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136321-14-7

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136321-14-7 Usage

Check Digit Verification of cas no

The CAS Registry Mumber 136321-14-7 includes 9 digits separated into 3 groups by hyphens. The first part of the number,starting from the left, has 6 digits, 1,3,6,3,2 and 1 respectively; the second part has 2 digits, 1 and 4 respectively.
Calculate Digit Verification of CAS Registry Number 136321-14:
(8*1)+(7*3)+(6*6)+(5*3)+(4*2)+(3*1)+(2*1)+(1*4)=97
97 % 10 = 7
So 136321-14-7 is a valid CAS Registry Number.

136321-14-7SDS

SAFETY DATA SHEETS

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

Version: 1.0

Creation Date: Aug 18, 2017

Revision Date: Aug 18, 2017

1.Identification

1.1 GHS Product identifier

Product name methylsulfanylmethane

1.2 Other means of identification

Product number -
Other names (13C)2-dimethyl sulfide

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:136321-14-7 SDS

136321-14-7Upstream product

136321-14-7Downstream Products

136321-14-7Relevant articles and documents

Simulations of Chemical Exchange Lineshapes in CP/MAS Spectra Using Floquet Theory and Sparse Matrix Methods

Hazendonk,Bain, Alex D.,Grondey,Harrison,Dumont

, p. 33 - 42 (2000)

This paper presents a general method for simulating the effect of chemical exchange on MAS NMR spectra of solid samples. The complication in MAS spectra is that the Hamiltonian itself is time-dependent, due to the spinning of the sample. The approach taken in this work is to use Floquet theory to convert the problem into a time-independent form, and then use established methods (used in liquid NMR simulations) to calculate the lineshape. Floquet theory has been admired for its elegance, but criticized for its computational inefficiencies. This is because it removes the time dependence of the system by expanding the problem in a Fourier-like series. This makes a relatively small, time-dependent calculation into a much larger time-independent one. Typically, we use twice as many Floquet blocks as there are spinning sidebands, so the increase in size is substantial. The problem that this creates stems from the fact that the usual Householder methods for diagonalizing a matrix scale as the cube of the size of the matrix. This would make a Floquet calculation prohibitively long. However, the Floquet matrix is inherently sparse, so sparse matrix methods can produce substantial computational savings. Also, fully diagonalizing a matrix is expensive, but converting the matrix to a tridiagonal form (using iterative Lanczos methods) is much cheaper. The use of the Lanczos methods makes the Floquet calculations feasible as a general method for systems of more than one spin. We show how to set up the full matrix describing chemical exchange in a spinning sample, but the details of how the Lanczos methods work are not included - they are described elsewhere. We then validate the theory by simulating the MAS spectra of dimethyl sulfone both with natural abundance 13C and with methyl groups labeled with 13C. The latter system has both dipolar and chemical shielding anisotropy terms contributing to the spectrum.

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