메뉴 건너뛰기




Volumn 113, Issue 4, 2014, Pages

Single-file charge storage in conducting nanopores

Author keywords

[No Author keywords available]

Indexed keywords

IONS; MONTE CARLO METHODS;

EID: 84905011703     PISSN: 00319007     EISSN: 10797114     Source Type: Journal    
DOI: 10.1103/PhysRevLett.113.048701     Document Type: Article
Times cited : (76)

References (62)
  • 1
    • 48749133278 scopus 로고    scopus 로고
    • SCIEAS 0036-8075 10.1126/science.1158736
    • J. Miller and P. Simon, Science 321, 651 (2008). SCIEAS 0036-8075 10.1126/science.1158736
    • (2008) Science , vol.321 , pp. 651
    • Miller, J.1    Simon, P.2
  • 4
    • 54949139227 scopus 로고    scopus 로고
    • NMAACR 1476-1122 10.1038/nmat2297
    • P. Simon and Y. Gogotsi, Nat. Mater. 7, 845 (2008). NMAACR 1476-1122 10.1038/nmat2297
    • (2008) Nat. Mater. , vol.7 , pp. 845
    • Simon, P.1    Gogotsi, Y.2
  • 5
    • 84878230759 scopus 로고    scopus 로고
    • ACHRE4 0001-4842 10.1021/ar200306b
    • P. Simon and Y. Gogotsi, Acc. Chem. Res. 46, 1094 (2013). ACHRE4 0001-4842 10.1021/ar200306b
    • (2013) Acc. Chem. Res. , vol.46 , pp. 1094
    • Simon, P.1    Gogotsi, Y.2
  • 6
    • 0034324931 scopus 로고    scopus 로고
    • JPSODZ 0378-7753 10.1016/S0378-7753(00)00485-7
    • A. Burke, J. Power Sources 91, 37 (2000). JPSODZ 0378-7753 10.1016/S0378-7753(00)00485-7
    • (2000) J. Power Sources , vol.91 , pp. 37
    • Burke, A.1
  • 7
    • 37349106546 scopus 로고    scopus 로고
    • IEEPAD 0018-9219 10.1109/JPROC.2007.892490
    • A. Burke, Proc. IEEE 95, 806 (2007). IEEPAD 0018-9219 10.1109/JPROC.2007.892490
    • (2007) Proc. IEEE , vol.95 , pp. 806
    • Burke, A.1
  • 8
    • 77955493138 scopus 로고    scopus 로고
    • PTRMAD 1364-503X 10.1098/rsta.2010.0109
    • P. Simon and Y. Gogotsi, Phil. Trans. R. Soc. A 368, 3457 (2010). PTRMAD 1364-503X 10.1098/rsta.2010.0109
    • (2010) Phil. Trans. R. Soc. A , vol.368 , pp. 3457
    • Simon, P.1    Gogotsi, Y.2
  • 9
    • 33749007675 scopus 로고    scopus 로고
    • Anomalous increase in carbon at pore sizes less than 1 nanometer
    • DOI 10.1126/science.1132195
    • J. Chmiola, G. Yushin, Y. Gogotsi, C. Portet, P. Simon, and P. Taberna, Science 313, 1760 (2006). SCIEAS 0036-8075 10.1126/science.1132195 (Pubitemid 44454146)
    • (2006) Science , vol.313 , Issue.5794 , pp. 1760-1763
    • Chmiola, J.1    Yushin, G.2    Gogotsi, Y.3    Portet, C.4    Simon, P.5    Taberna, P.L.6
  • 12
    • 78651476889 scopus 로고    scopus 로고
    • JCOMEL 0953-8984 10.1088/0953-8984/23/2/022201
    • S. Kondrat and A. Kornyshev, J. Phys. Condens. Matter 23, 022201 (2011). JCOMEL 0953-8984 10.1088/0953-8984/23/2/022201
    • (2011) J. Phys. Condens. Matter , vol.23 , pp. 022201
    • Kondrat, S.1    Kornyshev, A.2
  • 16
    • 53849083762 scopus 로고    scopus 로고
    • CEUJED 0947-6539 10.1002/chem.200800639
    • J. Huang, B. Sumpter, and V. Meunier, Chem. Eur. J. 14, 6614 (2008). CEUJED 0947-6539 10.1002/chem.200800639
    • (2008) Chem. Eur. J. , vol.14 , pp. 6614
    • Huang, J.1    Sumpter, B.2    Meunier, V.3
  • 19
    • 78651287572 scopus 로고    scopus 로고
    • PLEEE8 1539-3755 10.1103/PhysRevE.82.056102
    • M.S. Loth, B. Skinner, and B.I. Shklovskii, Phys. Rev. E 82, 056102 (2010). PLEEE8 1539-3755 10.1103/PhysRevE.82.056102
    • (2010) Phys. Rev. e , vol.82 , pp. 056102
    • Loth, M.S.1    Skinner, B.2    Shklovskii, B.I.3
  • 23
    • 77951106336 scopus 로고    scopus 로고
    • JCPSA6 0021-9606 10.1063/1.3376611
    • K. Kiyohara, T. Sugino, and K. Asaka, J. Chem. Phys. 132, 144705 (2010). JCPSA6 0021-9606 10.1063/1.3376611
    • (2010) J. Chem. Phys. , vol.132 , pp. 144705
    • Kiyohara, K.1    Sugino, T.2    Asaka, K.3
  • 24
    • 79955387704 scopus 로고    scopus 로고
    • JCPSA6 0021-9606 10.1063/1.3578468
    • K. Kiyohara, T. Sugino, and K. Asaka, J. Chem. Phys. 134, 154710 (2011). JCPSA6 0021-9606 10.1063/1.3578468
    • (2011) J. Chem. Phys. , vol.134 , pp. 154710
    • Kiyohara, K.1    Sugino, T.2    Asaka, K.3
  • 26
    • 84889631832 scopus 로고    scopus 로고
    • FDISE6 1359-6640 10.1039/c3fd00026e
    • A.A. Kornyshev, Faraday Discuss. 164, 117 (2013). FDISE6 1359-6640 10.1039/c3fd00026e
    • (2013) Faraday Discuss. , vol.164 , pp. 117
    • Kornyshev, A.A.1
  • 29
    • 36849134148 scopus 로고
    • JAPIAU 0021-8979 10.1063/1.1707360
    • E. Weber, J. Appl. Phys. 10, 663 (1939). JAPIAU 0021-8979 10.1063/1.1707360
    • (1939) J. Appl. Phys. , vol.10 , pp. 663
    • Weber, E.1
  • 30
    • 84905041719 scopus 로고    scopus 로고
    • Generally, the value of (Equation presented) can vary depending on the amount of voids or neutral solvent in the pore, and the pore width. However, this is not expected in neat ionic liquid.
    • Generally, the value of (Equation presented) can vary depending on the amount of voids or neutral solvent in the pore, and the pore width. However, this is not expected in neat ionic liquid.
  • 31
    • 43449135900 scopus 로고    scopus 로고
    • Fabrication of nanoporous superstructures through hierarchical self-assembly of nanoparticles
    • DOI 10.1039/b801864b
    • M. Kim, G.H. Jeong, K.Y. Lee, K. Kwon, and S.W. Han, J. Mater. Chem. 18, 2208 (2008). JMACEP 0959-9428 10.1039/b801864b (Pubitemid 351671695)
    • (2008) Journal of Materials Chemistry , vol.18 , Issue.19 , pp. 2208-2212
    • Kim, M.1    Jeong, G.H.2    Lee, K.Y.3    Kwon, K.4    Han, S.W.5
  • 36
    • 84905015404 scopus 로고    scopus 로고
    • For pores with thin walls such as graphene sheets, the situation may be different [37].
    • For pores with thin walls such as graphene sheets, the situation may be different [37].
  • 37
    • 84855370059 scopus 로고    scopus 로고
    • PRBMDO 1098-0121 10.1103/PhysRevB.84.235133
    • B. Skinner, M.M. Fogler, and B.I. Shklovskii, Phys. Rev. B 84, 235133 (2011). PRBMDO 1098-0121 10.1103/PhysRevB.84.235133
    • (2011) Phys. Rev. B , vol.84 , pp. 235133
    • Skinner, B.1    Fogler, M.M.2    Shklovskii, B.I.3
  • 38
    • 84904963176 scopus 로고    scopus 로고
    • See Supplemental Material at, which includes Refs. [39-43]
    • See Supplemental Material at http://link.aps.org/supplemental/10.1103/ PhysRevLett.113.048701, which includes Refs. [39-43]
  • 39
    • 33947706146 scopus 로고
    • JAPIAU 0021-8979 10.1063/1.1697690
    • C. Bouwkamp and N. De Bruijn, J. Appl. Phys. 18, 562 (1947). JAPIAU 0021-8979 10.1063/1.1697690
    • (1947) J. Appl. Phys. , vol.18 , pp. 562
    • Bouwkamp, C.1    De Bruijn, N.2
  • 40
    • 84904963172 scopus 로고    scopus 로고
    • P. Holoborodko, http://www.holoborodko.com/pavel/numerical-methods/ numerical-derivative/smooth-low-noise-differentiators/.
    • Holoborodko, P.1
  • 41
    • 84905015402 scopus 로고    scopus 로고
    • M.G. Martin, http://towhee.sourceforge.net/.
    • Martin, M.G.1
  • 42
    • 57149145251 scopus 로고    scopus 로고
    • JCPSA6 0021-9606 10.1063/1.3020439
    • R. Lynden-Bell, J. Chem. Phys. 129, 204503 (2008). JCPSA6 0021-9606 10.1063/1.3020439
    • (2008) J. Chem. Phys. , vol.129 , pp. 204503
    • Lynden-Bell, R.1
  • 43
    • 84862298283 scopus 로고    scopus 로고
    • JPCBFK 1520-6106 10.1021/jp301359w
    • D. Roy and M. Maroncelli, J. Phys. Chem. B 116, 5951 (2012). JPCBFK 1520-6106 10.1021/jp301359w
    • (2012) J. Phys. Chem. B , vol.116 , pp. 5951
    • Roy, D.1    Maroncelli, M.2
  • 44
    • 2342594608 scopus 로고    scopus 로고
    • JPCBFK 1520-6106 10.1021/jp036367i
    • Y. Burak and R.R. Netz, J. Phys. Chem. B 108, 4840 (2004). JPCBFK 1520-6106 10.1021/jp036367i
    • (2004) J. Phys. Chem. B , vol.108 , pp. 4840
    • Burak, Y.1    Netz, R.R.2
  • 45
    • 26544461319 scopus 로고
    • PLRAAN 0556-2791 10.1103/PhysRevA.4.1071
    • M. Blume, V. Emery, and R. Griffiths, Phys. Rev. A 4, 1071 (1971). PLRAAN 0556-2791 10.1103/PhysRevA.4.1071
    • (1971) Phys. Rev. A , vol.4 , pp. 1071
    • Blume, M.1    Emery, V.2    Griffiths, R.3
  • 46
    • 84904989379 scopus 로고    scopus 로고
    • The classical BEG model has been solved perturbatively in the limit of low applied field [47,48]. However, we obtain the exact solution in this work.
    • The classical BEG model has been solved perturbatively in the limit of low applied field [47,48]. However, we obtain the exact solution in this work.
  • 47
    • 0010657274 scopus 로고
    • JUPSAU 0031-9015 10.1143/JPSJ.25.322
    • T. Obokata and T. Ooucrn, J. Phys. Soc. Jpn. 25, 322 (1968). JUPSAU 0031-9015 10.1143/JPSJ.25.322
    • (1968) J. Phys. Soc. Jpn. , vol.25 , pp. 322
    • Obokata, T.1    Ooucrn, T.2
  • 50
    • 44349167850 scopus 로고    scopus 로고
    • IJMPEO 0129-1831 10.1142/S0129183108012303
    • J. Kopp, Int. J. Mod. Phys. C 19, 523 (2008); IJMPEO 0129-1831 10.1142/S0129183108012303
    • (2008) Int. J. Mod. Phys. C , vol.19 , pp. 523
    • Kopp, J.1
  • 51
    • 47049121187 scopus 로고    scopus 로고
    • IJMPEO 0129-1831 10.1142/S0129183108012649
    • J. Kopp Int. J. Mod. Phys. C 19, 845(E) (2008). IJMPEO 0129-1831 10.1142/S0129183108012649
    • (2008) Int. J. Mod. Phys. C , vol.19
    • Kopp, J.1
  • 52
    • 84904963173 scopus 로고    scopus 로고
    • (Equation presented) and (Equation presented).
    • (Equation presented) and (Equation presented).
  • 53
    • 84904963174 scopus 로고    scopus 로고
    • For (Equation presented), the capacitance-voltage curves will only shift.
    • For (Equation presented), the capacitance-voltage curves will only shift.
  • 56
    • 84905015400 scopus 로고    scopus 로고
    • In Ref. [54], the porous electrodes were fabricated by chlorination of carbides with wide or narrow pores corresponding to high or low chlorination temperatures. Some experiments [56] indicate that at low chlorination temperatures, there is an abundance of cylindrical and spherical pores. Thus, the presence of cylindrical pores, in combination with the results of Fig. 2(b), may explain the peak to no-peak transition observed in Ref. [54].
    • In Ref. [54], the porous electrodes were fabricated by chlorination of carbides with wide or narrow pores corresponding to high or low chlorination temperatures. Some experiments [56] indicate that at low chlorination temperatures, there is an abundance of cylindrical and spherical pores. Thus, the presence of cylindrical pores, in combination with the results of Fig. 2(b), may explain the peak to no-peak transition observed in Ref. [54].
  • 58
    • 84904963170 scopus 로고    scopus 로고
    • The microscopic lattice Hamiltonian for strongly ionophobic pores [(Equation presented), see Supplemental Material [38]] exactly fulfills particle-hole symmetry (Equation presented) with shifted energy and voltage ((Equation presented)), in analogy with [58,59].
    • The microscopic lattice Hamiltonian for strongly ionophobic pores [(Equation presented), see Supplemental Material [38]] exactly fulfills particle-hole symmetry (Equation presented) with shifted energy and voltage ((Equation presented)), in analogy with [58,59].
  • 59
    • 0008511327 scopus 로고
    • PRBMDO 0163-1829 10.1103/PhysRevB.45.11354 354
    • A.L. Efros, Phys. Rev. B 45, 11 354 (1992). PRBMDO 0163-1829 10.1103/PhysRevB.45.11354
    • (1992) Phys. Rev. B , vol.45 , pp. 11
    • Efros, A.L.1
  • 60
    • 84872903284 scopus 로고    scopus 로고
    • PRBMDO 1098-0121 10.1103/PhysRevB.87.035409
    • B. Skinner and B.I. Shklovskii, Phys. Rev. B 87, 035409 (2013). PRBMDO 1098-0121 10.1103/PhysRevB.87.035409
    • (2013) Phys. Rev. B , vol.87 , pp. 035409
    • Skinner, B.1    Shklovskii, B.I.2
  • 61
    • 84905015401 scopus 로고    scopus 로고
    • Our model assumes monodisperse pores which are experimentally realizable [34]. Weak polydispersity will reduce and broaden the peaks in capacitance [54], but the qualitative features shall remain intact.
    • Our model assumes monodisperse pores which are experimentally realizable [34]. Weak polydispersity will reduce and broaden the peaks in capacitance [54], but the qualitative features shall remain intact.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.