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757330

Sigma-Aldrich

Tin(IV) 2,3-naphthalocyanine dichloride

99%

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About This Item

Empirical Formula (Hill Notation):
C48H24Cl2N8Sn
CAS Number:
Molecular Weight:
902.37
UNSPSC Code:
12352103
NACRES:
NA.23

assay

99%

form

solid

mp

>300 °C (lit.)
>500 °C

λmax

~875 nm (film)(lit.)

SMILES string

Cl[Sn]1(Cl)n2c3nc4nc(nc5n1c(nc6nc(nc2c7cc8ccccc8cc37)c9cc%10ccccc%10cc69)c%11cc%12ccccc%12cc5%11)c%13cc%14ccccc%14cc4%13

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General description

Tin(IV) 2,3-naphthalocyanine dichloride (SnNcCl2) belongs to the family of metal based phthalocyanines. They are widely used as an electron donor material in organic photovoltaic (OPV) cells. The use of SnNcCl2 in OPVs increases its power conversion efficiencies since it absorbs light in the near infrared and infra-red portions of the electromagnetic spectrum which accounts for 50% of the solar photon flux.[1]

application

Used as an electron donor material in Organic Photovoltaic (OPV) Cells.[1][2]

Features and Benefits

Has a narrow energy gap which helps in optical absorption beyond a wavelength of 1100 nm in the infrared region.[1]

pictograms

Skull and crossbones

signalword

Danger

Hazard Classifications

Acute Tox. 3 Dermal - Acute Tox. 3 Inhalation - Acute Tox. 3 Oral - Eye Irrit. 2 - Skin Irrit. 2 - STOT SE 3

target_organs

Respiratory system

Storage Class

6.1C - Combustible acute toxic Cat.3 / toxic compounds or compounds which causing chronic effects

wgk_germany

WGK 3

flash_point_f

Not applicable

flash_point_c

Not applicable


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Tandem organic photodetectors with tunable, broadband response.
Menke, S. M., Pandey, R., & Holmes, R. J.
Applied Physics Letters, 101(22), 223-301 (2012)
Tin naphthalocyanine complexes for infrared absorption in organic photovoltaic cells
Pandey, R., Kerner, R. A., Menke, S. M., Holst, J., Josyula, K. V., & Holmes, R. J.
Organic Electronics, 14(3), 804-808 (2013)

Articles

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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