Fabrication and Testing of Nanoscale Devices Gurpreet Singh Assistant Professor, Mechanical and Nuclear Engineering Department, Kansas State University “http://www-personal.ksu.edu/~gurpreet/”
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Fabrication and Testing of Nanoscale Devices Gurpreet Singh Assistant Professor, Mechanical and Nuclear Engineering Department, Kansas State University “http://www-personal.ksu.edu/~gurpreet/” Overview • Introduction – CNT Mechanical Properties and Challenges – Introduction to 3-D nano-manipulation • Device Fabrication and Testing SEM Based FIB Based SEM vs. FIB Example: Fabrication and calibration of an individual MWCNT/sphere device as a mechanical force sensor. Additional Outcomes: Laser trapping in air. • Current Research Micro-nano piezoresistive sensors and piezoelectric nanowires, VT Electromechanical Testing stage, CU-Boulder SiCN coatings for high power laser thermal detectors, NIST-Boulder • Summary/Conclusion 2 Carbon Nanotubes SWCNT Graphene Sheet MWCNT Allotrope of Carbon D (SWNT): Few nm Do (MWNT): Up to hundreds of nm Aspect Ratio ≈ 104 3 Mechanical Properties: CNTs •Wong et.al. Science 1997 E = 1.28±0.59 TPa •Tombler et. al. Nature 2000 E ≈1.2 TPa •Falvo et.al. Nature 1997 Large local strains ≈16% •Yu et. al. Science 2000. E ≈ 270 to 950 GPa. st = 1163GPa. ef ≈12% (max.) Zhu et. al. PNAS 2005. sf≈ 15.84 GPa at ef = 1.56% “Primary focus is to include CNTs into engineered systems. And the potential to do4 this depends largely on the ability to manipulate them in 3-d space.” The Scale ∆ 107 m } } ∆ 107 m . NT Earth Lamp 5 Nanoscale Manipulation Strategies TEM Real time 2- D 3- D viewing Observation Manipulation SEM STM AFM 0.1 3- D Observation 2- D Manipulation 1 10 100 1000 Scale of Objects (nm) 6 Some Nano-manipulation Tools Quick foot Nanotechnology 19, 49, 495503 2008 Nanotechnology, 17, 10, 2434 2006 Yu et al. Science 2000 7 SEM Based Nano-manipulation Quick foot B C A Circular cover port w/ feed through 8 SEM Based Nano-manipulation (I) B (II) Quick foot C A (III) (IV) Circular cover port w/ feed through 9 SEM Chamber: Manipulator installed Electron Gun Sample Adapter Stage for Manipulator 10 Device Fabrication: Pick-n-Place CNT STEPS: a. Install and align the manipulator in SEM. b. Locate and separate individual CNT. c. Welding the CNT on support structure needle tips. (b) (a) (c) 11 G. Singh, P. Rice, R.L. Mahajan and J.R. McIntosh. Nanotechnology (2009). Welding Inside the SEM Acceleration Voltage 30 kV Adsorbed HCs or impurities Primary Electron Beam Oxygen molecule Free or Amorphous carbon CO or CO2 P. E. Pumped out volatile Water vapors S. E. MWCNT Resulting weld P.E. = 30 kV; S.E. ≈ (0 – 50) eV Dissociation of surface adsorbed impurity molecules (from the vacuum chamber) . 12 In-situ Mechanical Testing (A) AFM Tip Alignment AFM Tip Chip (glued to the W Tip) on which AFM Tip is mounted Tungsten Probe (mounted on Nano-Manipulator Arm) 13 G. Singh, P. Rice, R.L. Mahajan and J.R. McIntosh. Nanotechnology (2009). Tip Blunting Rubbing against Zirconia Substrate 14 Mechanical Characterization (B) Loading Test Direction of application of force 15 G. Singh, P. Rice, R.L. Mahajan and J.R. McIntosh. Nanotechnology (2009). Mechanical Characterization (GPa) Number d (nm) δmax. (nm) A (mm2) (x10-3) 1 200±20 150±10 31±6.2 420±42 0.013 ±0.004 2 110±11 200±20 9.5±1.9 560±56 0.029±0.008 3 60±6 290±29 2.8±0.5 812±81.2 0.145±0.043 • Fmax. (nominal) N (x10-9) The device breaks at the welds while CNT survives the load test. • F max. ≈ 1 N • Maximum weld strength observed was ~ 0.14 GPa. 16 Device Fabrication: Pick-n-Place GaN NW (a) (b) (c) (d) 17 GaN Nanowire: APT Specimen Preparation (a) (b) (c) (d) 18 FIB Based 3-D nano-manipulation FEI Helios 600 NanoLab Dual Beam at Virginia Tech and CU-Boulder • FE-SEM & FIB: Ga LMIS • 4 Gas Injector Systems •Dual Beam •Pt deposition (C9H16Pt) •SiO2 deposition (TEOS) •In-built Micromanipulator •Insulator Enhanced Etch (XeF2) •Gas Injectors •Selective Carbon Mill •Big Chamber • EBSD • Cryo Chamber • OmniprobeTM 19 Understanding the Geometry Beams Coincidence Point 52 ° 4.1 mm Image Source: internet 20 Understanding the Geometry 21 Eucentric height Ctrl + i Tungsten probe Needle (~0.5 mm); 100 um above the surface The value of Z at which tilt does not couple to sample translation is called the "eucentric" height. > Centering the feature > Couple mag. 22 Locating a NT and Pt deposition Making contact Pt Deposition Warm-up and insert Platinum deposition needle to avoid vibrations. Lock the stage. Fabricating devices using individual NTs 23 Separating a nanotube EBEAM Ion-BEAM 24 Fabricating devices using individual NTs FIB: Machining and Fabrication Si MEMS 25 CNT Device fabrication: SEM Vs. FIB 160 Electron Beam Ion Beam Estimated Time in min. 140 120 100 80 60 40 20 0 Sample Mounting/Alignments NT Location NT Welding Separation FIB Placement on test structure SEM w/ Nanomanipulator 26 Fabrication and Calibration of a CNT/sphere Device as a Mechanical Force Sensor Fabrication of CNT/Microsphere Device (I) (II) I.R. Camera (side view) (III) (IV) 28 Final Device Sphere d ≈ 4 m Sphere d ≈ 10 m 29 Application as a Mechanical Force Sensor • Mechanical force sensor for measuring forces (nN). Study of deformation behavior of Tissues/ Single cells, e.g., Kinocilium in Ciliary Bundles (sensory hairs). • Calibration Tests against a pre-calibrated Si tip-less cantilever (K = 0.0102 N/m). • Calculation of Bending Modulus of individual carbon nanotubes. 30 Applications in BioMechanics Sensory hair bundle present in Utricle (inner ear) Valentin Lulevich et al, Langmuir, 2006, 22 (19), 8151-8155• Source: Prof. Wally Grant, Biomedical Eng., Virginia Tech. 31 Alignment Inside SEM: Calibration Tests Cantilever Chip K calibrated = 0.0102 N/m Tip-less Cantilever Tungsten Probe 32 Image Analysis: Superimposition Application of load Red: zero load Blue/Green: final step 33 G. Singh et. al. Nanotechnology 18 475501 (2007). Force Vs Deflection : Calibration Tests Force Vs Sphere Deflection 4.5E-08 4.0E-08 l Å 8 m Force on Spher e (N) 3.5E-08 3.0E-08 l Å 10 m 2.5E-08 l Å 13 m 2.0E-08 1.5E-08 l Å 13.5 m 1.0E-08 l Å 15.5 m l Å 14.5 m 5.0E-09 0.0E+00 0 2 4 6 8 10 12 Deflection of the Sphere (microns) 34 Bending Modulus of Individual CNT • Linear Fit to Experimental Data FT = Kn. dn • For a Cantilever Beam Assumption: Fn (3Eb.I/Ln3). dn Eb KnLn3/3I 35 Bending Modulus: Results Ln (m) (±0.5) Kn(N/m)(10-3) Eb in GPa - 14.5 0.7±0.07 59±11.9 170.8 10 8 13.1±1.31 53±15.2 3 185.3 8 15.5 1.4±0.14 30±5.8 4 200* - 13 3.2±0.32 30±6.3 5 200* - 10 7.2±0.72 31±7.7 6 230.3 12 13.5 1.8±0.18 11±2.3 Nanotube Do (nm) 1 125* 2 Di (nm) 36 Summary • Fabricated a novel CNT/sphere device with varying CNT lengths and sphere diameters. • Performed in situ bending/calibration tests. Measured forces ranged (10-8 to 10 -9)N. Important features are the range of forces and the small size of the device. • No deflection of the cantilever tip was observed for nanotube lengths > 15 µm. • Bending modulus of individual CNTs ranged (11- 59) GPa depending on NT geometry. 37 Laser Trapping in Air NT Length> 15 m Laser Trapping in Air Specimen Plane Objective LASER 1064nm Optical Trap Highly focused Fnet = F1+ F2 Laser in n sphere>n medium Simple Schematic 39 Results: Laser Trapping 4 m polystyrene sphere on a ~25 m long CNT SEM 1064 nm IR Laser at 100 mW, Spot size ~ 1 m. 40 Results: Laser Trapping 11 m Polystyrene Sphere SEM Optical 1064 nm IR Laser at 100 mW, Spot size ~ 1 m. No Appreciable sphere movement was observed in this case. 41 Current Research on Polymer Derived SiCN •Micro-nano piezoresistive sensors and piezoelectric nanowires, VT •Electromechanical Testing stage, CU-Boulder •SiCN coatings for high power laser thermal detectors, NIST-Boulder 42 Multifunctional Micro-Nanosensors TYPE La0.8Sr0.2MnO3 SiCN CNTs Gage factor 3-5 1000-4000 ~800-3000 Stability Good Highly stable Stable Cost Low Expensive Medium Microsensor: SiCN-(La,Sr)MnO3 composites (Automobile Applications) (M. Karmarkar, G. Singh, S. Shah, R.L. Mahajan, and S. Priya. Large piezoresistivity phenomenon in SiCN – (La,Sr)MnO3 composites. Applied Physics Letters (2009).) Nanosensor: MWCNT+ SiCN (PDC): Coreshell geometry: Pressure sensor for harsh environments G. Singh, S. Priya, M. Hossu, S R Shah, S. Grover, Ali R Koymen and R L Mahajan. Synthesis, electrical and magnetic characterization of core-shell carbon nanotube – SiCN nanowires. [Available online]: (2009). 43 Multifunctional Micro-Nanosensors Cross-linking and Pyrolysis of Organic Polymer (Silazanes): 700-1000C H2/NH3 are released; leaving free ‘C’ behind C Atoms: sp2 to C; sp3 to Si; not bonded to N. Si Atoms: tetrahedrally to C and N. Nanodomains: 1-2 nm 44 Microsensor: SiCN-(La,Sr)MnO3 composites Si Map Mn Map Load cell readout sample Resistancemultimeter 45 Nano-sensor: Using Individual NWs SiCN coated Carbon nanotubes: cross-linking and pyrolysis of PUMVS on the surfaces of CNTs MWCNT SiCN Coated MWCNT 46 G Singh et al. Materials Letters 2009 Electromechanical Tensile Testing • • • • • Microfabricated test stage for tensile measurements of nanofibers Fixed and moving stages Fixed stage is electrically isolated from moving stage Thermal actuation AC Impedance measurement circumvents specimen contact resistance • Bending Beams as Springs, Lateral Stabilization, Heat Sinks, and Electrical Connections for Specimen Bending Beams Fixed Stage Moving Stage Thermal Actuator 47 Collaboration: V. Bright Group: CU-Boulder Electromechanical Tensile Testing 48 Collaboration: V. Bright Group: CU-Boulder Tensile Testing: CNT CNT J.J. Brown, J.W. Suk, G. Singh, A.I. Baca, D.A. Dikin, R.S. Ruoff, and V.M. Bright. Sensors and Actuators A: Physical [In Press] (2008). 49 Nanocoatings for High Power Laser Thermal Detectors • NIST in Boulder maintains thermal detectors as measurement standards for measuring optical power from laser sources (15000 W/cm2). • Continue to seek a black coating (high damage threshold, high thermal diffusivity and high optical absorbance) that can be easily applied and that is durable like enamel paint, yet with the desirable properties of carbon nanotubes (such as SiCN). • Fundamental understanding of the effect of laser irradiation on carbonaceuos nanomaterials. G. Singh, P. Rice, K. Hurst, J. Lehman and R.L. Mahajan, Applied Physics Letters, 91, 033101 (2007). Thermal Detector Coatings for IR Lasers The coated surface is exposed to lasers at 1.06 um and 10.6 um. These coatings showed no damage even at >10 kW/cm2. As Deposit 1.06 um 10. 6 um 51 Final Summary • There is a continuous need for testing standards at the nanoscale. • Electron microscope based manipulation works well for pick, place and fabrication of high aspect ratio nanowire based devices and larger size specimen. • FIB can be used to section and deposit material at the nanoscale. FIB based manipulation outperforms SEM based manipulation on many levels. • This work is important for fundamental understanding of the materials at nano-scale. It can be extended to the design and development of many other ‘proof of principle’ devices. • Fabrication of a novel CNT/sphere device: Development of high precision force sensor. • Laser Trapping in Air. Collaborative research on micro and nano composite materials (sensor), nanocoatings (IR Lasers, UV Lasers). • 52 Acknowledgements • Physics Department, Kansas State University. • Advisors and Mentors. • 1. 2. 3. 4. 5. 6. 7. Collaborators: ICTAS, Virginia Tech., NIST and Oak Ridge National Lab. Prof. Harry Dorn, Nichole Rylander, Tom Campbell, Rafael Davalos, S Priya Cindi Schwartz, Mary Morphew, Mark Ladinsky (Nano-knife project). Tasshi Dennis (Bio-Optics). John Lehman, Katie Hurst, Darryl (Excimer Laser Cleaning). Andrew Slifka and Damien (Optical Trapping). Corrie Spoon, Prof. Wally Grant (Engineering Science and Mechanics, VT). • M.E. Faculty members and students. 53 THANK YOU!! References 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. 16. J. Richard McIntosh, The Journal of Cell Biology, 153, F25 (2001). PhD Thesis, Luyten H, “The rheological and fracture properties of Gouda cheese”, Wageningen AG (1988). E. W. Wong, P. E. Sheehan, and C. M. Lieber, Science 277, 1971 (1997). M. R. Falvo, G. J. Clary, R. M. Taylor II, V. Chi, F. P. Brooks, Jr., S. Washburn, and R. Superfine, Nature (London) 389, 582 (1997). M. F. Yu, O. Lourie, M. J. Dyer, K. Moloni, T. F. Kelley, and R. S. Ruoff, Science, 287, 637 (2000). MS Dresselhaus, G. Dresselhaus, Ph. 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