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  • 1
    Online Resource
    Online Resource
    The Electrochemical Society ; 2018
    In:  ECS Meeting Abstracts Vol. MA2018-03, No. 1 ( 2018-07-13), p. 107-107
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2018-03, No. 1 ( 2018-07-13), p. 107-107
    Abstract: Today, intravascular catheter surgeries, which are kind of minimally invasive procedures, are widely used surgical techniques. As compared to conventional open surgery, incision size is small, and burden on patients is reduce. Therefore, the wounds associated with pain is small, and time to heal is also short. On the other hand, since operative field was restricted during surgery, operators need to have sufficient skill for intravascular catheter surgeries. To obtain it, operators must practice using artificial surgical simulators. Materials for surgical simulators are requires having physical properties as like human organs. Although lab animals have similar physical properties, they are not appropriate from an ethical perspective. Moreover, recently, silicone-based materials are used for surgical simulators, but their physical properties do not mimic those of human organs. Gel materials are expected for materials of surgical simulators, because their mechanical properties are similar to human organs and they contain large amounts of moisture. Besides, gel material can apply for fabrication of the complicate shape of human organs using 3D printer. The issue of practice using conventional surgical simulators is quantitative evaluation of operator skill. In the case of intravascular catheter surgeries, measurement of applied force to vessel wall by catheter and guide wire is an important function. Since vessel walls of patients are delicate, if devices applied excess force, and unexpected accidents such as vascular occlusion are attracted. In this study, we focused on the photoelasticity of gel materials. If vessel models are made of these gel materials, it is possible them to evaluate quantitative score of operator skill. To realize these surgical simulators, we developed the stress measurement system for photoelasticity of gel materials. Besides, we evaluated the physical properties such as mechanical properties and photoelastic coefficient of several gel materials using our developed system. We constructed new stress measurement system for photoelasticity of gel materials Our system consisted of several polarizers and wave plates, and it could measure the value of stress and direction of stress in X-Y plane from RGB values on color map. In order to minimize the overlap ratio of the same color in the color map, two 1 wave plates were insert to conventional observation system of circularly polarized wave and the insertion angle of two 1 wave plates is 30 degrees. We suggested analysis algorithm which enables to eliminate the effects of incident light and ambient light. As the results, we succeed to measure the tensile stress by our system during the tensile test of PVA hydrogel. Measurement error was less than 6.3% at the stress range from 0 to 80 kPa, and it is sufficient measurement resolution for evaluate stress during practice of intravascular catheter surgeries. Generally, Young’s moduli of human vessels depend on the organ and/or symptoms, and they are ranged from 0.02 to 3 MPa. Although mechanical properties of gel material can be adjusted by changing kinds of formulas and their concentrations, it is difficult that only one type gel coverall the range of Young’s moduli of human vessels. Therefore, the materials of surgical simulators are selected on demand from patient of case history. Finally, we investigated the Young’s moduli and photoelastic coefficients of two types of designable gels such as inter cross-linking network gels and double networks gels. As the results, two type gels exhibited photoelasticity. Young’s moduli of inter cross-linking network gels are approximately 1 MPa and the effect of formula concentration was slightly. On the other hand, the range of Young’s modulus of double networks gels was 0.12 to 0.77 MPa for strain range from 0 to 15%, and it was within the range of Young’s modulus of human vessels. Their photoelastic coefficients were 0.012 to 0.022 ×10 -9 Pa -1 . The measurement error of our system was 7.3%, and was acceptable.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2018
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  • 2
    Online Resource
    Online Resource
    The Electrochemical Society ; 2018
    In:  ECS Meeting Abstracts Vol. MA2018-03, No. 1 ( 2018-07-13), p. 30-30
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2018-03, No. 1 ( 2018-07-13), p. 30-30
    Abstract: Catheterization procedure is a typical example of minimally invasive medical treatment. This has the advantage that the physical burden on the patient can be remarkably reduced as compared with the conventional medical treatment method involving craniotomy or hemorrhage etc. However, on the other hand, since visual and tactile restrictions are limited at the time of surgery, physicians are required to have expert skill and many experiences. To raise the success rate of surgery irrespective of the amount of surgical experience, we have conducted a simple model using a glass tube and a simulation operation using an experimental animal, but they have low bio-reproducibility and ethical problems was there. In recent years, due to the development of new materials and the appearance of 3D printers, shape reproducibility has improved. A more desirable function of the surgical simulator is to visualize the force applied to the vessel wall surface by the catheter. This is because there is a danger of attracting vascular occlusion etc. when a large force is applied to the wall surface of the blood vessel. Therefore, it is considered important to quantitatively evaluate the operational feeling for simulated surgery. Therefore, we aim to manufacture a vascular surgical simulator with high bio-reproducibility that enables real-time stress measurement. In this research, stress visualization method using photoelastic effect is applied to surgical simulator. By using the photoelastic effect, it becomes possible to check the stress state of the entire field of view, and it is possible to obtain a stress state when a medical instrument such as a coil or a stent is inserted. Therefore, it is useful not only for training but also for the development of medical instruments. Heretofore, examples using PDMS and polyurethane elastomer as a surgical simulator material have been reported, but the longitudinal modulus of elasticity is high and it is unsuitable for a blood vessel model. Therefore, we focused on PVA hydrogel as surgical simulator material. PVA (polyvinyl alcohol) hydrogel is a material that can be expected to reproduce vascular tissue because its physical properties can be easily changed by changing the compounding ratio and degree of polymerization of powdered PVA. By changing the compounding ratio of powdered PVA in the range of 4-15 wt.%, We realized PVA hydrogel's longitudinal elastic modulus of 60-450 kPa. Since the longitudinal elastic modulus of human vascular tissue is 20-3000 kPa, PVA hydrogel is useful for reproducing soft vascular tissue. Further, the average photoelastic coefficient of PVA hydrogel is 2.30 × 10 -9 Pa -1 , which has a photoelastic coefficient greater than that of polyurethane elastomer which is a photoelastic material useful for photoelastic stress measurement. (photoelastic coefficient of polyurethane elastomer is 1.45 × 10 -9 Pa -1 .) Therefore, it was confirmed that it is a useful material for stress measurement using photoelastic effect. In this study, a simple blood vessel model was prepared using PVA hydrogel and simulated surgery using a catheter was performed. In addition, a photoelastic observation system was constructed for stress measurement, and a method for correcting the influence due to the presence of incident light, ambient light, and initial stress was examined. As a result, we successfully extracted and visualized the stress applied to the simple blood vessel model.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2018
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  • 3
    Online Resource
    Online Resource
    The Electrochemical Society ; 2010
    In:  ECS Transactions Vol. 33, No. 6 ( 2010-10-01), p. 661-667
    In: ECS Transactions, The Electrochemical Society, Vol. 33, No. 6 ( 2010-10-01), p. 661-667
    Abstract: One-dimensionally aligned Si quantum dots (Si-QDs) on ultrathin SiO2 have been prepared by controlling the selective growth conditions of low-pressure chemical vapor deposition (LPCVD) using pure SiH4 or 5% GeH4 diluted with He, the oxidation of the dots and the selective etching. Atomic force microscopy (AFM) observations and X-ray photoelectron spectroscopy (XPS) measurements confirm the selective etching of Ge oxide on pre-grown Si-QDs by annealing under vacuum condition and the subsequent selective growth of 2nd Si-QDs on the 1st Si-QDs. The temporal change in surface potential of the self-aligned Si-QDs after one electron injection from the tip to the dots changed in a stepwise manner with time due to electron transfer from the 2nd-dot to the 1st-dot. For the semitransparent Au-gate diodes, when carriers were injected to self-aligned Si-QDs from n-Si(100) substrate for electrons and from Au top electrode for holes, electroluminescence (EL) in the near-infrared region at room temperature becomes observable with an increase in the current at positive gate biases over the thresholds. It should be noted that the self-aligned Si-QDs enhance the emission intensity by a factor of ~2 compared with Si-QDs stacked structure under the same current density. This result indicates that self-aligned structure is suitable for an increase in recombination efficiency for EL.
    Type of Medium: Online Resource
    ISSN: 1938-5862 , 1938-6737
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2010
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  • 4
    Online Resource
    Online Resource
    The Electrochemical Society ; 2013
    In:  ECS Transactions Vol. 58, No. 9 ( 2013-08-31), p. 231-237
    In: ECS Transactions, The Electrochemical Society, Vol. 58, No. 9 ( 2013-08-31), p. 231-237
    Abstract: We have designed and fabricated hybrid nanodots structures, in which Si quantum dots (QDs) and either Ni-silicide or Pt-silicide nanodots (NDs) are stacked with ultrathin SiO 2 interlayer, as a novel functional floating gate (FG) to satisfy both multiple valued capability and large capacity on charge storage. Multiple-step charge injection to sililcide NDs through discrete energy states in Si-QDs and stable storage of many charges in deep potential wells in silicide NDs have been confirmed from electrical characteristics of MOS capacitors and transistors measured at room temperature. A unique optical response of the hybrid NDs FG to near-infrared light irradiation, which is caused by the transfer of photo-excited electrons from silicide NDs to Si-QDs, has also been demonstrated.
    Type of Medium: Online Resource
    ISSN: 1938-5862 , 1938-6737
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2013
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  • 5
    Online Resource
    Online Resource
    The Electrochemical Society ; 2014
    In:  ECS Meeting Abstracts Vol. MA2014-02, No. 35 ( 2014-08-05), p. 1850-1850
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2014-02, No. 35 ( 2014-08-05), p. 1850-1850
    Abstract: Nanometer-scale silicon structures have been attracted much attention because their novel functionalities such as multiple-valued charge storage [1], single-electron transfer [2] , electroluminescence (EL) [3], and electron emission [4] . Recently, we have succeeded in stacking Si quantum dots (Si-QDs) self-aligned by a selective growth technique focusing on the 2nd formation of Si-QDs on pre-grown Si-QDs [3], and demonstrated stable near-infrared EL from the self-aligned Si-QDs in a diode structure with semitransparent Au top electrode and n-Si(100) substrate under forward bias conditions over a threshold voltage as low as +1.2 V [3] . In this work, to get an insight into ballistical electron transport through self-aligned Si-QDs, we extended our research work to the spatially-resolved characterization of electron emission from self-aligned Si-QDs formed on ultrathin SiO 2 /n-Si(100) by using a conductive cantilever. Self-aligned Si-QDs with an areal density as high as ~10 11 cm -2 were fabricated on ~1.0nm-thick SiO 2 by process steps consisting of the first formation of Si-QDs by controlling low-pressure chemical vapor deposition (LPCVD) using pure SiH 4 , selective Ge-LPCVD from GeH 4 diluted with He, in-situ surface oxidation of the dots, thermal desorption of Ge oxide and subsequent 2nd formation of the Si-QDs. After the slight oxidation of the dot surface and boundaries between the 1st and the 2nd formed Si-QDs at 850°C, semitransparent Au top electrodes and the Al back contact to n-Si(100) were formed by thermal evaporation. The self-aligned formation of the Si-QDs with an areal as high as ~10 11 cm -2 and an average size of ~20 nm in diameter was confirmed by comparing topographic images taken just after the 1st Si-QDs formation and the 2nd one. TEM images also confirm the formation of ~1nm-thick oxide layer in-between self-aligned Si-QDs after the slight oxidation. In spatially-resolved characterization of electron emission from the align-dots through the Au top electrodes, current images were taken by using AFM in a non-contact mode keeping a distance of ~200nm from the sample surface by using a Au-coated Si cantilever with DC negative bias application to the Al back contact with respect to the grounded Au top electrode at room temperature in the atmosphere. With DC bias application over -7V, non-uniform image contrast due to electron emission from localized area being almost the same size of Si-QDs, emerged and was enhanced exponentially with an increase in the applied bias. From Fowler-Nordheim (FN) plots of observed field emission with an estimation of the potential drop in the topmost oxide on the self-aligned Si-QD, the emission current is likely to be limited by FN tunneling (Fig. 1). Considering the work function difference between n-Si(100) and Au-top electrode, the quantized energy states of the aligned dots can be placed at energies higher than the vacuum level of the top electrode when the DC biases over -7 V is applied as shown in the inset of Fig. 1. In tunneling from bottom to top dots, electrons can gain their kinetic energies efficiently as a result of reduced inelastic scattering.. Therefore, the observed electron emission is likely to be promoted by quasi-ballistic transport through aligned-dots structure. Acknowledgements This work was supported in part by Grant-in Aids for Scientific Research (A) No. 24246054 and Young Scientists (A) No. 25709023 from the Ministry of Education, Culture, Sports, Science and Technology, Japan and by JSPS Core-to-Core Program of International Collaborative Research Center on Atomically Controlled Processing for Ultralarge Scale Integration. In addition, the author deeply appreciates that the samples were fabricated successfully by utilizing the clean room facilities of Hiroshima Univ. References [1] M. Ikeda, Y. Shimizu, H. Murakami and S. Miyazaki, Jpn. J. Appl. Phys. 42 4134 (2003). [2] J. Ogi, Y. Tsuchiya, S. Oda and H. Mizuta, Microelectron. Eng., 85 1410 (2008). [3] K. Makihara, M. Ikeda, H. Deki, A. Ohta and S. Miyazaki, ECS Trans., 33 661. (2010). [4] J. Xu, J. Zhou, Y. Yao, Z. Cen, F. Song, L. Xu, J. Wan and K. Chen, Solid State Commun. 145 443 (2008).
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2014
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  • 6
    Online Resource
    Online Resource
    The Electrochemical Society ; 2012
    In:  ECS Meeting Abstracts Vol. MA2012-02, No. 43 ( 2012-06-04), p. 3154-3154
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2012-02, No. 43 ( 2012-06-04), p. 3154-3154
    Abstract: Abstract not Available.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2012
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  • 7
    Online Resource
    Online Resource
    The Electrochemical Society ; 2016
    In:  ECS Meeting Abstracts Vol. MA2016-02, No. 30 ( 2016-09-01), p. 2039-2039
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2016-02, No. 30 ( 2016-09-01), p. 2039-2039
    Abstract:  The achievement of intense light emission at room temperature from group-IV materials is a crucial step toward the accomplishment of fully-Si-based optoelectronics. Recently, Ge-nanostructures on Si or embedded in Si have been also studied to realize well-defined three-dimensional hole confinement in Ge-QDs with keeping electron transport efficiency, which can enhance carrier recombination efficiency [4-7]. In our previous paper, we have reported on the formation of Si quantum dots (Si-QDs) with Ge core with an areal density as high as ~10 11 cm -2 and their photoluminescence (PL) properties [8, 9]. We also demonstrated that, in this system, room temperature PL was promoted by hole confinement in Ge core reflecting the type II energy band discontinuity between Si clad and Ge core. In this work, we extended our research work to evaluate impact of Ge-core size on their PL characteristics.  After conventional wet-chemical cleaning steps, ~2.0 nm-thick SiO2 was grown on p-Si(100) by dry O2 oxidation at 850°C. The SiO2 surface was shortly dipped into a 0.1% HF solution to etch back the SiO2 and to obtain uniform surface termination with OH bonds. Subsequently, hemispherical Si-QDs with an areal dot density of ~10 11 cm -2 were formed from the thermal decomposition of pure SiH4 under 67 Pa at 550˚C. After that, Ge was deposited selectively on the pre-grown Si-QDs at 370°C by using GeH 4 diluted with 5% H 2 where the GeH 4 -LPCVD time was varied in the range from 2.5 to 3 min to control core size. After the Ge core deposition, Si clad was formed in the same chamber at 530ºC by LPCVD using SiH 4 under 2.7 Pa. Finally, the surface of the Si-QDs with Ge core was oxidized at room temperature by a remote VHF plasma of O 2 , which resulted in conformal coverage with a ~2.0 nm-thick SiO2 layer.  AFM images confirm that the areal dot density (~1.0×10 11 cm -2 ) remains unchanged after the Ge deposition regardless of deposition time. This result implies Ge was deposited selectively on the pre-grown Si-QDs. From the size distribution of the dot evaluated from AFM images taken at each process steps, we confirmed that average dot heights were increased by ~2 nm and ~6 nm with GeH 4 -LPCVD for 2.5 min and 3 min, respectively, in comparison to the pre-grown Si-QDs.  The Si-QDs with an average Ge dot size of 6nm shows PL signals peaked at ~0.69 eV at room temperature (Fig. 1). The observed PL peak is likely to be caused by radiative recombination of photogenerated electron-hole pairs through quantized states of the Ge core. It should be noted that, with a decrease in the core size down to ~2nm, PL signal was slightly shifted towered the high energy side by ~80 meV, although no significant change in the PL intensity was observed. This result can be interpreted as a result of increased quantized energy reflecting the size of the Ge core rather than the intermixing of the Si clad and Ge core.  In conclusion, we demonstrated room temperature PL from the Si-QDs with different sized Ge core. The PL from the Si-QDs with Ge core is dominated by the recombination of electron-hole pairs between quantized states of Ge core, and emission wavelength can be changed by controlling the Ge core size. Acknowledgments  This work was supported in part by Grant-in Aid for Scientific Research (S) 15H05762 of MEXT, Japan. References  [1] L. Pavesi et al., Nature 408 (2000) 440.  [2] R. J. Walters et al., Nature Materials 4 (2005) 143.  [3] J. Heitmann et al., Advanced Materials 17 (2005) 795.  [4] W. H. Chang et al., Appl. Phys. Lett. 83 (2003) 2958.  [5] V. G. Talalaev et al., Phys. Status Solidi A 198 (2003) R4.  [6] Y. N. Drozdov et al., Thin Solid Films 517 (2008) 398.  [7] X. Xu et al., J.Cryst. Growth 378 (2013) 636.  [8] Y. Darma et al., Nanotech 14 (2003) 413.  [9] K. Kondo et al., J.Appl. Phys. 119 (2016) 033103. Figure 1
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2016
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  • 8
    Online Resource
    Online Resource
    The Electrochemical Society ; 2007
    In:  ECS Meeting Abstracts Vol. MA2007-02, No. 25 ( 2007-09-28), p. 1276-1276
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2007-02, No. 25 ( 2007-09-28), p. 1276-1276
    Abstract: Abstract not Available.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2007
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  • 9
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2010-01, No. 17 ( 2010-02-05), p. 962-962
    Abstract: Abstract not Available.
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2010
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  • 10
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    Online Resource
    The Electrochemical Society ; 2020
    In:  ECS Meeting Abstracts Vol. MA2020-02, No. 24 ( 2020-11-23), p. 1725-1725
    In: ECS Meeting Abstracts, The Electrochemical Society, Vol. MA2020-02, No. 24 ( 2020-11-23), p. 1725-1725
    Abstract: Introduction 〉 A formation of single crystalline semiconductor such as Silicon on Sapphire substrate has been intensively studied for applying the high frequency devices with low power consumption and high-speed operation. Recently, two-dimensional honeycomb crystals consisted with Si and Ge atoms so called sillicene and germanene have been attracted much attention as a post-graphene material [1,2]. One of the key issues to exhibit their unique electronic properties for device application is the formation of silicone and germanene on the insulating substrate [3] . Therefore, the purpose of this work is to get an insight into the formation of ultra-thin Ge crystal on Sapphire substrate. We have investigated an influence of thermal annealing on the surface morphology and the solid-phase-crystallization of amorphous Ge thin films formed on Sapphire(0001) substrate. Experimental procedure 〉 Surface treatment of Sapphire(0001) substrate was performed by the ultrasonic cleaning with acetone and subsequent annealing at 1000 °C for 5 hours in N 2 ambience to obtain the cleaned flat surface. Then, a Ge thin film with a thickness of 8 nm was deposited by RF magnetron sputtering with a power density of 254 W/cm 2 at Ar pressure of ~0.9 Pa. In some samples, a SiO 2 capping layer with a thickness of ~ 15 nm was formed by ALD using BEDAS gas and O 2 plasma at a substrate temperature of 300ºC. After that, annealing in N 2 ambience at temperatures of 600 °C and 650 °C for 30 minutes were carried out to crystalize the Ge thin films. During the annealing, ramp rate was set at 20 °C/min. The surface morphology and crystallinity of the Ge thin layer for the samples were evaluated by atomic force microscope (AFM) and Raman scattering spectroscopy. Results and discussion 〉 Figure 1 shows the AFM topographic images of the Ge thin film formed on the Sapphire(0001) substrate after the annealing at 650 °C. It was also confirmed that atomically flat surface of Sapphire(0001) with step and terrace structure was obtained by the surface treatment, and the flatness was almost unchanged even after the deposition of Ge thin film and the SiO 2 capping layer (data not shown). For the samples after the annealing at 650 °C, the SiO 2 capping layer was effectively suppressed an increase in the surface roughness due to the Ge (or GeO) desorption and migration, and line shapes originated from the crystalline structure near the surface were partially detected in the AFM image (Fig. 1(a)). An impact of the annealing on the crystallinity of the Ge thin film for the samples with SiO 2 capping layer was evaluated from Raman scattering spectra excited by green laser with a wavelength of 532 nm as shown in Fig. 2. A broad Raman feature around 275 cm -1 due to the amorphous Ge (a-Ge) was dominant for the samples before the annealing and after the annealing at 600 °C. After the annealing at 650 ºC, a sharp signal of the TO phonon mode in the crystalline phase (c-Ge : ~300 cm -1 ) was clearly observed, which peak width was slightly larger than that of a reference spectrum of Ge substrate. Also, the peak tailing toward the lower Raman shift side from c-Ge signals originated from poly-crystalline were detected. From these results, it was found that the crystal nucleation in the 8 nm-thick amorphous Ge film on Sapphire(0001) substrate occurs at around 650 °C. In addition, the peak shift of c-Ge signals as compared to the reference Ge wafer was detected, which was likely to be responsible for the tensile stress caused by the lattice mismatch between Ge and Sapphire. In summary, the Ge thin films with a thickness of ~8nm on the cleaned Sapphire(0001) substrate was found to be crystallized with keeping the surface flatness using SiO 2 capping layer by the annealing at 650 ºC. References 〉 [1] K. Ito et al. , Jpn. J. Appl. Phys. 57 , 06HD08 (2018). [2] J. Yuhara et al. , ACS Nano 12 , 11632 (2018). [3] Z. Guo, et al. , J. Phys. Soc. of Jpn., 82 , 063714 (2013). Acknowledgement 〉 This work was supported in part by JSPS Grant-in Aids for Scientific Research Nos. 19H02169. Figure 1
    Type of Medium: Online Resource
    ISSN: 2151-2043
    Language: Unknown
    Publisher: The Electrochemical Society
    Publication Date: 2020
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