Archival Journals Publications

2015
A. Weathers, Khan, Z. U., Brooke, R., Evans, D., Pettes, M. T., Andreasen, J. W., Crispin, X., and Shi, L., “Significant Electronic Thermal Transport in the Conducting Polymer Poly(3,4-ethylenedioxythiophene),” Advanced Materials, vol. 27, pp. 2101–2106, 2015. Publisher's Version
L. A. Jauregui, Pettes, M. T., Rokhinson, L. P., Shi, L., and Chen, Y. P., “

Gate Tunable Relativistic Mass and Berry's phase in Topological Insulator Nanoribbon Field Effect Devices

,” Sci. Rep., vol. 5, pp. 8452, 2015. Publisher's Version
K. S. Olsson, Klimovich, N., An, K., Sullivan, S., Weathers, A., Shi, L., and Li, X., “

Temperature dependence of Brillouin light scattering spectra of acoustic phonons in silicon

,” Applied Physics Letters, vol. 106, pp. 051906, 2015. Publisher's Version
E. Fleming, Wen, S., Shi, L., and da Silva, A. K., “Experimental and theoretical analysis of an aluminum foam enhanced phase change thermal storage unit,” International Journal of Heat and Mass Transfer, vol. 82, pp. 273 - 281, 2015. Publisher's Version
V. Singh, Agarwal, R., Jurney, P., Marshall, K., Roy, K., Shi, L., and Sreenivasan, S. V., “

Scalable Fabrication of Low Elastic Modulus Polymeric Nanocarriers With Controlled Shapes for Diagnostics and Drug Delivery

,” Journal of Micro and Nano-Manufacturing, vol. 3, pp. 011002, 2015. Website
2014
S. N. Girard, Chen, X., Meng, F., Pokhrel, A., Zhou, J., Shi, L., and Jin, S., “Thermoelectric Properties of Undoped High Purity Higher Manganese Silicides Grown by Chemical Vapor Transport,” Chemistry of Materials, vol. 26, pp. 5097-5104, 2014. Publisher's Version
J. Buongiorno, Cahill, D. G., Hidrovo, C. H., Moghaddam, S., Schmidt, A. J., and Shi, L., “Micro- and Nanoscale Measurement Methods for Phase Change Heat Transfer on Planar and Structured Surfaces,” Nanoscale and Microscale Thermophysical Engineering, vol. 18, pp. 270-287, 2014. Publisher's VersionPDF icon phasechangemeasurements.pdf
H. Fateh, Baker, C. A., Hall, M. J., and Shi, L., “High fidelity finite difference model for exploring multi-parameter thermoelectric generator design space,” Applied Energy, vol. 129, pp. 373 - 383, 2014. Publisher's VersionAbstract
Abstract Thermoelectric generators (TEGs) are being studied and developed for applications in which waste heat, for example, from the exhaust of motor vehicles is converted into usable electricity. \{TEGs\} consisting of \{TE\} elements integrated with an exhaust heat exchanger require optimization to produce the maximum possible power output. Important optimization parameters include \{TE\} element leg length, fill fraction, leg area ratio between n- and p-type legs, and load resistance. A finite difference model was developed to study the interdependencies among these optimization parameters for thermoelectric elements integrated with an exhaust gas heat exchanger. The present study was carried out for \{TE\} devices made from n-type Mg2Si and p-type MnSi1.8 based silicides, which are promising \{TE\} materials for use at high temperatures associated with some exhaust heat recovery systems. The model uses specified convection boundary conditions instead of specified temperature boundary conditions to duplicate realistic operating conditions for a waste heat recovery system installed in the exhaust of a vehicle. The 1st generation, and an improved 2nd generation \{TEG\} module using Mg2Si and p-type MnSi1.8 based silicides were fabricated and tested to compare \{TE\} power generation with the numerical model. Important results include parameter values for maximum power output per unit area and the interdependencies among those parameters. Heat transfer through the void areas was neglected in the numerical model. When thermal contact resistance between the \{TE\} element and the heat exchangers is considered negligible, the numerical model predicts that any volume of \{TE\} material can produce the same power per unit area, given the parameters are accurately optimized. Incorporating the thermal contact resistance, the numerical model predicts that the peak power output is greater for longer \{TE\} elements with larger leg areas. The optimization results present strategies to improve the performance of \{TEG\} modules used for waste heat recovery systems.
X. Chen, Girard, S. N., Meng, F., Lara-Curzio, E., Jin, S., Goodenough, J. B., Zhou, J., and Shi, L., “

Approaching the Minimum Thermal Conductivity in Rhenium-Substituted Higher Manganese Silicides

,” Advanced Energy Materials, vol. 4, no. 14, pp. 1400452 , 2014. Publisher's VersionPDF icon re_substituted_hms_author_version.pdf
I. Jo, Pettes, M. T., Ou, E., Wu, W., and Shi, L., “Basal-plane thermal conductivity of few-layer molybdenum disulfide,” Applied Physics Letters, vol. 104, pp. 201902, 2014. Publisher's Version
V. Singh, Bougher, T. L., Weathers, A., Cai, Y., Bi, K., Pettes, M. T., McMenamin, S. A., Lv, W., Resler, D. P., Gattuso, T. R., Altman, D. H., Sandhage, K. H., Shi, L., Henry, A., and Cola, B. A., “High thermal conductivity of chain-oriented amorphous polythiophene,” Nature Nanotechnology, vol. 9, pp. 384-390, 2014. Publisher's VersionAbstract
Polymers are usually considered thermal insulators, because the amorphous arrangement of the molecular chains reduces the mean free path of heat-conducting phonons. The most common method to increase thermal conductivity is to draw polymeric fibres, which increases chain alignment and crystallinity, but creates a material that currently has limited thermal applications. Here we show that pure polythiophene nanofibres can have a thermal conductivity up to [sim]4.4 W m-1 K-1 (more than 20 times higher than the bulk polymer value) while remaining amorphous. This enhancement results from significant molecular chain orientation along the fibre axis that is obtained during electropolymerization using nanoscale templates. Thermal conductivity data suggest that, unlike in drawn crystalline fibres, in our fibres the dominant phonon-scattering process at room temperature is still related to structural disorder. Using vertically aligned arrays of nanofibres, we demonstrate effective heat transfer at critical contacts in electronic devices operating under high-power conditions at 200 [deg]C over numerous cycles.
A. L. Moore and Shi, L., “Emerging challenges and materials for thermal management of electronics,” Materials Today, vol. 17, pp. 163 - 174, 2014. Publisher's Version
C. A. Baker, Osman Emiroglu, A., Mallick, R., Ezekoye, O. A., Shi, L., and Hall, M. J., “Development of an Analytical Design Tool for Monolithic Emission Control Catalysts and Application to Nano-Textured Substrate System,” Journal of Thermal Science and Engineering Applications , vol. 6, no. 3, pp. 031014 - 031014, 2014. Publisher's VersionAbstract
An analytical transport/reaction model was developed to simulate the catalytic performance of ZnO nanowires as a catalyst support. ZnO nanowires were chosen because they have easily characterized, controllable features and a spatially uniform morphology. The analytical model couples convection in the catalyst flow channel with reaction and diffusion in the porous substrate material; it was developed to show that a simple analytical model with physics-based mass transport and empirical kinetics can be used to capture the essential physics involved in catalytic conversion of hydrocarbons. The model was effective at predicting species conversion efficiency over a range of temperature and flow rate. The model clarifies the relationship between advection, bulk diffusion, pore diffusion, and kinetics. The model was used to optimize the geometry of the experimental catalyst for which it predicted that maximum species conversion density for fixed catalyst surface occurred at a channel height of 520 μm.
C. - C. Chen, Li, Z., Shi, L., and Cronin, S. B., “Thermal interface conductance across a graphene/hexagonal boron nitride heterojunction,” Applied Physics Letters, vol. 104, pp. 081908, 2014. Publisher's Version
S. Wen, Fleming, E., Shi, L., and da Silva, A. K., “Numerical Optimization and Power Output Control of a Hot Thermal Battery with Phase Change Material,” Numerical Heat Transfer, Part A: Applications, vol. 65, pp. 825-843, 2014. Publisher's VersionAbstract
Numerical simulations were conducted to investigate the release of heat from a thermal storage unit, which we refer to as a hot thermal battery. The battery is composed of a hexagonal arrangement of parallel tubes through which a heat absorbing fluid flows, surrounded by phase change material (PCM) that fills spaces between adjacent tubes. The simulations implemented, aimed to optimize the battery such that it meets a total volume constraint while ensuring a critical power output before the phase change fronts of the PCM surrounding two adjacent heat transfer tubes merge—indicating the PCM is completely solidified—after which, only sensible heat can be released by the battery. It was found that the PCM latent heat has negligible impact on the optimal heat exchanger (HEx) design. In comparison, increasing either the flow velocity of the heat transfer fluid in the tubes or PCM thermal conductivity can significantly reduce the needed volume of heat exchanger. Additionally, a novel closed loop control modeling approach is proposed to dynamically tune the heat transfer fluid flow rate such that the thermal battery yields a constant power output. The flow tuning results indicate the optimal dynamic HTF velocity curve shape, obtained from closed-loop method, is unique and this optimal flow velocity is dependent on the location of the phase change front. Numerical results were also compared against hot battery discharge experiments, using both constant and dynamically tuned flow rates, indicating a good agreement for both cases.
D. G. Cahill, Braun, P. V., Chen, G., Fan, S. H., Goodson, K. E., Keblinski, P., King, W. P., Mahan, G. D., Majumdar, A., Maris, H. J., Phillpot, S. R., Pop, E., and Shi, L., “Nanoscale Thermal Transport II: 2003-2012,” Applied Physics Reviews, vol. 1, pp. 011305, 2014. LinkAbstract
A diverse spectrum of technology drivers such as improved thermal barriers, higher efficiency thermoelectric energy conversion, phase-change memory, heat-assisted magnetic recording, thermal management of nanoscale electronics, and nanoparticles for thermal medical therapies are motivating studies of the applied physics of thermal transport at the nanoscale. This review emphasizes developments in experiment, theory, and computation in the past ten years and summarizes the present status of the field. Interfaces become increasingly important on small length scales. Research during the past decade has extended studies of interfaces between simple metals and inorganic crystals to interfaces with molecular materials and liquids with systematic control of interface chemistry and physics. At separations on the order of , the science of radiative transport through nanoscale gaps overlaps with thermal conduction by the coupling of electronic and vibrational excitations across weakly bonded or rough interfaces between materials. Major advances in the physics of phonons include first principles calculation of the phonon lifetimes of simple crystals and application of the predicted scattering rates in parameter-free calculations of the thermal conductivity. Progress in the control of thermal transport at the nanoscale is critical to continued advances in the density of information that can be stored in phase change memory devices and new generations of magnetic storage that will use highly localized heat sources to reduce the coercivity of magnetic media. Ultralow thermal conductivity—thermal conductivity below the conventionally predicted minimum thermal conductivity—has been observed in nanolaminates and disordered crystals with strong anisotropy. Advances in metrology by time-domain thermoreflectance have made measurements of the thermal conductivity of a thin layer with micron-scale spatial resolution relatively routine. Scanning thermal microscopy and thermal analysis using proximal probes has achieved spatial resolution of 10 nm, temperature precision of 50 mK, sensitivity to heat flows of 10 pW, and the capability for thermal analysis of sub-femtogram samples.
H. X. Ji, Sellan, D. P., Pettes, M. T., Kong, X. H., Ji, J. Y., Shi, L., and Ruoff, R. S., “Enhanced Thermal Conductivity of Phase Change Materials with Ultrathin-Graphite Foams for Thermal Energy Storage,” Energy & Environmental Science, vol. 7, pp. 1185–1192, 2014. LinkAbstract
For thermophysical energy storage with phase change materials (PCMs), the power capacity is often limited by the low PCM thermal conductivity (κPCM). Though dispersing high-thermal conductivity nanotubes and graphene flakes increases κPCM, the enhancement is limited by interface thermal resistance between the nanofillers, among other factors such as detrimental surface scattering of phonons. Here, we demonstrate that embedding continuous ultrathin-graphite foams (UGFs) with volume fractions as low as 0.8–1.2 vol% in a PCM can increase κPCM by up to 18 times, with negligible change in the PCM melting temperature or mass specific heat of fusion. The increase in κPCM, thermal cycling stability, and applicability to a diverse range of PCMs suggests that UGF composites are a promising route to achieving the high power capacity targets of a number of thermal storage applications, including building and vehicle heating and cooling, solar thermal harvesting, and thermal management of electrochemical energy storage and electronic devices.
M. T. Pettes and Shi, L., “A Reexamination of Phonon Transport through a Nanoscale Point Contact in Vacuum,” Journal of Heat Transfer, vol. 136, no. 3, pp. 032401, 2014. LinkAbstract
Using a silicon nitride cantilever with an integral silicon tip and a microfabricated platinum–carbon resistance thermometer located close to the tip, a method is developed to concurrently measure both the heat transfer through and adhesion energy of a nanoscale point contact formed between the sharp silicon tip and a silicon substrate in an ultrahigh vacuum atomic force microscope at near room temperature. Several models are used to evaluate the contact area critical for interpreting the interfacial resistance. Near field-thermal radiation conductance was found to be negligible compared to the measured interface thermal conductance determined based on the possible contact area range. If the largest possible contact area is assumed, the obtained thermal interface contact resistance can be explained by a nanoconstriction model that allows the transmission of phonons from the whole Brillouin zone of bulk Si with an average finite transmissivity larger than 0.125. In addition, an examination of the quantum thermal conductance expression suggests the inaccuracy of such a model for explaining measurement results obtained at above room temperature.
2013
B. A. Cola, Daiguji, H., Dames, C., Fang, N., Fushinobu, K., Inoue, S., Kikugawa, G., Kohno, M., Kumar, S., Li, D. Y., Lukes, J. R., Malen, J. A., McGaughey, A. J. H., Nakabeppu, O., Pipe, K., Reddy, P., Shen, S., Shi, L., Shibahara, M., Taguchi, Y., Takahashi, K., Yamamoto, T., and Zolotoukhina, T., “Report on the Seventh U.S. –Japan Joint Seminar on Nanoscale Transport Phenomena — Science and Engineering,” Nanoscale and Microscale Thermophysical Engineering , vol. 17, pp. 25-49, 2013. LinkAbstract
The seventh U.S.–Japan Joint Seminar on Nanoscale Transport Phenomena was held in Shima, Japan, from December 11 to 14, 2011. The goals of this joint seminar were to provide a critical assessment of the state of the art and future directions in the field of nanoscale transport phenomena and energy conversion processes, to foster U.S.–Japan collaborations, and to provide international exposure to a new generation of scientists in this field. Issues discussed in the joint seminar were organized in 10 topical sessions, including (1) nanoscale thermophysical measurements; (2) optical characterization; (3) thermal and molecular transport; (4) phonon transport modeling; (5) energy storage and conversion; (6) nanoscale fluidics and phase change phenomena; (7) biological and organic systems; (8) interfacial thermal transport; (9) novel thermoelectric and thermal management materials; and (10) nanocarbon materials and devices. In addition to these topical sessions, the joint seminar featured an opening plenary session and a closing plenary session as well as an expert panel, where leading experts provided critical assessment of the past progress and addressed future directions in the field. In addition, an evening poster session provided opportunities for graduate and postdoc students to present their latest research results. About 35 researchers from Japan and 31 researchers from the United States participated in the meeting. The meeting was organized by S. Maruyama, K. Fushinobu, L. Shi, and J. Lukes together with about 20 other participants who served as session chairs. Summaries of different sessions of the seminar were prepared by the session and conference chairs and are collected into this report.
D. R. Birt, An, K. M., Weathers, A., Shi, L., Tsoi, M., and Li, X. Q., “"Brillouin Light Scattering Spectra as Local Temperature Sensors for Thermal Magnons and Acoustic Phonons,” Appl. Phys. Lett., vol. 102, pp. 082401, 2013. LinkAbstract
We demonstrate the use of the micro-Brillouin light scattering (micro-BLS) technique as a local temperature sensor for magnons in a permalloy (Py) thin film and phonons in the glass substrate. When the Py film is uniformly heated, we observe a systematic shift in the frequencies of two thermally excited perpendicular standing spin wave modes. Fitting the temperature dependent magnon spectra allows us to achieve a temperature resolution better than 2.5 K. In addition, we demonstrate that the micro-BLS spectra can be used to measure the local temperature of magnons and the relative temperature shift of phonons across a thermal gradient. Such local temperature sensors are useful for investigating spin caloritronic and thermal transport phenomena in general.

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