored. As illustrated below (Fig. 9),probe yield was consistently improved around the wafer edgeon wafers where the focus invalid area was reduced.

    Fig. 8. Critical Dimension Scanning Electron Microscope (CDSEM)image shows marginal focus of BC (the top row, slots 16-19 exposed withFIA = 7 mm) compared to optimized Focus (the bottom row, slots 1-4,exposed with FIA = 3 mm).

    Fig. 9. Probe yield maps show defective die inked out due to poor focus atthe BC layer (the top row of wafers exposed with FIA = 7 mm) comparedto optimized focus (the bottom row, exposed with FIA = 3 mm).

    The Contact Via (CV) layer, drawn to sub-micron geome-tries, is another feature that is highly sensitive to focus in theBiHEMT technology. The CV layer is patterned to multiplelayers, and requires careful depth of focus characterization toensure the via remains at dimension in the BiHEMT topogra-phy. Fig. 10 (below) shows the improvement in depth of focuson partial fields as the focus invalid area is reduced from 7 mmto 3 mm.

    The first three wafers in Fig. 10 (top row) were exposedwith a focus invalid area set to 3 mm. Thus, adequate depth offocus on partial fields was achieved. The bottom three waferswere exposed with a focus invalid area increased to 7 mm.Thus, the contact via feature was exposed at a marginal focuscondition and poorly patterned.

    The Gate Layer (GL) is patterned at the bottom level of thetopography at sub-micron geometries, often in long serpentine“finger” patterns that require a carefully controlled retrograderesist profile. Perturbations in focus can easily lead to missinggate “fingers” as shown in Fig. 11. The degree to which theGate Layer is impacted by poor focus depends on wafer edgeprocess variation, including variation in film thickness, waferflatness, chuck flatness, and contamination that perturbs thefocal plane of a given field. Fig. 12 below shows a severecase of missing GL on a partial field, where adequate depth offocus was not achieved. By activating as many focus channelsas possible on a given field, the probability of successfullycompensating for this process variation is increased. Thus, by

  • BEST AND TIKU: GDPW AND YIELD OPTIMIZATION FOR GaAs ICs WITH SUB-MICRON FEATURES 521

    Fig. 10. SEM image shows the impact of the focus invalid area exposureparameter on the contact via feature across six different wafers (A, B, C, D, E,and F). Note that this via resides in the same partial field on each wafer. Thetop row (wafers A, B, C) represents the reduced focus invalid area exposurecondition. The bottom row (wafers D, E, F) represents the controlled exposurecondition.

    Fig. 11. Optical image shows missing and displaced gate layer (GL).

    reducing the focus invalid area, yield loss due to missing GLwas minimized.

    C. Improving Detection of Overlay Error

    Lens aberrations induce CD and overlay variation, whichtends to increase further as field size increases. Moreover, vari-ations in CD between two layers can impact the overall overlaybudget. Increased CD variation of two stacked layers reducesthe overlay budget between them. Using BiHEMT technology,both the base contact (BC) and the BP layer align directly tothe emitter contact (EC), making the alignment between BCand BP indirect. In this investigation, a box-in-box measure-ment structure was added to the process control module (PCM)

    Fig. 12. The above image shows a severe GL defect, where GL is completelymissing on portions of the feature.

    Fig. 13. Overlay results between three wafers show poor X and Y-overlay(primary y-axis) control in four field corners compared to the field center.A reticle field size of 20.520 mm × 20.710 mm was used in this example.

    to directly measure overlay between BC and BP as an indicatorof overlay capability at larger BiHEMT field sizes.

    A measurement methodology was then developed using thisstructure to ensure that BC did not fall off of BP as field sizeincreased. Specifically, BC alignment to BP was most criticalin the field corners, where lens aberrations caused the mostsignificant overlay variation. An automated overlay measure-ment recipe was created to measure the X and Y alignmentof BC to BP across multiple fields in the center and cornersof each field. Fig. 13 demonstrates the differences in overlaydistribution from field center to field corners.

    As shown in Fig. 14, this difference tends to magnify as fieldsize increases. In this case, field size increased to 21.280 mm× 21.800 mm.

  • 522 IEEE TRANSACTIONS ON SEMICONDUCTOR MANUFACTURING, VOL. 32, NO. 4, NOVEMBER 2019

    Fig. 14. Overlay results of three wafers (slots 5, 10, 15) are shown, comparingX-OL and Y-OL in field corners to overlay in field center. A field size of21.280 mm × 21.800 mm was used.

    Fig. 15. Overlay results between three wafers show poor X and Y-overlay(primary y-axis) control in four field corners compared to the field center.A reticle field size of 20.520 mm × 20.710 mm was used in this example.

    While field center to field corner overlay variation may beadequate between two layers exposed on the same exposuretool, it must also be sufficient between two layers exposed ondifferent tools. More specifically, the differences in both stagecalibration and lens aberrations between two steppers mustbe considered when changing reticle field size. Fig. 15 belowshows resulting overlay differences between field center andfield corners for wafers exposed on the same stepper at boththe BC and BP layers using the same reticle size representedpreviously in Fig. 13.

    While the overlay variation remains higher in the fieldcorners relative to the field center, the overall variation isimproved in this case study by using the same stepper toexpose both the BC and BP layers. In doing so, differences inimage placement error (IME) between two different stepperswere minimized.

    IV. CONCLUSION

    Effectively minimizing partial fields and mitigating therisk of edge-field focus failures was paramount in evalu-ating increased BiHEMT reticle field sizes. Ultimately, themost significant contributing factor in improving yield wasthe optimization of the focus invalid area to mitigate edge-fieldfocus failures. Finally, developing a detection methodology tomonitor potential unintended consequences of larger field sizeswas critical to our success. As a result of these efforts, wehave developed the tools and infrastructure necessary to con-fidently optimize GDPW while improving stepper throughput,consistency in device performance and product quality.

    ACKNOWLEDGMENT

    The authors would like to acknowledge the contribu-tions of colleagues in both the Advanced Technology Groupand Process Engineering, particularly Ravi Ramanathan,Randy Bryie for his guidance, and Steve Mayer for his insightinto Canon stepper theory of operation.

    Relative to the CS-MANTECH paper, this paper presentsadditional data and data analysis (including additional figures)in Sections III-B and III-C. Additional explanation was addedregarding the algorithm and the focus invalid area parameterdiscussed herein. Additional clarification was added through-out the paper as well as in the conclusion. Slight changesin format, grammar, and wording were made throughout thepaper as well.

    NOMENCLATURE

    GDPW: Gross Die Per WaferIC: Integrated CircuitGaAs: Gallium ArsenideFIA: Focus Invalid AreaFET: Field-Effect TransistorHEMT: High-Electron-Mobility TransistorBiHEMT: Bipolar High Electron Mobility TransistorPHEMT: Pseudomorphic-High-Electron-Mobility-

    TransistorCDSEM: Critical Dimension Scanning Electron

    MicroscopePCM: Process Control ModuleIME: Image Placement ErrorCD: Critical DimensionBC: Base ContactBP: Base PedestalEC: Emitter ContactCV: Contact Via.

    REFERENCE

    [1] R. M. Best and S. K. Tiku, “Gross die per wafer and yield optimizationfor GaAs ICs with sub-micron features,” in Proc. CS-MANTECH,Minneapolis, MN, USA, Apr./May 2019, pp. 279–282.

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