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BIS(ETHYLBENZENE)CHROMIUM [MIXTURE OF (C2H5)XC6H6-X WHERE X = 0-4)] is a chemical with a specific purpose. Lookchem provides you with multiple data and supplier information of this chemical.

12212-68-9

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12212-68-9 Usage

Check Digit Verification of cas no

The CAS Registry Mumber 12212-68-9 includes 8 digits separated into 3 groups by hyphens. The first part of the number,starting from the left, has 5 digits, 1,2,2,1 and 2 respectively; the second part has 2 digits, 6 and 8 respectively.
Calculate Digit Verification of CAS Registry Number 12212-68:
(7*1)+(6*2)+(5*2)+(4*1)+(3*2)+(2*6)+(1*8)=59
59 % 10 = 9
So 12212-68-9 is a valid CAS Registry Number.

12212-68-9SDS

SAFETY DATA SHEETS

According to Globally Harmonized System of Classification and Labelling of Chemicals (GHS) - Sixth revised edition

Version: 1.0

Creation Date: Aug 19, 2017

Revision Date: Aug 19, 2017

1.Identification

1.1 GHS Product identifier

Product name bis(η-ethylbenzene)chromium(0)

1.2 Other means of identification

Product number -
Other names .Bis(

1.3 Recommended use of the chemical and restrictions on use

Identified uses For industry use only.
Uses advised against no data available

1.4 Supplier's details

1.5 Emergency phone number

Emergency phone number -
Service hours Monday to Friday, 9am-5pm (Standard time zone: UTC/GMT +8 hours).

More Details:12212-68-9 SDS

12212-68-9Relevant academic research and scientific papers

Gas-phase electronic absorption spectroscopy of substituted bis(η6-benzene)chromium derivatives: Rydberg transitions in bis(η6-anisole)chromium and bis(η6-2,6- dimethylpyridine)chromium

Ketkov,Domrachev,Ob'edkov,Vasil'kov,Yur'eva,Mehnert

, p. 1932 - 1937 (2004)

Gas-phase electronic absorption spectra of chromium bisarene complexes with oxygen- and nitrogen-containing ligands, (η6-PhOMe) 2Cr (1) and (η6-2,6-Me2C5H 3N)2Cr (2), were first measured. Rydberg bands disappearing on going to the condensed-phase spectra were revealed. The first ionization potentials of complexes 1 and 2 (5.30 and 5.40 eV, respectively) were determined from the Rydberg frequencies. The Rydberg transitions were assigned and the corresponding Rydberg term values and quantum defects were determined. The effect of heteroatoms on the Rydberg structure parameters was revealed by comparing the spectra of complexes 1 and 2 with those of unsubstituted analogs. The appearance, in the ligand side chain, of an oxygen atom capable of being involved in conjugation with the π-electron system of the aromatic ring results in substantial broadening of the observed Rydberg bands. This can be associated with an increased ligand contribution to the HOMO of the sandwich compound. The influence of the oxygen atom on the ionization energy of the molecule is insignificant. In contrast to this, introduction of a nitrogen atom into the carbocycle leads to a noticeable increase in the ionization potential of the molecule, while the ligand contribution to the HOMO of the complex remains practically unchanged.

Zero kinetic energy spectroscopy: Mass-analyzed threshold ionization spectra of chromium sandwich complexes with alkylbenzenes, (η6- RPh)2Cr (R = Me, Et, i-Pr, t-Bu)

Ketkov, Sergey Y.,Selzle, Heinrich L.,Cloke, F. Geoffrey N.,Markin, Gennady V.,Shevelev, Yury A.,Domrachev, Georgy A.,Schlag, Edward W.

, p. 11298 - 11303 (2011/02/16)

For over 25 years zero kinetic energy (ZEKE) spectroscopy has yielded a rich foundation of high-resolution results of molecular ions. This was based on the discovery in the late 60's of long-lived ion states throughout the ionization continuum of molecular ions. Here, an example is chosen from another fundamental system pioneered at this university. The mass-analyzed threshold ionization (MATI) spectra of jet-cooled chromium bisarene complexes (η6-RPh)2Cr (R = Me (1), Et (2), i-Pr (3), and t-Bu (4)) have been measured and interpreted on the basis of DFT calculations. The MATI spectra of complexes 1 and 2 appear to reveal features arising from ionizations of the isomers formed by the rotation of one arene ring relative to the other. The 1 and 2 MATI spectra show two intense peaks corresponding to the 000 ionizations with inverse intensity ratios. As indicated by the DFT calculations, the intensity ratio change on going from 1 to 2 results from different isomers contributing to each MATI peak. The ionization energies corresponding to the 000 peaks are 42746 ± 5 and 42809 ± 5 cm-1 for compound 1 and 42379 ± 5 and 42463 ± 5 cm-1 for complex 2. The 1 and 2 spectra show also the weaker features representing transitions to the vibrationally excited cationic levels, the signals of individual rotamers being detected and assigned on the basis of calculated vibrational frequencies. The MATI spectra of compounds 3 and 4 reveal only one strong peak because of close ionization potentials of the isomers contributing to the MATI signal. The 3 and 4 ionization energies are 42104 ± 5 and 41917 ± 5 cm-1, respectively. The precise values of ionization energies obtained from the MATI spectra reveal a nonlinear dependence of the IE on the number of Me groups in the alkyl substituents of (η6-RPh)2Cr. This can be explained by an increase in the molecular zero point energies on methylation of the substituents.

The electronic absorption spectra of the alkyl-substituted derivatives of bis(benzene)chromium(0) in the vapour phase

Domrachev, G. A.,Ketkov, S. Yu.,Razuvaev, G. A.

, p. 341 - 348 (2007/10/02)

The UV and visible absorption spectra of (arene)2chromium(0) (arene=benzene (I), toluene (II), ethylbenzene (III), cumene (IV), tert-butylbenzene (V), mesitylene (VI)) in the vapour phase have been invesigated.Four band systems A, B, C and D are revealed in the spectra.The bands of the system with the shortest wavelengths, D, represent the Rydberg series.The first ionisation potentials IPa1g of I-VI determined from the Rydberg band frequencies are 5.45, 5.29, 5.25, 5.21, 5.18 and 5.01 eV respectively.The Rydberg bands correspond to the allowed electrodipole transitions from the highest occupied moloecular orbital (MO) a1g to the vacant MO of either the a2u or e1u type.System C corresponds to the intense band of the solution spectra.The electronic transition e2g -> e*2u obviously makes a great contribution to this system.System B is assigned to the transition from a1g to vacant a2u or e1u MO, which can be Rydberg orbitals.System A can be assigned to the a1g -> e*2u transition or to the Rydberg transition, which is forbidden in the D6h point group but becomes allowed upon reduction of symmetry.

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