Feng-Chun Hsia
Research Subjects
Feng-Chun Hsia has a total of 72 co-authors. Here are the top co-authors by number of shared publications:
- Dai-Ming Tang
Research Center for Materials Nanoarchitectonics, National Institute for Materials Science, 1-1 Namiki, Tsukuba, Ibaraki 305-0044, Japan
5 shared publications - Dmitri Golberg
ARC Research Hub in Zero‐emission Power Generation for Carbon Neutrality, Centre for Materials Science, and School of Chemistry and Physics Queensland University of Technology Brisbane Queensland Australia
5 shared publications Daniel Bonn
Van der Waals-Zeeman Institute, Institute of Physics, University of Amsterdam, Science Park 904, 1098 XH Amsterdam, Netherlands
4 shared publications- Masanori Mitome
National Institute for Materials Science, Tsukuba, Japan
4 shared publications - Xin Zhou
Friedrich-Alexander-Universität Erlangen-Nürnberg, Institute of Micro- and Nanostructure Research (IMN) and Center for Nanoanalysis and Electron Microscopy (CENEM), Cauerstr. 3, 91058 Erlangen, Germany
4 shared publications - Yoshio Bando
AIIM Building Innovation Campus, University of Wollongong
4 shared publications
Latest Publications
- 16 December 2022
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 129 (25) , 256101
Nonmonotonic Friction due to Water Capillary Adhesion and Hydrogen Bonding at Multiasperity Interfaces
Capillary adhesion due to water adsorption from the air can contribute to friction, especially for smooth interfaces in humid environments. We show that for multiasperity (naturally oxidized) Si-on-Si interfaces, the friction coefficient goes through a maximum as a function of relative humidity. An adhesion model based on the boundary element method that takes the roughness of the interfaces into account reproduces this nonmonotonic behavior very well. Remarkably, we find the dry friction to be significantly lower than the lubricated friction with macroscopic amounts of water present. The difference is attributed to the hydrogen-bonding network across the interface. Accordingly, the lubricated friction increases significantly if the water is replaced by heavy water () with stronger hydrogen bonding.- 16 December 2022
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 129 (25) , 256101
Nonmonotonic Friction due to Water Capillary Adhesion and Hydrogen Bonding at Multiasperity Interfaces
Capillary adhesion due to water adsorption from the air can contribute to friction, especially for smooth interfaces in humid environments. We show that for multiasperity (naturally oxidized) Si-on-Si interfaces, the friction coefficient goes through a maximum as a function of relative humidity. An adhesion model based on the boundary element method that takes the roughness of the interfaces into account reproduces this nonmonotonic behavior very well. Remarkably, we find the dry friction to be significantly lower than the lubricated friction with macroscopic amounts of water present. The difference is attributed to the hydrogen-bonding network across the interface. Accordingly, the lubricated friction increases significantly if the water is replaced by heavy water () with stronger hydrogen bonding.- Open Access
- 11 March 2022
- Published by American Physical Society (APS) in Physical Review Applied
- Vol. 17 (3) , 034034
Contribution of Capillary Adhesion to Friction at Macroscopic Solid–Solid Interfaces
Capillary adhesion is commonly present in ambient conditions. It can be measured in single-asperity contacts through atomic force microscopy using a sharp probe that is pulled off a smooth substrate. However, for macroscopic multiasperity interfaces, the measured adhesive force is always close to zero because of the elastic energy stored into the deformation of surface roughness; this is known as the adhesion paradox. Here, we experimentally show how capillary adhesion influences friction between macroscopic -on- interfaces, covered with native oxide, in two vapor environments: humid air and isopropyl alcohol (IPA) vapor. To quantify the adhesion contribution to friction, we present a boundary element method that successfully models the interplay between capillary adhesion, surface topography, and friction without adjustable parameters and show that the evolution of the surface topography during sliding dramatically increases capillary adhesion and thus friction. Replacing the water vapor with an organic (IPA) vapor, we find a lower adhesion due to the smaller surface tension.- 11 March 2022
- Published by American Physical Society (APS) in Physical Review Applied
- Vol. 17 (3) , 034034
Open AccessContribution of Capillary Adhesion to Friction at Macroscopic Solid–Solid Interfaces
Capillary adhesion is commonly present in ambient conditions. It can be measured in single-asperity contacts through atomic force microscopy using a sharp probe that is pulled off a smooth substrate. However, for macroscopic multiasperity interfaces, the measured adhesive force is always close to zero because of the elastic energy stored into the deformation of surface roughness; this is known as the adhesion paradox. Here, we experimentally show how capillary adhesion influences friction between macroscopic -on- interfaces, covered with native oxide, in two vapor environments: humid air and isopropyl alcohol (IPA) vapor. To quantify the adhesion contribution to friction, we present a boundary element method that successfully models the interplay between capillary adhesion, surface topography, and friction without adjustable parameters and show that the evolution of the surface topography during sliding dramatically increases capillary adhesion and thus friction. Replacing the water vapor with an organic (IPA) vapor, we find a lower adhesion due to the smaller surface tension. - 24 December 2021
- Published by American Association for the Advancement of Science (AAAS) in Science
- Vol. 374 (6575) , 1616-1620
Semiconductor nanochannels in metallic carbon nanotubes by thermomechanical chirality alteration
Straining to make a transistor: The use of carbon nanotubes (CNTs) as short-channel-length transistors will require control of their chirality, which determines whether they are semiconducting or metallic and if they form strong, low-resistance contacts. Tang et al . fabricated CNT intramolecular transistors by progressive heating and straining of individual CNTs within a transmission electron microscope. Changes to chirality along sections of the nanotube created metallic-to-semiconducting transitions. A semiconducting nanotube channel was covalently bonded to the metallic nanotube source and drain regions. The resulting CNT intramolecular transistors had channel lengths as short as 2.8 nanometers. —PDS
- 24 December 2021
- Published by American Association for the Advancement of Science (AAAS) in Science
- Vol. 374 (6575) , 1616-1620
Semiconductor nanochannels in metallic carbon nanotubes by thermomechanical chirality alteration
Straining to make a transistor: The use of carbon nanotubes (CNTs) as short-channel-length transistors will require control of their chirality, which determines whether they are semiconducting or metallic and if they form strong, low-resistance contacts. Tang et al . fabricated CNT intramolecular transistors by progressive heating and straining of individual CNTs within a transmission electron microscope. Changes to chirality along sections of the nanotube created metallic-to-semiconducting transitions. A semiconducting nanotube channel was covalently bonded to the metallic nanotube source and drain regions. The resulting CNT intramolecular transistors had channel lengths as short as 2.8 nanometers. —PDS
- Open Access
- 21 December 2021
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 3 (4) , 043204
Rougher is more slippery: How adhesive friction decreases with increasing surface roughness due to the suppression of capillary adhesion
Friction originates at the area of real contact which depends on the (changing) surface topography. Observing and measuring the area of real contact at multi-asperity interfaces is difficult, making it challenging to quantitatively study the interplay between the frictional force and surface topography. In this paper, we systematically manipulate surface topography and use a fluorescence microscopy-based contact visualization technique to reveal this interplay. We demonstrate good agreement between elastoplastic boundary element method contact calculations and experimental visualization of the area of real contact. While the area of real contact and thus contact pressure could be varied by a factor of 4 through control of the surface topography, this had only a modest effect on the coefficient of friction (CoF). We do find a small but systematic increase in the proportionality constant between frictional force and normal force (CoF) with decreasing surface roughness. The observation that smoother surfaces have a greater CoF is due to capillary adhesion between the two surfaces. We quantitatively model this behavior using a simple capillary adhesion model without adjustable parameters. Our results provide quantitative insights into the interplay between contact mechanics, friction, and capillary adhesion. A predictive understanding of this interplay is essential to demanding applications such as precision positioning.
- 21 December 2021
- Published by American Physical Society (APS) in Physical Review Research
- Vol. 3 (4) , 043204
Open AccessRougher is more slippery: How adhesive friction decreases with increasing surface roughness due to the suppression of capillary adhesion
Friction originates at the area of real contact which depends on the (changing) surface topography. Observing and measuring the area of real contact at multi-asperity interfaces is difficult, making it challenging to quantitatively study the interplay between the frictional force and surface topography. In this paper, we systematically manipulate surface topography and use a fluorescence microscopy-based contact visualization technique to reveal this interplay. We demonstrate good agreement between elastoplastic boundary element method contact calculations and experimental visualization of the area of real contact. While the area of real contact and thus contact pressure could be varied by a factor of 4 through control of the surface topography, this had only a modest effect on the coefficient of friction (CoF). We do find a small but systematic increase in the proportionality constant between frictional force and normal force (CoF) with decreasing surface roughness. The observation that smoother surfaces have a greater CoF is due to capillary adhesion between the two surfaces. We quantitatively model this behavior using a simple capillary adhesion model without adjustable parameters. Our results provide quantitative insights into the interplay between contact mechanics, friction, and capillary adhesion. A predictive understanding of this interplay is essential to demanding applications such as precision positioning.
- Open Access
- 8 February 2021
- Published by American Physical Society (APS) in Physical Review X
- Vol. 11 (1) , 011025
Friction on Ice: How Temperature, Pressure, and Speed Control the Slipperiness of Ice
We present sphere-on-ice friction experiments as a function of temperature, contact pressure, and speed. At temperatures well below the melting point, friction is strongly temperature dependent and follows an Arrhenius behavior, which we interpret as resulting from the thermally activated diffusive motion of surface ice molecules. We find that this motion is hindered when the contact pressure is increased; in this case, the friction increases exponentially, and the slipperiness of the ice disappears. Close to the melting point, the ice surface is plastically deformed due to the pressure exerted by the slider, a process depending on the slider geometry and penetration hardness of the ice. The ice penetration hardness is shown to increase approximately linearly with decreasing temperature and sublinearly with indentation speed. We show that the latter results in a nonmonotonic dependence of the ploughing force on sliding speed. Our results thus clarify the complex dependence of ice friction on temperature, contact pressure, and speed.
- 8 February 2021
- Published by American Physical Society (APS) in Physical Review X
- Vol. 11 (1) , 011025
Open AccessFriction on Ice: How Temperature, Pressure, and Speed Control the Slipperiness of Ice
We present sphere-on-ice friction experiments as a function of temperature, contact pressure, and speed. At temperatures well below the melting point, friction is strongly temperature dependent and follows an Arrhenius behavior, which we interpret as resulting from the thermally activated diffusive motion of surface ice molecules. We find that this motion is hindered when the contact pressure is increased; in this case, the friction increases exponentially, and the slipperiness of the ice disappears. Close to the melting point, the ice surface is plastically deformed due to the pressure exerted by the slider, a process depending on the slider geometry and penetration hardness of the ice. The ice penetration hardness is shown to increase approximately linearly with decreasing temperature and sublinearly with indentation speed. We show that the latter results in a nonmonotonic dependence of the ploughing force on sliding speed. Our results thus clarify the complex dependence of ice friction on temperature, contact pressure, and speed.
- Open Access
- 1 February 2020
- Published by Elsevier in Tribology International
- Vol. 142
Wear particle dynamics drive the difference between repeated and non-repeated reciprocated sliding
- 1 February 2020
- Published by Elsevier in Tribology International
- Vol. 142
Open AccessWear particle dynamics drive the difference between repeated and non-repeated reciprocated sliding
- Open Access
- 26 February 2019
- Published by Royal Society of Chemistry (RSC) in Nanoscale Advances
- Vol. 1 (5) , 1784-1790
Realization and direct observation of five normal and parametric modes in silicon nanowire resonators by in situ transmission electron microscopy
In situ TEM observation of the 5th order normal and parametric resonances for precise evaluation of Si NWs' elastic moduli.
- 26 February 2019
- Published by Royal Society of Chemistry (RSC) in Nanoscale Advances
- Vol. 1 (5) , 1784-1790
Open AccessRealization and direct observation of five normal and parametric modes in silicon nanowire resonators by in situ transmission electron microscopy
In situ TEM observation of the 5th order normal and parametric resonances for precise evaluation of Si NWs' elastic moduli.
- 30 November 2018
- Published by Wiley in Physica Status Solidi (RRL) – Rapid Research Letters
- Vol. 13 (3)
Tunable Mechanical and Electrical Properties of Coaxial BN‐C Nanotubes
Heterostructures provide a great chance to tune the properties and functions of a nanomaterial, e.g., its mechanical and electrical properties, and thus allowing for the design and realization of novel nanoelectromechanical devices. Boron nitride and carbon nanotubes, with similar structure and mechanical properties but dramatically different electrical properties, are ideal candidates for investigating nanoscale heterostructured materials. In this work, graphitic C‐coated BN nanotubes (BN‐C NTs) were synthesized and their mechanical and electrical properties were simultaneously measured using in situ high‐resolution transmission electron microscopy (TEM). As a function of the coated carbon content, the elastic modulus obtained from second order harmonic resonance of heterostructured nanotubes could be tuned from ∼140 to ∼700 GPa, and their electrical resistivity could be adjusted within three orders of magnitude from ∼0.16 to ∼2.5×10−4 Ω · m. This work opens the way for making custom‐designed heterostructures for the requirements of specific applications.
- 30 November 2018
- Published by Wiley in Physica Status Solidi (RRL) – Rapid Research Letters
- Vol. 13 (3)
Tunable Mechanical and Electrical Properties of Coaxial BN‐C Nanotubes
Heterostructures provide a great chance to tune the properties and functions of a nanomaterial, e.g., its mechanical and electrical properties, and thus allowing for the design and realization of novel nanoelectromechanical devices. Boron nitride and carbon nanotubes, with similar structure and mechanical properties but dramatically different electrical properties, are ideal candidates for investigating nanoscale heterostructured materials. In this work, graphitic C‐coated BN nanotubes (BN‐C NTs) were synthesized and their mechanical and electrical properties were simultaneously measured using in situ high‐resolution transmission electron microscopy (TEM). As a function of the coated carbon content, the elastic modulus obtained from second order harmonic resonance of heterostructured nanotubes could be tuned from ∼140 to ∼700 GPa, and their electrical resistivity could be adjusted within three orders of magnitude from ∼0.16 to ∼2.5×10−4 Ω · m. This work opens the way for making custom‐designed heterostructures for the requirements of specific applications.
- 1 November 2018
- Published by Elsevier in Ultramicroscopy
- Vol. 194, 108-116
Chirality transitions and transport properties of individual few-walled carbon nanotubes as revealed by in situ TEM probing
- 1 November 2018
- Published by Elsevier in Ultramicroscopy
- Vol. 194, 108-116
Chirality transitions and transport properties of individual few-walled carbon nanotubes as revealed by in situ TEM probing
- Open Access
- 14 February 2018
- Published by Springer Nature in Scientific Reports
- Vol. 8 (1) , 1-10
Mesoscopic physical removal of material using sliding nano-diamond contacts
Wear mechanisms including fracture and plastic deformation at the nanoscale are central to understand sliding contacts. Recently, the combination of tip-induced material erosion with the sensing capability of secondary imaging modes of AFM, has enabled a slice-and-view tomographic technique named AFM tomography or Scalpel SPM. However, the elusive laws governing nanoscale wear and the large quantity of atoms involved in the tip-sample contact, require a dedicated mesoscale description to understand and model the tip-induced material removal. Here, we study nanosized sliding contacts made of diamond in the regime whereby thousands of nm3 are removed. We explore the fundamentals of high-pressure tip-induced material removal for various materials. Changes in the load force are systematically combined with AFM and SEM to increase the understanding and the process controllability. The nonlinear variation of the removal rate with the load force is interpreted as a combination of two contact regimes each dominating in a particular force range. By using the gradual transition between the two regimes, (1) the experimental rate of material eroded on each tip passage is modeled, (2) a controllable removal rate below 5 nm/scan for all the materials is demonstrated, thus opening to future development of 3D tomographic AFM.
- 14 February 2018
- Published by Springer Nature in Scientific Reports
- Vol. 8 (1) , 1-10
Open AccessMesoscopic physical removal of material using sliding nano-diamond contacts
Wear mechanisms including fracture and plastic deformation at the nanoscale are central to understand sliding contacts. Recently, the combination of tip-induced material erosion with the sensing capability of secondary imaging modes of AFM, has enabled a slice-and-view tomographic technique named AFM tomography or Scalpel SPM. However, the elusive laws governing nanoscale wear and the large quantity of atoms involved in the tip-sample contact, require a dedicated mesoscale description to understand and model the tip-induced material removal. Here, we study nanosized sliding contacts made of diamond in the regime whereby thousands of nm3 are removed. We explore the fundamentals of high-pressure tip-induced material removal for various materials. Changes in the load force are systematically combined with AFM and SEM to increase the understanding and the process controllability. The nonlinear variation of the removal rate with the load force is interpreted as a combination of two contact regimes each dominating in a particular force range. By using the gradual transition between the two regimes, (1) the experimental rate of material eroded on each tip passage is modeled, (2) a controllable removal rate below 5 nm/scan for all the materials is demonstrated, thus opening to future development of 3D tomographic AFM.