Asymmetric fluid-structure dynamics in nanoscale imprint lithography

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JointsJointsFigure 3.3 Multi-imprint α-β template orientation stagesTo study the effect of the etch barrier on orientation alignment, only oneorientation direction is required to decouple the effect of the pressure distributionon α and β misalignment. A semi-circle notched flexure design was used toprovide the necessary kinematics. This stage is shown in Figure 3.4. It can beseen in the equations 5 developed by Paros and Weisbord, that the flexure iscompliant about only one axis. The notched flexure acts as a revolute joint whereits center of rotation coincides with an axis on the surface of the template thatpasses through the center of the template surface.Axis of RotationFigure 3.4 One degree-of-freedom template orientation stage5 See Appendix B.45
The one degree-of-freedom template orientation stage was designed toexperimentally study the imprinting forces and gap sensing tool as well as tovalidate the numerical model of the squeeze film flow of the etch barrier. Thetorsional stiffness of this stage was designed to be similar to the template stagesfrom the multi-imprint stepper. The stiffness coefficient for each of the templateorientation stage (Figure 3.3) from the stepper was approximately 55 N-m/rad.From equation B.1, the radius (R) for the notched flexure was chosen as 1.27 mm,the equivalent depth (b) was 8.9 mm, and the minimum cross-sectional thickness(t) was 1 mm. This results in a torsional stiffness of 64 N-m/rad.As of the writing of this thesis, the design of a complete templateorientation stage to provide the appropriate kinematics for the active stage testbed has not been finalized.3.2.3 High-Resolution Actuation SystemIn order to minimize undesirable grinding motion, each actuation legconsists of a revolute flexure joint (R), a motorized micrometer (P), a.k.a. DC-Mike actuators, a quartz force sensor, and a universal joint (U) connected inseries. One RPU actuation leg is shown in Figure 3.5. Each actuation leg isconnected in parallel with a distributed flexure ring to the active stage basestructure. Three actuation legs form a tripod for an RPU stage, where the threeattachment locations on the distributed flexure ring specify the orientation plane.Each component of the actuation system must be stiff in the lateral directions.46
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Asymmetric Fluid-StructureDynamics
Page 5 and 6:
AcknowledgementsFirst of all, I wou
Page 7 and 8: Table of ContentsList of Tables ...
Page 9 and 10: 6.2.3 Control Software ............
Page 11 and 12: List of FiguresFigure 1.1 Optical m
Page 13 and 14: Figure 6.9 Force due to fluid press
Page 15 and 16: The exponential escalation in the c
Page 17 and 18: 1.2.1 Optical Lithography Process O
Page 19 and 20: patterns to the desired specificati
Page 21 and 22: 1.3 STEP AND FLASH IMPRINT LITHOGRA
Page 23 and 24: transferlayerwaferStep 1: Spin-coat
Page 25 and 26: the etch barrier fluid has an infin
Page 27 and 28: Researchers at the University of Te
Page 29 and 30: stage development. Design requireme
Page 31 and 32: minimum and maximum base layer thic
Page 33 and 34: square plate with fluid completely
Page 35 and 36: 7. The fluid is assumed incompressi
Page 37 and 38: ⎛ ∂ ⎞⎜τdz ⎟dxdy⎝+ τ
Page 39 and 40: where V 1 and V 2 correspond to U 1
Page 41 and 42: ddx⎛⎜h⎝3dp ⎞ ∂h⎟ = 12µ
Page 43 and 44: dhdtLzhθh αh βxx αx = 0 x βFig
Page 45 and 46: C2hhtanθ2 21= αxαxβxαxβ( ) (
Page 47 and 48: ⎛⎜ hD⎜⎝6C ⎞1tanθ⎟24µh
Page 49 and 50: at the plate edges. Freeland obtain
Page 51 and 52: For the case of 10 psi of pressure,
Page 53 and 54: are the same as the width of the tr
Page 55 and 56: orientation stages relative to the
Page 57: Wafer ChuckAir SolenoidMounting Pla
Page 61 and 62: Figure 3.7 Initial and final desire
Page 63 and 64: 7645321Figure 3.8 Active stage prot
Page 65 and 66: Chapter 4: Real-Time Gap Sensing Vi
Page 67 and 68: R( λ)( 4πnd/ λ)2 2 −2αd−αd
Page 69 and 70: Rate Monitoring and is adapted for
Page 71 and 72: 10090807060PSD504030201000 500 1000
Page 73 and 74: the multi-imprint and active stage
Page 75 and 76: 5.2.2 Composite Stiffness and Dampi
Page 77 and 78: ( )2πR−1.5clamping length of 1.5
Page 79 and 80: 65actuator height, micron432100 0.1
Page 81 and 82: time marching is required to minimi
Page 83 and 84: 5.4 SQUEEZE FILM DYNAMICS OF INCLIN
Page 85 and 86: force, lb504540353025201510500 0.05
Page 87 and 88: improve upon these results by tunin
Page 89 and 90: Again, Figure 5.12 shows that a bas
Page 91 and 92: optically flat quartz plate coated
Page 93 and 94: optic probe was illuminated with a
Page 95 and 96: Figure 6.3 Screenshot of control so
Page 97 and 98: 6.3 EXPERIMENTAL PROCEDUREExperimen
Page 99 and 100: film thickness, nm40003800360034003
Page 101 and 102: Figure 6.6 shows that the force due
Page 103 and 104: similar. In Figures 6.7 and 6.8, th
Page 105 and 106: 500045004000film thickness, nm35003
Page 107 and 108: Figure 6.13 shows the force-time pl
Page 109 and 110:
⎛ n ⎞in the FFT that is not ind
Page 111 and 112:
when measuring thin layers in the r
Page 113 and 114:
is a major milestone. The next step
Page 115 and 116:
7.2.4 Control schemeThe ultimate go
Page 117 and 118:
Assuming the liquid perfectly wets
Page 119 and 120:
ase h (for a semi-circular notch,h
Page 121 and 122:
Chou, S. Y., P .R. Krauss, and P. J
Page 123 and 124:
Tripp, J. H. 1983. Surface roughnes
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Asymmetric fluid-structure dynamics in nanoscale imprint lithography

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