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[Co(dibenzoylmethane-H)2(2,4,6-tris(4-pyridyl)-1,3,5-triazine)](n)*nTHF is a chemical with a specific purpose. Lookchem provides you with multiple data and supplier information of this chemical.

949573-41-5

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949573-41-5 Usage

Check Digit Verification of cas no

The CAS Registry Mumber 949573-41-5 includes 9 digits separated into 3 groups by hyphens. The first part of the number,starting from the left, has 6 digits, 9,4,9,5,7 and 3 respectively; the second part has 2 digits, 4 and 1 respectively.
Calculate Digit Verification of CAS Registry Number 949573-41:
(8*9)+(7*4)+(6*9)+(5*5)+(4*7)+(3*3)+(2*4)+(1*1)=225
225 % 10 = 5
So 949573-41-5 is a valid CAS Registry Number.

949573-41-5Downstream Products

949573-41-5Relevant academic research and scientific papers

Preparation and structure of three solvatomorphs of the polymer [Co(dbm)2(4ptz)]n: Spin canting depending on the supramolecular organization

Barrios, Leoni A.,Ribas, Joan,Aromi, Guillem,Ribas-Arino, Jordi,Gamez, Patrick,Roubeau, Olivier,Teat, Simon J.

, p. 7154 - 7162 (2007)

The syntheses and X-ray structures of three isomeric 1D coordination polymers are reported. The complex [Co-(dbm)2(MeOH)2] (1) was used as a precursor in these reactions. The preparation and structure of 1 is also presented; this mononuclear complex is in the cis configuration because this allows the formation of a network of intermolecular hydrogen bonds in the solid state. Reaction of 1 with 2,4,6-tris-(4-pyridyl)-1,3,5-triazine (4ptz) yields the polymers [Co(dbm)2(4ptz)]n·nTHF (2a), [Co(dbm)2(4ptz)]n·0.75nTHF·0.5nEt 2O (2b), and [Co(dbm)2(4ptz)]n-3nDMF (2c) in the form of zigzag chains, instead of the expected honeycomb architectures. This is because of the establishment of extended π-π stacking throughout these solids, which could not have occurred otherwise. Compounds 2a, 2b, and 2c are solvatomorphs, and formation of either one of them depends on the exact conditions of crystallization, which lead to significant differences in the supramolecular organization of the chains. Bulk magnetic measurements on 2a reveal weak antiferromagnetic exchange within the chains and small ordering throughout the solid that results in the manifestation of the phenomenon of spin canting, whereas for 2c the different supramolecular organization causes the antiferromagnetic exchange not to result in spin canting.

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