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12254-85-2

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12254-85-2 Usage

Chemical Properties

tetr crystal(s); -60 mesh with 99% purity [LID94] [CER91]

Check Digit Verification of cas no

The CAS Registry Mumber 12254-85-2 includes 8 digits separated into 3 groups by hyphens. The first part of the number,starting from the left, has 5 digits, 1,2,2,5 and 4 respectively; the second part has 2 digits, 8 and 5 respectively.
Calculate Digit Verification of CAS Registry Number 12254-85:
(7*1)+(6*2)+(5*2)+(4*5)+(3*4)+(2*8)+(1*5)=82
82 % 10 = 2
So 12254-85-2 is a valid CAS Registry Number.
InChI:InChI=1/As.Cr/q-3;+3

12254-85-2 Well-known Company Product Price

  • Brand
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  • Alfa Aesar

  • (39205)  Chromium arsenide, 99% (metals basis)   

  • 12254-85-2

  • 5g

  • 651.0CNY

  • Detail
  • Alfa Aesar

  • (39205)  Chromium arsenide, 99% (metals basis)   

  • 12254-85-2

  • 25g

  • 5379.0CNY

  • Detail

12254-85-2SDS

SAFETY DATA SHEETS

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

Version: 1.0

Creation Date: Aug 11, 2017

Revision Date: Aug 11, 2017

1.Identification

1.1 GHS Product identifier

Product name arsanylidynechromium

1.2 Other means of identification

Product number -
Other names Chromium arsenide

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:12254-85-2 SDS

12254-85-2Downstream Products

12254-85-2Relevant articles and documents

Single crystal growth of the new pressure-induced-superconductor CrAs via chemical vapor transport

Zhu, Xiangde,Ling, Langsheng,Han, Yuyan,Xu, Junmin,Wang, Yongjian,Zhang, Hongwei,Zhang, Changjin,Pi, Li,Zhang, Yuheng

, p. 57 - 60 (2016)

Mono-arsenide CrAs, endures a helical anti-ferromagnetic order transition at ~265 K under ambient pressure. Recently, pressure-induced-superconductivity was discovered vicinity to the helical anti-ferromagnetic order in CrAs [Wei Wu et al., Nature Communications 5, 5508 (2014).]. However, the size of crystal grown via tin flux method is as small as 1 mm in longest dimension. In this work, we report the single crystal growth of CrAs with size of 1 × 5 × 1 mm3 via chemical vapor transport method and its physical properties.

DOUBLE EXCHANGE IN CrxMn1 - xAs COMPOUNDS.

Woehl,Berg,Baerner

, p. 179 - 190 (1980)

The magnetic moment M and the specific resistivity rho are measured for temperatures between 5 and 300 K and for eight different compositions. Characteristic temperatures are used to construct a magnetic phase diagram. The magnetic phases between ferromagnetic MnAs and antiferromagnetic CrAs are explained on the basis of two competing superexchange-double exchange magnetic couplings.

Superconductivity of 2.2K under pressure in helimagnet CrAs

Kotegawa, Hisashi,Nakahara, Shingo,Tou, Hideki,Sugawara, Hitoshi

, (2014)

We report resistivity measurements of the helimagnet CrAs under pressures. The helimagnetic transition with TN ~ 265K at ambient pressure is completely suppressed above a critical pressure of Pc ~ 0.7 GPa, and superconductivity is observed at ~2.2K for zero resistance, which exists in a wide pressure range extending beyond 3 GPa. Both the upper critical field Hc2 and the coeffi cient A in the resistivity increase toward Pc, suggesting that the superconductivity of CrAs is mediated by electronic correlations enhanced in the vicinity of the helimagnetic phase.

Next-nearest neighbour contributions to the XPS binding energies and XANES absorption energies of P and As in transition-metal arsenide phosphides MAs 1-yPy having the MnP-type structure

Grosvenor, Andrew P.,Cavell, Ronald G.,Mar, Arthur

, p. 2549 - 2558 (2009/02/06)

X-ray photoeleetron spectroscopic (XPS) and X-ray absorption near-edge spectroscopic (XANES) measurements have been made for several series of metal arsenide phosphides MAs1-yPy, (M= Co, Fe, Cr) that adopt the MnP-type structure. The P and As XPS binding energies (BEs) and XANES absorption energies of the metal arsenide phosphides do not follow the trend observed for the simple binary phosphides or arsenides, a deviation that arises from the combination of nearest and nextnearest neighbour contributions acting on the P or As photoemission or absorption site. The P 2p3/2 BEs and K-edge absorption energies are lower in MAs1-yPy than in MP because the P atoms are more negatively charged and because the P photoemission or absorption site is screened to a greater extent by less positively charged nearest-neighbour M atoms and more negatively charged next-nearest neighbour P atoms. The As L3- and K-edge absorption energies are higher in MAs1-yPy than in MAs primarily because the As atoms are less negatively charged. The M charge has been evaluated from analysis of the M 2p XPS spectra and the M L- and K-edge XANES spectra.

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