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745944

Sigma-Aldrich

D102 Dye

95% (HPLC)

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About This Item

Fórmula empírica (Notação de Hill):
C37H30N2O3S2
Número CAS:
Peso molecular:
614.78
Código UNSPSC:
12352103
ID de substância PubChem:
NACRES:
NA.23

Ensaio

95% (HPLC)

forma

powder

pf

238-243 °C

λmax

499 nm in DMF

cadeia de caracteres SMILES

S=C(S/C1=C\C(C=C2)=CC3=C2N(C4=CC=C(C=C(C5=CC=CC=C5)C6=CC=CC=C6)C=C4)C7C3CCC7)N(CC(O)=O)C1=O

InChI

1S/C37H30N2O3S2/c40-35(41)23-38-36(42)34(44-37(38)43)22-25-16-19-33-31(21-25)29-12-7-13-32(29)39(33)28-17-14-24(15-18-28)20-30(26-8-3-1-4-9-26)27-10-5-2-6-11-27/h1-6,8-11,14-22,29,32H,7,12-13,23H2,(H,40,41)/b34-22-

chave InChI

XGMCROHUTRXETK-VQNDASPWSA-N

Descrição geral

D102 Dye is a low cost indoline based organic dye that can be used as a photosensitizer. Its power conversion efficiency is over 4% with a strong absorption coefficient (55800 Lmol-1cm-1 at 490nm). It has a high extinction coefficient in comparison to the ruthenium dye. It can improve the performance of electrochemical devices.

Aplicação

D102 Dye can be used as a sensitizing material that can be coated on the semiconducting electrode for the fabrication of metal-free dye sensitized solar cells.
Photosensitive Red dye having excellent photoelectric conversion efficiency as a metal-free dye. Efficiency of DSSC device - η > 5.4%
Cell area: 0.25 cm2 (0.5 cm × 0.5 cm)
TiO2 Thickness: 5 μm
TiO2: screen printing
Electrolyte: 0.1 M LiI; 0.05 M I2; 0.6 M Dimethyl propylimidazolium
Iodide; 0.05 M t-Butylpyridine in 3-Methoxypropionitrile
Light source: AM1.5
Counter Electrode: Pt/Cr spatter glass
Dye adsorption: 30 °C/ in 3 hr. (t-BuOH/acetonitrile soln.)

Informações legais

Product of Mitsubishi Paper Mills; Ltd

Pictogramas

Exclamation mark

Palavra indicadora

Warning

Frases de perigo

Classificações de perigo

Acute Tox. 4 Oral

Código de classe de armazenamento

11 - Combustible Solids

Classe de risco de água (WGK)

WGK 3

Ponto de fulgor (°F)

Not applicable

Ponto de fulgor (°C)

Not applicable


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Artigos

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While dye sensitization as the basis for color photography has been accepted for a very long time,1 attempts to use this principle for the conversion of solar light to electricity generally had resulted only in very low photocurrents, below 100 nA/cm

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