Nano fabrication by e-beam lithographie - uni-jena.de...Introduction to Nanooptics, Summer Term...
Transcript of Nano fabrication by e-beam lithographie - uni-jena.de...Introduction to Nanooptics, Summer Term...
Introduction to nanooptics, Summer Term 2012, Abbe School of Photonics, FSU Jena, Prof. Thomas Pertsch
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Lecture 14
Nano fabrication by e-beam lithographie
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
• Introduction • Motivation • General EBL process • Fundamentals
• Basics and Physics of EBL • Resist Technology • Charging • EBL Writing Strategies • Interaction between E-beam and Substrate • Proximity Effect • Proximity Function • Periodic Structures • Resolution Limits in EBL
• Some Special Exposure Techniques • Cell Projection Exposure • Variable Dose Exposure • Mask Preparation for Lift-Off • Overlay Exposure
Electron Beam Lithography - EBL
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Example: Diffraction grating on 9“ fused silica mask blank
Electron Beam Lithography
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Def Lithography: “Method for printing on a smooth surfcace” Photolith., UV lith., Interference lith., Scanning probe lith., X-Ray lith., EBL,…
Why EBL? • far-field imaging technique à diffraction resolution limit (Abbe)
• sub-100nm-features: lde Broglie ~100nm à Uelectron ~12 eV
• high technological standard of electron beam control and manipulation
• capable to structure arbitrary (non-periodic, non-symmetric) patterns
Applications of EBL • mask fabrication (e.g. chromium on glass)
• direct writing (rapid prototyping)
• nano devices in research and development (R&D)
Requirements of EBL • Extremly complex technological background, clean room
• Neccessatiy of experienced staff to operate an EBL system
Motivation
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Positive resist Negative resist
Functional layer (optional)
Substrate
Resist Exposure
Development
Dry Etching Deposition of functional layer
Removal of Resist
Lift-Off
Final Element
Subtractive method Additive method
Final Element
...
General EBL Process
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
1) Sample preparation
Silica substrate
Resist Thin TCO layer
2) E-Beam Lithography
3) Resist development
4) Layer deposition
Layer stack (Au, MgO, Au)
5) Covered resist structure
6) Wet-chemical lift-off
Process Development: Lift-Off
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Lift-Off: Critical Steps Achieve an undercut resist profile
Top-Resist (low sensitivity)
E-Beam
(Thick) Resist & • Low beam energy • Overexposure • Overdevelopment
E-Beam
Bottom-resist (high sensitivity)
à Rule of thumb: Resist thickness ~ 2-3x thickness of layer(s) to be lifted
Thick Resist: J Clean Lift-Off, elevated Lift-Layer L Lateral resolution diminished due
to enhanced electron scattering
Thin Resist: J Higher lateral resolution
L Less undercut, Lift-Off unstable
Limits of aspect ratio
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Lift-Off: Critical Steps Highly Directional Deposition
Flawless Mask Lift-Off • Long soaking of sample in solvent (>10 hours) • Support Lift-Off by elevated temperature and Mega- / Ultrasonic
Sputtering:
Thermal Evaporation:
• Evaporation is preferable • Maximize distance between deposition source and target (>0,5 m) • Clear / Activate Sample Surface à Ar-Plasma, Heating,...
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Etching: Critical Steps
• Atomic lattices of different materials do not „fit“ perfectly • Resist coating and tempering (180° C) leads to stress induced bubbles and cracks • Not suitable for EBL L
• No reactive dry etching for gold available • Physical layer removal by Ion Beam Etching (IBE) • Very low selectivity, thick resist mask needed, no etch stop L
Dry Etching
Resist Coating & Tempering
• IBE on metals can lead to redepostion and metal-resist compounds • These turn out to be chemically very stable and hardly soluble • Pattern often spoiled by „garden fences“ L
Resist Removal
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
electromagnetic electrostatic
F = q · (E + v x B)
Either magnetic or electrostatic fields can be used to focus electrons
just as glass lenses are used to focus rays of light.
à Electron Optics by an electro-magnetical lens system
à Analogy to Beam-Optics
E-Beam Deflection and Focus
Fundamentals
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
variable angular apertures
cross over
shaped beam
Variable shaped beam
circular aperture
cross over
Gaussian spot
Gaussian beam
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electron optics
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resolution: >5nm >50nm
writing speed: low fast
E-Beam Imaging Systems
electron optics
Fundamentals
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Fundamentals
Variable shaped beam Gaussian beam E-Beam Imaging Systems
E-beam writer LION LV1 masks max. 5” x 5” wafer max. 5” beam 2nm overlay 50nm incr. 2.5 (0.1) nm
E-beam writer Vistec SB 350 masks max. 9” x 9” wafer max. 9” resolution 50nm overlay 14nm incr. 1.0nm
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Fundamentals
Variable shaped beam Gaussian beam E-Beam Imaging Systems
E-beam writer LION LV1 masks max. 5” x 5” wafer max. 5” beam 2nm overlay 50nm incr. 2.5 (0.1) nm
E-beam writer Vistec SB 350 masks max. 9” x 9” wafer max. 9” resolution 50nm overlay 14nm incr. 1.0nm
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Fragmentation of PMMA (Polymethylmethacrylate) during exposure
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Result: PMMA-chains split, enhanced solubility in MIBK (Methylisobutylketone)
Fundamentals
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Change of resist solubility a liquid developer
Positive Resist: Average molecular weight reduced by exposure → exposed area is solved much faster in developer and thus removed
Negative Resist: Average molecular weight increased by exposure (cross-linking of molecules) → unexposed area is removed in developer
e.g. PMMA: MIBK : Isopropanol 1:1, t=30...60 sec, Stop in Isopropanol, N2-Drying
Fundamentals
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
• Introduction • Motivation • General EBL process • Fundamentals
• Basics and Physics of EBL • Resist Technology • Charging • EBL Writing Strategies • Interaction between E-beam and Substrate • Proximity Effect • Proximity Function • Periodic Structures • Resolution Limits in EBL
• Some Special Exposure Techniques • Cell Projection Exposure • Variable Dose Exposure • Mask Preparation for Lift-Off • Overlay Exposure
Electron Beam Lithography - EBL
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Resist Technology
Sample Preparation: Coating & Tempering
1. Spin Coating 2. Tempering (Pre-Exposure-Bake)
Hotplate (or oven)
Typical tempering figures: T= 90...210 °C t = 5...30 min
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Dose D = Deposited electrical charge per area unit [µC/cm2]
I – current, t – exposure time, F – area, j – current density
Resist properties: Sensitivity & Contrast
Contrast curve measurement: Expose uniform square areas (e.g. 100µm) with increasing dose
Increase of Dose Value
Resist Technology
tjF
tID ×=×
=
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
Contrast curve measurement
Increase of Dose Value
Increase of Dose Value
Real (non-binary) resist
0 %
100 %
Resist hight after developm
ent
Ideal (binary) resist
Sensitivity D0 = Threshold dose, for which a (large) area of a
given resist is completely removed (clearing dose)
D0
D0
Resist properties: Sensitivity & Contrast
Resist Technology
Introduction to Nanooptics, Summer Term 2012, Abbe School of Photonics, Jena, Prof. Thomas Pertsch
∞
D1 D0
Resist properties: Sensitivity & Contrast
10 0.0
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Ideal resist g = Real resist (Zep520) =18
Dose [µC/cm2]
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t Hig
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g
Quantitative measure for binary behaviour of a resist
(slope in contrast kurve)
Resist Technology
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