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Strain Engineering of Thermal Transport in Nanocrystalline
Materials
Brandon N. DavisPhD Student
Department of Mechanical Engineering
Oral Preliminary ExamMay 14, 2014
Advisor: Prof. Sandeep KumarCommittee: Prof. Javier Garay, Prof. Masaru Rao, Prof. Lorenzo Mangolni
2
Nanomechanics and Multiphysics Lab
Presentation Outline
• Background– Part I: Thermoelectric Materials– Part II: Strain Engineering– Part III: Lead Telluride
• Proposed Research Plan• Future Work
3
Nanomechanics and Multiphysics Lab
Presentation Outline
• Objective• Background– Part I: Thermoelectric Materials– Part II: Strain Engineering– Part III: Lead Telluride
• Proposed Research Plan• Future Work
4
Nanomechanics and Multiphysics Lab
Background: Applications
• We can take advantage of the “Seebeck Effect” and use the heat generated to create electrical current
Example: Satellite Example: Car Exhaust
(1) http://www.spacetoday.org/(2) http://www.gizmag.com/
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Nanomechanics and Multiphysics Lab
Background: Applications
• Thermoelectric Generators is an example of a thermoelectric material exhibiting the “Seebeck Effect”
• Using p and n type semiconductors
• Connected electrically in series thermally in parallel
• Quiet, Reliable, Cheap, Durable
• Potential for heat reclamation in car exhaust systems
• VERY INEFFICIENT
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Nanomechanics and Multiphysics Lab
Background: Thermoelectric Materials
Temperature Gradient
Electrical Potential
Materials that exhibit a change in temperature can create an electrical potential
Materials that exhibit a change in electrical potential can generate a temperature difference
Known as Seebeck Effect
Known as Peltier Effect
http://www.thermoelectrics.caltech.edu/
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Nanomechanics and Multiphysics Lab
Background: Seebeck Effect
http://www.thermoelectrics.caltech.edu/
Hot
Cold
NP
•Discovered by Thomas Seebeck in 1821•Hot and Cold side •Electron build up causes electric potential•Voltage drop is the result
Holes Electrons
8
Nanomechanics and Multiphysics Lab
• Thermal Efficiency equation describes the maximum efficiency of thermoelectric materials
Background: Thermal Efficiency
𝑧𝑇= 𝑆2𝜎𝑇𝑘
S – Seebeck coefficient (add units)
σ– Electric conductivity (add units)
T – Absolute temperature
k – Thermal conductivity
zT – Figure of merit
• Part of my goal is to increase the zT of a material
• Typical zT <1
G. Jeffrey Snyder et. Al. :complex thermoelectric materials. Nature publishing group February 2008
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Nanomechanics and Multiphysics Lab
Background: Thermal Transport
• Our goal is to optimize the properties of thermoelectric materials by specifically improving the thermal transport of the material
PbTeStrategies to improve the Figure of Merit (zT)
New Material DesignNanostructuring/ Interface
Engineering
Alloying NanoinclusionsNanocrystalline grain structure
Heterostructures
10
Nanomechanics and Multiphysics Lab
Presentation Outline
• Objective• Background– Part I: Thermoelectric Materials– Part II: Strain Engineering– Part III: Lead Telluride
• Proposed Research Plan• Future Work
11
Nanomechanics and Multiphysics Lab
Background: Strain Engineering
• Strain engineering is a technique used to improve the performance of materials
• Using strain engineering to improve the performance of the thermoelectric material, PbTe
Strain Engineering can be used for and applied to:
• Influence the properties of a material
• Tune to specific parameters• Effect the carrier mobility and
band gap of materials
• Nanocrystalline & Nanostructured Materials• Semiconductors• Thermoelectrics
12
Nanomechanics and Multiphysics Lab
Background: Current Methods
• Current method of strain engineeringTension
Compression
Compression
Tension
Lattice match
Dislocation + Defect Trap
Relaxation
Lattice Mismatch
EpilayerSubstrate
13
Nanomechanics and Multiphysics Lab
Background: Four Key of Strain Engineering
• The implementation of strain engineering can be classified by four processes
This process will be further outlined and applied to our proposed processJu Li et. al. “Elastic strain engineering for unprecedented materials properties” Materials research Socciety February 2014 vol 39
Synthesizing Load Bearing
Nanostructures
Applying Force to the Material
Measuring Strain
Prediction of Strain Effect
14
Nanomechanics and Multiphysics Lab
Background: Characterizing Strain Engineering
• Relating strain engineering to the figure of merit (zT)
Small Grain
𝒛𝑻=𝑺𝟐𝝈𝑻𝒌
Electric Conductivity
Thermal ConductivityPhonon
Large Grain
Electron
15
Nanomechanics and Multiphysics Lab
Presentation Outline
• Objective• Background– Part I: Thermoelectric Materials– Part II: Strain Engineering– Part III: Lead Telluride
• Proposed Research Plan• Future Work
16
Nanomechanics and Multiphysics Lab
Background: Lead Telluride
• Narrow gap material
• Rock Salt Structure (NaCl)
• Is optimum for mid-temperature application
• Operates in the temperature range of 500k- 900 K
• Has shown to have a maximum zT of 2
1. http://www.webelements.com/2. Y. Q Cao et. al. “Low thermal conductivity and improved figure of merit in fine-grain binary PbTe
thermoeletric alloys
17
Nanomechanics and Multiphysics Lab
Presentation Outline
• Objective• Background– Part I: Thermoelectric Materials– Part II: Strain Engineering– Part III: Lead Telluride
• Proposed Research Plan• Future Work
18
Nanomechanics and Multiphysics Lab
Nanofab : Photolithography and Sputtering
Synthesizing Load Bearing
Nanostructures
Applying Force to the Material
Measuring Strain
Prediction of Strain Effect
19
Nanomechanics and Multiphysics Lab
Proposed Research: Nanofab Process
Step 1: Create Mask
Design
Step 2: Use photolithography
to transfer pattern (frontside and
backside)
Step 3: DRIE Etch
Step 4: Hydro Fluoric (HF)
Vapor Etch
Specimen and MEMS Device Ready for
Experimentation and Analysis
20
Nanomechanics and Multiphysics Lab
Nanofab: Mask
• L-edit Mask Design
Backside Alignment
MEMS DeviceMask with MEMS Device
21
Nanomechanics and Multiphysics Lab
Nanofab: Process Flow
Photo Resist Substrate PbTeSilicon Oxide
MASK
MASK
Deep Reactive Ion Etching
22
Nanomechanics and Multiphysics Lab
Nanofab: MEMS Device and Experiment
Synthesizing Load Bearing
Nanostructures
Applying Force to the Material
Measuring Strain
Prediction of Strain Effect
25
Nanomechanics and Multiphysics Lab
Experiment and Analysis
Synthesizing Load Bearing
Nanostructures
Applying Force to the Material
Measuring Strain
Prediction of Strain Effect
26
Nanomechanics and Multiphysics Lab
Raman Spectroscopy
• A laser is focused on to the sample
• This excites and scatters the phonons across the material
• Raman light reflected and collected
• Measure the total phonon scattering to understand thermal conductivity and strain being applied
http://chemie.uni-paderborn.de/
27
Nanomechanics and Multiphysics Lab
Prediction of Strain
Synthesizing Load Bearing
Nanostructures
Applying Force to the Material
Measuring Strain
Prediction of Strain Effect
28
Nanomechanics and Multiphysics Lab
Presentation Outline
• Objective• Background– Part I: Thermoelectric Materials– Part II: Strain Engineering– Part III: Lead Telluride
• Proposed Research Plan• Future Work
29
Nanomechanics and Multiphysics Lab
Future Work
• 3 omega method to measure the eletrical conductivity
• Use 4 probe method to measure the thermal conductivity
30
Nanomechanics and Multiphysics Lab
Proposed Research Timeline
2013-14 2014-15 2015-2016 2016-2017
Su Fa W Spr Su fa w Spr Su Fa W Spr Su Fa W Spr
Phase 1
Phase2
phase3
31
Nanomechanics and Multiphysics Lab
Acknowledgements• Nanomechanics and Multiphysics Lab
– Principal Investigator Prof. Sandeep Kumar– Mr. Devil Garcia
• Nanofabrication Facility @ UCR & UCSD– Mr. Mark Heiden– Mr. Dexter Humphrey– Other names from UCSD
• Oral Prelim Committee– Principal Investigaor Prof. Sandeep Kumar– Prof. Lorenzo Mangolini– Prof. Javier E. Garay (double check middle initial)– Prof. Masaru P. Rao
GEM Fellowship Award Year 2014
33
Nanomechanics and Multiphysics Lab
Background: PbTE response to Temp
• At Temperature range 400 C – 600 C Dramatic Increase in zT