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12010-49-0

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12010-49-0 Usage

Check Digit Verification of cas no

The CAS Registry Mumber 12010-49-0 includes 8 digits separated into 3 groups by hyphens. The first part of the number,starting from the left, has 5 digits, 1,2,0,1 and 0 respectively; the second part has 2 digits, 4 and 9 respectively.
Calculate Digit Verification of CAS Registry Number 12010-49:
(7*1)+(6*2)+(5*0)+(4*1)+(3*0)+(2*4)+(1*9)=40
40 % 10 = 0
So 12010-49-0 is a valid CAS Registry Number.

12010-49-0SDS

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 bismuth,lutetium

1.2 Other means of identification

Product number -
Other names Lutetium bismuthide

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:12010-49-0 SDS

12010-49-0Downstream Products

12010-49-0Relevant articles and documents

Supercooling of In2Bi and InBi melts

Aleksandrov,Frolova

, p. 227 - 230 (2004)

The effect of melt overheating ΔT+ on the critical supercooling ΔT- of liquid In2Bi and InBi is studied by cyclic thermal analysis. It is shown that, the ΔT- for In2Bi is ?2.0 K, independent of the me

Crystal structure of InBi under pressure up to 75 GPa

Degtyareva,Winzenick,Holzapfel

, p. 4975 - 4978 (2008/10/08)

InBi is studied by energy-dispersive diffraction with synchrotron radiation in a diamond-anvil cell under pressure up to 75 GPa. Three phase transitions are observed from its initial tetragonal structure tP4 with c/a≈0.95 to another tP4 structure with c/a≈0.65 typical for the β-Np structure, than to a disordered tetragonal body-centered structure tI2, and finally some hints are obtained for a transition to a cubic body-centered structure cI2. All these transformations are reversible with large hysteresis. InBi(tI2), phase III, shows initially a steep increase in c/a from 0.91 to 0.94, in the pressure range from 20 to 30 GPa, and a nearly constant value of about 0.96 above 55 GPa. Hints for the possible stability of a new phase IV are noticed in the present experiments on decompression from 75 GPa as admixture of new lines to phase III giving strong indications for a first-order phase transition with large hysteresis. The origin of the tetragonal distortion and the transformation to a cubic phase are discussed from the point of view of nesting the Fermi sphere in the Brillouin zone.

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