Chain Scissionable Resists Based on Poly(acetal) Motif for Extreme Ultraviolet Lithography A Dissertation Presented to the Faculty of the Graduate School of Cornell University In Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy By Jingyuan Deng December 2022 © 2022 Jingyuan Deng i ABSTRACT Chain Scissionable Resists Based on Poly(acetal) for Extreme Ultraviolet Lithography Jingyuan Deng, Ph.D. Cornell University, 2022 Scissionable polymers are polymers that will depolymerize under different stimuli including acid, base, and free radicals. These polymers have been investigated in the development of photoresists and other degradable materials. This work focuses on the poly(phthalaldehyde), PPA, family of scissionable polymers. The PPA backbone consists of acetal linkages that are very sensitive to acids. Upon exposure to acids, the polymer chain depolymerizes to its corresponding monomers. This depolymerization behavior makes PPAs excellent candidates as photoresist materials. Several new architectures are being explored. For example, PPAs with tethered photoacid generators (PAG)s, which release acid upon irradiation, depolymerize upon exposure followed by a post exposure bake step. The depolymerized monomers in exposed areas could be easily removed using appropriate organic solvents while the unexposed areas remain unchanged. Therefore, both unsubstituted and substituted PPAs may equally serve as a positive tone photoresist. This study focuses on the development of low exposure dose, sensitive PPA photoresists, which do not suffer from materials stochastic issues related to non-uniformities at nanoscale present in multi-component systems for extreme ultraviolet lithography (EUVL). In order to improve the lithographic performance of the PPA photoresists, the structure of the polymer backbone as well as PAGs are being investigated and tailored ii for EUVL. Aryl sulfonates, imidosulfonates, and iminosulfonates were prepared as non- ionic PAGs for PPA photoresists. The steric and electronic nature of these sulfonate PAGs can be easily tuned to optimize acid generation efficiency and their compatibility with a polymer photoresist matrix. All synthesis, characterization, and lithographic evaluation will be presented. iii BIOGRAPHICAL SKETCH Jingyuan Deng was born in Zhengzhou, Henan, China in October 1993. He believes “justice without force is powerless; force without justice is tyrannical” and started practicing Kyokushi Karate at the age of 16. He attended Nagoya University in 2012 and graduated with a B.E. in chemistry. After graduating from Nagoya University, he moved to the University of Tokyo to study organometallic and polymer chemistry under the supervision of Kyoko Nozaki. Upon completing his M.E. from the University of Tokyo, Jingyuan moved to Cornell University to pursue a doctorate degree in 2018. At Cornell University, he developed photoresist materials for EUV lithography in collaboration with Intel Corporation. He finished his Ph.D. degree in 2022 and decided to further pursue his career in semiconductor industry. iv This dissertation is dedicated to my mother and father, who taught me the meaning of love, persistence, and life. v ACKNOWLEDGEMENTS First, I would like to express my heartfelt gratitude to my advisor, Prof. Christopher Ober for providing funding and space for me to conduct research in his group. I would also like to thank my committee members, Prof. Brett Fors and Prof. Frank Schroeder for their helpful discussions. Prof. Nozomi Ando encouraged me to face the challenges and difficulties in graduate school at the beginning of my Ph.D. study. Without her kind encouragement, it was impossible for me to complete a Ph.D. degree. I would like to thank my collaborators from Intel Corporation, Dr. Grant Kloster, Dr. Patrick Theofanis, and Dr. Marie Krysak. In particular, I would like to express my gratitude to Dr. James Blackwell for very helpful discussion and also helping with various aspects of my research. In addition, I greatly appreciate Prof. Denbeaux’s help from SUNY POLY institute on EUV exposures. Being a graduate student in chemistry conducting research in materials science at Cornell has been a unique experience to me. The best part of this experience was about meeting a variety of people. Dr. Atsushi Ozaki, a visiting scholar from Tokyo University of Agriculture and Technology helped me tremendously when I was a first year graduate student. In my second year, I met Yusuke Otsubo, a visiting scholar from JSR Corporation and learned interesting industrial knowledge in photoresist materials from him. In my third year, I met my coworker, Sean Bailey, who later became my best amigo and deeply influenced me as a researcher as well as a person. Other than people at Cornell, I have many more to express my appreciation. I thank Prof. Nozaki for encouraging me to pursue happiness, and Prof. Shintani for inspiring me to be vi Last but not least, I would like to thank my Kyokushin Karate shihan, Hitoshi Kiyama for teaching me how to cope with adversity in my life. I will never be flattered by power and I will never give into violence. a better chemist. I thank Dr. Falk Seidel for various discussions and support. Kimihiro Nakamura, Satoko Takaoka, Hina Yasuda, and Chihiro Kengoyama were my peers back at the University of Tokyo. The time we spent together makes me stronger and fearless. My favorite philosopher, Arthur Schopenhauer wrote “Our happiness lies entirely outside us; for it exists only in the heads of others” in his essays, The Wisdom of Life. I do not believe in imaginary happiness. I will be patient and courageous throughout my life. Hopefully, at the end of my journey, I can make my life with less suffering. vii TABLE OF CONTENTS CHAPTER 1: INTRODUCTION Abstract.............................................................................................................................1 1.1 Introduction................................................................................................................2 1.1.1 Chemical Amplification 1.1.2 Photoacid Generators (PAGs) 1.2 Self-Immolative Polymers.........................................................................................11 1.2.1 Poly(phthalaldehyde)s 1.2.2 Poly(olefin sulfone)s 1.3 EUV Lithography......................................................................................................25 1.3.1 Development of EUV Technology 1.3.2 Resist Materials for EUV Lithography 1.4 Summary...................................................................................................................34 1.5 References.................................................................................................................35 CHAPTER 2: REVIEW OF ESSENTIAL USE OF PHOTOACID GENERATORS IN LITHOGRAPHIC PATTERNING AND PROCESSING Abstract...........................................................................................................................39 2.1 Introduction..............................................................................................................40 2.2 Photoacid Generators...............................................................................................44 2.3 Ionic Photoacid Generators......................................................................................49 2.4 Nonionic Covalent Photoacid Generators................................................................52 2.5 Polymer-Bound PAGs...............................................................................................55 viii 2.6 Alternatives to Fluorinated PAGs ...........................................................................57 2.7 Conclusions..............................................................................................................63 Acknowledgements.........................................................................................................64 2.8 References.................................................................................................................65 CHAPTER 3: TWO COMPONENT PHOTORESIST SYSTEM BASED ON POLY(ACETAL) MOTIF FOR EUV LITHOGRAPHY Abstract...........................................................................................................................68 3.1 Introduction..............................................................................................................69 3.2 Experimental............................................................................................................72 3.2.1 General Procedures 3.2.2 Syntheses and Characterizations of Monomers, Polymers, and PAGs 3.2.3 TGA Analysis of Polymers 3.2.4 SEM Characterization of Patterns for DUV Lithography 3.2.5 MS Experiment on EUV Exposed Samples 3.2.6 Outgassing Experiment 3.2.7 Lithographic Performance: Linear vs Cyclic 3.2.8 Supplemental EUV Contrast Curves 3.3 Results and Discussion............................................................................................93 3.3.1 Synthesis of Monomers, Polymers, and PAGs 3.3.2 DUV Exposure 3.3.3 EUV Exposure 3.3.4 Mechanistic Study 3.3.5 DFT Calculations ix 3.4 Conclusions............................................................................................................116 Acknowledgements.......................................................................................................117 3.5 References...............................................................................................................117 CHAPTER 4: END-CAP ENABLED SELF-IMMOLATIVE PHOTORESISTS BASED ON POLY(ACETAL) MOTIF FOR EUV LITHOGRAPHY Abstract........................................................................................................................129 4.1 Introduction...........................................................................................................130 4.2 Experimental..........................................................................................................131 4.2.1 General Procedures 4.2.2 Syntheses and Characterizations of Monomers, and Polymers 4.2.3 TGA Analysis of Polymers 4.3 Results and Discussion..........................................................................................138 4.3.1 Photodegradation under UV Irradiation 4.3.2 EUV Exposure 4.4 Conclusions............................................................................................................146 Acknowledgements.......................................................................................................146 4.5 References..............................................................................................................147 CHAPTER 5: SINGLE COMPONENT PHOTORESIST SYSTEM BASED ON POLY(ACETAL) MOTIF FOR EUV LITHOGRAPHY Abstract.........................................................................................................................153 5.1 Introduction............................................................................................................154 5.2 Experimental...........................................................................................................159 x 5.2.1 General Procedures 5.2.2 Syntheses and Characterizations of Monomers, Polymers, and PAGs 5.2.3 TGA Analysis of Polymers 5.2.4 NMR Experiments on PAG 1 5.2.5 MS Experiments on PAG 1 and PAG 2 5.2.6 MS Experiments on EUV Exposed Samples 5.2.7 Relative Stereochemistry Determination of Diacetal Products 5.2.8 AFM Film Roughness Measurements 5.2.9 NMR Experiments for Copolymer Ratio Determination 5.2.10 Suzuki-Miyaura Reaction Condition Screening 5.2.11 Gamma Calculation from EUV Contrast Curves 5.2.12 Polymer Ceiling Temperature Calculations 5.3 Results and Discussion............................................................................................210 5.3.1 PAG Design 5.3.2 Synthesis of PAG Tethered Monomers and Polymers 5.3.3 EUV Exposure 5.3.4 DFT Calculations 5.4 Conclusions............................................................................................................230 Acknowledgements.......................................................................................................231 5.5 References..............................................................................................................232 CHAPTER 6: CONCLUSIONS AND FUTURE WORK xi LIST OF FIGURES CHAPTER 1 Figure 1. 1 Flowchart for patterning process. 3 Figure 1. 2 Flowchart for patterning process showing different tools. 4 Figure 1. 3 The concept of chemical amplification. 8 Figure 1. 4 Chemical structures of APEX and ESCAP. 9 Figure 1. 5 Linear and cyclic poly(phthalaldehyde)s. 13 Figure 1. 6 End-capped poly(phthalaldehyde)s. 15 Figure 1. 7 Pendent groups that have been successfully incorporated into the poly(olefin sulfone) backbone. 17 Figure 1. 8 Degradation Mechanism of Poly(olefin sulfone)s (a) Acid (b) Free-Radical (c) Base. 19 Figure 1. 9 Structures Poly(vinyl butyl carbonate sulfone)s. 20 Figure 1. 10 SEM image of polymer with [(o-nitrobenzyl)oxy]carbonyl group film after UV irradiation at 100 mJ/cm2.23 24 Figure 1. 11 Scheme showing the trade-off among resolution, LER, and sensitivity. 27 Figure 1. 12 Planar molecular glass resists (R is a protecting group). 30 Figure 1. 13 Cyclic molecular glass resists (R is a protecting group). 31 Figure 1. 14 Hybrid organic-inorganic nanoparticle resist for EUV lithography. 33 CHAPTER 2 Figure 2. 1 Representative ionic PAGs: 1, 2, 3, 4 Sulfonium PAG and 5, 6 Iodonium PAG. 46 xii Figure 2. 2 Representative nonionic covalent PAGs. 47 Figure 2. 3 Proposed photolysis mechanism for diaryliodonium salt under DUV exposure. 50 Figure 2. 4 Proposed photolysis mechanism for triarylsulfonium salt. 51 Figure 2. 5 Photoacid generation mechanism for aryl sulfonate esters. 53 Figure 2. 6 Photoacid generation mechanism for iminosulfonates and imidosulfonates. 54 Figure 2. 7 Examples of polymer-bound PAGs. (a) Single CF2 unit next to sulfonate21 and (b) single CF2 unit next to sulfonate in a structure that falls apart on exposure; groups (R1, and R2) not specified groups while R3 is a linking group. 56 Figure 2. 8 Chemical structure for non-PFAS covalent PAGs: (a) nitrobenzyl ester and (b) terarylene backbone-based PAG. 58 Figure 2. 9 Chemical structures of untraditional ionic PAGs: (a) 2- phenoxytetrafluoroethane sulfonate PAG and (b) pentacyanocyclopentadienide PAGs. 58 Figure 2. 10 Chemical structures for natural products-based PAGs. 62 CHAPTER 3 Figure 3. 1 TGA measurement of cPPA polymers. 5% weight loss at 128 ˚C. 84 Figure 3. 2 TGA measurement of Br-lPPA polymers. 5% weight loss at 178 ˚C. 85 Figure 3. 3 1:1 Line space pattern with feature size 512 nm observed under SEM after exposure of 50 mJ/cm2 deep UV (248nm) exposure using PAG 3. 86 Figure 3. 4 MS showing compound with molecular formula: C11H7NO + H+ 87 Figure 3. 5 MS showing compound with molecular formula: C8H5BrO2 + H+ 88 Figure 3. 6 MS showing compound with molecular formula: C13H6F3NO5S + H+. The last small peak without labeling is m/z=397.99487. 89 xiii Figure 3. 7 MS spectrum showing outgassing species of P1 under EUV radiation. 90 Figure 3. 8 Mid-UV exposure: a) Patterns observed using Br-cPPA. b) Patterns observed using Br-lPPA. 91 Figure 3. 9 EUV contrast curves for PAG 3–9 shown in logarithmic scale. 92 Figure 3. 10 Chemical structures of PPA derivatives. 94 Figure 3. 11 chemical structures of PAG 1 to 9. 95 Figure 3. 12 DUV contrast curves for PAG 1–4. 99 Figure 3. 13 EUV contrast curves for PAG 3–9. 101 Figure 3. 14 GPC chromatogram of polymer resist (blue plot), EUV sample (red plot), and Br-oPA monomer (black plot). 104 Figure 3. 15 PAG degradation mechanism induced by EUV photons. 105 Figure 3. 16 Proposed decomposition mechanism of PAG 9 under EUV radiation. 107 Figure 3. 17 FOD plots at σ = 0.005 e Bohr–3 (FT-B97M-V/def2-TZVPP (Tel = 5000 K) level) for neutral and radical anions of PAG 3 to 8 (FOD in yellow). 110 Figure 3. 18 Potential energy surface along N–O bond calculated at FT-TPSS-D4/def2- SVP (Tel=5000K) level for PAG 4, 6, 7, and 8. 114 Figure 3. 19 Empirical relationship between VEA corrected activation energy and photospeed. 115 CHAPTER 4 Figure 4. 1 TGA measurement of Br-lPPA-OTf polymers. 136 Figure 4. 2 TGA measurement of Naph-lPPA-OTf polymers. 137 Figure 4. 3 1H NMR spectra of 2 a) before UV irradiation b) after UV irradiation for 30 minutes c) after UV irradiation for 30 minutes and heated at 110 ˚C for 5 minutes. 140 xiv Figure 4. 4 1H NMR spectra of 3 a) before UV irradiation b) after UV irradiation for 30 minutes c) after UV irradiation for 30 minutes and heated at 110 ˚C for 5 minutes. The embedded picture showed the change of color before and after the photodegradation experiment. 141 Figure 4. 5 EUV contrast curve for 1 to 3. 143 CHAPTER 5 Figure 5. 1 a) Linear PPA with PAG blending. b) PPA with photoactive end-cap. c) Functionalized cyclic PPA with PAG tethering. 158 Figure 5.2. DART-MS spectrum taken on PAG 1 48 h after isolation (positive mode).185 Figure 5.3. DART-MS spectrum taken on PAG 1 48 h after isolation (negative mode).185 Figure 5.4. DART-MS spectrum taken on PAG 2 (positive mode). 186 Figure 5.5. DART-MS spectrum taken on photoresist formulation containing PAG 2 after EUV exposure (positive mode). 187 Figure 5.6. DART-MS spectrum taken on photoresist formulation containing PAG 2 after EUV exposure (negative mode). 188 Figure 5.7. DART-MS spectrum taken on photoresist formulation containing PAG 2 after EUV exposure (negative mode). 188 Figure 5.8. Cis and trans conformation of 4-bromophthalaldehyde diacetal. 189 Figure 5.9. Structures showing atom numbering for 4-boronic acid pinacol ester (Bpin) phthalaldehyde diacetal cis and trans isomers. 190 Figure 5.10. Full 2D NOESY spectrum of 4-Bpin phthalaldehyde diacetal containing both diastereomers in DMSO-d6. 191 xv Figure 5.11. 2D NOESY spectrum of 4-Bpin phthalaldehyde diacetal containing both diastereomers in DMSO-d6 with display trimmed to areas of interest. Numbers in blue and black indicate assignments for the cis and trans isomers, respectively. 192 Figure 5.12. Expansion of 2D NOESY of 4-Bpin phthalaldehyde diacetal containing both diastereomers in DMSO-d6 showing the methoxy to acetal NOE correlations. Lines and numbers in blue and black indicate assignments for the cis and trans isomers, respectively. Figure 5.13. 2D 13C-coupled 1H/13C HSQC-NOESY spectrum of 4-bromophthalaldehyde diacetal containing both diastereomers in DMSO-d6. HSQC correlations are displayed with a single blue contour level and NOE correlations are contoured in red. 194 Figure 5.14. Structures showing atom numbering for 4-bromophthalaldehyde diacetal used in this discussion. 195 Figure 5.15. Figure showing the magnetization transfer pathway for homonuclear NOESY and 1H/13C HSQC-NOESY experiments. 196 Figure 5.16. Expansion of the 2D, 13C-coupled 1H/13C HSQC-NOESY spectrum of 4- bromophthalaldehyde diacetal containing both diastereomers in DMSO-d6 showing NOE correlations between methoxy groups of the cis isomer. Red and blue contours represent NOE and HSQC correlations, respectively. 199 Figure 5.17. Chemical structures of formulation 1. 199 Figure 5.18. Chemical structure of formulation 2. 199 Figure 5.19. AFM film roughness measurements for formulation 1. 199 Figure 5.20. AFM film roughness measurements for formulation 2. 200 Figure 5.21. 1H NMR spectrum showing the monomer ratio in PA 3 after complete degradation in CDCl3. 201 xvi Figure 5.22. 1H NMR spectrum showing the monomer ratio in PA 4 after complete degradation in CDCl3. 202 Figure 5.23. 1H NMR spectrum showing the monomer ratio in PA 5 after complete degradation in CDCl3. 203 Figure 5.24. Chemical structures of ligands used in Suzuki-Miyaura reaction condition screening. 205 Figure 5.25. Gamma calculation for resists PA 4 and 5 from EUV contrast curves in logarithmic scale. 206 Figure 5.26. PAG tethered PPAs. 207 Figure 5.27. ΔS calculation for the model reaction. 208 Figure 5.28. Tc calculation for PAS 1. 208 Figure 5.29. Tc calculation for PAS 2. 208 Figure 5.30. Tc calculation for PAS 3. 209 Figure 5.31. Tc calculation for PAS 4. 209 Figure 5.32. EUV contrast curve for PA 1 to PA 6. 223 Figure 5.33. Model Molecules SC 1 to 3 for DFT Calculations. 226 Figure 5.34. FOD plots at σ = 0.005 e Bohr–3 (FT-B97M-V/def2-TZVPP (Tel = 5000 K) level) for radical anions of SC 1 to 3 (FOD in yellow). 227 Figure 5.35. a) PAGs are tethered with the resist, the photogenerated acid after exposure is confined in vicinity of the reactive polymer backbone with smaller diffusion radius. b) PAGs are blended with the resist, the photogenerated acid after exposure diffuses with larger diffusion radius. 229 xvii LIST OF TABLES Table 3. 1 Table summarizing results of EA, photospeed, bond dissociation energy (BDE), and ΔG‡ for PAG 3 to 8. aFor PAG 3 and 5, it is the C–O BDE. 109 Table 4. 1 Calculated values of VEA and BDE for SEC 1 and 5. 146 Table 5.1. Suzuki-Miyaura reaction condition screening results. 205 Table 5.2. Results of Tc calculations. 210 Table 5.3. Results of surface roughness measurements. 226 Table 5.4. Table summarizing results of VEA, BDE, and photospeed for SC 1–3 and PAGs 1–4. 228 1 CHAPTER 1 INTRODUCTION Abstract The semiconductor industry continues to make progress on patterning technology in the nanometer dimension, enabling the fabrication of advanced electronic products. High resolution lithography is the key process for high volume manufacturing (HVM) of such semiconductor devices. Photoresist materials innovation must keep up with the patterning technology revolution. The semiconductor industry currently utilizes extreme ultraviolet (EUV) technology for HVM of sub–7 nm resolution processing and beyond. This chapter will discuss the process of lithography and the development of photoresist materials with emphasis on chain scissionable polymers and EUV lithography. 2 1.1 Introduction Photolithography has been employed for creating patterns in nanometer resolution on thin films for fabrication of advanced structures and devices in the semiconductor industry. The advancements in semiconductor processing have improved the performance of semiconductor devices dramatically in the past decades. This dramatic improvement was made possible by reducing the minimum feature size on chips, with said miniaturization which is driven by the famous “Moore’s law”.1 According to “Moore’s law”, the circuit density (number of transistors in a dense integrated circuit) doubles approximately every two years. In order to meet the denser fabrication expectations set by “Moore’s law”, an urgent revolution is needed for both lithography tools and photoresist materials. Lithography originated as a planographic printmaking process where a feature is drawn onto a flat stone through a chemical reaction. Modern lithography refers to a patterning process in which a feature from a photomask is transferred onto a silicon wafer. This patterning process utilizes photoresist materials, which react with radiation sources (such as UV light) to cause a solubility switch. The process begins with spin coating a photoresist solution onto a silicon wafer. The wafer is then soft baked to remove residual solvent from the film. During the exposure process, radiation is passed through a photomask, transferring the feature to the film. After exposure, the silicon wafer is baked at elevated temperature to accelerate the chemical transformation, causing the solubility in the exposed area on the film to switch. The coated silicon wafer is then immersed into a developer, dissolving the exposed area of a positive tone photoresist, or the unexposed portion of a negative tone photoresist. As the last step, the feature on the photomask can be successfully transferred onto the silicon wafer by a process called etching. 3 Figure 1. 1 Flowchart for patterning process. Prepared silicon wafer Spin Coating & Soft bake Photoresist film Exposure Radiation Mask Post-exposure bake Remove mask Development Pattern 4 Figure 1. 2 Flowchart for patterning process showing different tools. Step 1: Sample preparation: polymer, PAG in solvent Step 2: Spin Coating Step 3: Lithography Step 4: Spectroscopy & Characterization 254nm ABM Contact Lithography 248nm ASML DUV Stepper JEOL Ebeam Lithography Tool AFM Profilometer Ellipsometer SEM 1 2 3 4 EUV Exposure Tool 5 The flowchart for patterning process is shown in (Figure 1. 1). Different exposure wavelengths necessitate the employment of different tools. For example, deep-UV exposure may involve the usage of a 254 nm ABM contact aligner or a 248 nm ASML DUV stepper. For patterning characterization, atomic force microscopy (AFM) and scanning electron microscope (SEM) are popular tools to use as shown in (Figure 1. 2). Several parameters must be accounted for when designing photoresist materials. The first parameter is the solubility of the photoresist material in a casting solvent. Casting solvents used in semiconductor industry usually have high boiling points and high viscosity, such as propylene glycol monomethyl ether acetate (PGMEA) and γ- butyrolactone (GBL). Photoresist materials must be completely soluble in the casting solvent. The second relevant parameter is film formation, meaning that the photoresist materials need to be able to form an amorphous film and show good adhesion to the hydrophilic silicon wafer.2 Polymers are excellent candidates for photoresist materials as they are usually amorphous, and their polarity can be easily tailored though post- polymerization functionalization reactions. Thirdly, to ensure the photons from radiation are not wasted, the photoresist materials must show high absorption at the wavelength of the applied radiation. Fourthly, photoresist materials must exhibit high glass transition temperatures (Tg) as a low Tg will limit the processing window since the pattern will collapse if the post-exposure bake temperature is higher than Tg. Lastly, the photoresist materials must show sufficient resistance towards the etching process. The relative etching resistance can be roughly estimated by the Ohnishi parameter.3 6 𝑉 ∝ 𝑁 𝑁! − 𝑁" In the above expression, V represents the etching rate, N represents the represents the total number of atoms in the molecule, Nc represents the total number of carbon atoms, and No represents the total number of oxygen atoms. According to the Ohnishi parameter, etching rate is inversely proportional to the effective carbon content in the photoresist materials. One of the most important implications of this fact is that the inclusion of ring structures in the photoresist material can significantly increase etching resistance by increasing the relative amount of carbon content.4 In addition to the five central parameters discussed, consideration must be given to storage and thermal stability, sensitivity, and cost of the material. We focus on sensitivity in the next section. 7 1.1.1 Chemical Amplification Sensitivity is one of the most critical parameters of a photoresist material as it is directly proportional to wafer throughput and chips’ manufacturing expenditure. In order to further enhance the sensitivity of photoresist materials, Ito, Wilson, and Fréchet proposed the concept of chemical amplification.5 Essentially, chemical amplification refers to an acid catalyzed deprotection reaction as shown in (Figure 1. 3). The photoresist material contains an acid-labile functional group, which is often the tert- Butyloxycarbonyl (tBoc) protecting group shown in Figure 1. 3. It is mixed with a photoacid generator (PAG), which generates acid upon exposure. The generated acid causes tBoc protecting group to deprotect, which transforms the photoresist material from lipophilic to hydrophilic. This solubility switch enables the exposed area to be dissolved in the basic aqueous developer, tetramethylammonium hydroxide (TMAH), while keeping the unexposed area unaltered. As shown in figure Figure 1. 3, one proton catalyzes a cascade of deprotecting reactions, enabling one photon to trigger numerous chemical transformations. The rate of this catalysis reaction is further accelerated by the postexposure bake procedure at elevated temperature. Even though chemically amplified resists (CARs) are based on the first developed CAR system poly(4-hydroxystyrene) (PHOST) as shown in Figure 1. 3,5 other improved version of PHOST exist, such as environmentally stable chemically amplified photoresist (ESCAP) and APEX shown in (Figure 1. 4).6-7 CAR systems have served as the cornerstone for advanced photolithography and are still evolving today. However, chemically amplified resists have become overly complicated, causing resist design to be painted into a corner. A new architecture for 8 Figure 1. 3 The concept of chemical amplification. n O O O n OH Lipophilic Hydrophilic H Acid Catalyzed Deprotection 9 Figure 1. 4 Chemical structures of APEX and ESCAP. O O OH APEX n m O O O n OH m ESCAP V 10 photoresist materials is urgently needed. 1.1.2 Photoacid Generators (PAGs) Photoacid generators are compounds capable of generating acids upon exposure to radiation.8 These compounds were used for photocationic polymerizations for various types of monomers, including epoxys, vinyl ethers, etc.9 After Ito, Wilson, and Fréchet proposed the concept of chemical amplification in 1980s, wide varieties of PAGs have been designed specifically for photolithography as PAGs could be used to generate acid upon exposure to light, resulting in the removal of the protecting groups on the polymer resin to cause a solubility switch. There are two groups of PAGs: ionic and covalent. The ionic PAGs are onium salts, with triarylsulfonium or diaryliodonium triflate salts most commonly used. These ionic PAGs are capable of generating strong acids with excellent quantum yield. Covalent PAGs are sulfonate esters or sulfonyl compounds, which are capable of generating sulfonic acids or sulfinic acids upon exposure to light. The detailed chemical structures for both ionic and covalent PAGs and photodegradation mechanism will be presented in chapter 2. 11 1.2 Self-Immolative Polymers. Self-immolative polymers are polymers that depolymerize end-to-end under different stimuli including acid, base, and free radicals.10 They have been studied intensively in recent decades because of their unique depolymerization behavior. These stimuli- responsive materials are critical to the development of transient electronics, photolithography, sensors, and drug delivery.11 There are two different ways of triggering depolymerization of self-immolative polymers. One is through end-cap cleavage, and the other is through backbone cleavage. The depolymerization process can be either reversible or irreversible. Reversible self-immolative polymers depolymerize back to the monomers that they were synthesized from. Therefore, the monomers can be repolymerized to generate the polymers. Irreversible self-immolative polymers depolymerize to form molecules that are different from the monomers that they were synthesized from. In this section, I will introduce two different self-immolative polymers, poly(phthalaldehyde)s and poly(olefin sulfone)s, two reversible self-immolative polymers. Reversible self-immolative polymers possess low ceiling temperatures (Tc), which is defined by the equation below: 𝑇! = Δ𝐻 Δ𝑆 Δ𝐻 is the change of enthalpy of the polymerization reaction, and Δ𝑆 is the change of entropy of the polymerization reaction. Self-immolative polymers with high molecular weight can only be synthesized below the ceiling temperature. These polymers are usually kinetically trapped by either end-capping or cyclization below the ceiling temperature to prevent depolymerization from happening at temperature higher than the ceiling 12 temperature. However, when the end-cap is removed or the backbone is cleaved, the polymer will depolymerize. The self-immolative polymer I have studied in my Ph.D. career, poly(phthalaldehyde) (PPA), has been previously used in high resolution photolithography as, for example, mask making.12 The PPA backbone consists of acetal linkages that are very sensitive to acids. Upon exposure to acids, the polymer chain depolymerizes to its corresponding monomers. 1.2.1 Poly(phthalaldehyde)s Poly(phthalaldehyde)s are synthesized through polymerization reactions from the dialdehyde monomer, o-phthalaldehyde. There are two topologies reported from literature on poly(phthalaldehyde)s, cyclic and linear (Figure 1. 5).12 Cyclic poly(phthalaldehyde)s are synthesized through cationic polymerizations using Lewis acid catalyst including BF3·OEt2, TiCl4, and SnCl4.13 Linear poly(phthalaldehyde)s are synthesized through anionic polymerizations with end-caps using anionic initiators such as t-BuOLi, sodium with naphthalene or benzophenone, etc.14 Poly(phthalaldehyde)s found applications in photolithography in 1980s by Ito, Wilson and coworkers for dry developing resist materials.5 Poly(phthalaldehyde)s plus PAG formulations showed high sensitivity under exposure of UV light. However, the project tumbled at IBM as the depolymerization product, which is the monomer o-phthalaldehyde, is too volatile and contaminates expensive optics inside of the exposure tools. Based on this unique feature of poly(phthalaldehyde)s, Moore and coworkers developed transient electronics for free- standing transistor arrays.11 Depolymerization of poly(phthalaldehyde)s could also be triggered mechanically.15 Moore and coworkers discovered that depolymerization of poly(phthalaldehyde)s with molecular weight above 30 kg/mol could be triggered by 13 Figure 1. 5 Linear and cyclic poly(phthalaldehyde)s. OO O OO O R R R n OO O R2R1 n R Linear Cyclic 14 mechanical forces applied using pulsed ultrasound. Depolymerization of linear poly(phthalaldehyde)s can also be triggered by removing the end-caps. Phillips and coworkers synthesized poly(phthalaldehyde)s with different end-caps that react with specific chemical stimuli (Figure 1. 6).16 Tert-butyldimethylsilyl end-capped poly(phthalaldehyde)s react with fluoride ions, and allyl carbonate end- capped poly(phthalaldehyde)s react with Pd(0) species. A substantial amount of research and significant advancements have been achieved on unsubstituted poly(phthalaldehyde)s. However, functionalized poly(phthalaldehyde)s are rarely reported due to synthetic challenges.17 I developed a new synthetic methodology for rapid and efficient synthesis of functionalized poly(phthalaldehyde)s. Details will be presented in chapter 5. 15 Figure 1. 6 End-capped poly(phthalaldehyde)s. OO O R n O O OO O R nSi Allyl carbonate Tert-butyldimethylsilyl 16 1.2.2 Poly(olefin sulfone)s Poly(olefin sulfone) is known as one of the self-immolative polymers that could depolymerize under different stimuli. Once the stimulus is applied, the cleavage at the relatively weak C–S bond on the polymer backbone will initiate the depolymerization process, which releases gaseous SO2 and the corresponding vinyl monomer. This depolymerization process is reversible. If the depolymerized monomers can be collected, it is possible to polymerize them again, which gives the possibility for sustainable chemistry. Poly(olefin sulfone) is synthesized from SO2 and vinyl monomers through free radical polymerization using initiators such as tert-butyl hydroperoxide at –78 ˚C with excellent functional group tolerance as shown in (Scheme 1. 1). Scheme 1. 1 Copolymerization of olefins with SO2. Other than tert-butyl hydroperoxide, benzoyl peroxide and diethyl ether peroxides could also be used as polymerization initiators. General olefin monomers such as 1-butene, 1- pentene, 1-hexene, cyclopentene, and cyclohexene could be used as the vinyl monomers. Poly(olefin sulfone) synthesized by a free radial pathway is an alternating copolymer, consisting of the vinyl monomer and sulfur dioxide in 1 to 1 ratio.18 In the past decades, a wide variety of vinyl monomers has been successfully incorporated into the polymer backbone and some of the pendent group examples are shown in (Figure 1. 7). R –78 °C SO2 tBuOOH S O O R n 17 Figure 1. 7 Pendent groups that have been successfully incorporated into the poly(olefin sulfone) backbone. O O O O O O O O Cl O O O O O O N H O O O O Pendent Groups (R) a b c d e h f i j kg N3 18 There are 3 different pathways which will lead to polymer degradation: acid, free radical, and base. Degradation mechanisms are shown in (Figure 1. 8). Among these degradation mechanisms, degradation under basic conditions has been studied extensively because of the controllability of this process. The most acidic protons on the polymer backbone are the ones on the carbon atoms adjacent to SO2 groups, which is a very strong electron- withdrawing group. Under basic conditions, one of these protons will react with base and the whole polymer chain is depolymerized back to the vinyl monomer and SO2.19 Poly(olefin sulfone)s with tunable thermal stability has been reported by Jeffrey Moore and coworkers in 2015. A series of poly(vinyl butyl carbonate sulfone)s has been synthesized with tert-, sec-, iso-, and n-butyl groups on the carbonate moiety (Figure 1. 9) and their thermal stability was evaluated by thermogravimetric analysis (TGA).20 According to the literature, the thermal degradation of poly(alkyl olefin sulfone)s goes through a concerted β-elimination mechanism with a 5-membered ring transition state.21 The stability of the polymer backbone is significantly affected by sterically bulky tert- butyl carbonate groups. As expected, the less bulky the side group is, the more stable the polymer backbone will be. According to TGA analysis, P1 has the lowest degradation temperature, 91˚C. P2, which has a sec-butyl groups on the carbonate moiety showed higher degradation temperature, 167 ˚C. P3 and P4 with iso-, and n-butyl groups on the carbonate moiety showed the highest degradation temperature, which is 213 ˚C. From the observed trend, less substituted β-carbon on the carbonate moiety increased the thermal stability of the resulting polymer. Researchers also investigated the possibility of using poly(olefin sulfone)s as photoresist materials. A poly(olefin sulfone) (POS) tethered or mixed with a photobase 19 Figure 1. 8 Degradation Mechanism of Poly(olefin sulfone)s (a) Acid (b) Free-Radical (c) Base. S R O O H S R O OH H H R + H– S O OH S O O + R S R O O S R O O S O O S R O OR + R + S O O S O O H R S O O S R O O Nu S O O R S O S R O O O + R + S O O a) b) c) 20 Figure 1. 9 Structures Poly(vinyl butyl carbonate sulfone)s. O O O S O O n O O O S O O n O O O S O O n O O O S O O n P1 P2 P3 P4 21 generator (PBG), which releases base upon irradiation, depolymerizes upon irradiation followed by post exposure bake as shown in (Scheme 1. 2).22 Scheme 1. 2 Depolymerization of POS with PBG. Sasaki and coworkers synthesized poly(olefin sulfone) with photobase generators, including oxime urethane group and [(o-nitrobenzyl)oxy]carbonyl group incorporated into the main polymer backbone.23 These photobase generators could release primary- or secondary-amino groups through decarboxylation process as shown in (Scheme 1. 3). Scheme 1. 3 Structures of poly(olefin sulfone)s with pendant photobase generators and the photochemical reactions of the pendant group. In order to evaluate these materials’ lithographic performance, DMSO was used as the solvent to dissolve the polymer materials, and the film was made by spin-coating the solution onto a glass plate. The coated glass plates were then irradiated with UV light. With the exposure dosage of 1 J/cm2, about 7% of the oxime urethane groups transformed S O O n PBG Irradiation S O O n Base Heat S O O + R S CH2 O O HC H2 C H N C O N O CH3 Irradiation S CH2 O O HC H2 C NH2 + CO2 N CH3 N H3C + S CH2 O O HC H2 C H N C O O N C O H2 C O O2N Irradiation S CH2 O O HC H2 C H N C O O NH + CO2 + HC O2N O 22 to primary amino groups through photolysis. With the same exposure dosage, about 16% of the [(o-nitrobenzyl)oxy]carbonyl groups transformed to secondary amino groups through an internal redox reaction. Therefore, the [(o-nitrobenzyl)oxy]carbonyl group exhibited the highest photosensitivity. After exposure with UV light, post exposure bakes at 130 °C for 60 s were employed to further accelerate the depolymerization process. Finally, the glass plates were washed with 0.012 M HCl for 30 s to wash away the depolymerized monomers and the residual amines. The SEM image of a 40 μm line and space pattern is shown in (Figure 1. 10). In 2011, Whittaker and coworkers prepared a series of polymers that constitute poly(olefin sulfone) backbone and poly(methyl methacrylate) (PMMA) side chains for extreme ultraviolet lithography. The poly(olefin sulfone) backbone depolymerizes rapidly upon exposure to EUV photons, and PMMA side chains were designed to increase the overall stability of the polymer structure.24 Atom transfer radical polymerization (ATRP) was utilized to synthesize PMMA macromonomers with olefin group chain end. Polymerizing the PMMA macromonomers with sulfur dioxide and pentene to form the poly(olefin sulfone) backbone generates the final material as shown in (Scheme 1. 4). Synthesized polymers were exposed to EUV photons to create line and space pattern. The mixture of isopropyl alcohol (IPA) and methylisobutylketone (MIBK) with a ratio of 90/10 was used as the developer to remove depolymerized monomers. AFM was used to characterize the resulting patterns. From AFM images, 30 nm line and space patterns were created. However, bridging and pattern collapse could be seen. 23 Scheme 1. 4 Synthesis of allyl-terminated PMMA macromers and poly(1-pentene-co- PMMA sulfone)s with a comb architecture. O Br O + O O Cu(I)Br Toluene 90 °C O O Br OO = –78 °C SO2 tBuOOH 1-pentene S O O S S O O O O 24 Figure 1. 10 SEM image of polymer with [(o-nitrobenzyl)oxy]carbonyl group film after UV irradiation at 100 mJ/cm2.23 25 1.3 EUV Lithography Extreme ultraviolet (EUV) lithography, which employs a 13.5 nm wavelength light source, is used to create patterns with a resolution below 10 nm. According to “Moore’s law”, the circuit density (number of transistors in a dense integrated circuit) doubles approximately every two years. In order to meet denser fabrication expectations set by “Moore’s law”, an urgent revolution is needed for both lithography tools and photoresist materials. For optical lithography, the feature size (resolution) is dictated by Rayleigh’s equation: 𝑅 = 𝑘 𝜆 𝑁𝐴 where R is the resolution limit of the feature. The Rayleigh coefficient k is governed by the processing conditions, and λ represetns the optical wavelength. NA is the numerical aperture, which is determined by the imaging system including the optical lens and media. 1.3.1 Development of EUV Technology In order to print smaller features, according to Rayleigh’s equation, the optical wavelength must be shorter, numerical aperture must be higher, or Rayleigh coefficient k1 must be smaller. In the semiconductor industry, the optical wavelength for photolithography has shortened from 436 nm (visible g-line), 365 nm (ultraviolet i-line), 248 nm (KrF laser) and 193 nm (ArF laser). The numerical aperture can be increased by changing the media with higher refractive index. This has led to the advent of 193 nm 26 immersion lithography. The Rayleigh coefficient k could be deceased via multiple patterning technology. By combining multiple cycles of exposures and etching, feature density can be enhanced even without shorter optical wavelength exposure source or a medium with higher refractive index. With multiple patterning technology, it is possible to achieve features with 10 nm size. However, for feature sizes smaller than 10 nm, multiple patterning technology becomes too costly and complicated in processing. These constraints have motivated the semiconductor industry to develop EUV technology for sub 10 nm resolution lithography. Currently, the leading semiconductor corporations have accomplished the fabrication of 7 nm and 5 nm nodes utilizing EUV technology and are working on the fabrication of 3 nm and 2 nm nodes. 1.3.2 Resist Materials for EUV Lithography The performance of a photoresist material is evaluated by several parameters including line edge roughness (LER), resolution, sensitivity (photospeed), outgassing, photo- absorption, and etching resistance. In the era of chemically amplified resists (CARs), the trade-off among resolution, LER, and sensitivity (RLS trade-off) (the so called “triangle of death”) is infamous (shown in Figure 1. 11).25 The RLS trade-off prevents the optimization of resolution, sensitivity, and LER at the same time. A photoresist material that has high sensitivity and resolution must subsequently show large LER values. The simplified notation for RLS trade-off, known as the Z-parameter,26 is shown in the equation below: 27 Figure 1. 11 Scheme showing the trade-off among resolution, LER, and sensitivity. Resolution LWR Sensitivity LER due to photon shot noise The most difficult technical requirement for EUV resist is simultaneous improvement in resolution, LWR, and sensitivity (RLS). (1) RLS trade off problem There are two important problems in EUV resists (2) Photon shot noise problem E UVL Workshop 2017 28 𝑍 = 𝑅# × 𝐿$ × 𝐷 R stands for resolution, L is the LER, and D is the minimum dosage required to completely remove the resist film from the silicon wafer. The smaller the Z value, the better the overall performance of the resist material is. Poly(4-hydroxystyrene) and its derivatives were commonly used as CAR type photoresist materials for deep UV lithography.27 In the past decades, they have been tailored to EUV technology. The semiconductor industry has realized 12 nm patterning with exposure dosage of 30 mJ/cm2 using CAR based photoresist materials. However, considering low EUV photon absorption of carbon and oxygen atoms, continuing use of CAR based photoresist materials for sub 10 nm pattering utilizing EUV technology is not ideal as the photon density from EUV radiation is much lower compared to that in deep UV radiation with the same dosage. In order to circumvent this obstacle, researchers have synthesized fluorinated derivatives of poly(4-hydroxystyrene) polymers and they showed more than doubled EUV absorption coefficient.28 Another issue associated with CAR based photoresist materials is the control of stochastics. The PAG molecules are usually blended with polymer matrix in CARs, which results in an inhomogeneous distribution of PAGs and polymers. In order to minimize this inhomogeneity, researchers synthesized polymers with PAG molecules covalently bound to the polymer backbone.27 The PAG tethered CARs showed better LER, resolution and sensitivity compared to the PAG blended CARs. As the feature size becomes smaller and smaller, LER becomes a significant challenge. Photoresist materials based on polymer materials are polydisperse having uneven distribution of molecular weights, which exacerbates the stochastics issues.29 Photoresist 29 materials based on molecular glasses have garnered increasing attention as it consists of monodisperse small molecules that form a glassy amorphous state at room temperature. Molecular glass resists have high glass transition temperature, which is beneficial for thin film formation. The monodisperse building blocks of molecular glass resists are beneficial for patterning with higher resolution and lower LER values. High thermal stability of molecular glass resists allows higher processing temperature for PAB and PEB. Ober and coworkers proposed the design guidelines for designing molecular glass resists.30 They can be categorized into planar and branched molecular glass based on phenolic and phenylbenzene derivatives (Figure 1. 12),31 and cyclic molecular glass based on calix[n]arene and calix[4]resorcinarene derivatives (Figure 1. 13).32 Ober and coworkers have studied the structure-property relationship on poly(4-hydroxystyrene) derived molecular glass resists and discovered that the glass transition temperature of these resists increases with increasing size of the molecules.33 Henderson and coworkers have synthesized epoxide functionalized molecular glass resists for e-beam lithography.34 Line space patterning with 35 nm half-pitch resolution and exposure dosage 20 μC/cm2 was achieved. Molecular glass resists derived from calix[n]arene core has also been intensively studied. Ober and coworkers synthesized t-BOC protected C-4- hydroxyphenyl-calix[4]resorcinarenes derivatives as positive tone molecular glass resists for EUV lithography. Line space patterning with 30 nm half-pitch resolution, exposure dosage 22 mJ/cm2 was well resolved.32 In recent years, photoresist materials based on hybrid organic-inorganic architecture have attracted much attention from both the academia and the semiconductor industry. In 2010, Ober and coworkers developed organic ligand stabilized HfO2 nanoparticles that 30 Figure 1. 12 Planar molecular glass resists (R is a protecting group). OR RO OR OR RO OR RO OR RO OR OR OR RO RO OR OR OR RO OR OR OR RO OR OR OR OR RO RO 31 Figure 1. 13 Cyclic molecular glass resists (R is a protecting group). RO OR RO RO RO OR OR OR RO OR RO RO RO OR OR OR RO OR RO RO RO OR OR OR RO OR ORRO RO OR RO RO RO OR OR OR RO OR RO RO RO OR OR OR O O OO RO OR RO RO RO OR OR OR 32 are readily miscible with polymer photoresist materials for 193 nm lithography.35 These high refractive index and high transparency HfO2 nanocomposites showed higher resistance to plasma etching processes and were able to resolve 200 nm line/space patterns under e-beam radiation. In later research, Ober and coworkers have found that by coordinating photo-switchable ligands directly to the metal oxide core renders the metal complex a photoresist material (Figure 1. 14).36-37 Methacrylic acid was used as the photo-switchable ligand that coordinates to a hafnium/zirconium oxide core. When mixed with a photoradical initiator or PAG, this metal oxide nanoparticle could be used as a dual-tone photoresist materials for EUV lithography. Zirconium oxide based resist showed higher sensitivity under EUV exposure. Line space patterning with 26 nm half- pitch resolution and exposure dosage 4.2 mJ/cm2 was achieved.38 The mechanism for triggering the solubility switch of these metal oxide based photoresists is not fully understood. Li, Giannelis and coworkers observed that there was a significant change in nanoparticle sizes before and after exposure due to ligand exchange, which might contribute to the solubility difference.39 As these metal oxide based photoresists show high EUV absorption as well as high etching resistance, researchers developed other organometallic photoresists based on different metals including tin, titanium, antimony, bismuth, and palladium.40-41 33 Figure 1. 14 Hybrid organic-inorganic nanoparticle resist for EUV lithography. 34 1.4 Summary The semiconductor industry continues to make progress on patterning technology in nanometer dimension, which enables the fabrication of advanced electronic products. EUV technology has become the most reliable choice for high volume manufacturing for sub-10 nm node. In order to take full advantage of EUV technology, novel photoresist materials must be developed. For CAR based photoresist materials, as PAG concentration is limited by the RLS-trade off, it is challenging to design resist materials with high resolution and sensitivity but low LER. Molecular glass based resists, based on acid catalyzed deprotection mechanism, possess low sensitivity in general. Metal oxide based resists show great resolution, sensitivity, LER, and high etching resistance. However, the mechanism for the solubility switch is not fully understood, which may hinder the development of these resists. Chain scissionable photoresist have garnered increasing attention in recent years. As discussed in 1.2.2, researchers studied the thermal stability of poly(olefin sulfone)s and attempted to utilize them as photoresist materials for EUV lithography. However, these materials suffer from narrow substrate scope, dark loss, severe outgassing, and low sensitivity issues. Eventually, they were abandoned as photoresist materials. As discussed in 1.2.1, Ito, Wilson and coworkers attempted to use poly(phthalaldehyde)s as dry developing resist materials for photolithography in 1980s.5 However, the project failed as the depolymerization product, o-phthalaldehyde was too volatile and contaminated expensive optics inside of the exposure tools. These issues could be solved by synthesizing phthalaldehyde derivatives with higher thermal stability, which will be presented in chapter 3. 35 1.5 References 1. Bondyopadhyay, P. K., Moore's law governs the silicon revolution. Proceedings of the Ieee 1998, 86 (1), 78-81. 2. Kim, J.-B.; Yun, H.-J.; Kwon, Y.-G.; Lee, B.-W., Adhesion-promoted copolymers for 193-nm photoresists without cross-linking during lithographic process. Journal of Photopolymer Science and Technology 2000, 13 (4), 629-634. 3. Gokan, H.; Esho, S.; Ohnishi, Y., Dry Etch Resistance of Organic Materials. Journal of the Electrochemical Society 1983, 130 (1), 143-146. 4. Kunz, R.; Palmateer, S.; Forte, A.; Allen, R.; Wallraff, G.; Di Pietro, R.; Hofer, D., Limits to etch resistance for 193-nm single-layer resists. SPIE: 1996; Vol. 2724. 5. Ito, H.; Willson, C. G., Chemical amplification in the design of dry developing resist materials. Polymer Engineering & Science 1983, 23 (18), 1012-1018. 6. Breyta, G.; Hofer, D. C.; Ito, H.; Seeger, D.; Petrillo, K.; Moritz, H.; Fischer, T., The Lithographic Performance and Contamination Resistance of a New Family of Chemically Amplified DUV Photoresists. Journal of Photopolymer Science and Technology 1994, 7 (3), 449-460. 7. Poppe, J.; Neureuther, A., Improved performance of Apex-E photoresist with the application of the electric field enhanced PEB. SPIE: 2004; Vol. 5376. 8. Martin, C. J.; Rapenne, G.; Nakashima, T.; Kawai, T., Recent progress in development of photoacid generators. Journal of Photochemistry and Photobiology C: Photochemistry Reviews 2018, 34, 41-51. 9. Decker, C.; Moussa, K., Kinetic study of the cationic photopolymerization of epoxy monomers. Journal of Polymer Science Part A: Polymer Chemistry 1990, 28 (12), 3429-3443. 10. Yardley, R. E.; Kenaree, A. R.; Gillies, E. R., Triggering Depolymerization: Progress and Opportunities for Self-Immolative Polymers. Macromolecules 2019, 52 (17), 6342-6360. 11. Hernandez, H. L.; Kang, S.-K.; Lee, O. P.; Hwang, S.-W.; Kaitz, J. A.; Inci, B.; Park, C. W.; Chung, S.; Sottos, N. R.; Moore, J. S.; Rogers, J. A.; White, S. R., Triggered Transience of Metastable Poly(phthalaldehyde) for Transient Electronics. Advanced 36 Materials 2014, 26 (45), 7637-7642. 12. Wang, F.; Diesendruck, C. E., Polyphthalaldehyde: Synthesis, Derivatives, and Applications. Macromol Rapid Commun 2018, 39 (2). 13. Aso, C.; Tagami, S., Cyclopolymerization of o-phthalaldehyde. Journal of Polymer Science Part B: Polymer Letters 1967, 5 (3), 217-220. 14. Aso, C.; Tagami, S., Polymerization of Aromatic Aldehydes. III. The Cyclopolymerization of Phthaldehyde and the Structure of the Polymer. Macromolecules 1969, 2 (4), 414-419. 15. Diesendruck, C. E.; Peterson, G. I.; Kulik, H. J.; Kaitz, J. A.; Mar, B. D.; May, P. A.; White, S. R.; Martínez, T. J.; Boydston, A. J.; Moore, J. S., Mechanically triggered heterolytic unzipping of a low-ceiling-temperature polymer. Nature Chemistry 2014, 6 (7), 623-628. 16. Seo, W.; Phillips, S. T., Patterned Plastics That Change Physical Structure in Response to Applied Chemical Signals. Journal of the American Chemical Society 2010, 132 (27), 9234-9235. 17. Lutz, J. P.; Davydovich, O.; Hannigan, M. D.; Moore, J. S.; Zimmerman, P. M.; McNeil, A. J., Functionalized and Degradable Polyphthalaldehyde Derivatives. Journal of the American Chemical Society 2019, 141 (37), 14544-14548. 18. Cais, R. E.; O'Donnell, J. H.; Bovey, F. A., Copolymerization of Styrene with Sulfur Dioxide. Determination of the Monomer Sequence Distribution by Carbon-13 NMR. Macromolecules 1977, 10 (2), 254-260. 19. Shinoda, T.; Nishiwaki, T.; Inoue, H., Decomposition of poly(4-hydroxystyrene sulfone) in alkaline aqueous solutions. Journal of Polymer Science Part A: Polymer Chemistry 2000, 38 (15), 2760-2766. 20. Lee, O. P.; Lopez Hernandez, H.; Moore, J. S., Tunable Thermal Degradation of Poly(vinyl butyl carbonate sulfone)s via Side-Chain Branching. ACS Macro Letters 2015, 4 (7), 665-668. 21. Cubbage, J. W.; Vos, B. W.; Jenks, W. S., Ei Elimination:  An Unprecedented Facet of Sulfone Chemistry. Journal of the American Chemical Society 2000, 122 (20), 4968-4971. 22. Suyama, K.; Shirai, M., Photobase generators: Recent progress and application 37 trend in polymer systems. Progress in Polymer Science 2009, 34 (2), 194-209. 23. Yaguchi, H.; Sasaki, T., Photoinduced Depolymerization of Poly(olefin sulfone)s Possessing Photobase Generating Groups in the Side Chain. Macromolecules 2007, 40 (26), 9332-9338. 24. Lawrie, K. J.; Blakey, I.; Blinco, J. P.; Cheng, H. H.; Gronheid, R.; Jack, K. S.; Pollentier, I.; Leeson, M. J.; Younkin, T. R.; Whittaker, A. K., Chain scission resists for extreme ultraviolet lithography based on high performance polysulfone-containing polymers. Journal of Materials Chemistry 2011, 21 (15). 25. Mojarad, N.; Gobrecht, J.; Ekinci, Y., Beyond EUV lithography: a comparative study of efficient photoresists' performance. Scientific Reports 2015, 5 (1), 9235. 26. Higgins, C. D.; Szmanda, C. R.; Antohe, A.; Denbeaux, G.; Georger, J.; Brainard, R. L., Resolution, Line-Edge Roughness, Sensitivity Tradeoff, and Quantum Yield of High Photo Acid Generator Resists for Extreme Ultraviolet Lithography. Japanese Journal of Applied Physics 2011, 50, 036504. 27. Itani, T.; Kozawa, T., Resist Materials and Processes for Extreme Ultraviolet Lithography. Japanese Journal of Applied Physics 2013, 52 (1R), 010002. 28. Yamamoto, H.; Kozawa, T.; Tagawa, S.; Yukawa, H.; Sato, M.; Onodera, J., Enhancement of Acid Production in Chemically Amplified Resist for Extreme Ultraviolet Lithography. Applied Physics Express 2008, 1, 047001. 29. Patsis, G. P.; Gogolides, E., Effects of model polymer chain architectures and molecular weight of conventional and chemically amplified photoresists on line-edge roughness. Stochastic simulations. Microelectronic Engineering 2006, 83 (4), 1078-1081. 30. De Silva, A.; Felix, N. M.; Ober, C. K., Molecular Glass Resists as High- Resolution Patterning Materials. Advanced Materials 2008, 20 (17), 3355-3361. 31. De Silva, A.; Ober, C. K., Hydroxyphenylbenzene derivatives as glass forming molecules for high resolution photoresists. Journal of Materials Chemistry 2008, 18 (16), 1903-1910. 32. Chang, S. W.; Ayothi, R.; Bratton, D.; Yang, D.; Felix, N.; Cao, H. B.; Deng, H.; Ober, C. K., Sub-50 nm feature sizes using positive tone molecular glass resists for EUV lithography. Journal of Materials Chemistry 2006, 16 (15), 1470-1474. 33. De Silva, A.; Lee, J.-K.; André, X.; Felix, N. M.; Cao, H. B.; Deng, H.; Ober, C. 38 K., Study of the Structure−Properties Relationship of Phenolic Molecular Glass Resists for Next Generation Photolithography. Chemistry of Materials 2008, 20 (4), 1606-1613. 34. Lawson, R. A.; Lee, C.-T.; Yueh, W.; Tolbert, L.; Henderson, C. L., Epoxide functionalized molecular resists for high resolution electron-beam lithography. Microelectronic Engineering 2008, 85 (5-6), 959-962. 35. Bae, W. J.; Trikeriotis, M.; Sha, J.; Schwartz, E. L.; Rodriguez, R.; Zimmerman, P.; Giannelis, E. P.; Ober, C. K., High refractive index and high transparency HfO2 nanocomposites for next generation lithography. Journal of Materials Chemistry 2010, 20 (25), 5186-5189. 36. Trikeriotis, M.; Bae, W. J.; Schwartz, E.; Krysak, M.; Lafferty, N.; Xie, P.; Smith, B.; Zimmerman, P.; Ober, C.; Giannelis, E., Development of an inorganic photoresist for DUV, EUV, and electron beam imaging. SPIE: 2010; Vol. 7639. 37. Krysak, M.; Trikeriotis, M.; Schwartz, E.; Lafferty, N.; Xie, P.; Smith, B.; Zimmerman, P.; Montgomery, W.; Giannelis, E.; Ober, C., Development of an inorganic nanoparticle photoresist for EUV, e-beam, and 193nm lithography. SPIE: 2011; Vol. 7972. 38. Trikeriotis, M.; Krysaki, M.; Chung, Y. S.; Ouyang, C.; Cardineau, B.; Brainard, R.; Ober, C. K.; Giannelis, E. P.; Cho, K., Nanoparticle photoresists from HfO2 and ZrO2 for EUV patterning. Journal of Photopolymer Science and Technology 2012, 25 (5), 583- 586. 39. Li, L.; Chakrabarty, S.; Spyrou, K.; Ober, C. K.; Giannelis, E. P., Studying the Mechanism of Hybrid Nanoparticle Photoresists: Effect of Particle Size on Photopatterning. Chemistry of Materials 2015, 27 (14), 5027-5031. 40. Toriumi, M.; Sato, Y.; Koshino, M.; Suenaga, K.; Itani, T., Metal resist for extreme ultraviolet lithography characterized by scanning transmission electron microscopy. Applied Physics Express 2016, 9 (3), 031601. 41. Passarelli, J.; Murphy, M.; Del Re, R.; Sortland, M.; Hotalen, J.; Dousharm, L.; Fallica, R.; Ekinci, Y.; Neisser, M.; Freedman, D.; Brainard, R., Organometallic carboxylate resists for extreme ultraviolet with high sensitivity. Journal of Micro/Nanolithography, MEMS, and MOEMS 2015, 14 (4), 043503. 39 CHAPTER 2 REVIEW OF ESSENTIAL USE OF PHOTOACID GENERATORS IN LITHOGRAPHIC PATTERNING AND PROCESSING (Published as: Ober, C.; Kafer, F.; Deng, J. Review of essential use of fluorochemicals in lithographic patterning and semiconductor processing. J. Micro/Nanopatterning, Mater., Metrol. 2022, 21, 010901.) Abstract We identify and describe categories of fluorochemicals used to produce advanced semiconductors within the lithographic patterning manufacturing processes. Topics discussed include the per- and polyfluoroalkyl substance (PFAS) materials used and their necessary attributes for successful semiconductor manufacturing, consisting of photoacid generators, fluorinated polyimides, poly(benzoxazole)s, antireflection coatings, topcoats, and embedded barrier layers, fluorinated surfactants, and materials for nanoimprint lithography. In particular, an explanation is given of the particular function that these PFAS materials contribute. It is noted that in almost all cases fluorine-free alternatives are very unlikely to provide the essential properties present in PFAS systems. Nonfluorinated alternative compounds are discussed where available. Author Contribution C.K.O designed the review. J.D. contributed to the PAG section in this review. F. K. contributed to the other sections. 40 2.1 Introduction The use of fluorochemicals in lithography and semiconductor patterning plays a critical role in the success of semiconductor technology. The addition of small quantities of fluorinated mate- rials enables patterning capabilities that are otherwise not possible to achieve, and this leads to superior device performance. The compact size of the fluorine atom and its strong electron- withdrawing characteristics make it stand out in the periodic table and gives fluorocarbon mate- rials unique properties, unmatched by other chemical compounds. Fluorochemicals have found use in semiconductor processing for good technical reasons. 1. The presence of fluorine near acidic groups can convert them from an acid to a superacid, an essential characteristic for photoacid generators (PAGs) needed in advanced photoresists. 2. Fluorocarbon materials have low surface energy characteristics and act as superior barrier layers (including water repellence), which provide useful properties in photoresists and in antireflection coatings used in immersion lithography while also providing excellent release properties because they do not adhere strongly to other materials. 3. Fluorinated materials have unique solubility characteristics and can prevent intermixing between layers in a complex system such as an antireflection coating. Fluorinated materials are both hydrophobic and oleophobic and thus have reduced or no miscibility with essentially all fluorine-free classes of polymers. 4. Fluoropolymers have a low refractive index compared with any material except air and 41 provide useful optical properties in photoresists and antireflection coatings. 5. They possess low dielectric constant and are especially good electrical insulators, an important feature when polyimides are patterned and retained in the final device. This document provides a systematic overview of the photolithography process and key fluorinated materials involved, provides insight into performance requirements, and describes why fluorinated chemicals help achieve needed characteristics. Photolithography, a critical process step in the production of a semiconductor, uses a photoresist to transfer a pattern. The primary component of a photoresist is a photopolymer whose solubility will be changed upon exposure to short wavelength radiation. In addition, the photo- resist contains a deposition solvent and several small- molecule compounds. The desired solubility change must be great enough that a developer (a solvent that removes the unwanted region of a resist pattern) does not swell the remaining photoresist. The development process must be able to discriminate between exposed and unexposed regions as small as a few nanometers in size. The unremoved photoresist must protect the underlying substrate from the next process steps in semiconductor manufacturing. Each stage in the process must be virtually perfect with yields well above 99%, because there may be hundreds of process steps used to manufacture each advanced semiconductor device. Without those very high yields, semiconductor manufacturing would fail. The basic lithography process used globally today for advanced semiconductor manufacturing and the foreseeable future employs chemically amplified photoresists. Chemical amplification was a key invention needed to overcome the challenge of limited light sources but was also found to provide superior patterning performance. In such resist 42 systems a photopolymer that contains acid cleavable protecting groups is combined with a photoactive compound, such as a PAG. In its native state, the photoresist polymer with protecting groups is soluble in organic solvents. Upon exposure to UV radiation, the PAG releases acid. Frequently, a subsequent post- exposure bake (PEB) step leads to the acid- catalyzed removal of protecting groups, thereby transforming the hydrophobic photopolymer into one that is soluble in an aqueous base developer. The single photon of light needed to release one acidic proton is “amplified” by the more efficient acid- catalyzed deprotection process. By transforming the solubility of the photoresist, a high contrast patterning process needed in semiconductor manufacturing becomes possible. The combination of photoresist polymer and PAG to make the photoresist system is an essential part of this process and fluorination in the PAG provides the high acidity necessary for chemical amplification to work and will be described subsequently. One of the special features of the C─F bond is its strength compared with the C─C bond due to the electron-withdrawing power of the fluorine atom. This attribute is the basis of many of the technical benefits of fluorinated materials in semiconductor processing but leads to its chemical stability and environmental persistence. Fluorination brings specific improvement in performance, and its targeted incorporation can minimize the quantities of material needed to achieve that performance. Such aspects are discussed in the context of PAGs. Thus, despite the remarkable performance improvement in many aspects of the lithographic process provided by fluorochemicals (PFAS) that makes possible the semiconductor revolution with its benefit to society, the large and growing environmental and societal concerns surrounding PFAS may counterbalance the positive technological benefits of these materials. The reader is referred to a discussion of such PFAS concerns in a well-written review article, but photolithography chemicals are 43 largely glossed over.1 Going forward, due to environmental and regulatory concerns, performance equivalent alternatives for many of these applications still need to be identified and this will be a major research challenge. Based on concerns regarding the high persistence, bioaccumulation potential, and potential toxicity of PFAS studied to date, it has been suggested that the use of PFAS be limited to essential uses only. We discuss whether viable alternatives exist for each of these applications and the characteristics that must be achieved to find an alternative compound where none currently exists. Finally, we apply the essential use concept described by Cousins et al.2 to show that these compounds should be considered essential for certain processes in semiconductor manufacturing (i.e., photolithography and patterning) because they provide for vital functions and are currently without established alternatives. The prior paper did an excellent job of discussing different aspects of PFAS use. In this paper, we focus our discussion of essential use as “necessary for highly important purposes in semiconductor manufacturing for which alternatives are not yet established.” We describe the many uses and unique properties of PFAS chemicals, which in our opinion justifies their current use as essential in microelectronics manufacturing and for which alternatives have not yet been adequately identified. This paper is not intended to be an extensive listing of every example of fluorochemical used in photolithography but does attempt to explain strategies and classes of material used in the manufacturing of semiconductors. 44 2.2 Photoacid Generators PAGs are photoactive compounds that generate acids upon exposure to high-energy light [deep ultraviolet (DUV) or extreme ultraviolet (EUV)]. These photoactive compounds were originally used for applications in photopolymerization in the early 1960s.3 After the introduction of chemically amplified resists (CARs) in the 1980s, they have been used in semiconductor manufacturing as key components in advanced photoresists. It is important to understand that the process of chemical amplification requires a very strong acid in the PAG to function well. PAGs are now highly evolved with over 40 years of in- depth research and development for photoresist applications. A positive tone resist polymer after deprotection, for example, contains weak acid groups that will act to buffer (weaken) the acidity of the deprotection process. Without the presence of the strong fluorosulfonic (or stronger) acid, the catalyzed deprotection process will be less efficient or may not even occur. Sulfonate anions without fluorination have repeatedly been shown to be inadequate for use ineffective 193 nm chemically amplified photoresists and this is well known in the photoresist community. The unique characteristics of fluorine (noted below), which lead to very strong proton donation by fluorinated sulfonic acids, are essential in CARs. This intrinsic benefit of fluorinated acids makes it extremely difficult to eliminate the use of fluorinated acids whilst retaining the key performance characteristics of CARs needed for advanced photolithography in microelectronics manufacturing. Other attributes of a PAG that depend less on the acid and more on the chromophore include quantum yield at the wavelength of use, the sensitivity of the overall resist formulation (e.g., 15 to 60 mJ⁄cm2), miscibility in the resist matrix, thermal and hydrolytic stability and shelf life of the photoresist, solubility in aqueous base developer for positive tone develop or organic solvent for negative tone development followed by 45 removal in the resist strip operation. In general, PAGs are divided into two categories: either ionic or covalent (nonionic) structures. As the name suggests, ionic PAGs consist of two portions: a cation and an anion. In addition, covalent PAGs are uncharged, nonpolar com- pounds that are constructed of covalent bonds but are generally less sensitive and therefore less effective than ionic PAGs. The availability of both ionic and covalent PAGs offers process flexibility. In some cases, the presence of ionic groups may lead to storage instability of the photoresist mixture or the inhomogeneous distribution of photoactive compounds in the photoresist, thus making a nonionic PAG necessary. However, most photoresist compositions that are used in semiconductor manufacturing employ ionic PAGs because of their greater sensitivity. Examples of PAGs are shown in Figure 2. 1. In either case, a fluorinated sulfonic acid would be used to make an effective PAG. The photoefficiency difference between ionic and covalent PAGs, which leads to higher quantum yields in the ionic PAG is controlled by the cation.4 The low diffusivity and high strength of the acid resulting from the photolysis of the cation are controlled by the resulting accompanying fluorosulfonate anion. These anions are used in virtually all current commercial photo- resists. Limited diffusivity is important to achieving high- resolution patterns because excess diffusion of the PAG has been shown to limit the resolution of the images produced in a CAR. While aromatic sulfonic esters are shown in some nonionic PAGs described in Figure 2. 2, the strength of the resulting sulfonic acid after photolysis is not as high as the ionic PAGs with fluorinated sulfonate anions. Covalent PAGs do not suffer from the sorts of phase separation, low miscibility, and dark loss (the dissolution of unexposed photoresist) issues that may occur in ionic PAG- containing resist formulations, but the quantum yield of photoacid generation is generally lower for covalent PAGs so this and other factors drive the ultimate choice of PAG.5 46 Figure 2. 1 Representative ionic PAGs: 1, 2, 3, 4 Sulfonium PAG and 5, 6 Iodonium PAG. O O F F S OO O S S O O O F F F S 1 2 O N O I PF6 Br 5 O S FF F F O O O S 3 S O O O F F FF F F F F F S 4 I S O O O F F FF F F F F F 6 47 Figure 2. 2 Representative nonionic covalent PAGs. O N O O S O O F F FF F F F F F 9 S O O O O S O O O 7 8 48 In order to increase the acidity of the photoacid, perfluorinated methylene units may be placed next to the sulfonate group in both ionic and covalent PAGs. The polarization present in the C─F bond due to the electronwithdrawing character of fluorine stabilizes the acid anion and makes the acid stronger. A sulfonic acid such as methane sulfonic acid has a pKa of −2 (already a strong acid) but trifluoromethyl sulfonic acid (triflic acid) has a pKa of −14. Any induction effect is significantly smaller after two or three CF2 units, so the relative benefit of fluorination is significantly reduced as the neighboring CF2 units are further away from the acid group. The original choice of longer sequence perfluorinated sulfonates (six or more) has not been explained in patents or the literature but was likely due to the effectiveness of the resulting PAG, the reduced diffusivity because it is a larger molecule, its availability, and the lack of volatility in this material. For example, the volatility of the small triflate anion limits its use in a production photoresist PAG because the resulting concentration gradients in such photoresist films harm performance. However, shorter CF2 segments (1 or 2) next to the anion and connected to other units of higher mass have been shown to make effective PAGs. Finally, the diffusivity of the PAG will affect pattern resolution (less diffusion enhances resolution) and can be addressed by the use of a higher molar mass PAG/acid and even covalent attachment of the PAG to the photoresist polymer itself. Although actively used in some applications, triflic acid is not always a useful component in a PAG since it may have significant deficiencies when used in a very high-resolution CAR system; it is volatile and may evaporate during the PEB step leading to composition gradients that are detrimental to image resolution and it readily diffuses during annealing, which may, in turn, lead to pattern degradation from deprotection chemistry occurring in unexposed areas, effectively reducing image contrast and disrupting pattern formation. 49 2.3 Ionic Photoacid Generators Most ionic PAGs used in lithography are onium salt derivatives. Such ionic compounds consist of an onium moiety as the cation and sulfonate groups as the anion. Upon exposure, photolysis occurs and photoacid is formed. The quantum yield of the photoacid is directly impacted by the cation fragment. The acidity of the generated photoacid as noted above is controlled by the anionic fragment in the PAG (usually a fluorinated sulfonic acid). The rate of photoacid release is controlled by both cation and anion. ionic PAGs are generally composed of either diaryliodonium or triarylsulfonium photoactive units to form a salt with an appropriate anion. Triarylsulfonium PAGs usually have longer shelf life compared with diaryliodonium salt. However, a diaryliodonium salt has higher absorptivity in particular for next-generation 13.5-nm wavelength EUV photons. The mechanism of photolysis of diaryliodonium salt and triarylsulfonium salts6 has been studied extensively. Reported photolysis mechanisms for diaryliodonium salt and triarylsulfonium salts are shown in Figure 2. 3 and Figure 2. 4, respectively.7 The quantum yield of the photoacid is directly impacted by the cation fragment. The acidity of the generated photoacid as noted above is controlled by the anionic fragment in the PAG (usually a fluorinated sulfonic acid). The rate of photoacid release is controlled by both cation and anion. In Figure 2. 3, the energy required to cleave the aromatic C (sp2) and iodine bond is somewhat higher compared with the energy required to promote bond cleavage between the aromatic C (sp2) and sulfur bond. Generally, the sulfonium PAG family is more widely used than iodonium PAGs considering its greater sensitivity and longer shelf life when used in either DUV or EUV lithography. Solid state studies at 193, 248, and 266 nm exposures reveal additional products including in all cases, two previously unreported triphenyl sulfonium photoproducts, triphenylene, and 50 Figure 2. 3 Proposed photolysis mechanism for diaryliodonium salt under DUV exposure. I A hv I A I A + RH R I + + AH 51 Figure 2. 4 Proposed photolysis mechanism for triarylsulfonium salt. 52 dibenzothiophene. 2.4 Nonionic Covalent Photoacid Generators Although ionic PAGs have higher sensitivity in lithographic applications, they may be less soluble and more prone to phase separation in photoresist formulations. It is worth recalling that the PAG is needed to generate acid in the exposed regions to deprotect the photoresist and thereby change its solubility. Uniform distribution of a PAG is an essential attribute to excellent performance in a photoresist. Detrimental interaction between ionic structures in a photoresist and an ionic PAG may also occur in future resist materials.8 To overcome such issues, covalent PAGs may be attractive alternatives. In general, covalent PAGs are derivatives of aryl sulfonates,9 iminosulfonates,10 and imidosulfonates.11 Arylsulfonate esters can be easily synthesized from phenol and sulfonyl chlorides. A similar effort to create fluorinated sulfonate ester-containing covalent PAGs has not taken place because such PAGs have not been as effective in photoresist applications. The photoacid generation mechanism is proposed based on the nonfries photolytic ArO─S bond cleavage (pathway A) or pseudofries rearrangement (pathway B), which is more likely to occur for electron-rich aryl sulfonates as shown in Figure 2. 5.12-13 It is worth noting that in pathway A, in the presence of oxygen and water, stronger sulfonic acid is generated. In the absence of oxygen, weaker sulfurous acid is produced. Iminosulfonates and imidosulfonates have similar chemical structures with the N─O bond undergoing homolytic cleavage upon irradiation to generate sulfonyloxy radicals, which subsequently capture hydro gens from nearby molecules to afford the corresponding sulfonic acid as shown in Figure 2. 6. 53 Figure 2. 5 Photoacid generation mechanism for aryl sulfonate esters. Ar S O O O Irradiation Ar S O O O Ar S O O O + H2O / O2 Ar S O O HO + OH (1) –SO2 Ar(2) H2O + H2SO3 Photoacid Generation Ar S O O O Irradiation Ar S O O + O Ar S O O OH Photoacid Generation Pathway A Pathway B 54 Figure 2. 6 Photoacid generation mechanism for iminosulfonates and imidosulfonates. N O S O O R N O S O O R O O Irradiation O S O O R HO S O O R Photoacid Generation Iminosulfonates Imidosulfonates 55 2.5 Polymer-Bound PAGs One approach to increasing the resolution to photolithography is to employ PAG that is incorporated into the photoresist polymer structure. It has the advantage of making the distribution more uniform and at the same time limits the diffusivity of the sulfonate anion since it is bound to the photoresist polymer. Resolution is set in part by the diffusivity of the PAG in the photoresist formulation, which is associated with the size of the molecule. The smaller the anion, the farther the photogenerated proton can diffuse in a given time. If the PAG acid diffuses too broadly then deprotection of the photoresist takes place in unwanted regions and makes the pattern larger, less precise, and “blurry.” These pattern irregularities are characterized in terms of line edge roughness, line width roughness, and critical dimension uniformity. Examples of bound-PAG structures have been reported and two are described below shown in Figure 2. 7.14 This strategy also lowers concerns about “stochastics,” i.e., the chemical heterogeneity of a photoresist mixture at the dimensions of the pattern are thought to also contribute to the limit of resolution of today’s most advanced lithographic processes. Upon exposure, the fluorosulfonate group becomes protonated, catalyzes deprotection of the rest of the photoresist chain, but the strongly acidic proton cannot diffuse broadly because it remains near the anion bound to the polymer chain and thereby forms higher resolution patterns. By attaching the same number of PAG units to each polymer chain, then the PAG is uniformly distributed throughout the photoresist film. This strategy is being seriously considered for future generations of photoresists, particularly for use in EUV lithography.15 These examples share several common features, including the attachment of the anion to the polymer backbone. Since many CAR photoresists are based on (meth) acrylates, examples reported for 193 nm (DUV) resists possess a sulfonate anion and an adjacent CF2 unit, 56 Figure 2. 7 Examples of polymer-bound PAGs. (a) Single CF2 unit next to sulfonate21 and (b) single CF2 unit next to sulfonate in a structure that falls apart on exposure; groups (R1, and R2) not specified groups while R3 is a linking group. 57 which then is connected to the methacrylate monomer through an ester linkage. While it has not been established if one or two CF2 units are needed to produce sufficiently strong anion, this example demonstrates one approach and good prospects for polymer-bound PAGs. 2.6 Alternatives to Fluorinated PAGs PAGs other than iodonium and sulfonium units as well as those that do not contain traditional PFAS have also been studied for use in photolithography. To be used successfully in a CAR photoresist, the resulting acid must be as acidic as a perfluorosulfonic acid, lack volatility so that it does not evaporate during the PEB step, and in the next generation photoresists possess minimum diffusivity (to enable high- resolution pattern formation). The PAG-resist combination should have a sensitivity in the range between 10 and 75 mJ⁄cm2 under exposure conditions i.e., the source wavelength and tool-specific settings. Some new photoresists attach the PAG directly to the photopolymer chain to both limit diffusion and deal with issues of stochastic variations that may be present in photoresists consisting of mixtures of polymer and photoactive molecules. Nontraditional PFAS Covalent PAGs: Nitrobenzyl esters have found some application in DUVL and may be extendable to EUV lithography. Such molecules can generate photoacid upon irradiation through o-nitrobenzyl rearrangement to generate nitrobenzaldehyde and a sulfonic acid such as triflic acid shown in Figure 2. 8. The chemical structure is shown in Figure 2.8 (a). The terarylene skeleton-based self- contained PAG is another potential candidate for some applications. The photoacid generation is triggered by the 6π-electro-cyclization reaction of photochromic triangular terarylenes.16 The chemical structure is shown in Figure 2.8 (b). Similarly, a triflate ester 58 Figure 2. 8 Chemical structure for non-PFAS covalent PAGs: (a) nitrobenzyl ester and (b) terarylene backbone-based PAG. NO2 OTf a S N S S N OTf Ph Ph b 59 is used in the reported structure to release triflic acid upon exposure. While these and other structures can be used to demonstrate PAG concepts, they are unlikely to be as useful in new high-resolution photoresist systems because they use triflate groups. Alternative acids may be used to make more suitable PAGs from the moieties in Figure 2.8. Should a useful PAG be produced from these types of photoactive structures the resulting sulfonic acid will need to be less volatile and less mobile in the polymer film. A higher molar mass, much less volatile, lower diffusivity anion might work well with these materials in a functioning photoresist system. Nontraditional PFAS Ionic PAGs: Ionic PAGs derived from 2-phenoxytetrafluoroethane sulfonate were introduced by Ober and coworkers in 2007.17 This PAG was tested under e-beam and EUV radiation and showed high sensitivity, resolution, and acceptably low line edge deviations. The use of such a fluorosulfonic acid has the advantage that it limits fluorine content yet produces a very strong acid with both limited volatility and diffusivity by placing a CF2 group next to the acid group. Such an approach (discussed more below) can be used to minimize fluorine incorporation while placing this structure where it is most valuable. Its chemical structure is shown in Figure 2. 9. This PAG was tested for its environmental degradation and its effect on bacterial populations when first reported and found to be benign under the rules of that time. The good lithographic results suggest that shorter fluorinated segments (two or possibly one CF2 unit adjacent to the sulfonic acid) may make useful ionic PAGs. It should be noted that the building blocks for sulfonic acids with one CF2 are the subject of experimental studies. The pentacyanocyclopentadienide PAG is another potential ionic PAG candidate in some applications. Its lithographic performance was demonstrated by Varanasi and coworkers in 2010, and it stands out for the amount of publicity it received.18 60 Figure 2. 9 Chemical structures of untraditional ionic PAGs: (a) 2- phenoxytetrafluoroethane sulfonate PAG and (b) pentacyanocyclopentadienide PAGs. O S FF F F O O O S a S CN NC CN CN NC b 61 The chemical structure is shown in Figure 2. 9 (b). While announced in 2010 as part of IBM’s efforts to reduce Perfluorooctanoic acid (PFOA) in its manufacturing process, to the best of our knowledge, this PAG was not commercialized. Finally, PAGs based on glucose or other natural products have been explored. These PAGs were demonstrated to be functional materials for some high- resolution photoresist applications enabling sub-100nm features using ArF laser and e- beam lithography. Moreover, these PAGs showed successful microbial degradation to smaller molecular units under aerobic conditions. The chemical structures are shown in Figure 2. 10. Such studies revealed the successful biodegradation of these PFAS units to smaller oxidized components as well as low bacterial cytotoxicity14, 19 of the photoactive sulfonium subunit. In general, the anionic units underwent biodegradation using sludge from a local municipal waste water treatment plant. The sugar or cholesterol groups appeared to degrade easily leaving only a short, fluorinated acid residue. An advantage of these structures is that the residues retain polar functional groups and are therefore more hydrophilic than PFOS/PFAS units. This makes them less likely to accumulate in fatty tissues, but further studies are needed to identify any bioaccumulation characteristics. The photoactive cation unit but not the fluorinated anion was generally found to be cytotoxic to the bacteria. Importantly, the short, fluorinated segment enabled the formation of a high-performance PAG that could be subjected to successful biological degradation. More recently, patents have appeared that describe the goal of which is intended to deliver strong PAG performance and minimize the size of the fluorinated unit in the 62 Figure 2. 10 Chemical structures for natural products-based PAGs. 63 fluorosulfonic acid or eliminate it entirely. These patents claim excellent lithographic performance. These and other patents describe PAGs with shorter fluorinated segments, some of which are designed to fall into small molecular pieces. To assess their viability as alternative PAGs their performance characteristics (sensitivity, acid strength, and diffusivity) and environmental characteristics (fluorine content, degradation products, and toxicity) will need to be assessed. 2.7 Conclusions The use of fluorination in PAGs is to enhance the acidity (make pKa ≪ 1) of the acid produced in the region of exposure of a photoresist. The formation of acid to induce a solubility change is the critical step in today’s chemically amplified photoresists, the workhorse family of photoresists that enable the production of the vast majority of semi- conductors. The presence of a fluorinated unit adjacent to the sulfonic acid gives the acid its ability to efficiently release a proton that reacts with the resist polymer to create a solubility switch. Subsequent development forms a pattern in the photoresist. Today there is no effective alternative to a fluorinated sulfonic acid and this situation applies to chemically amplified photoresists across all wavelengths of lithography from 248 nm to EUV. Efforts to reduce the amount of fluorination in a PAG molecule have been demonstrated, but a survey of the current literature has not shown that complete elimination of fluorination has produced a successful alternative. However, it is very likely that fluorine- free alternatives, which perform equally well and can easily take the place of the fluorinated compounds used today, will be more widely used, and developed in the coming years. Fluorinated polyimides use the presence of a fluorinated unit to 64 improve the dielectric constant of the material and make it a better insulator while retaining excellent thermal stability. This combination of characteristics has not been effectively achieved by alternate means. Fluorinated materials play a useful and often essential role in many aspects of semiconductor processing. These fluorochemicals are employed as com- ponents of PAGs, as components of photoresists, as elements of high-temperature polymers, and as ingredients in ARCs, BARCs, and as topcoats, frequently satisfying the “essential use” criterion. However, there is a strong societal interest in eliminating their use, and “essential use” is a stopgap situation in which replacements are actively sought. The “essential use” concept expects that PFAS uses considered essential today should be continually reviewed for potential removal or replacement by new technologies and be targeted by innovation toward alternatives. The concept does not support long-term and large-scale remediation technologies to justify the ongoing use of PFAS chemicals. Thus, the challenges going forward are to find a means to replace PFAS components that achieve or surpass today’s current performance characteristics in the following current and possible future lithography systems. Acknowledgements The authors gratefully acknowledge the Semiconduct