TY - JOUR
T1 - Novel Electromechanical Phenomena at the Nanoscale
T2 - Phenomenological Theory and Atomistic Modeling
AU - Tagantsev, Alexander K.
AU - Meunier, Vincent
AU - Sharma, Pradeep
N1 - Funding Information:
Sharma would like to acknowledge fruitful collaborations with his students, Mohamed Sabri Majdoub, Nikhil Sharma, and Ravi Maranganti and Professors Tahir Cagin and Chad Landis. Funding support from the National Science Foundation: Clark Cooper (CMMI 0708096) and Ken Chong (CMMI 0826153) is gratefully acknowledged. Tagantsev acknowledges financial support by the Swiss National Science Foundation. Meunier was sponsored by the Laboratory Directed Research and Development Program of Oak Ridge National Laboratory, managed by UT–Battelle, LLC for the U.S. Depart ment of Energy under Contract No. De–AC05–00OR22725.
PY - 2009/9
Y1 - 2009/9
N2 - In the past two decades, the fact that "small is different" has been established for a wide variety of phenomena, including electrical, optical, magnetic, and mechanical behavior of materials. However, one largely untapped but potentially very Important area of nanoscience involves the interplay of electricity and mechanics at the nanoscale. In this article, predicated on both phenomenological approaches and atomistic calculations, we summarize the state-of-the-art in understanding electromechanical coupling at the nanoscale. First, we address flexoelectricity-the coupling of strain gradient to polarization. Flexoelectricity exists in both piezoelectric and nonpiezoelectric dielectrics. As a high-order spatial-dispersion effect, the flexoelectricity becomes more and more important with the reduction of the spatial scale of the problem. Exploitation of this phenomenon and the associated nanoscale size effects can lead to tantalizing applications, such as "piezoelectric nanocomposites without using piezoelectric materials." The second issue concerns electromechanical effects at the dielectricJmetal interface. An interface in solids typically exhibits a lower symmetry compared to that of the associated adhering materials. This symmetry reduction can drastically affect the electromechanical and dielectric behavior of the material at the nanoscale.
AB - In the past two decades, the fact that "small is different" has been established for a wide variety of phenomena, including electrical, optical, magnetic, and mechanical behavior of materials. However, one largely untapped but potentially very Important area of nanoscience involves the interplay of electricity and mechanics at the nanoscale. In this article, predicated on both phenomenological approaches and atomistic calculations, we summarize the state-of-the-art in understanding electromechanical coupling at the nanoscale. First, we address flexoelectricity-the coupling of strain gradient to polarization. Flexoelectricity exists in both piezoelectric and nonpiezoelectric dielectrics. As a high-order spatial-dispersion effect, the flexoelectricity becomes more and more important with the reduction of the spatial scale of the problem. Exploitation of this phenomenon and the associated nanoscale size effects can lead to tantalizing applications, such as "piezoelectric nanocomposites without using piezoelectric materials." The second issue concerns electromechanical effects at the dielectricJmetal interface. An interface in solids typically exhibits a lower symmetry compared to that of the associated adhering materials. This symmetry reduction can drastically affect the electromechanical and dielectric behavior of the material at the nanoscale.
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U2 - 10.1557/mrs2009.175
DO - 10.1557/mrs2009.175
M3 - Article
AN - SCOPUS:70349656451
SN - 0883-7694
VL - 34
SP - 643
EP - 647
JO - MRS Bulletin
JF - MRS Bulletin
IS - 9
ER -