Announcements

Published Online: February 28 2007 | ss20070129a1
Keywords: polyaniline nanotube | metal polyaniline | mesostructures | microstructures | order | size | nanopolymer | nanoelectronics | full polymer-based electronics | synthesis | MnO2 nanowires | chemical liquid deposition | diffusion-controlled growth

Logic of Polyaniline Nanotubes

Lin PU
Do these findings along with many polyaniline mesostructures and conceptual devices suggest that we should start a new chapter on full polymer-based electronics with polyaniline nanotubes and films, which is just similar to what we have done well for inorganic carbon nanotube? It may be in time.

 

 

Nanotubes and nanowires hold special positions in nanoscience. The fascination is not only because of their elegant symmetry, but also because of the theoretical simplicity and the maneuverability of the material's integration. Different from nanodot, the microscale length of nanoline offers us an easy access to low-dimensional confinement by microscale manipulation  [ 1 ], which is important to the device fabrication, and more importantly, to comprehensive applications of nanoelectronics. That's why finding new one-dimensional structures remains hot topics. Interestingly, this hot sometimes makes us feel difficult to depict appropriate relationship between nanoscience and nanolines because it seems a dilemma of the chicken or the egg, but we are clear that we will still mumble a published route for nanomaterials that it is good if it can make them with right quality, and better to get simultaneously with high yield; and best to get a semiconductor that can be doped n- or p-type. 

 

We have known many one-dimensional objects: the inorganic or organic, the insulator, semiconductor or metal, and the crystalline or amorphous [ 2 ]. However, due to the complexity, outstanding challenges hold in those organic species. The omnipotent potentials have been revealed for carbon nanotubes, but it is only at the primary stage to tell exactly what an organic nanotube can be competent for the leading role of the polymer nanoelectronics. 

 

Who can be next VIP in nanopolymers? Key successes in today's microelectronics kindly imply that the possibility is larger to start with those conducting-tunable materials. Therefore, the conjugated polymers of polyacetylene, polythiophene and polyaniline come into view as their novel properties and big potentials in polymer electronics have been demonstrated in the past three decades [ 3, 4 ]. 

 

For example, as a model polymer, polyaniline can be reversibly non-redox doped/de-doped via simple acid protonation/base deprotonation with little or no degradation of the polymer backbone (Figure1). The conductivity of its emeraldine base form can be changed from 10^-10   to 10^0~1 Siemens per centimeter by 'protonic-acid doping' with, for example 1 M aqueous HCl-during which the number of electrons associated with the polymer chain remain unchanged [ 3 ]; 

 

However, charge transport in conducting polymers, as in all metals and semiconductors, is limited by a combination of intrinsic electron-photon scattering and sample imperfection. Although metallic levels of conductivities have been identified for partially oriented and heavily doped polyacetylene, the absence of a metal-like temperature dependence suggests that the observed values are not intrinsic. [ 4 ]

 

Polyaniline

 

Hopefully, the stone came last year [ 5 ]. It's the emeraldine base form of polyaniline film doped with camphor sulphonic acid. By using of self-stabilized polymerization, Korean researchers got it with conductivity three times than that of the samples made by conventional methods [ 6 ]. They and A. J. Heeger finally proved a metal polyaniline that possesses right temperature dependence of conductivity and a metal-like plasma-frequency in the near infrared. This frequency defines a metallic optical reflectivity that can be accurately fitted by the Drude model, which is used to explain charge transport of metal through the free-electron approximation.

 

"In fact, the surprise is just how like an ordinary metal polyaniline turns out to be." said Richard Friend [ 7 ], "this finding pitches the metallic model against a different model, loosely referred as to as the 'polaron model' 4 ], that over the past two decades has been the favoured explanation of polymer conductivity."

 

Obviously, the metallic transport in polyaniline as well as the fabrication details will remain a contentious issue in near future. Beyond the favoured polaron model or the modified Drude model [ 8 ], what are the intrinsic causes of the transition from polaronic conductor to simple metal? Of which does a factor deserve more recognition during synthesizing? In the route of metal polyaniline [ 6 ], the polymerization is performed in a heterogeneous biphasic system of organic and aqueous medium without any stabilizers, in terms of main modification with which the monomers and growing polymer chains act as stabilizers, resulting in enough dispersion of the organic phase within the aqueous reaction medium. Supporting with the spectroscopic evidence of X-ray diffraction, a higher weight of spontaneous order arising in the polyaniline backbone should be responsible for the metallic behavior, hinted the authors [ 5 ]. 

 

Up to date, because of light atom weights of C, H and O etc., we can't see the lattice structures of polymer chain by high resolution TEM. This limitation much impedes us to develop more improved synthesis, and decisively correlate ordered packing of polymer chains with performances' enhancement. Most often we prefer to believe in this correlation for low-dimensional materials while there is still hesitation. The spectroscopic evidence is not enough. Why?

 

The properties of bulk solid material, thus the electronic structure is sensitive to micro/mesoscopic environment (defects and doped impurities etc.) as well as macroscopic arrangement of the inorganic lattice or organic chain (the long-range order). When the dimension shrinks down to the nanometer regime, many classical concepts face the definitions' limes. One big topic is what an aggregation of atoms can be called a solid, which is very related to hot words of 'size' or 'size-selected/control', and 'shape' or 'shape-control' in nanoscience. 

 

For bulk polycrystalline material, the shape effect, so-called the boundary conditions of the potential field in physics, has no evident influence on many macroscopic properties. It's partially because those different functional responses, such as the mechanical, thermal and electromagnetic responses, intrinsically take effect on different scales, and many mesoscopic effects are statistically screened or neutralized due to lager-size aggregation of randomly oriented single crystallites; Moreover, some physical responses can show in combined features that have one-to-more correspondences to different featured sizes (order parameters). Therefore, a nanoscale entity may show a bulk-like property here and yet can act with low-dimensional effect there. This combination poses great difficulty on applying classical models to nano-phenomena as well as the redefining of the concepts [ 9 ]. That's why we should be very careful when we only extract the conclusions from those spectroscopic evidences that may screen true origin.

However, before getting an image of polymer chains with atomic resolution, we have no choice but to rely on this phenomenological deduction. We hope that it's reasonable in most cases. In general, as expected, the physics of low-dimensional systems provides additional guidance for property tailoring. For example, possibly due to better packing and alignment of the polymer chain, the template-synthesized polypyrrole fiber has higher conductivity comparing with its bulk counterpart [ 10 ]. And there are also so many polyaniline mesostructures and conceptual devices that tell the stories with similar implications on order [ 11 ].

 

 

Figure 2 Polyaniline Nanoplates

HRimage

ScideaNews.com: grid-like polyaniline nanoplates

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Figure 2
[left]
TEM images of the textured polyaniline plates (Fig.2a & b) elucidate the fine structures of two typical structures revealed by SEM (Fig.2c). It is evident that the ladderlike structure (a) is the base of formation for the gridlike one (b). The inset in (b) shows a typical gridlike structure. c) SEM image of the gridlike plate.
[right] Possible mechanism of the self-organization during polymerization

  
Reaction conditions: [Aniline] = 0.10 M, [FeCl3] = 0.20 M , [HCl] = 1.0 M ; hydrothermal reaction at 120 oC for 60 hours, followed with 5 min water cooling. 
Scale bars: 1 μm, the inset in (b) has the same scale. 

Credit:Scidea Art 2007 Source: ScideaNews.com

 

Figure 3 Polyaniline Nanotubes

HRimage

 ScideaNews.com: Polyaniline Nanotubes

 HRimage

Cover story of Advanced Materials
Issue 20070206 
Polyaniline Nanotubes

Polyaniline nanotubes can be synthesized through a chemical template method. The shape and major parameters of the tubes are precisely controlled by the reactive templates of MnO2 nanowires, which also act as the oxidative initiator for polymerization. The cover image shows an example where the rectangular tubes are cloned from the cryptomelane-phase MnO2, as reported on p. 461 by Shi and co-workers.  

Pan LJ, Pu L, Shi Y, Song SY, Xu Z, Zhang R & Zheng YD,
Synthesis of Polyaniline Nanotubes with a Reactive Template of Manganese Oxide
Adv. Mater. 19 (3), 461-464 (2007).
 DOI :: 10.1002/adma.200602073 | CrossRef
 Wiley-VCH ::  Cover Story . Abs . Refs . PDF . Supp.Info.

Credit:Scidea Art 2007 Source: ScideaNews.com

 

 

 

 

Figure 4 Polyaniline Nanotubes

HRimage

ScideaNews.com: Polyaniline Nanotubes

HRimage

 

Figure 4

a) [Upper] SEM image of the reactive template of cryptomelane-phase MnO2 nanowires. Scale bar: 1μm; b) [Bottom, left] SEM image of the polyaniline nanotubes with rectangular cross-section (note the zone of fracture). Scale bar: 200 nm; and c) [Bottom, right] TEM image shows that the polyaniline nanotubes have high-quality. Scale bar: 1μm.
 Note that the scale bar in upper image can be used as the size indicator for bottom two images. 

Credit:Scidea Art 2007 Source: ScideaNews.com  

   

On my own experiences, I prefer to believe the microstructural explanation of the metallic polyaniline, i.e., the conductivity increasing with higher order. Recently, we reported some novel polyaniline mesostructures made through hydrothermal method [ 12 ]. The samples show evident changing in PL intensity and conductivity, and therefore the electronic structure, is sensitive to the microstructures, namely, can be tuned by the processing conditions with fine controlling of reaction rate. Among the samples with different morphologies, there is a surprise of the grid-like polyaniline nanoplate (Figure 2). The TEM observation reveals its fine structure consisting of the parallel nanowires arrays in different layer. We do not know why polyaniline there prefers to dominantly directional growth, but some clues indicate that the 'seeding' plates with polarized edges, developing in the early term of the synthesis, should be attributed to this ordered growth. Therefore, polyaniline-depositing on a charged substrate can be a right direction to further improve the self-organization during polymerization.

 

This deduction may be supported by our recent work on polyaniline nanotubes that published as the cover story in 6 February 2007 issue of Advanced Materials [13, Figure3]. We use manganese oxide as the physical template and the chemical oxidative initiator for the aniline polymerization. The template can be removed after the reaction, as manganese oxide is reduced into soluble Mn2+ ions [Figure4]. Many polyaniline mesostructures, such as nanotubes, spherical tube brushes, and double-shell nanotubes, can be fabricated using this method. 

 

In our synthesis, cryptomelane-phase manganese oxide nanowires [ 14 ], β-manganese oxide nanotubes [ 15 ], and β- and ε-manganese oxide nanowires [ 16 ] were used as templates for polyaniline nanotubes; the templates had to be washed thoroughly before use.Manganese oxide has a variety of applications, for examples, mild oxidizing catalysis, ion-exchange processes, magnetic applications, and field of electrochemistry such as cathode materials in alkaline and rechargeable batteries. There exist many effective routes for precisely controlled synthesizing of manganese oxide mesostructures, such as helices, colloidal crystals, three–dimensional structures, nanowires and nanotubes, with several crystallographic forms of α-, β-, γ- and ε-type [ 14-19 ].

 

Thereby, our method that using manganese oxide nanolines as reactive templates gives a big chance for the fabrication of polyaniline nanotubes. Moreover, as a 'side-effect', and also because of the importance of polyaniline, our method suggests that further attention should be imposed on exploring novel manganese oxide mesostructures as well as the improved synthesis with better size- and shape/morphology-control.

 

Furthermore, the method may be suitable for making nanotubes of other conductive/conjugated polymers of polypyrrole, and insulative polymers of polyacrylonitrile. This is because the oxidant potential of MnO2 (1.23 V) is higher than the half-wave potentials of their polymerization reaction.

 

It should be pointed here that the quality of polyaniline nanotubes from the template nanowires of cryptomelane-phase manganese oxide is very high. To my best knowledge, it's the best one among all the reported polyaniline nanotubes. Note that the larger diameter of the well-faced cryptomelane-phase manganese oxide nanowires provide enough smooth surfaces for the slow growth of polyaniline. Indeed these outer faces can act as the substrates used in conventional chemical vapor deposition (CVD). The underlying mechanism can be of diffusive nature and bears much resemblance to growing SiO2 film by thermal oxidation of Si substrate. I would like to call this diffusion-controlled procedure as chemical liquid deposition (CLD).

Do these findings along with many polyaniline mesostructures and conceptual devices suggest that we should start a new chapter on full polymer-based electronics with polyaniline nanotubes and films, in terms of a possibility in which the comprehensive modification of conductivity can be gotten from insulator, semiconductor to metal in nanopolymer, which is just similar to what we have done well for inorganic carbon nanotube?

It may be in time.  

 

* Lin Pu is in the Physics Department of Nanjing University, Nanjing 210093, CHINA.

 

Acknowledgment 

We acknowledge financial support from NSFC (Grants 60676006 & 60225014) and 973 project (Grant G2001CB3095). 

 

References

 

1

A random notes on low-dimensional confinement.

The following comment is cited from Prof. Uzi Landman's essay where he prefers to say the nano "size" as a phenomenon-dependent characteristic length.

Landman U,
Materials by numbers: computations as tools of discovery
PNAS, 102(19), 6671-6678 (2005).
DOI :: 10.1073/pnas.0408038102 | CrossRef
PNAS :: Abs . Full . PDF . Supp.Info.

 

In most cases, when the nonscalable regime is approached, the physical size of the system along at least one of the coordinate axes becomes comparable to a phenomenon-dependent characteristic length; examples include: conductance quantization occurring when the diameter of the constriction (e.g., a nanowire) approaches the electronic Fermi-wavelength (typically 0.5 nm in metals), i.e., "when the electron feels the boundary"; transport in a wire becoming ballistic (rather then diffusive) when the length of the wire is shorter then the electron mean-free-path (1); a column (or a jet) of invicid fluid becoming unstable when its length equals approximately nine times its radius (this length equals the wavelength of the fastest growing varicose instability mode, known as the Rayleigh instability; ref. 2); and the mechanical response and deformation modes of nanocrystals becoming dislocationless when their physical dimensions are comparable to the dislocation core size, resulting in enhanced mechanical strength of nanoscale crystallites and nanowires (3, 4), as well as mechanical reversibility (4) and absence of work-hardening.

 
 (1)Landauer R,
Philos. Mag. 21, 863-873 (1970). 
 (2)Rayleigh JWS,
Proc. R. Soc. London 10, 4-13 (1879).
 (3)Landman U, Luedtke WD, Burnham NA & Colton RJ,
Atomistic mechanisms and dynamics of adhesion, nanoindentation, and fracture
Science 248(4954), 454-461 (1990).
DOI :: 10.1126/science.248.4954.454 | CrossRef
AAAS :: TOCRefs. PDF
 (4)Landman U, Luedtke WD, Salisbury BE & Whetten RL,
Reversible Manipulations of Room Temperature Mechanical and Quantum Transport Properties in Nanowire Junctions
Phys. Rev. Lett. 77 (7), 1362-1365 (1996). 
DOI :: 10.1103/PhysRevLett.77.1362 | CrossRef
APS ::  AbsRefs . PDF
2Coming soon.
3 
(1)

Alan G. MacDiarmid

The Nobel Prize in Chemistry, 2000
       "for the discovery and development of conductive polymers"

Nobel Lecture
Alan G. MacDiarmid 
"Synthetic Metals": A Novel Role for Organic Polymers
NobelPrize.org | Video . PDF
 

Alan G. MacDiarmid died on 7 February 2007.

MacDiarmid AG,
"Synthetic Metals": A Novel Role for Organic Polymers

Angew. Chem. 113, 2649-2659 (2001);
Angew. Chem. Int. Ed. 40, 2581-2590 (2001) and references therein;
DOI: 10.1002/1521-3773(20010716)40:14<2581::AID-ANIE2581>3.0.CO;2-2 | CrossRef
WILEY-VCH ::  Abs . RefsFull . PDF 

(2)Huang WS, Humphrey BD & MacDiarmid AG,
J. Chem. Soc. Faraday Trans. 82, 2385-(1986);
(3)Chiang JC & MacDiarmid AG. 
'Polyaniline': Protonic acid doping of the emeraldine form to the metallic regime
Synth. Met.  13(1-3), 193-205 (1986); 
DOI:: 10.1016/0379-6779(86)90070-6 | CrossRef 
Elsevier::  Abs . Refs . PDF 
(4)MacDiarmid AG & Epstein AJ,
Secondary doping in polyaniline
Synth. Met. 69 (1-3), 85-92 (1995); 
DOI:: 10.1016/0379-6779(94)02374-8 | CrossRef 
Elsevier::  Abs . Refs . PDF
(5)MacDiarmid AG, Jones WE Jr, Norris ID, Gao J, Johnson AT Jr, Pinto NJ & Hone J, 
Electrostatically-generated nanofibers of electronic polymers  
Synth. Met. 119 (1-3), 27-30 (2001);  
DOI:: 10.1016/S0379-6779(00)00597-X | CrossRef 
Elsevier::  AbsFull . PDF 
(6)Norris ID, Shaker MM, Ko FK & MacDiarmid AG,
Electrostatic fabrication of ultrafine conducting fibers: polyaniline/polyethylene oxide blends  
Synth. Met. 114 (2), 109-114 (2000). 
DOI:: 10.1016/S0379-6779(00)00217-4 | CrossRef 
Elsevier::  Abs . Full . PDF 
4

Alan J. Heeger

The Nobel Prize in Chemistry, 2000       

"for the discovery and development of conductive polymers" 

Nobel Lecture
Alan Heeger

Semiconducting and Metallic Polymers: The Fourth Generation of Polymeric Materials
NobelPrize.org | Video . PDF 

Heeger AJ, Kivelson S, Schrieffer JR & Su WP,
Solitons in conducting polymers
Rev. Mod. Phys. 60 (3): 781-850 (1988).
DOI :: 10.1103/RevModPhys.60.781 | CrossRef
APS ::  Abs . Refs . PDF

5Lee KH, Cho S, Park SH, Heeger AJ, Lee CW & Lee SH,
Metallic transport in polyaniline
Nature 441 (7089), 65 (2006);
DOI :: 10.1038/nature04705 | CrossRef
 NPG ::  Abs . Fig&Table . Full . PDF
6Lee SH, Lee DH, Lee KH & Lee CW,
High-performance polyaniline prepared via polymerization in a self-stabilized dispersion
Adv. Funct. Mater. 15, 1495 (2005).

DOI :: 10.1002/adfm.200400467 | CrossRef
 Wiley-VCH :: AbsRefs . PDF
7Friend R
Materials science: Polymers show they're metal
Nature 441 (7089), 37-37 (2006).
DOI :: 10.1038/441037a  | CrossRef
 NPG :: AbsPDF
8Kohlman RS, Zibold A, Tanner DB, Ihas GG, Ishiguro T, Min YG, MacDiarmid AG & A. J. Epstein AJ,
Limits for Metallic Conductivity in Conducting Polymers
Phys. Rev. Lett. 78 (20), 3915-3918 (1997).
DOI :: 10.1103/PhysRevLett.78.3915 | CrossRef
 APS :: Abs . Refs . PDF 
9Refs. coming soon: For example, the cluster, an aggregation of 10-10^3 atoms (diameter =1-5 nm), can be solid-like at low temperatures and liquid-like at high temperatures, but in contrast to the bulk behavior an intermediate range of temperatures exists where cluster shows both solid and liquid behavior. As a consequence of this the heat capacity does not show a discontinuity but a smooth peak. [*]
10 
(1)Jérôme C & Jérôme R,
Electrochemical Synthesis of Polypyrrole Nanowires
Angew. Chem. 110, 2639-2642 (1998);
Angew. Chem. Int. Ed.
37 (18), 2488-2490 (1998);
DOI :: 10.1002/(SICI)1521-3773(19981002)37:18<2488::AID-ANIE2488>3.0.CO;2-O | CrossRef
 Wiley-VCH  :: AbsPDF
(2)Parthasarathy RV & Martin CR,
Template-Synthesized Polyaniline Microtubules
Chem. Mater. 6 (10), 1627-1632 (1994).
DOI :: 10.1021/cm00046a011  | CrossRef
 ACS :: AbsPDF
11 
(1)Wu CG & Bein T,
Conducting Polyaniline Filaments in a Mesoporous Channel Host
Science 264 (5166), 1757-1759 (1994);
DOI :: 10.1126/science.264.5166.1757 | CrossRef
 AAAS :: TOC . Abs . RefsPDF
(2)Liang L, Liu J, Windisch CF, Exarhos GJ & Lin YH,
Direct Assembly of Large Arrays of Oriented Conducting Polymer Nanowires
Angew. Chem. 114, 3817-3820 (2002);
Angew. Chem. Int. Ed. 41 (19), 3665-3668 (2002);
DOI :: 10.1002/1521-3773(20021004)41:19<3665::AID-ANIE3665>3.0.CO;2-B | CrossRef
 Wiley-VCH :: AbsRefs . Full . PDF
(3)Ikkala O & ten Brinke G,
Functional Materials Based on Self-Assembly of Polymeric Supramolecules
Science 295 (5564), 2407-2409 (2002);
DOI :: 10.1126/science.1067794 | CrossRef
 AAAS ::  AbsFull . PDF
(4)Spange S,
Insulated Nanowire Bundles through Consecutive Template Synthesis
Angew. Chem. 115, 4568-4570 (2003);
Angew. Chem. Int. Ed., 42 (37), 4430-4432 (2003);
DOI :: 10.1002/anie.200301654 | CrossRef
 Wiley-VCH  ::  Abs . Refs . Full . PDF
(5) 
 Huang JX & Kaner RB,
Nanofiber Formation in the Chemical Polymerization of Aniline: A Mechanistic Study
Angew. Chem. 116, 5941-5945 (2004);
Angew. Chem. Int. Ed.
43 (43), 5817-5821 (2004);
DOI :: 10.1002/anie.200460616 | CrossRef
 Wiley-VCH ::  AbsRefs . Full . PDF
 Huang JX, Virji S, Weiller BH & Kaner RB,
Polyaniline Nanofibers: Facile Synthesis and Chemical Sensors
J. Am. Chem. Soc. 125 (2), 314-315 (2003);
DOI :: 10.1021/ja028371y | CrossRef
 ACS ::  AbsFull . PDF
 Huang JX & Kaner RB,
A General Chemical Route to Polyaniline Nanofibers
J. Am. Chem. Soc. 126 (3), 851-855 (2004);
DOI :: 10.1021/ja0371754  | CrossRef
 ACS ::  AbsFull . PDF
 Huang JX, Virji S, Weiller BH & Kaner RB,
Nanostructured Polyaniline Sensors
Chem. Eur. J., 10 (6), 1314-1319 (2004);
DOI :: 10.1002/chem.200305211 | CrossRef
 Wiley-VCH ::  AbsFull . PDF
 Virji S, Huang JX, Kaner RB & Weiller BH,
Polyaniline Nanofiber Gas Sensors: Examination of Response Mechanisms
Nano Lett. 4 (3), 491-496 (2004);
DOI :: 10.1021/nl035122e  | CrossRef
 ACS ::  AbsFull . PDF
 Huang JX & Kaner RB,
Flash welding of conducting polymer nanofibres
Nat. Mater. 3 (11), 783-786 (2004).
DOI :: 10.1038/nmat1242  | CrossRef
 NPG :: Abs . Fig&Table . Full . PDF . Supp.Info.
(6)Zhang XY, Goux WJ & Manohar SK,
Synthesis of Polyaniline Nanofibers by "Nanofiber Seeding" 
J. Am. Chem. Soc. 126 (14), 4502-4503 (2004).
DOI :: 10.1021/ja031867a  | CrossRef
 ACS ::  Abs . Full . PDF . Supp.Info.
(7) 
 Li WG & Wang HL,
Oligomer-Assisted Synthesis of Chiral Polyaniline Nanofibers
J. Am. Chem. Soc. 126 (8), 2278-2279 (2004);
DOI :: 10.1021/ja039672q | CrossRef
 ACS ::  AbsFull . PDF
 Wei Y, Jang GW, Chan CC, Hsueh KF, Hariharan R, Patel SA & Whitecar CK,
Polymerization of aniline and alkyl ring-substituted anilines in the presence of aromatic additives
J. Phys. Chem. 94 (19), 7716-7721 (1990);
DOI :: 10.1021/j100382a073 | CrossRef
 ACS ::  AbsPDF
 Shim YB & Park SM,
Electrochemistry of conductive polymers VII. Autocatalytic rate constant for polyaniline growth
Synth. Met. 29 (1), 169-174 (1989);
DOI :: 10.1016/0379-6779(89)90293-2 | CrossRef
 Elsevier ::  AbsRefs. PDF
(8) 
 Wei ZX & Wan MX,
Hollow Microspheres of Polyaniline Synthesized with an Aniline Emulsion Template
Adv. Mater. 14 (18), 1314-1317 (2002);
DOI :: 10.1002/1521-4095(20020916)14:18<1314::AID-ADMA1314>3.0.CO;2-9  | CrossRef
 Wiley-VCH ::  Abs . Refs . PDF
 Wei ZX, Zhang ZM & Wan MX,
Formation Mechanism of Self-Assembled Polyaniline Micro/Nanotubes  
Langmuir 18 (3), 917-921 (2002);
DOI :: 10.1021/la0155799 | CrossRef
 ACS ::  AbsFull . PDF
 Zhang ZM, Wei ZX & Wan MX,
Nanostructures of Polyaniline Doped with Inorganic Acids 
Macromolecules 
35 (15), 5937-5942 (2002).
DOI ::  10.1021/ma020199v | CrossRef
 ACS ::  Abs . Full . PDF
 Zhang LJ & Wan MX,
Self-Assembly of Polyaniline - From Nanotubes to Hollow Microspheres  
Adv. Funct. Mater. 13 (10), 815-820 (2003);
DOI :: 10.1002/adfm.200304458 | CrossRef
 Wiley-VCH  ::  AbsRefs . PDF
 Qiu HJ, Zhai J, Li SH, Jiang L & Wan MX,
Oriented Growth of Self-Assembled Polyaniline Nanowire Arrays Using a Novel Method  
Adv. Funct. Mater. 13 (12), 925-928 (2003);
DOI :: 10.1002/adfm.200304366 | CrossRef
 Wiley-VCH ::  Abs . Refs . PDF
 Zhang LJ, Long YZ, Chen ZJ & Wan MX,
The Effect of Hydrogen Bonding on Self-Assembled Polyaniline Nanostructures
Adv. Funct. Mater. 14 (7), 693-698 (2004).
DOI :: 10.1002/adfm.200305020 | CrossRef
 Wiley-VCH  ::  Abs . Refs . Full . PDF
(9)Ramanathan K, Bangar MA, Yun M, Chen W, Mulchandani A & Myung NV,
Individually Addressable Conducting Polymer Nanowires Array
Nano Lett. 4 (7), 1237-1239 (2004).
DOI :: 10.1021/nl049477p | CrossRef
 ACS ::  Abs . Full . PDF 
(10) 
 Khan MA & Armes SP,
Conducting Polymer-Coated Latex Particles 
Adv. Mater. 12 (9), 671-674 (2000);
DOI :: 10.1002/(SICI)1521-4095(200005)12:9<671::AID-ADMA671>3.0.CO;2-3 | CrossRef
 Wiley-VCH ::  Abs . PDF
 Caruso F,
Nanoengineering of Particle Surfaces  
Adv. Mater. 13 (1), 11-22 (2001);
DOI :: 10.1002/1521-4095(200101)13:1<11::AID-ADMA11>3.0.CO;2-N | CrossRef
 Wiley-VCH ::  AbsPDF
 Wang D & Caruso F,
Fabrication of Polyaniline Inverse Opals via Templating Ordered Colloidal Assemblies
Adv. Mater. 13 (5), 350-354 (2001);
DOI :: 10.1002/1521-4095(200103)13:5<350::AID-ADMA350>3.0.CO;2-X | CrossRef
 Wiley-VCH ::  AbsPDF
 Kim D, Choi J, Kim JY, Han YK & Sohn D,
Size Control of Polyaniline Nanoparticle by Polymer Surfactant  
Macromolecules 35 (13), 5314-5316 (2002);
DOI :: 10.1021/ma020162a | CrossRef
 ACS ::  AbsFull . PDF
 Shi XY, Briseno AL, Sanedrin RJ & Zhou FM.
Formation of Uniform Polyaniline Thin Shells and Hollow Capsules Using Polyelectrolyte-Coated Microspheres as Templates
Macromolecules 36 (11), 4093-4098 (2003);
DOI :: 10.1021/ma034185g | CrossRef
 ACS ::  Abs . Full . PDF . Supp.Info.
 Mezzenga R, Ruokolainen J, Fredrickson GH, Kramer EJ, Moses D, Heeger AJ & Ikkala O.
Templating Organic Semiconductors via Self-Assembly of Polymer Colloids
Science 299 (5614), 1872-1874 (2003).
DOI :: 10.1126/science.1081334 | CrossRef
 AAAS :: AbsFull . PDF . Supp.Info.
(11) 
 Doblhofer K & Rajeshwar K,
Handbook of Conducting Polymers, M. Dekker, New York, 1998;
 Chandrasekhar P,
Conducting Polymers, Fundamentals and Applications, Kluwer, 1999;
 McQuade DT, Pullen AE & Swager TM,
Conjugated Polymer-Based Chemical Sensors
Chem. Rev. 100 (7), 2537-2574 (2000);
DOI :: 10.1021/cr9801014 | CrossRef
 ACS ::  Full . PDF
 Novák P, Müller K, Santhanam KSV & Haas O.
Electrochemically Active Polymers for Rechargeable Batteries  
Chem. Rev. 97 (1), 207-282 (1997);
DOI :: 10.1021/cr941181o | CrossRef
 ACS ::  Full . PDF
(12) 
 Gustafsson G, Gao Y, Treacy GM, Klavetter F, Colaneri N & Heeger AJ,
Flexible light-emitting diodes made from soluble conducting polymers 
Nature 357 (6378), 477-479 (1992);
DOI :: 10.1038/357477a0 | CrossRef
 NPG :: TOC . Refs . PDF
 Oyama N, Tatsuma T, Sato T & Sotomura T,
Dimercaptan−polyaniline composite electrodes for lithium batteries with high energy density
Nature 373 (6515), 598-600 (1995);
DOI :: 10.1038/373598a0 | CrossRef
 NPG :: TOC . Refs . PDF
 Kumar D & Sharma RC,
Advances in conductive polymers
Eur. Polm. J., 34 (8), 1053-1060 (1998);
DOI :: 10.1016/S0014-3057(97)00204-8 | CrossRef
 Elsevier ::  AbsPDF
 Sheats JR, Chang YL, Roitman DB & Stocking A,
Chemical Aspects of Polymeric Electroluminescent Devices
Acc. Chem. Res. 32 (3), 193-200 (1999);
DOI ::  10.1021/ar980061q | CrossRef
 ACS ::  Full . PDF
 Lu W, Fadeev AG, Qi BH, Smela E, Mattes BR, Ding J, Spinks GM, Mazurkiewicz J, Zhou DZ, Wallace GG, MacFarlane DR, Forsyth SA & Forsyth M,
Use of Ionic Liquids for -Conjugated Polymer Electrochemical Devices
Science 297 (5583), 983-987 (2002);
DOI :: 10.1126/science.1072651 | CrossRef
 AAAS ::  AbsFull . PDF . Supp.Info.
 Kanungo M, Kumar A & Contractor AQ,
Microtubule Sensors and Sensor Array Based on Polyaniline Synthesized in the Presence of Poly(styrene sulfonate)
Anal. Chem. 75 (21), 5673-5679 (2003);
DOI :: 10.1021/ac034537h | CrossRef
 ACS ::  AbsFull . PDF
 Hohnholz D, Okuzaki H & MacDiarmid AG,
Plastic Electronic Devices Through Line Patterning of Conducting Polymers  
Adv. Funct. Mater. 15 (1), 51-56 (2005).
DOI :: 10.1002/adfm.200400241 | CrossRef
 Wiley-VCH ::  Abs . Refs. PDF
12Pan LJ, Pu L, Shi Y, Sun T, Zhang R & Zheng YD,
Hydrothermal Synthesis of Polyaniline Mesostructures
Adv. Funct. Mater. 16 (10), 1279 (2006).
DOI :: 10.1002/adfm.200500543 | CrossRef
 Wiley-VCH ::  Abs . Refs . PDF
13Pan LJ, Pu L, Shi Y, Song SY, Xu Z, Zhang R & Zheng YD,
Synthesis of Polyaniline Nanotubes with a Reactive Template of Manganese Oxide
Adv. Mater. 19 (3), 461-464 (2007).
 DOI :: 10.1002/adma.200602073 | CrossRef
 Wiley-VCH ::  Cover Story . Abs . Refs . PDF . Supp.Info.
14Yuan JK, Li WN, Gomez S & Suib SL,
Shape-Controlled Synthesis of Manganese Oxide Octahedral Molecular Sieve Three-Dimensional Nanostructures
J. Am. Chem. Soc. 127 (41), 14184-14185 (2005).
 DOI ::  10.1021/ja053463j | CrossRef
 ACS ::   Abs . Full . PDF
15Zheng DS, Sun SX, Fan WL, Yu HY, Fan CH, Cao GX, Yin ZL & Song XY,
One-Step Preparation of Single-Crystalline β–MnO2 Nanotubes.
J. Phys. Chem. B 109 (34), 16439-16443 (2005).
 DOI ::  10.1021/jp052370l | CrossRef
 ACS ::  Abs . Full . PDF . Supp.Info.
16 
 Wang X & Li YD,
Synthesis and Formation Mechanism of Manganese Dioxide Nanowires/Nanorods 
Chem. Eur. J. 9 (1), 300-306 (2003).
 DOI :: 10.1002/chem.200390024 | CrossRef
 Wiley-VCH ::  Abs . Refs . Full . PDF 
 Wang X & Li YD,
Selected-Control Hydrothermal Synthesis of α- and β-MnO2 Single Crystal Nanowires
J. Am. Chem. Soc. 124 (12), 2880 (2002).
 DOI :: 10.1021/ja0177105 | CrossRef
 ACS ::  Abs . Full . PDF 
 
17 
 Active group on the mesostructural materials of manganese oxide: 
The research group of Prof. Steven L. Suib gives great attention on the fabrication of mesostructural MnOx and the derivates.
(1)Shen YF, Zerger RP, DeGuzman RN, Suib SL, McCurdy L, Potter DI & O'Yang CL,
Science 260 (5107), 511 (1993);
Manganese Oxide Octahedral Molecular Sieves: Preparation, Characterization, and Applications
 DOI :: 10.1126/science.260.5107.511 | CrossRef
 AAAS ::  Abs . Refs . PDF 
(2)Giraldo O, Brock SL, Marquez M, Suib SL, Hillhouse H & Tsapatsis M,
Nature 405 (6782), 38-38 (2000);
Materials: Spontaneous formation of inorganic helices
 DOI :: 10.1038/- | CrossRef
 NPG ::  TOC . PDF | Nature online misses the weblink of this paper. Herein the PDF link is of an notes on the same page.
(3)Giraldo O, Brock SL, Wills WS, Marquez M, Suib SL & Ching S,
Manganese Oxide Thin Films with Fast Ion-Exchange Properties
J. Am. Chem. Soc. 122 (38), 9330-9331 (2000);

 DOI :: 10.1021/ja001860i | CrossRef
 ACS ::  Full . PDF 
(4)Son YC, Makwana VD, Howell AR, Suib SL,
Angew. Chem. 113, 4410 (2001);
Angew. Chem. Int. Ed. 40 (22), 4280-4283 (2001);
Efficient, Catalytic, Aerobic Oxidation of Alcohols with Octahedral Molecular Sieves
 DOI :: 10.1002/1521-3773(20011119)40:22<4280::AID-ANIE4280>3.0.CO;2-L | CrossRef
 Wiley-VCH ::  Abs . Refs . Full . PDF 
(5) Giraldo O, Durand JP, Ramanan H, Laubernds K, Suib SL, Tsapatsis M, Brock SL & Marquez M,
Angew. Chem. 115, 3011 (2003);
Angew. Chem. Int. Ed. 42 (25), 2905-2909 (2003);
Dynamic Organization of Inorganic Nanoparticles into Periodic Micrometer-Scale Patterns
 DOI :: 10.1002/anie.200250712 | CrossRef
 Wiley-VCH ::  Abs . Refs . Full . PDF 
(6)Yuan JK, Laubernds K, Villegas J, Gomez S & Suib SL,
Adv. Mater. 16 (19), 1729-1732 (2004);
Spontaneous Formation of Inorganic Paper-Like Materials
 DOI :: 10.1002/adma.200400659 | CrossRef
 Wiley-VCH ::  Abs . Refs . Full . PDF 
(7) Shen XF, Ding YS, Liu J, Cai J, Laubernds K, Zerger RP, Vasiliev A, Aindow M & Suib SL,
Adv. Mater. 17 (7), 805-809 (2005);
Control of Nanometer-Scale Tunnel Sizes of Porous Manganese Oxide Octahedral Molecular Sieve Nanomaterials
 DOI :: 10.1002/chem.200390024 | CrossRef
 Wiley-VCH ::  Abs . Refs . PDF 
(8) Ding YS, Shen XF, Gomez S, Luo H, Aindow M & Suib SL,
Adv. Funct. Mater. 16 (4), 549-555 (2006);
 
Hydrothermal Growth of Manganese Dioxide into Three-Dimensional Hierarchical Nanoarchitectures
----
on
ε-MnO2
 DOI :: 10.1002/adfm.200500436 | CrossRef
 Wiley-VCH ::  Abs . Refs . PDF 
(9)Li WN, Yuan JK, Shen XF, Gomez-Mower S, Xu LP, Sithambaram S, Aidow M & Suib SL, 
Hydrothermal Synthesis of Structure- and Shape-Controlled Manganese Oxide Octahedral Molecular Sieve Nanomaterials
Adv. Funct. Mater. 16, 1247-1253 (2006). 
 DOI :: 10.1002/adfm.200500504
 | CrossRef
 Wiley-VCH ::  Abs . Refs . PDF 
  
18Armstrong AR & Bruce PG,
Nature 381 (6582), 499-500 (1996).

Synthesis of layered LiMnOas an electrode for rechargeable lithium batteries
 DOI :: 10.1038/381499a0 | CrossRef
 NPG ::  Abs . Refs . PDF 
19 
(1) Winter M, Besenhard JO, Spahr ME & Novák P,
Adv. Mater. 10 (10), 725-763 (1998);
Insertion Electrode Materials for Rechargeable Lithium Batteries
 DOI :: 10.1002/(SICI)1521-4095(199807)10:10<725::AID-ADMA725>3.0.CO;2-Z | CrossRef
 Wiley-VCH ::  Abs . PDF 
(2) Ammundsen B & Paulsen J,
Adv. Mater. 13 (12-13), 943-956 (2001);
Novel Lithium-Ion Cathode Materials Based on Layered Manganese Oxides
 DOI :: 10.1002/1521-4095(200107)13:12/13<943::AID-ADMA943>3.0.CO;2-J | CrossRef
 Wiley-VCH ::  Abs . PDF 
(3)Ma R, Bando Y, Zhang L & Sasaki T,
Adv. Mater. 16 (11), 918-922 (2004).
Layered MnO2 Nanobelts: Hydrothermal Synthesis and Electrochemical Measurements
 DOI :: 10.1002/adma.200306592 | CrossRef
 Wiley-VCH ::  Abs . Refs . PDF 
  

 

Citation

 

Lin PU, Logic of Polyaniline Nanotubes, Scidea Sketch 1 (2), ss20070129a1 (2007).
doi: 10.3128/ ss20070129a1 | Scidea ::  Abs . FullCrossRef
Scidea Sketch :: ISSN: 1992 - 8548
 

 

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