Spectroscopy — Conductive MOFs with tailored polarization loss for broadband absorption at ultrathin thickness

Measurement evidence

Spectroscopy

Conductive MOFs with tailored polarization loss for broadband absorption at ultrathin thickness · Zhang W., Luo J., Shi J. et al. · Nano Research · 2025 · 94907919

2 measurement groups · 13 results

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

FT-IR spectroscopy

CuM-HHTP sample set · Powder

NICOLET NEXUS-670; 4000-400 cm-1 range.

Context
pristine bimetallic conductive MOF powders
Measurement source
1 · Characterizations
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
FTIR C=O vibration1633 cm-1Text
Rounded Reported
3 · 3.1 · Fig. 1(c)
FTIR C-OH vibration990 cm-1Text
Rounded Reported
3 · 3.1 · Fig. 1(c)
FTIR metal-oxygen coordination band530 cm-1Text
Rounded Reported
3 · 3.1 · Fig. 1(c)
FTIR O-H stretching vibration3430 cm-1Text
Rounded Reported
3 · 3.1 · Fig. 1(c)

X-ray photoelectron spectroscopy

CuZn-1 · Powder

THERMO SCIENTIFIC ESCALAB 250Xi; representative CuZn-1 survey, C 1s, Zn 2p, and Cu 2p spectra.

Context
pristine bimetallic conductive MOF powder
Measurement source
3-4 · 3.1 · Figs. 1(d)-1(g)
PropertyReported valueNormalised valueUncertaintyOrigin and qualitySource
C 1s C=O binding energy288.59 eVText
Exact Reported
3 · 3.1 · Fig. 1(e)
C 1s C-C/C=C binding energy284.80 eVText
Exact Reported
3 · 3.1 · Fig. 1(e)
C 1s C-O binding energy286.19 eVText
Exact Reported
3 · 3.1 · Fig. 1(e)
Cu+ 2p1/2 binding energy933.14 eVText
Exact Reported
4 · 3.1 · Fig. 1(g)
Cu+ 2p3/2 binding energy952.82 eVText
Exact Reported
4 · 3.1 · Fig. 1(g)
Cu2+ 2p1/2 binding energy934.76 eVText
Exact Reported
4 · 3.1 · Fig. 1(g)
Cu2+ 2p3/2 binding energy954.60 eVText
Exact Reported
4 · 3.1 · Fig. 1(g)
Zn 2p1/2 binding energy1022.57 eVText
Exact Reported
4 · 3.1 · Fig. 1(f)
Zn 2p3/2 binding energy1045.69 eVText
Exact Reported
4 · 3.1 · Fig. 1(f)