Spectroscopy — Cofacial Assembly of Metallomacrocycles as an Approach to Controlling Lattice Architecture in Low-Dimensional Molecular Solids. Chemical, Structural, Oxidation-State, Transport, and Optical Properties of the Coordination Polymer [Fe(phthalocyaninato)(μ-pyrazine)]n and the Consequences of Halogen Doping

Measurement evidence

Spectroscopy

Cofacial Assembly of Metallomacrocycles as an Approach to Controlling Lattice Architecture in Low-Dimensional Molecular Solids. Chemical, Structural, Oxidation-State, Transport, and Optical Properties of the Coordination Polymer [Fe(phthalocyaninato)(μ-pyrazine)]n and the Consequences of Halogen Doping · Diel B.N., Inabe T., Jaggi N.K. et al. · Journal of the American Chemical Society · 1984 · 3207-3214

4 measurement groups · 19 results

Reported values remain attached to the sample, method, conditions, extraction quality and source location that produced them.

X-band ESR spectroscopy

{[Fe(Pc)(mu-pyz)]I2.60}n · Pellet

Powder ESR of {[Fe(Pc)(pyz)]I2.29}n at room temperature and 77 K; 100 kHz field modulation; DPPH calibration.

Temperature
room temperature and 77 K
Geometry
powder sample
Context
iodine-doped target sample
Measurement source
3212 · Electron Spin Resonance Spectroscopy
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
ESR broad component linewidth at 77 Kca. 100 Gca.Text
Approximate
3212 · Electron Spin Resonance Spectroscopy
ESR g value at 77 Kg = 2.015Text
Exact Reported
3212 · Electron Spin Resonance Spectroscopy
ESR broad component linewidth at room temperatureapproximately 400 GapproximatelyText
Approximate
3212 · Electron Spin Resonance Spectroscopy
ESR g value at room temperatureg = 2.036Text
Exact Reported
3212 · Electron Spin Resonance Spectroscopy

transmission infrared and optical reflectance spectroscopy

{[Fe(Pc)(mu-pyz)]I2.60}n · Pellet

Transmission IR on Nujol mulls between KBr plates; reflectance 300-4000 cm^-1 using near-normal unpolarised radiation on pressed pellets.

Temperature
room temperature
Geometry
pressed pellets, 13 mm diameter and 0.75-1.0 mm thick for reflectance
Context
pristine and iodine-doped polymer samples
Measurement source
3211 · Doped Polymers. Transmission Infrared and Specular Reflectance Spectroscopy · Figures 3-4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
plasmalike reflectance feature in {[Fe(Pc)(pyz)]I2.60}nexceedingly weak and obscured by molecular features; no quantitative analysis undertakenText
Qualitative
3211 · Doped Polymers. Transmission Infrared and Specular Reflectance Spectroscopy · Figure 4

57Fe Mossbauer spectroscopy

Table V Fe(Pc)(pyz) Mossbauer series · Powder

Room temperature or 4.2 K constant-acceleration spectra; fitted to a single quadrupolar doublet.

Temperature
298 K and 4.2 K
Geometry
powder specimens with effective thickness 0.10-0.13 mg/cm2 of 57Fe
Context
precursor, pristine polymer and iodine-doped target samples
Measurement source
3211 · Mossbauer Spectroscopy · Table V
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Mossbauer isomer shift, pristine {[Fe(Pc)(pyz)]-0.3C6H5Cl}ndelta = 0.500 (2) mm/s at 298 K(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V
Mossbauer quadrupole splitting, pristine {[Fe(Pc)(pyz)]-0.3C6H5Cl}nQS = 2.054 (2) mm/s at 298 K(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V
Mossbauer isomer shift, Fe(Pc)(pyz)2delta = 0.500 (2) mm/s at 298 K(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V
Mossbauer quadrupole splitting, Fe(Pc)(pyz)2QS = 2.006 (2) mm/s at 298 K(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V
Mossbauer isomer shift, {[Fe(Pc)(pyz)]I0.77}n at 298 Kdelta = 0.500 (2) mm/s(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V
Mossbauer quadrupole splitting, {[Fe(Pc)(pyz)]I0.77}n at 298 KQS = 2.042 (2) mm/s(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V
Mossbauer isomer shift, {[Fe(Pc)(pyz)]I0.77}n at 4.2 Kdelta = 0.580 (2) mm/s(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V
Mossbauer quadrupole splitting, {[Fe(Pc)(pyz)]I0.77}n at 4.2 KQS = 1.900 (2) mm/s(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V
Mossbauer isomer shift, {[Fe(Pc)(pyz)]I2.54}ndelta = 0.491 (2) mm/s at 298 K(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V
Mossbauer quadrupole splitting, {[Fe(Pc)(pyz)]I2.54}nQS = 1.990 (2) mm/s at 298 K(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V
Mossbauer isomer shift, {[Fe(Pc)(pyz)]I2.76}ndelta = 0.498 (2) mm/s at 298 K(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V
Mossbauer quadrupole splitting, {[Fe(Pc)(pyz)]I2.76}nQS = 2.034 (2) mm/s at 298 K(2)Table
Exact Reported
3211 · Mossbauer Spectroscopy · Table V

resonance Raman spectroscopy

{[Fe(Pc)(mu-pyz)]I2.54}n, eq 5 · Pellet

Ar+ excitation at 5145 Angstrom; powders in spinning 5 mm Pyrex tubes; 180 deg backscattering geometry.

Geometry
powder in spinning Pyrex tube
Context
iodine-doped target samples
Measurement source
3210 · Doped Polymers. Resonance Raman Spectroscopy · Figure 2
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
resonance Raman polyiodide band107 cm^-1Text
Exact Reported
3210 · Doped Polymers. Resonance Raman Spectroscopy · Figure 2
resonance Raman polyiodide band173 cm^-1Text
Exact Reported
3210 · Doped Polymers. Resonance Raman Spectroscopy · Figure 2