Highly conductive metallophthalocyanine assemblies. Structure, charge transport, and anisotropy in the metal-free molecular metal H2(Pc)I

T. Inabe; T. J. Marks; R. L. Burton; J. W. Lyding; W. J. McCarthy; C. R. Kannewurf; G. M. Reisner; F. H. Herbstein

doi:10.1016/0038-1098(85)90656-8

Highly conductive metallophthalocyanine assemblies. Structure, charge transport, and anisotropy in the metal-free molecular metal H₂(Pc)I

T. Inabe, T. J. Marks, R. L. Burton, J. W. Lyding, W. J. McCarthy, C. R. Kannewurf, G. M. Reisner, F. H. Herbstein

Research output: Contribution to journal › Article › peer-review

Abstract

That a metal ion is not required for high electrical conductivity is unequivocally demonstrated by structural, charge transport, optical, and magnetic characterization of the simplest phthalocyanine "molecular metal" H₂(Pc)I. The crystal structure consists of staggered H₂(Pc)^+0.33 units stacked at 3.251(3) Å intervals and parallel chains of I^-₃ counterions. At 300 K, σ_{{norm of matrix}} = 700 Ω^-1 cm^-1 and σ_{{norm of matrix}} σ⊥ > 500. At 15 K, σ_∼ reaches a maximum of ca. 4000 Ω^-1 cm^-1 and falls only to ca. 3500 Ω^{-1{norm of matrix}} cm^-1 at 1.5 K. Analysis of single crystal polarized specular reflectance data (ir to uv) yields ω_p = 6360(30) cm^-1 and a tight-binding bandwidth of 1.3(1) eV. The magnetic susceptibility is Pauli-like (X_S = 2.21(5) × 10^-4 emu mol^-1) except for a small, sample dependent Curie component.

Original language	English (US)
Pages (from-to)	501-504
Number of pages	4
Journal	Solid State Communications
Volume	54
Issue number	6
DOIs	https://doi.org/10.1016/0038-1098(85)90656-8
State	Published - May 1985
Externally published	Yes

ASJC Scopus subject areas

Chemistry(all)
Condensed Matter Physics
Materials Chemistry

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Highly conductive metallophthalocyanine assemblies. Structure, charge transport, and anisotropy in the metal-free molecular metal H₂(Pc)I. / Inabe, T.; Marks, T. J.; Burton, R. L.; Lyding, J. W.; McCarthy, W. J.; Kannewurf, C. R.; Reisner, G. M.; Herbstein, F. H.

In: Solid State Communications, Vol. 54, No. 6, 05.1985, p. 501-504.

Research output: Contribution to journal › Article › peer-review

@article{8e55c916f5534e78be584a9ca15861e0,

title = "Highly conductive metallophthalocyanine assemblies. Structure, charge transport, and anisotropy in the metal-free molecular metal H2(Pc)I",

abstract = "That a metal ion is not required for high electrical conductivity is unequivocally demonstrated by structural, charge transport, optical, and magnetic characterization of the simplest phthalocyanine {"}molecular metal{"} H2(Pc)I. The crystal structure consists of staggered H2(Pc)+0.33 units stacked at 3.251(3) {\AA} intervals and parallel chains of I-3 counterions. At 300 K, σ{norm of matrix} = 700 Ω-1 cm-1 and σ{norm of matrix} σ⊥ > 500. At 15 K, σ∼ reaches a maximum of ca. 4000 Ω-1 cm-1 and falls only to ca. 3500 Ω-1{norm of matrix} cm-1 at 1.5 K. Analysis of single crystal polarized specular reflectance data (ir to uv) yields ωp = 6360(30) cm-1 and a tight-binding bandwidth of 1.3(1) eV. The magnetic susceptibility is Pauli-like (XS = 2.21(5) × 10-4 emu mol-1) except for a small, sample dependent Curie component.",

author = "T. Inabe and Marks, {T. J.} and Burton, {R. L.} and Lyding, {J. W.} and McCarthy, {W. J.} and Kannewurf, {C. R.} and Reisner, {G. M.} and Herbstein, {F. H.}",

note = "Funding Information: This research was supported by the NSF through the Northwestern Materials Research Center (Grant DMR82-16972, TJM and CRK), by the Office of Naval Research (TJM), and by the U.S.-Israel Binatlonal Science Foundation (Grant 2281/80, FHH and TJM). We are grateful to Dr. P. Bauer-schmldt and Mr. H. Scbarf (Carl Zelss) and Dr. K. Krlshnan (Digilab) for generous assistance with the reflectivity measurements.",

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doi = "10.1016/0038-1098(85)90656-8",

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T1 - Highly conductive metallophthalocyanine assemblies. Structure, charge transport, and anisotropy in the metal-free molecular metal H2(Pc)I

AU - Inabe, T.

AU - Marks, T. J.

AU - Burton, R. L.

AU - Lyding, J. W.

AU - McCarthy, W. J.

AU - Kannewurf, C. R.

AU - Reisner, G. M.

AU - Herbstein, F. H.

N1 - Funding Information: This research was supported by the NSF through the Northwestern Materials Research Center (Grant DMR82-16972, TJM and CRK), by the Office of Naval Research (TJM), and by the U.S.-Israel Binatlonal Science Foundation (Grant 2281/80, FHH and TJM). We are grateful to Dr. P. Bauer-schmldt and Mr. H. Scbarf (Carl Zelss) and Dr. K. Krlshnan (Digilab) for generous assistance with the reflectivity measurements.

PY - 1985/5

Y1 - 1985/5

N2 - That a metal ion is not required for high electrical conductivity is unequivocally demonstrated by structural, charge transport, optical, and magnetic characterization of the simplest phthalocyanine "molecular metal" H2(Pc)I. The crystal structure consists of staggered H2(Pc)+0.33 units stacked at 3.251(3) Å intervals and parallel chains of I-3 counterions. At 300 K, σ{norm of matrix} = 700 Ω-1 cm-1 and σ{norm of matrix} σ⊥ > 500. At 15 K, σ∼ reaches a maximum of ca. 4000 Ω-1 cm-1 and falls only to ca. 3500 Ω-1{norm of matrix} cm-1 at 1.5 K. Analysis of single crystal polarized specular reflectance data (ir to uv) yields ωp = 6360(30) cm-1 and a tight-binding bandwidth of 1.3(1) eV. The magnetic susceptibility is Pauli-like (XS = 2.21(5) × 10-4 emu mol-1) except for a small, sample dependent Curie component.

AB - That a metal ion is not required for high electrical conductivity is unequivocally demonstrated by structural, charge transport, optical, and magnetic characterization of the simplest phthalocyanine "molecular metal" H2(Pc)I. The crystal structure consists of staggered H2(Pc)+0.33 units stacked at 3.251(3) Å intervals and parallel chains of I-3 counterions. At 300 K, σ{norm of matrix} = 700 Ω-1 cm-1 and σ{norm of matrix} σ⊥ > 500. At 15 K, σ∼ reaches a maximum of ca. 4000 Ω-1 cm-1 and falls only to ca. 3500 Ω-1{norm of matrix} cm-1 at 1.5 K. Analysis of single crystal polarized specular reflectance data (ir to uv) yields ωp = 6360(30) cm-1 and a tight-binding bandwidth of 1.3(1) eV. The magnetic susceptibility is Pauli-like (XS = 2.21(5) × 10-4 emu mol-1) except for a small, sample dependent Curie component.

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