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Au(C4H9)2C6H3C20H2N4(C2H5)4(CH3)4C6H4I(1+)*BF4(1-)=Au(C4H9)2C6H3C20H2N4(C2H5)4(CH3)4C6H4IBF4 is a chemical with a specific purpose. Lookchem provides you with multiple data and supplier information of this chemical.

879417-15-9

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879417-15-9 Usage

Check Digit Verification of cas no

The CAS Registry Mumber 879417-15-9 includes 9 digits separated into 3 groups by hyphens. The first part of the number,starting from the left, has 6 digits, 8,7,9,4,1 and 7 respectively; the second part has 2 digits, 1 and 5 respectively.
Calculate Digit Verification of CAS Registry Number 879417-15:
(8*8)+(7*7)+(6*9)+(5*4)+(4*1)+(3*7)+(2*1)+(1*5)=219
219 % 10 = 9
So 879417-15-9 is a valid CAS Registry Number.

879417-15-9Upstream product

879417-15-9Downstream Products

879417-15-9Relevant academic research and scientific papers

Bridge-dependent electron transfer in porphyrin-based donor-bridge-acceptor systems

Kilsa,Kajanus,Macpherson,Martensson,Albinsson

, p. 3069 - 3080 (2001)

Photoinduced electron transfer in donor-bridge-acceptor systems with zinc porphyrin (or its pyridine complex) as the donor and gold(III) porphyrin as the acceptor has been studied. The porphyrin moieties were covalently linked with geometrically similar bridging chromophores which vary only in electronic structure. Three of the bridges are fully conjugated π-systems and in a fourth, the conjugation is broken. For systems with this bridge, the quenching rate of the singlet excited state of the donor was independent of solvent and corresponded to the rate of singlet energy transfer expected for a Foerster mechanism. In contrast, systems with a π-conjugated bridging chromophore show a solvent-dependent quenching rate that suggests electron transfer in the Marcus normal region. This is supported by picosecond transient absorption measurements, which showed formation of the zinc porphyrin radical cation only in systems with π-conjugated bridging chromophores. On the basis of the Marcus and Rehm-Weller equations, an electronic coupling of 5-20 cm-1 between the donor and acceptor is estimated for these systems. The largest coupling is found for the systems with the smallest energy gap between the donor and bridge singlet excited states. This is in good agreement with the coupling calculated with quantum mechanical methods, as is the prediction of an almost zero coupling in the systems with a nonconjugated bridging chromophore.

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