Modeling of Environmentally Friendly Siloxane- Based Lithography Solvents

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Transcription:

Modeling of Environmentally Friendly Siloxane- Based Lithography Solvents Gregory N. Toepperwein, Dan Rynearson, Juan J. de Pablo Christine Ouyang, Chris Ober 17 November 2011 1

Motivation Drive to reduce device dimensions has many obstacles remaining in its path. Pattern collapse due to finite size effects and increased capillary forces during rinse LER due to acid diffusion Environmental concerns Stoykovich, Cao, Yoshimoto, Ocola, Nealey, Advanced Materials 15 1180 (2003) Yoshimoto Stoykovich Cao, de Pablo, Nealey; Journal of Applied Physics (2004) 2

scco 2 as a Solvent No surface tension reduced capillary forces => abates pattern collapse Plasticizes polymeric photoresist reduced LER Requires additives to enhance resist solubility or new resists Developed with TMAH, 122nm lines. Developed with QAS/scCO 2, 42nm lines. 260nm 260nm Wagner, DeYoung, Harbinson; SPIE Vol.6153 (2006) Zweber, Wagner, DeYoung, Carbonell; Langmuir (2009) Goldfarb, de Pablo, Nealey, Simons, Moreau, Angelopoulos (2000) G.N. Toepperwein Task 1674.004 3 Nov. 17, 2011

Objectives Environmental goals Methodology Super critical carbon dioxide Use with traditional photoresists Use with molecular glass photoresists Linear methyl siloxanes Benefits Model development Model validation Use with traditional photoresists Exploration of dissolution mechanism Future Work 4

ESH Metrics and Impact 1. Reduction in the use or replacement of ESH problematic materials 100% reduction in the use of aqueous base TMAH developer 2. Reduction in emission of ESH problematic material to environment Up to 100% reduction in VOCs and HAPs emission 3. Reduction in the use of natural resources (water and energy) Eliminate water usage Reduction in energy for water treatment and purification 4. Reduction in the use of chemicals Minimal use of organic solvents 5

Why a Non-Aqueous Developer Solvent? Environmentally friendly, zero VOC solvent Highly tunable solvating power (T,P) Leaves no residue Clean separations One-phase fluid Zero surface tension Transport, viscosity between that of liquid and gas Nonpolar, inert character S + L Potential to reduce LER and eliminate pattern collapse 6

Collaboration Ober Group Synthesize photoresists Development process Provide experimental results Calixerene Computer Simulations Pre-screening of possible photoresist structures Provide information on dissolution mechanism at a molecular level Time (1ns-2ns between images) de Pablo Group 7

Model Long-range interactions OPLS Model: V tot = V LJ + V coul + V bon + V ang + V tors Short-range interactions r-r 0 C O H Intermolecular V LJ V coul 4 r q i q j 4 0 r 12 r 6 Intramolecular 2 1 V bon 2 k bon r r 0 1 V ang 2 k ang 0 V tors n 2 k n 1 cos n 0-0.32-0.32 O C 0.65 O OPLS force field employed for most parameters We calculated charges (q i ) using quantum mechanics 8

Film Energy Calculation Thin films of resist equilibrated in solvent via MD simulation Integrating the force on each chain as a function of position provide free energy Force Center of Film If the energy is lower at the surface than the center, the film is unstable Energy Insoluble resist zero line Soluble resist Distance from Center of Film G.N. Toepperwein Task 1674.004 9 Nov. 17, 2011

Sample Result: ESCAP Energy Curve CF 3 CF 2 COO N (CH 23 ) COO 3 (CF 2 ) 5 CF 3 CH 2 3 N (CH 2 ) 3 (CF CF 2 5 QAS-A1 2 ) 5 CF 3 CH 2 3 CF CF 3 QAS-7 2 5 CF 3 QAS-4 QAS-7 CH 3 COO N (CH 3 COO 2 ) 3 (CF 2 ) 5 CF 3 * OH * 59 16 25 O O N CH (CH 2 3 2 ) 3 (CF 2 ) 5 CF 3 CH CF 2 5 2 3 CF CF 3 QAS-4 2 5 CF 3 QAS-4 hps PS TBA 10

Sample Result: ESCAP Energy Curve Experimental Results: No salt 0 nm/sec QAS-7 0 nm/sec QAS-4 25 nm/sec Only addition of QAS4 to ESCAP results in reduced energy at surface of film (right of plot), indicating eventual dissolution Viability confirmed experimentally 11

ESCAP Results Carbon Dioxide Phase Carbon Dioxide Phase Polymer Resist Phase Force Polymer Resist Phase scco2 not shown for clarity Green ESCAP resist Blue QAS-4 Cyan Carbon (Extracted Chain) Red Oxygen (Extracted Chain) White Hydrogen (Extracted Chain) 12

ESCAP Results QAS Anion ESCAP monomer scco2 not shown for clarity The OH group of ESCAP associates with the anions. Contacts last >500 ps. Purple ESCAP Green Fluorine (QAS-4) Cyan Carbon (QAS-4) Red Oxygen (QAS-4) White Hydrogen (QAS-4) 13

Comprehensive Understanding Examined polymer resist dissolution enhancement for both protected and unprotected resist PASS Possible Pass FAIL Untested Develop mechanistic understanding Additive Photoresist ESCAP 193nm PHOST Calixarene 14

Additive Principles for DMAA QAS4 was effective due to hydrogen bonding; can we repeat this effect in a non fluorinate additive? * * OH DMAA 59 16 25 O HO O ESCAP 59 16 25 O O O O PHOST DMAA enhances ESCAP solubility in scco 2 Unlike QAS4, does not aid PHOST development 15

DMAA Mechanism Additive was based on applying our understanding of QAS4 effectiveness on ESCAP DMAA demonstrates similar hydrogen bonding Ineffective with PHOST; obstructs terminal t butyl group, instead exposing polar region, reducing scco 2 solubility Can develop nonfluorinated additives, but they are more resist-specific 16

Molecular Glass Photoresist Low molecular weight materials capable of forming solidlike structures Improved LER More soluble than larger chemicals Calixarene 17

Predictive Power of Simulations: Calixarene Molecular glass photoresist capable of high-resolution patterns (low LER) We demonstrated potential of this via simulation before experiment Capable of dissolution in scco 2 without any additive (first material to show this property, shown below) Time (1-2 ns between images) in CO 2 18 18

Silcon-Based Solvents Linear methyl siloxanes Low molecular weight Contain only silicon, carbon, hydrogen, and oxygen Non polar solvent Solvent power can be enhanced by adding additives Low in toxicity, VOC exempt Non ozone depleting Degrade to naturally occurring compounds Low surface tension 19

Objectives Generate the definitive molecular model for siloxane solvents Complete parameterization of all bonds, charges, etc. Reproduction of experimentally obtained chemical properties (density, heat of vaporization, etc.) Study behavior of traditional photoresists in siloxanes 20

Model Chose functional form consistent with generic formalism to enable transferability Parameters derived from quantum mechanical calculation and experimental analysis Modeled six elementary building blocks from which an arbitrary structure can be created Model Formalism: Intermolecular Intramolecular Sample elementary building blocks: Si-O-Si-H Si-O-Si-C Si-O-Si-O 21

Quantum Mechanics HMD Siloxane Provides a detailed description of electron position as we probe different configurations Can determine charges (q i ) directly Map energy as a function torsion angle, etc. rb3lyp model with 6-311+g(2d,p) basis set Si-O-Si-O Torsional Angle HOMO 0 o 60 o 120 o 180 o LUMO 22

Potential Fitting Torsional Sample Si-O-Si-C and Si-O-Si-O torsions most important parameters in determining shape of the solvents Torsional parameters fit to capture difference between quantum mechanical results and non-bonded interactions Si-O-Si-H Si-O-Si-C Si-O-Si-O 23

Intermolecular Interactions Having built a complete intramolecular model from quantum mechanics, we now tune intermolecular many-body interactions to match experiment HMD Siloxane 24

Model Verification Heat of Vaporization (kcal/mol) Specific Heat (cal/g*k) Density (g/ml) Dipole Moment (Debye) Dielectric Constant HMD Siloxane OMT Siloxane DMT Siloxane Experimental Model Experimental Model Experimental Model 7.1 7.3 8.5 11.0 12.0 12.3 0.46 0.50 0.29 0.48 0.41 0.53 0.764 0.761 0.820 0.813 0.854 0.852 Unknown 1.016 Unknown 1.203 Unknown 2.0553 Unknown 1.339 Unknown 1.400 Unknown 1.875 Good agreement with known properties 25

Energy Use Waste treatment is a major cost Must separate solvent from dissolved polymer Siloxanes solvents require less heat to distill Half the heat capactity Order of magnitude lower heat of vaporization Solvent TMAH HMD Siloxane C p 3.2-4.18 J/g K 1.83 J/g K T boil 383K 373K H vap >2260 J/g 296 J/g 26

Calixarene Molecular glass resist Inherently low LER More soluble than polymers Selective dissolution proved by Ober group exposed unexposed HMD Siloxane Dose:350 mj/cm 2 PEB:90 o C, 30 sec OMT Siloxane Dose:250 mj/cm 2 PEB:90 o C, 30 sec DMT Siloxane Dose:300 mj/cm 2 PEB:90 o C, 30 sec G.N. Toepperwein Task 1674.004 27 Nov. 17, 2011

Calixarene Results Calixarene after 10ns in siloxane solvents: Unexposed photoresist breaking away from surface Exposed photoreist makes smooth interface Negative tone resists Excellent agreement with experiment HMD Siloxane OMT Siloxane DMT Siloxane unexposed exposed unexposed exposed unexposed exposed G.N. Toepperwein Task 1674.004 28 Nov. 17, 2011

Calixarene Patterning 40nm TOK photoresist DMTS: HMDSO=1:20 at 40 o C for 40 minutes Resist film thickness ~350 nm 29

ESCAP ESCAP is our model EUV photoresist Model previously developed and tested for scco 2 NNDMTS In experiment, chemically modified by NNDMTS: Si N NNDMTS Identical Topology Si atom makes group slightly bulkier, makes group more polar (N,N-Dimethyl)trimethyl silane Similarity between exposed and unexposed form makes ESCAP a serious test of model sensitivity Chemistry shown independent of specific siloxane solvent used 30

ESCAP Results Model predicts only unexposed films to be unstable: Negative Tone Results from experimental collaborator corroborate result Solvent: DMTS/Decamethyltetrasiloxane e beam dose = 20 μc/cm 2 Solvent: Hexamethyldisiloxane Photoresist:ESCAP Chemical modifier: NNDMTS Solvent: Decamethyltetrasiloxane Dose = 20 μc/cm 2 PEB: 115 o C, 60 sec 31

PHOST Results n O O O PBOCST UV H + n DMTS O O O insoluble in silicone-fluids Chain beginning to pull free of surface n OH DMTS n O CH 3 Si H 3 C CH 3 soluble in silicone-fluids Solvent: DMTS/Octamethyltrisiloxane e-beam dose = 100μC/cm 2 32

ESCAP in Solution What is the mechanism for ESCAP dissolution? Need to understand structure of polymer in solvent and film Steered MD Forces system to go through a range of configurations Provides estimate of free energy Use radius of gyration of polymer in solvent 33

Stretching Movie 34

Stretching Result Curve Exposed: prefers to extend modified region while coiling HMD Siloxane is borderline poor solvent Unexposed: prefers extended form, has meta stable coil HMD Siloxane is a good solvent, but dissolution requires exposed film surface to have correct confirmation 35

Flux Tempered Meta-Dynamics Steered MD accuracy depends on pulling rate Too time consuming to get high accuracy Need to refine free energy estimate with different method Flux Tempered Meta Dynamics (in progress) Use initial estimate obtained by Steered MD Bias sampling to negate current free energy estimate Measure time to sample all configurations during long simulation, estimate correction measure rate 36

Conclusion Alternative solvents are promising Environmentally benign Help abate pattern collapse Generic solutions possible Molecular simulation aids development Screen without synthesizing Develop mechanistic understanding Siloxane Solvents Non toxic Energy efficient Effective Still exploring mechanistic understanding 37

Acknowledgements Richard Schenker, Michael J Leeson, Alan M Myers Abnihov Rastogi, Manabu Tanaka, Christine Ouyang, Chris Ober Robert A. Riggleman, Jesse Q. Bond IMEC Jacob Adams Prof. Tadatomi Nishikubo and Prof. Hiroto Kudo (Kanagawa Univ.) Takeshi Iwai Ryan Callahan ICPST-25 Cornell Univ. Ober group 38