Spectroscopy — Superexchange Charge Transport in Loaded Metal Organic Frameworks

Measurement evidence

Spectroscopy

Superexchange Charge Transport in Loaded Metal Organic Frameworks · Neumann T., Liu J., Wachter T. et al. · ACS Nano · 2016 · 7085-7093

5 measurement groups · 24 results

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

Infrared reflection absorption spectroscopy (IRRAS)

F4-TCNQ-loaded HKUST-1 SURMOF, 5 spray cycles · Thin Film

Bruker VERTEX 80v, grazing-incidence reflection at 80 degrees relative to surface normal, 2 cm-1 resolution, MCT detector.

Context
F4-TCNQ-loaded sample compared with pristine and drop-cast F4-TCNQ reference
Measurement source
7089 · Results and Discussion · Figure 4d
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
F4-TCNQ C=N stretch reference2227 cm-1Text
Exact Reported
7089 · Results and Discussion · Figure 4d
F4-TCNQ-loaded HKUST-1 C=N split band2222 cm-1Text
Exact Reported
7089 · Results and Discussion · Figure 4d
F4-TCNQ-loaded HKUST-1 C=N split band2185 cm-1Text
Exact Reported
7089 · Results and Discussion · Figure 4d

Infrared reflection absorption spectroscopy (IRRAS)

TCNQ-loaded HKUST-1 SURMOF, 10 spray cycles · Thin Film

Bruker VERTEX 80v, grazing-incidence reflection at 80 degrees relative to surface normal, 2 cm-1 resolution, MCT detector.

Context
TCNQ-loaded sample compared with pristine and drop-cast TCNQ reference
Measurement source
7089 · Results and Discussion · Figure 4c
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
HKUST-1 COO asymmetric IRRAS band1656 cm-1Text
Exact Reported
7089 · Results and Discussion · Figure 4c
HKUST-1 COO symmetric IRRAS band1455 cm-1Text
Exact Reported
7089 · Results and Discussion · Figure 4c
HKUST-1 COO symmetric IRRAS band1386 cm-1Text
Exact Reported
7089 · Results and Discussion · Figure 4c
Drop-cast TCNQ C=N stretch reference2227 cm-1Text
Exact Reported
7089 · Results and Discussion · Figure 4c
TCNQ-loaded HKUST-1 C=N split band2200 cm-1Text
Exact Reported
7089 · Results and Discussion · Figure 4c
TCNQ-loaded HKUST-1 C=N split band2165 cm-1Text
Exact Reported
7089 · Results and Discussion · Figure 4c
TCNQ-loaded HKUST-1 new C=C ring stretch band1354 cm-1Text
Exact Reported
7089 · Results and Discussion · Figure 4c

Raman spectroscopy

F4-TCNQ-loaded HKUST-1 SURMOF, 5 spray cycles · Thin Film

Bruker Senterra Raman microscope, 532 nm excitation, 60 s integration, 3 co-additions.

Context
F4-TCNQ-loaded 5-cycle sample compared with pristine and drop-cast F4-TCNQ reference
Measurement source
S10-S11 · 2.3.2 Characterization by vibrational spectroscopies · Figure S8
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Drop-cast F4-TCNQ Raman C=N stretch2225 cm-1Text
Exact Reported
S10 · 2.3.2 Characterization by vibrational spectroscopies · Figure S8
F4-TCNQ-loaded Raman C=N stretch shift2225 cm-1 shifted to 2235 cm-1Text
Exact Reported
S10 · 2.3.2 Characterization by vibrational spectroscopies · Figure S8
F4-TCNQ-loaded Raman C=C ring stretch shift1662 cm-1 shifted to 1644 cm-1Text
Exact Reported
S10 · 2.3.2 Characterization by vibrational spectroscopies · Figure S8
F4-TCNQ-loaded Raman C=C wing stretch shift1454 cm-1 shifted to 1392 cm-1Text
Exact Reported
S10 · 2.3.2 Characterization by vibrational spectroscopies · Figure S8

Raman spectroscopy

TCNQ-loaded HKUST-1 SURMOF, 10 spray cycles · Thin Film

Bruker Senterra Raman microscope, 532 nm excitation, 60 s integration, 3 co-additions.

Context
TCNQ-loaded 10-cycle sample compared with pristine and drop-cast TCNQ reference
Measurement source
S3-S7 · 1.5; 2.1.2 Characterization by vibrational spectroscopies · Figure S4
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
Drop-cast TCNQ Raman C=N stretch2226 cm-1Text
Exact Reported
S7 · 2.1.2 Characterization by vibrational spectroscopies · Figure S4
TCNQ-loaded Raman C=N split band2222 cm-1Text
Exact Reported
S7 · 2.1.2 Characterization by vibrational spectroscopies · Figure S4
TCNQ-loaded Raman C=N split band2208 cm-1Text
Exact Reported
S7 · 2.1.2 Characterization by vibrational spectroscopies · Figure S4
New TCNQ-loaded Raman band1270 cm-1Text
Exact Reported
S7 · 2.1.2 Characterization by vibrational spectroscopies · Figure S4
New TCNQ-loaded Raman band1330 cm-1Text
Exact Reported
S7 · 2.1.2 Characterization by vibrational spectroscopies · Figure S4
New TCNQ-loaded Raman band1638 cm-1Text
Exact Reported
S7 · 2.1.2 Characterization by vibrational spectroscopies · Figure S4
TCNQ C=C ring stretch shift after loading1601 cm-1 shifted to 1605 cm-1Text
Exact Reported
S7 · 2.1.2 Characterization by vibrational spectroscopies · Figure S4
TCNQ C=C wing stretch shift after loading1454 cm-1 shifted to 1374 cm-1Text
Exact Reported
S7 · 2.1.2 Characterization by vibrational spectroscopies · Figure S4

ToF-SIMS depth profiling

TCNQ-loaded HKUST-1 SURMOF, 20 spray cycles · Thin Film

TOF.SIMS5 with Bi3+ primary ion pulses at 25 keV; C60+ erosion at 20 keV, 1.1 nA over 750 x 750 um2; UHV base pressure <1e-8 mbar.

Atmosphere
UHV
Context
TCNQ-loaded depth-profile sample
Measurement source
S4-S8 · 1.5; 2.1.3 Time-of-flight secondary ion mass spectrometry · Figure S5
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
TCNQ depth homogeneityhomogeneous loading throughout the entire depth of the HKUST-1 SURMOFText
Qualitative
S8 · 2.1.3 Time-of-flight secondary ion mass spectrometry · Figure S5
ToF-SIMS sputter equilibrium fluence3.5 x 10^13 ions/cm2Text
Exact Reported
S8 · 2.1.3 Time-of-flight secondary ion mass spectrometry · Figure S5