Nano-Lithography with Metastable Helium Claire Allred, Jason Reeves, Christopher Corder, Harold Metcalf IQEC: June 4, 2009 Supported by: ONR and Dept.

Slides:



Advertisements
Similar presentations
Femtosecond lasers István Robel
Advertisements

Thermal properties of laser crystal Rui Zhang ACCL Division V, RF-Gun Group Feb 20, 2015 SuperKEKB Injector Laser RF Gun Review.
Anodic Aluminum Oxide.
Measuring the Speed of Light Jack Young Rich Breazeale Ryan Phelan.
Ashida lab Toyota yusuke
KAPITZA-DIRAC EFFECT Eric Weaver Phys 4P62. General Outline  Theorized in 1933 by Kapitza and Dirac  Reflection of electrons from standing light waves.
Laser-Assisted Direct Imprint (LADI) Technology S. Y. Chou, C. Keimel, and J. Gu, Ultrafast and direct imprint of nanostructures in silicon, Nature, 417.
General Properties of Light Light as a wave Speed Wave properties: wavelength, frequency, period, speed, amplitude, intensity Electromagnetic wave.
Generation of short pulses
Development of Scanning Probe Lithography (SPL)
Absorption and emission processes
Imaging of flexural and torsional resonance modes of atomic force microscopy cantilevers using optical interferometry Michael Reinstaedtler, Ute Rabe,
Atomic Structure. X-ray Spectrum Continuous spectrum Characteristic spectrum.
EE235 Class Presentation on Nanoimprint Lithography (Spring 2007) Fabrication of photonic crystal structures on light emitting diodes by nanoimprint lithography.
Interference Diffraction and Lasers
Chapter 5: Wave Optics How to explain the effects due to interference, diffraction, and polarization of light? How do lasers work?
4-1 Chap. 7 (Optical Instruments), Chap. 8 (Optical Atomic Spectroscopy) General design of optical instruments Sources of radiation Selection of wavelength.
Properties of ElectroMagnetic Radiation (Light)
1 Waves, Light & Quanta Tim Freegarde Web Gallery of Art; National Gallery, London.
Top-down approach for formation of nanostructures: Lithography with light, electrons and ions Seminar Nanostrukturierte Festkörper, Martin Hulman.
McGill Nanotools Microfabrication Processes
TRIµP Laser Spectroscopy: Status and Future U Dammalapati TRI  P Facility Lasers for Na  -decay Ra Spectroscopy & EDM Towards cooling of Heavy Alkaline.
B.SC.II PAPER-B (OPTICS and LASERS) Submitted by Dr. Sarvpreet Kaur Assistant Professor PGGCG-11, Chandigarh.
High Harmonic Generation in Gases Muhammed Sayrac Texas A&M University.
An Introduction. The first step on the road to laser was the publication of paper by Albert Einstein in 1916 –describing how atoms could interact with.
1 P1X: Optics, Waves and Lasers Lectures, Lasers and their Applications i) to understand what is meant by coherent and incoherent light sources;
Kinetic Investigation of Collision Induced Excitation Transfer in Kr*(4p 5 5p 1 ) + Kr and Kr*(4p 5 5p 1 ) + He Mixtures Md. Humayun Kabir and Michael.
Interaction of radiation with atoms and ions (I) Absorption- Stimulated emission E1E1 E2E2 W 12 =W 21 Spontaneous emission More definitionsCross section.
1 My Chapter 28 Lecture. 2 Chapter 28: Quantum Physics Wave-Particle Duality Matter Waves The Electron Microscope The Heisenberg Uncertainty Principle.
Techniques for Synthesis of Nano-materials
Center for Materials for Information Technology an NSF Materials Science and Engineering Center Nanolithography Lecture 15 G.J. Mankey
Chemistry is in the electrons Electronic structure – how the electrons are arranged inside the atom Two parameters: –Energy –Position.
Progress towards laser cooling strontium atoms on the intercombination transition Danielle Boddy Durham University – Atomic & Molecular Physics group.
Tunable, resonant heterodyne interferometer for neutral hydrogen measurements in tokamak plasmas * J.J. Moschella, R.C. Hazelton, M.D. Keitz, and C.C.
Single atom manipulations Benoît Darquié, Silvia Bergamini, Junxiang Zhang, Antoine Browaeys and Philippe Grangier Laboratoire Charles Fabry de l'Institut.
Observation of ultrafast nonlinear response due to coherent coupling between light and confined excitons in a ZnO crystalline film Ashida Lab. Subaru Saeki.
Proximity Effect in Electron Beam Lithography
Lithography. MAIN TYPES OF LITHOGRAPHY: * Photolithography * Electron beam lithography –X-ray lithography –Focused ion beam lithography –Neutral atomic.
日 期: 指導老師:林克默、黃文勇 學 生:陳 立 偉 1. Outline 1.Introduction 2.Experimental 3.Result and Discussion 4.Conclusion 2.
November 14, 2013 Mechanical Engineering Tribology Laboratory (METL) Experimental and Analytical Investigation of Transient Friction Abdullah Alazemi Ph.D.
Scanning capacitance microscopy
Min Hyeong KIM High-Speed Circuits and Systems Laboratory E.E. Engineering at YONSEI UNIVERITY
-Plasma can be produced when a laser ionizes gas molecules in a medium -Normally, ordinary gases are transparent to electromagnetic radiation. Why then.
Laser Cooling and Trapping Magneto-Optical Traps (MOTs) Far Off Resonant Traps (FORTs) Nicholas Proite.
Lithography in the Top Down Method New Concepts Lithography In the Top-Down Process New Concepts Learning Objectives –To identify issues in current photolithography.
Waves, Light & Quanta Tim Freegarde Web Gallery of Art; National Gallery, London.
Presented by Darsen Lu (3/19/2007)
2. Design Determine grating coupler period from theory: Determine grating coupler period from theory: Determine photonic crystal lattice type and dimensions.
LITHOGRAPHY IN THE TOP-DOWN PROCESS - BASICS
Nanolithography Using Bow-tie Nanoantennas Rouin Farshchi EE235 4/18/07 Sundaramurthy et. al., Nano Letters, (2006)
Lithography. Lithography in the MEMS context is typically the transfer of a pattern to a photosensitive material by selective exposure to a radiation.
Controlled fabrication and optical properties of one-dimensional SiGe nanostructures Zilong Wu, Hui Lei, Zhenyang Zhong Introduction Controlled Si and.
Speaker: Shiuan-Li Lin Advisor : Sheng-Lung Huang
Rydberg atoms part 1 Tobias Thiele.
Mg Films Grown by Pulsed Laser Deposition as Photocathodes: QE and surface adsorbates L. Cultrera INFN – National Laboratories of Frascati.
Optical Vortices and Electric Quadrupole transitions James Bounds.
Laser Cooling and Trapping
Four wave mixing in submicron waveguides
Lithography.
Light-Matter Interaction
Lecture 7 Fundamentals of Multiscale Fabrication
Interaction between Photons and Electrons
7x7 surface have been removed and deposited.
Principle of Mode Locking
Layer Transfer Using Plasma Processing for SMART-Wafer
SILICON MICROMACHINING
Nanocharacterization (III)
Anti-Reflective Coatings
H’(t)=E-M field D  = - fi Transition dipole moment.
Rayat Shikshan Sanstha’s S. M. Joshi College, Hadapsar
Presentation transcript:

Nano-Lithography with Metastable Helium Claire Allred, Jason Reeves, Christopher Corder, Harold Metcalf IQEC: June 4, 2009 Supported by: ONR and Dept. of Education

Atomic Nanofabrication Direct Deposition. –Done with Na at Bell Labs in 1992 –Since demonstrated with Cr. Resist Assisted. –Patterned atoms interact with a resist changing its wetting properties. –Substrate is processed in a second step producing permanent patterns. –Done with noble gases, alkali & alkaline metals and group III elements. Review article: Meschede et.al. J. Phys. D. 36(2003) R17. Nanometer scale patterning of neutral atoms and subsequent pattern preservation on a surface.

Some Motivation Massive parallel fabrication of nanostructures. Spectroscopically determined accuracy. Detailed study of the limits of optical forces. Applications to meta-material fabrication and photonic crystals.

Brief Outline Experimental System: atomic beam and lithography process. Numerical Simulations: Trajectory calculations. Experimental Results: geometrical mask and light mask. Experimental System Numerical Simulations Experimental Results

Metastable Helium 20eV of internal energy. Doubly disallowed decay gives a lifetime of 8000s. Specific transition information: – nm –  = 98ns Experimental System Numerical Simulations Experimental Results Atom Bichromatic Force Atomic Beam Lithography Process

The Bichromatic Force Two frequencies give an amplitude modulated carrier wave. –Carrier frequency (  1 +  2 )/2 at atomic resonance. –Envelope frequency (  1 -  2 )/2=  bichro. Amplitude modulation satisfies pi pulse condition:  =  bichro /4 Absorption from left gives  p = +  k Stimulated emission from the right gives  p = +  k Experimental System Numerical Simulations Experimental Results Atom Bichromatic Force Atomic Beam Lithography Process  /  bichro

Force Profile Ordinary Optical Molasses { δ/k k/k/ kk Experimental System Numerical Simulations Experimental Results Atom Bichromatic Force Atomic Beam Lithography Process

The Bichromatic Force for Collimation: Experimental System Numerical Simulations Experimental Results Atom Bichromatic Force Atomic Beam Lithography Process Zero velocity is shifted

Collimation Sequence Experimental System Numerical Simulations Experimental Results Atom Bichromatic Force Atomic Beam Lithography Process Source -kv±  +kv±  -kv±  +kv±  -kv±  2.3 mrad 1.1 mrad  =-5   =-  v l =1125±220 m/s

Sample Preparation Si wafers from Montco Silicon Technologies. 5 Å Cr adhesion layer and 250Å Au layer evaporated by Scientific Coatings. Diced in the Lukens Laboratory. Clean wafers: –Acetone. –Ethanol –Pirahna Assemble resist: nonanethiol. Experimental System Numerical Simulations Experimental Results Atom Bichromatic Force Atomic Beam Lithography Process 1-nonanethiol

Neutral Atom Lithography On impact He* deposits energy and becomes g.s. of He. Part of thiol C chain is broken and an extra electron weakens neighboring chain. Wet chemical etch removes Au where thiols are damaged. Samples are examined using an Atomic Force Microscope and a Scanning Electron Microscope. Experimental System Numerical Simulations Experimental Results Atom Bichromatic Force Atomic Beam Lithography Process He* He ~7min Standard Gold Etchant: 1M KOH 0.1M K2S2O3 0.01M K3Fe(CN) M K4Fe(CN)6 3H20

Focusing vs. Channeling Trajectories Experimental System Numerical Simulations Experimental Results Trajectory Calculations Monte Carlo Calculations McClelland, JOSA B 12 (1995)1761 Focusing RegimeChanneling Regime Coordinate System

Geometrical Mask Use micromesh (2000 lines per inch) to pattern resist. Peak dosage of 3 * atoms / mm 2 and 7min etch time gives sharp features. Edge resolution of 80nm. Experimental System Numerical Simulations Experimental Results Geometrical Mask Channeling Light Mask Focusing Light Mask Conclusions

Channeling Regime: P=4P 0 Line spacing of 499±3nm on AFM. Line Spacing of 566±14nm on SEM. Line widths 100nm.  =+490MHz=+300  dosage = 1.5*10 12 atoms/mm 2 Experimental System Numerical Simulations Experimental Results Geometrical Mask Channeling Light Mask Focusing Light Mask Conclusions

Focusing Regime: P=P 0 Transverse velocity distribution in the numerical simulations is probably incorrect. Very faint lines, only visible in SEM or the FFT of AFM scans. Experimental System Numerical Simulations Experimental Results Geometrical Mask Channeling Light Mask Focusing Light Mask Conclusions

Results Performed numerical simulations. Measured the edge resolution to be ~80nm. This is limited by wafer processing techniques. Demonstrated patterning in the focusing and channeling regime. Experimental System Numerical Simulations Experimental Results Channeling Light Mask Focusing Light Mask Velocity Offset Conclusions

Cool wafer pictures Supporting Material

The Radiative Force |e> |g> |e> |g> |e> |g> |e> |g> Atoms and Light Experimental System Numerical Simulations Experimental Results Monochromatic Forces Polychromatic Forces Atoms

Optical Molasses Force [  k  / 2 ] Atoms and Light Experimental System Numerical Simulations Experimental Results Monochromatic Forces Polychromatic Forces Atoms

The Light Shift and Dipole Force Light adds an off diagonal perturbation to the Hamiltonian that describes the atom. –Energies are shifted: –New eigenstates are mixtures of pure states. In a standing wave light field, the intensity of the light changes over half a wavelength. –Spatial modulation of the separation of the energy levels results in a force. –Red detuned light attracts atoms. –Blue detuned light repels atoms. Atoms and Light Experimental System Numerical Simulations Experimental Results Monochromatic Forces Polychromatic Forces Atoms

Laser System Whole system is seeded with an extended cavity DBR diode laser. Laser is kept on resonance with saturation spectroscopy. Double passed AOM produces four frequencies in two beams. –Shift the center velocity. –Phase delay between counter propagating pi pulses. Two AOM's produce light for three optical molasses stages. Atoms and Light Experimental System Numerical Simulations Experimental Results Laser System Vacuum System Atomic Beam Lithography Process  +kv+   +kv-   -kv+   -kv-  To Vacuum System 60 MHz Fiber Amplifiers PZT Diode 82 MHz 89 MHz 90 MHz To Lock  -kv+  m1  -kv-  m1  -kv+  m2  -kv-  m2

SAS Supporting Material

Vacuum System Atoms and Light Experimental System Numerical Simulations Experimental Results Laser System Vacuum System Atomic Beam Lithography Process

OBE's Supporting Material

Initial Population Atoms and Light Experimental System Numerical Simulations Experimental Results Trajectory Calculations Monte Carlo Calculations Position DistributionVelocity Distribution Coordinate System:

Focusing and Channeling Experimental System Numerical Simulations Experimental Results Trajectory Calculations Monte Carlo Calculations

Standard Selective Etch Supporting Material ~7min Standard Gold Etchant: 1M KOH 0.1M K2S2O3 0.01M K3Fe(CN) M K4Fe(CN)6 3H20 Metal Oxidation Or Reduction of Oxidizer