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39332-13-3

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39332-13-3 Usage

Description

Tin Arsenide (SnAs) is a compound that consists of tin and arsenic elements. It is a p-type semiconductor material with a layered structure, which exhibits unique electronic and thermal properties. These characteristics make it a promising candidate for various applications in the field of solid-state devices.

Uses

Used in Semiconductor Industry:
Tin Arsenide is used as a doping agent for [application reason] enhancing the performance of solid-state devices such as transistors. Its p-type semiconductor properties allow for better control of electrical conductivity, which is crucial in the development of advanced electronic components.
Used in Transistor Manufacturing:
Tin Arsenide is used as a doping agent in the manufacturing of transistors for [application reason] improving their electrical and thermal performance. The incorporation of tin arsenide in heavily doped Gallium Arsenide (GaAs) enhances the overall efficiency and reliability of transistors, which are essential components in various electronic devices and systems.

Check Digit Verification of cas no

The CAS Registry Mumber 39332-13-3 includes 8 digits separated into 3 groups by hyphens. The first part of the number,starting from the left, has 5 digits, 3,9,3,3 and 2 respectively; the second part has 2 digits, 1 and 3 respectively.
Calculate Digit Verification of CAS Registry Number 39332-13:
(7*3)+(6*9)+(5*3)+(4*3)+(3*2)+(2*1)+(1*3)=113
113 % 10 = 3
So 39332-13-3 is a valid CAS Registry Number.
InChI:InChI=1/As.Sn/q-3;+3

39332-13-3 Well-known Company Product Price

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  • Alfa Aesar

  • (36363)  Tin arsenide, 99.999% (metals basis)   

  • 39332-13-3

  • 1g

  • 194.0CNY

  • Detail
  • Alfa Aesar

  • (36363)  Tin arsenide, 99.999% (metals basis)   

  • 39332-13-3

  • 5g

  • 573.0CNY

  • Detail
  • Alfa Aesar

  • (36363)  Tin arsenide, 99.999% (metals basis)   

  • 39332-13-3

  • 25g

  • 2352.0CNY

  • Detail

39332-13-3SDS

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 TIN ARSENIDE

1.2 Other means of identification

Product number -
Other names Tinarsenide,99.9(metalsbasis)

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:39332-13-3 SDS

39332-13-3Upstream product

39332-13-3Downstream Products

39332-13-3Relevant articles and documents

Synthesis, crystal structure, and thermoelectric properties of clathrates in the Sn-In-As-I system

Kelm, Evgeny A.,Olenev, Andrei V.,Bykov, Mikhail A.,Sobolev, Alexey V.,Presniakov, Igor A.,Kulbachinskii, Vladimir A.,Kytin, Vladimir G.,Shevelkov, Andrei V.

, p. 2059 - 2067 (2011)

Clathrates of the general formula Sn24-x- γInxAs22-yI8 have been synthesized with xmax = 10.7. They crystallize in the clathrate-I type of crystal structure, space group Pmβar{3}ν, with the cubic unit cell parameter ranging from a = 11.088 (x = 0) to a = 11.343 (x = 10.7) A. The crystal structure refined for five compositions with different indium contents revealed that despite the linear dependence of the unit cell parameter upon x the details of the crystal structure change twice upon varying the indium contents. These changes occur without altering the space group and show up in positional disorder of atoms within the framework and the concomitant change of the coordination of part of tin atoms from 3+2 to 3+3, which is additionally confirmed by the Moessbauer spectroscopy data. In general, these changes reflect the transition from the Sn24P 19.3I8 structure type for high indium contents to the Sn20.5As22I8 structure type for low indium contents. It is shown that the Sn24-x-γIn xAs22-yI8 clathrates have n-type conductivity with high values of the Seebeck coefficient ranging from -322 to -594 γVA·K-1 at room temperature. They display an abnormally low thermal conductivity at 293 K, from 0.36 to 0.57 WA·m-1A·K-1. The calculated thermoelectric figure-of-merit for Sn24-x-γIn xAs22-yI8 has its room-temperature maximum at 0.041 for x = 6.5. Copyright

Sn4As3 revisited: Solvothermal synthesis and crystal and electronic structure

Kovnir, Kirill,Kolen'ko, Yury V.,Baranov, Alexey I.,Neira, Ines S.,Sobolev, Alexey V.,Yoshimura, Masahiro,Presniakov, Igor A.,Shevelkov, Andrei V.

, p. 630 - 639 (2009)

A facile one pot method of synthesis of tin arsenide Sn4As3 starting from metallic tin and elemental arsenic under mild solvothermal conditions in ethylenediamine in the presence of ammonium chloride is offered. The dissolving of the

SnAs: A 4K weak type-II superconductor with non-trivial band topology

Sharma,Karn,Sharma, Prince,Gurjar, Ganesh,Patnaik,Awana

, (2021/09/30)

Superconductors with non-trivial band topology are emerging as one of the best avenues to study quantum anomalies and experimental realization of Majorana Fermions. This article reports the successful crystal growth of superconducting SnAs, which can have topologically non-trivial states, as evidenced in DFT (Density Functional Theory) calculations, Z2 invariants and topological surface states. Here, we followed a two-step method to grow SnAs crystal. The powder XRD (X-ray Diffractometry) pattern of synthesized crystal ensures that the crystal is grown in a single phase with a NaCl type cubic structure and the EDAX (Energy Dispersive X-ray Analysis) endorses the stoichiometry of the as-grown sample. The DFT calculations performed with and without inclusion of spin-orbit coupling (SOC) show band inversion at various k symmetry points near the Fermi level. The recorded Raman spectra show two different modes, which are assigned as A1 and ETO vibrations. The ZFC (Zero-Field Cooled) & FC (Field Cooled), as well as the isothermal M ? H (Magnetization vs. field) measurements, are also performed for the topological non-trivial SnAs superconductor, which eventually confirm the weak type-II superconductivity at 4K. Various other superconductivity parameters viz. kappa parameter, coherence length, and penetration depth are also calculated to probe the as-grown sample's characteristics.

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