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Journal articles on the topic 'Mixed conduction'

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Author: Grafiati
Published: 10 December 2022
Last updated: 28 January 2023

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1

Lesnic, D. "Heat conduction with mixed derivatives." International Journal of Computer Mathematics 81, no. 8 (August 2004): 971–77. http://dx.doi.org/10.1080/00207160410001715294.

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2

Wang, Mao-yuan, and Li-gan Qiu. "Mixed Conduction in BaCe0.8Pr0.2O3-Ceramic." Chinese Journal of Chemical Physics 21, no. 3 (June 2008): 286–90. http://dx.doi.org/10.1088/1674-0068/21/03/286-290.

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3

Li, Linhao, Ming Li, Ian M. Reaney, and Derek C. Sinclair. "Mixed ionic–electronic conduction in K1/2Bi1/2TiO3." Journal of Materials Chemistry C 5, no. 25 (2017): 6300–6310. http://dx.doi.org/10.1039/c7tc01786c.

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4

Garcia, Michele Vargas, Dayane Domeneghini Didoné, José Ricardo Gurgel Testa, Rúbia Soares Bruno, and Marisa Frasson de Azevedo. "Visual Reinforcement Audiometry and Steady-State Auditory Evoked Potential in infants with and without conductive impairment." Revista CEFAC 20, no. 3 (May 2018): 324–32. http://dx.doi.org/10.1590/1982-0216201820312217.

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ABSTRACT Purpose: to compare the findings of minimum levels of answers through air and bone conductions between the Visual Reinforcement Audiometry and the Steady-State Auditory Evoked Potential in infants from six to twelve months, with and without conductive disorder. Methods: sixty children aged six to twelve months were evaluated, 30 presenting conductive disorder, and 30 not presenting it. Children with malformation in the external auditory meatus with neurological alteration and / or genetic syndrome were excluded, as well as patients with sensorineural or mixed hearing loss. The infants were subjected to Visual Reinforcement Audiometry and Steady-State Auditory Evoked Potential evaluation through air and bone conduction on the same day. The results of both assessments were compared and correlated. Results: in the comparison through air conduction, for the group without conductive disorder of the medium ear, the minimum levels of response for 500 and 1000Hz were lower (better thresholds) for Steady-State Auditory Evoked Potential in both ears, and through bone conduction were very similar in all frequencies. Concerning the infants that present conductive disorder, the responses through air conduction were better in all frequencies evaluated when obtained via Steady-State Auditory Evoked Potential test. Through bone conduction, the results were very similar for both groups. Conclusion: it was possible to compare the findings to the minimum levels of response through air and bone conductions between the Visual Reinforcement Audiometry and the Steady-State Auditory Evoked Potential, being that the comparison for bone conduction in both groups presents an equivalence in the results, being very similar. In addition, for the air conduction, in the control group, there was proximity of responses of some frequencies, while the values for the Steady-State Auditory Evoked Potential test were better than the behavioral responses in the conductive disorder group.
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5

KUWABARA, K., M. ITOH, and K. SUGIYAMA. "Ionic-electronic mixed conduction in LixV2O5." Solid State Ionics 20, no. 2 (April 1986): 135–39. http://dx.doi.org/10.1016/0167-2738(86)90020-2.

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6

Sreepathi Rao, S., K. V. Satyanarayana Rao, K. Narashima Reddy, J. Siva Kumar, and U. V. Subba Rao. "Conduction mechanism in mixed polymer films." Materials Science and Engineering: B 8, no. 2 (May 1991): 125–27. http://dx.doi.org/10.1016/0921-5107(91)90025-q.

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7

Qiu, Li-Gan, and Gui-Lin Ma. "Mixed Conduction in Tb2O3 Doped BaCeO3." Chinese Journal of Chemistry 24, no. 11 (November 2006): 1564–69. http://dx.doi.org/10.1002/cjoc.200690293.

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8

Zhang, Haomiao, and Benjamin A. Wilhite. "Electrical conduction and reaction analysis on mixed-conducting iron-doped barium zirconate." Solid State Ionics 286 (March 2016): 7–18. http://dx.doi.org/10.1016/j.ssi.2015.11.023.

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9

Shan, Ke, and Zhong-Zhou Yi. "Electrical conduction behavior of mixed ionic-electronic conductor Y0.08Sr0.92Ti1−Sc O3−δ." Scripta Materialia 114 (March 2016): 70–73. http://dx.doi.org/10.1016/j.scriptamat.2015.08.008.

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10

Choi, Gyeong M., and Harry L. Tuller. "Nonstoichiometry and Mixed Conduction in alpha-Ta2O5." Journal of the American Ceramic Society 73, no. 6 (June 1990): 1700–1704. http://dx.doi.org/10.1111/j.1151-2916.1990.tb09815.x.

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11

Sata, N., H. Yugami, Y. Akiyama, H. Sone, N. Kitamura, T. Hattori, and M. Ishigame. "Proton conduction in mixed perovskite-type oxides." Solid State Ionics 125, no. 1-4 (October 1999): 383–87. http://dx.doi.org/10.1016/s0167-2738(99)00199-x.

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12

Sharon, Y., and J. R. Goldstein. "Mixed Conduction in an Active Porous Electrode." Journal of The Electrochemical Society 140, no. 6 (June 1, 1993): 1655–60. http://dx.doi.org/10.1149/1.2221618.

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13

George, A. M., and A. N. Virkar. "Mixed iono-electronic conduction in β-LaNb3O9." Journal of Physics and Chemistry of Solids 49, no. 7 (January 1988): 743–51. http://dx.doi.org/10.1016/0022-3697(88)90023-6.

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14

Gomes, E., F. M. Figueiredo, and F. M. B. Marques. "Mixed conduction induced by grain boundary engineering." Journal of the European Ceramic Society 26, no. 14 (January 2006): 2991–97. http://dx.doi.org/10.1016/j.jeurceramsoc.2006.02.017.

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15

Park, Hee Jung, Chan Kwak, and Sang Mock Lee. "Mixed conduction behavior in nanostructured lanthanum gallate." Electrochemistry Communications 11, no. 5 (May 2009): 962–64. http://dx.doi.org/10.1016/j.elecom.2009.02.035.

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16

MARIN, M., S. VLASE, I. M. FUDULU, and G. PRECUP. ""On instability in the theory of dipolar bodies with two-temperatures"." Carpathian Journal of Mathematics 38, no. 2 (February 28, 2022): 459–68. http://dx.doi.org/10.37193/cjm.2022.02.15.

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"In this paper we approach a generalized thermoelasticity theory based on a heat conduction equation in bodies with dipolar structure, the heat conduction depends on two distinct temperatures, the thermodynamic temperature and the conductive temperature. In our considerations the difference between two temperatures is highlighted by the heat supply. For the mixed initial boundary value problem defined in this context, we prove the uniqueness of a solution corresponding some specific initial and boundary conditions. Also, if the initial energy is negative or null, we prove that the solutions of the mixed problem are exponentially unstable."
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17

Qi, X. "Electrical conduction and hydrogen permeation through mixed proton–electron conducting strontium cerate membranes." Solid State Ionics 130, no. 1-2 (May 1, 2000): 149–56. http://dx.doi.org/10.1016/s0167-2738(00)00281-2.

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18

Matsumoto, Hiroshige. "Application of Protonic Conduction in Perovskite-Type Oxides: Mixed Proton-Electron-Conducting Membrane for Hydrogen Separation." Advances in Science and Technology 45 (October 2006): 2024–32. http://dx.doi.org/10.4028/www.scientific.net/ast.45.2024.

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Hydrogen separation is one of the key techniques for the forthcoming hydrogen economy. This paper describes a possible electrochemical method and materials for hydrogen separation: mixed proton-electron-conducting membrane that can permeate hydrogen selectively from hydrogen-containing gases, such as reformed gases of hydrocarbons. Proton-conducting perovskite-type solid electrolytes are first introduced as the base material of the mixed conductor. Some transition metal-doped perovskites are shown to have a mixed conductivity of protonic and electronic charge carriers, revealed by electrochemical and X-ray-spectroscopic measurements.
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19

Thomas, Elayne M., Phong H. Nguyen, Seamus D. Jones, Michael L. Chabinyc, and Rachel A. Segalman. "Electronic, Ionic, and Mixed Conduction in Polymeric Systems." Annual Review of Materials Research 51, no. 1 (July 26, 2021): 1–20. http://dx.doi.org/10.1146/annurev-matsci-080619-110405.

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Polymers that simultaneously transport electrons and ions are paramount to drive the technological advances necessary for next-generation electrochemical devices, including energy storage devices and bioelectronics. However, efforts to describe the motion of ions or electrons separately within polymeric systems become inaccurate when both species are present. Herein, we highlight the basic transport equations necessary to rationalize mixed transport and the multiscale material properties that influence their transport coefficients. Potential figures of merit that enable a suitable performance benchmark in mixed conducting systems independent of end application are discussed. Practical design and implementation of mixed conducting polymers require an understanding of the evolving nature of structure and transport with ionic and electronic carrier density to capture the dynamic disorder inherent in polymeric materials.
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20

Mizuno, M., K. Honda, H. Nakayama, and T. Uchida. "VRH conduction in TTF salts with mixed anions." Synthetic Metals 85, no. 1-3 (March 1997): 1599–600. http://dx.doi.org/10.1016/s0379-6779(97)80367-0.

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21

Yu, Ilhwan, Daeyoung Jeon, Bryan Boudouris, and Yongho Joo. "Mixed Ionic and Electronic Conduction in Radical Polymers." Macromolecules 53, no. 11 (May 15, 2020): 4435–41. http://dx.doi.org/10.1021/acs.macromol.0c00460.

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22

Cui, Xiaoyan, Tingjing Hu, Jingshu Wang, Junkai Zhang, Rui Zhao, Xuefei Li, Jinghai Yang, and Chunxiao Gao. "Mixed conduction in BaF2 nanocrystals under high pressure." RSC Advances 7, no. 20 (2017): 12098–102. http://dx.doi.org/10.1039/c6ra27837j.

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23

Oliva, Isaias, Atsunobu Masuno, Hiroyuki Inoue, Hiromasa Tawarayama, and Hiroshi Kawazoe. "Mixed conduction in alkali niobium tungsten phosphate glasses." Solid State Ionics 206 (January 2012): 45–49. http://dx.doi.org/10.1016/j.ssi.2011.10.018.

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24

SETTER, M. "A comprehensive method to characterize mixed conduction electrolytes." Solid State Ionics 28-30 (September 1988): 1579–85. http://dx.doi.org/10.1016/0167-2738(88)90423-7.

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25

Poe, Brent T., Claudia Romano, Danilo Di Genova, Harald Behrens, and Piergiorgio Scarlato. "Mixed electrical conduction in a hydrous pantellerite glass." Chemical Geology 320-321 (August 2012): 140–46. http://dx.doi.org/10.1016/j.chemgeo.2012.05.023.

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26

LIANG, K., and A. NOWICK. "High-temperature protonic conduction in mixed perovskite ceramics." Solid State Ionics 61, no. 1-3 (May 1993): 77–81. http://dx.doi.org/10.1016/0167-2738(93)90337-3.

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27

Lenyuk, M. P., and K. V. Lakusta. "Hyperbolic heat-conduction equation. Mixed boundary-value problem." Journal of Engineering Physics and Thermophysics 82, no. 1 (January 2009): 170–75. http://dx.doi.org/10.1007/s10891-009-0177-x.

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28

Meng, Qing-Long, Heng-Chang Liu, Zhiwei Huang, Shuang Kong, Xiaowei Lu, Patrick Tomkins, Peng Jiang, and Xinhe Bao. "Mixed conduction properties of pristine bulk graphene oxide." Carbon 101 (May 2016): 338–44. http://dx.doi.org/10.1016/j.carbon.2016.01.087.

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29

Robinson, Donald A., Michael E. Foster, Christopher H. Bennett, Austin Bhandarkar, Elizabeth R. Webster, Aleyna Celebi, Nisa Celebi, et al. "Electrochemically Tunable Mixed Valence Conduction in Ruthenium Hexacyanoruthenate." ECS Meeting Abstracts MA2022-02, no. 59 (October 9, 2022): 2216. http://dx.doi.org/10.1149/ma2022-02592216mtgabs.

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Reversible electrochemical doping of ruthenium hexacyanoruthenate, a type of Prussian blue analogue (PBA), enables the on-demand tuning of electronic conductivity by more than four orders of magnitude. Inkjet-printed electrochemical random access memory (ECRAM) devices based on Ru-PBA and lithium- or proton-conducting ionogel electrolytes exhibit excellent switching efficiency and long-term memory retention, important characteristics for analog artificial synapses in neuromorphic circuits. We also demonstrate excellent biocompatibility with live neurons and the use of Ru-PBA ECRAM devices to detect dopamine, promising first steps toward connecting artificial and biological neural networks. In-situ probing of metal-metal charge transfer by UV/Vis/NIR absorption spectroscopy reveals a switching mechanism whereby electrochemically tunable valence mixing between N-coordinated Ru sites controls the carrier concentration and mobility, as independently supported by both Marcus-Hush electron transfer theory and more conventional band structure predictions from DFT. The experimental agreement achieved by both theoretical approaches supports a general mechanistic picture that intramolecular charge transfer reactions, more commonly studied in polynuclear mixed valence small molecules, are central to electronic conductivity in extended coordination frameworks.
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30

Skarżyński, Piotr H., Anna Ratuszniak, Bartłomiej Król, Magdalena Kozieł, Kamila Osińska, Katarzyna B. Cywka, Anna Sztabnicka, and Henryk Skarżyński. "The Bonebridge in Adults with Mixed and Conductive Hearing Loss: Audiological and Quality of Life Outcomes." Audiology and Neurotology 24, no. 2 (2019): 90–99. http://dx.doi.org/10.1159/000499363.

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Background: Considering that hearing loss has a significant impact on social functioning, everyday activity and a person’s emotional state, one of the most important goals of hearing rehabilitation with bone conduction devices is improvement in a patient’s quality of life. Objectives: To measure self-assessed quality of life in patients implanted with the Bonebridge, a bone conduction device. Method: Prospective, observational, longitudinal study with one treatment group. Twenty-one patients with mixed or conductive hearing loss were included, and each individual served as its own control. The Abbreviated Profile of Hearing Aid Benefit (APHAB) was used to measure patient-reported quality of life before intervention and at 3 and 6 months after activation of the device. At the same time frames, pure-tone audiometry and speech understanding in quiet and in noise were tested. Results: Hearing-specific quality of life increased significantly after intervention and remained stable up to 6 months. Both word recognition in quiet and speech reception threshold in noise were significantly better after 6 months compared to before surgery. Outcomes of aided speech understanding were independent of initial bone conduction thresholds and equally high (word recognition score >75%) across the device’s indication range. Conclusions: The Bonebridge provides not only significant audiological benefit in both speech understanding in quiet and in noise, but also increases self-perceived quality of life in patients suffering from mixed and conductive hearing loss. Together with a very low rate and minor nature of adverse events, it is the state-of-the-art solution for hearing rehabilitation in patients with mixed or conductive hearing loss up to a bone conduction threshold of 45 dB HL.
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31

Georgescu, Madalina, V. Budu, Daniela Vrinceanu, and Magdalena Cernea. "BONEBRIDGE – ACTIVE BONE CONDUCTION HEARING AID." Scientific Bulletin of Electrical Engineering Faculty 18, no. 1 (April 1, 2018): 40–43. http://dx.doi.org/10.1515/sbeef-2017-0020.

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Abstract For individuals with conductive or mixed hearing loss, a bone conduction system can be a very effective treatment option. These systems bypass the outer and middle ear to send sound vibrations directly to the cochlea. This offers a natural sound quality for recipients. BONEBRIDGE is the first active, intact skin hearing implant for bone conduction stimulation, ideal for moderate to severe conduction hearing losses. It is a semi-implantable system, consisting of a surgical implantable part and an externally worn audio processor. Biomaterials used proved their safety, with very low rate of medical complications (skin infections, chronic suppurative otitis media, biofilm formation or extrusion).
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32

Deslouis, C., T. El Moustafid, M. M. Musiani, and B. Tribollet. "Mixed ionic-electronic conduction of a conducting polymer film. Ac impedance study of polypyrrole." Electrochimica Acta 41, no. 7-8 (May 1996): 1343–49. http://dx.doi.org/10.1016/0013-4686(95)00455-6.

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33

Chole, Richard A., Timothy E. Hullar, and Lisa G. Potts. "Conductive Component After Cochlear Implantation in Patients With Residual Hearing Conservation." American Journal of Audiology 23, no. 4 (December 2014): 359–64. http://dx.doi.org/10.1044/2014_aja-14-0018.

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Purpose Changes in auditory thresholds following cochlear implantation are generally assumed to be due to damage to neural elements. Theoretical studies have suggested that placement of a cochlear implant can cause a conductive hearing loss. Identification of a conductive component following cochlear implantation could guide improvements in surgical techniques or device designs. The purpose of this study is to characterize new-onset conductive hearing losses after cochlear implantation. Method In a prospective study, air- and bone-conduction audiometric testing were completed on cochlear implant recipients. An air–bone gap equal to or greater than 15 dB HL at 2 frequencies determined the presence of a conductive component. Results Of the 32 patients with preoperative bone-conduction hearing, 4 patients had a new-onset conductive component resulting in a mixed hearing loss, with air-conduction thresholds ranging from moderate to profound and an average air–bone gap of 30 dB HL. One had been implanted through the round window, 2 had an extended round window, and 1 had a separate cochleostomy. Conclusions Loss of residual hearing following cochlear implantation may be due in part to a conductive component. Identifying the mechanism for this conductive component may help minimize hearing loss. Postoperative hearing evaluation should measure both air- and bone-conduction thresholds.
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34

Uhler, Kristin M., Aoi A. Hunsaker, Nathaniel Greene, Kerry A. Walker, and Andrew D. Brown. "Toward improved measurement of infant bone conduction auditory brainstem responses." Journal of the Acoustical Society of America 151, no. 4 (April 2022): A257. http://dx.doi.org/10.1121/10.0011248.

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Newborn hearing screening has led to improved detection and treatment of hearing loss (HL) in infants and young children, supporting improved communication outcomes in early childhood and beyond. However, current screening protocols are not equally sensitive to all forms of HL, limiting diagnostic accuracy and, ultimately, identification of appropriate treatment options. Correspondingly, treatment outcomes in children with HL remain quite variable. One fundamental and persistent challenge is the assessment of bone conduction hearing, which is essential to differentiate conductive versus sensorineural pathology. Whereas hearing via air conduction can be effectively assessed using the auditory brainstem response (ABR), a noninvasive electrophysiologic measure, bone conduction ABR measurements suffer from comparatively poor signal quality (including significant stimulus artifact), transducer acoustic output limitations, and generally lower test-retest reliability. Here we evaluated the prospective benefits of measuring infant bone conduction ABRs using a modified bone conduction transducer designed to reduce stimulus artifact and thereby improve measurement quality. Measurements obtained using a standard bone conduction transducer were compared on several dimensions to measurements obtained using the modified transducer. Improved bone conduction measurement tools are expected to support improved detection and classification of conductive and mixed HL, leading to improved treatment outcomes for this important patient population.
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35

Agrinskaya, N. V., V. I. Kozub, and D. S. Poloskin. "Mixed conduction in doped semiconductor structures related to quasi-metallic conduction in the impurity band." Semiconductors 44, no. 4 (April 2010): 472–77. http://dx.doi.org/10.1134/s1063782610040111.

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36

Cerdà, J., J. R. Morante, and Anita Lloyd Spetz. "New Tunnel Schottky SiC Devices Using Mixed Conduction Ceramics." Materials Science Forum 433-436 (September 2003): 949–52. http://dx.doi.org/10.4028/www.scientific.net/msf.433-436.949.

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37

Ullmann, H., and K. Teske. "The Sr-Ce-O System: Ionic and Mixed Conduction." Solid State Phenomena 39-40 (December 1994): 107–12. http://dx.doi.org/10.4028/www.scientific.net/ssp.39-40.107.

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38

SMOLINSKI, P. "Parallel Mixed-Time Integration Methods for Unsteady Heat Conduction." Computer-Aided Civil and Infrastructure Engineering 3, no. 3 (November 6, 2008): 215–26. http://dx.doi.org/10.1111/j.1467-8667.1988.tb00251.x.

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39

Li, Cheng, Keaton Larson Lesnik, Yanzhen Fan, and Hong Liu. "Millimeter scale electron conduction through exoelectrogenic mixed species biofilms." FEMS Microbiology Letters 363, no. 15 (June 7, 2016): fnw153. http://dx.doi.org/10.1093/femsle/fnw153.

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40

Schacham, S. E., E. J. Haugland, R. A. Mena, and S. A. Alterovitz. "Mixed carrier conduction in modulation‐doped field effect transistors." Applied Physics Letters 67, no. 14 (October 2, 1995): 2031–33. http://dx.doi.org/10.1063/1.115068.

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41

Sapurina, I. Yu, M. E. Kompan, A. G. Zabrodskii, J. Stejskal, and M. Trchova. "Nanocomposites with mixed electronic and protonic conduction for electrocatalysis." Russian Journal of Electrochemistry 43, no. 5 (May 2007): 528–36. http://dx.doi.org/10.1134/s1023193507050059.

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42

Unemoto, Atsushi, Naoto Kitamura, Koji Amezawa, and Tatsuya Kawada. "Proton-Electron Mixed Conduction Properties in (Ce,Sr)PO4." ECS Transactions 13, no. 26 (December 18, 2019): 337–45. http://dx.doi.org/10.1149/1.3050405.

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43

RUTMAN, J., S. RAZ, and I. RIESS. "Reducing over potential by surface mixed ionic–electronic conduction." Solid State Ionics 177, no. 19-25 (October 15, 2006): 1771–77. http://dx.doi.org/10.1016/j.ssi.2006.04.012.

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44

Yoo, Han-Ill, and Doh-Kwon Lee. "Onsager coefficients of mixed ionic electronic conduction in oxides." Solid State Ionics 179, no. 21-26 (September 15, 2008): 837–41. http://dx.doi.org/10.1016/j.ssi.2008.01.039.

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45

Mbaye, M., P. Vasseur, E. Bilgen, A. K. Chenak, and Not Available Not Available. "Mixed convection and conduction heat transfer in open cavities." Heat and Mass Transfer 30, no. 4 (April 1, 1995): 229–35. http://dx.doi.org/10.1007/s002310050015.

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46

Hossain, M. A., and H. S. Takhar. "Radiation-conduction interaction in mixed convection along rotating bodies." Heat and Mass Transfer 33, no. 3 (December 11, 1997): 201–8. http://dx.doi.org/10.1007/s002310050179.

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47

Park, Young Min, and Gyeong Man Choi. "Mixed Ionic and Electronic Conduction in YSZ‐NiO Composite." Journal of The Electrochemical Society 146, no. 3 (March 1, 1999): 883–89. http://dx.doi.org/10.1149/1.1391696.

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48

Renna, Lawrence A., Julia D. Lenef, Monojit Bag, and D. Venkataraman. "Mixed Ionic-Electronic Conduction in Binary Polymer Nanoparticle Assemblies." Advanced Materials Interfaces 4, no. 20 (August 7, 2017): 1700397. http://dx.doi.org/10.1002/admi.201700397.

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49

Chenak, A. K., M. Mbaye, P. Vasseur, and E. Bilgen. "Mixed convection and conduction heat transfer in open cavities." Heat and Mass Transfer 30, no. 4 (April 1995): 229–35. http://dx.doi.org/10.1007/bf01602767.

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50

DRACHE, M., P. CONFLANT, and J. BOIVIN. "Anionic conduction properties of BiCaPb mixed oxides☆." Solid State Ionics 57, no. 3-4 (October 1992): 245–49. http://dx.doi.org/10.1016/0167-2738(92)90154-h.

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