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N Type , InAs( Indium Arsenide ) Substrate , 3”, Prime Grade

Categories InAs Wafer
Brand Name: PAM-XIAMEN
Place of Origin: China
MOQ: 1-10,000pcs
Payment Terms: T/T
Supply Ability: 10,000 wafers/month
Delivery Time: 5-50 working days
Packaging Details: Packaged in a class 100 clean room environment, in single container, under a nitrogen atmosphere
product name: InAs Substrate Wafer
Wafer Diamter: 3 inch
Conduction Type: N Type
Grade: Prime Grade
Wafer Thickness: 600±25um
keyword: Indium Arsenide InAs wafer
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N Type , InAs( Indium Arsenide ) Substrate , 3”, Prime Grade

N Type , InAs( Indium Arsenide ) Substrate , 3”, Prime Grade


PAM-XIAMEN offers InAs wafer – Indium Arsenide which are grown by LEC(Liquid Encapsulated Czochralski) or VGF(Vertical Gradient Freeze) as epi-ready or mechanical grade with n type, p type or undoped in different orientation(111),(100) or (110). PAM-XIAMEN can provide epi ready grade InAs wafer for your MOCVD & MBE epitaxial application .Please contact our engineer team for more wafer information.


3" InAs Wafer Specification

ItemSpecifications
DopantStannumSulphur
Conduction TypeN-typeN-type
Wafer Diameter3"
Wafer Orientation(100)±0.5°
Wafer Thickness600±25um
Primary Flat Length22±2mm
Secondary Flat Length11±1mm
Carrier Concentration(5-20)x1017cm-3(1-10)x1017cm-3
Mobility7000-20000cm2/V.s6000-20000cm2/V.s
EPD<5x104cm-2<3x104cm-2
TTV<12um
BOW<12um
WARP<15um
Laser markingupon request
Suface finishP/E, P/P
Epi readyyes
PackageSingle wafer container or cassette

What is the InAs Process?

InAs wafers must be prepared prior to device fabrication. To start, they must be completely cleaned to remove any damage that might have occurred during the slicing process. The wafers are then Chemically Mechanically Polished/Plaranrized (CMP) for the final material removal stage. This allows for the attainment of super-flat mirror-like surfaces with a remaining roughness on an atomic scale. After that is completed, the wafer is ready for fabrication.

Electrical properties of InAs Wafer

Basic Parameters

Breakdown field≈4·104 V cm-1
Mobility of electrons≤4·104 cm2V-1s-1
Mobility of holes≤5·102 cm2 V-1s-1
Diffusion coefficient of electrons≤103 cm2s-1
Diffusion coefficient of holes≤13 cm2 s-1
Electron thermal velocity7.7·105 m s-1
Hole thermal velocity2·105 m s-1

Mobility and Hall Effect

Electron Hall mobility versus temperature for different electron concentration:
full triangles no= 4·1015 cm-3,
circles no= 4·1016cm-3,
open triangles no= 1.7·1016cm-3.
Solid curve-calculation for pure InAs.
Electron Hall mobility versus electron concentration. T = 77 K.
Electron Hall mobility versus electron concentration T = 300 K

Electron Hall mobility (R·σ) in compensated material

Curven cm-3Na+Nd cm-3θ=Na/Nd
18.2·10163·10170.58
23.2·10176.1·10180.9
35.1·10163.2·10180.96
43.3·10167.5·10170.91
57.6·10153.4·10170.95
66.4·10153.8·10170.96
73.3·10153.9·10170.98

Electron Hall mobility versus transverse magnetic field, T = 77 K.
Nd (cm-3):
1. 1.7·1016;
2. 5.8·1016.

At T = 300 K the electron Hall factor in pure n-InAs rH ~1.3.

Hole Hall mobility (R·σ) versus temperature for different acceptor densities.
Hole concentration at 300 K po (cm-3): 1. 5.7·1016; 2. 2.6·1017; 3. 4.2·1017; 4. 1.3·1018.
Hall coefficient versus temperature for different acceptor densities.
Hole concentration at 300 K po (cm-3): 1. 5.7·1016; 2. 2.6·1017; 3. 4.2·1017; 4. 1.3·1018.

Transport Properties in High Electric Fields

Steady state field dependence of the electron drift velocity, 300 K,
F || (100). Theoretical calculation
Field dependence of the electron drift velocity at different transverse magnetic fields for long (microsecond) pulses.
Experimental results, 77 K
Magnetic field B(T): 1. 0.0; 2. 0.3; 3. 0.9; 4. 1.5.
Field dependence of the electron drift velocity, 77 K.
Solid lines show results of theoretical calculation for different non-parabolicity
α (eV-1): 1. 2.85; 2. 2.0; 3. 1.5.
Points show experimental results for very short (pico-second pulses)

Impact Ionization

The dependence of ionization rates for electrons αi and holes βi versus 1/F, T =77K

For electrons:

αi = αoexp(-Fno/ F)
αo = 1.8·105 cm-1;
Fno = 1.6·105 V cm-1 (77 K)

For holes:

βi = βoexp(-Fpo/ F)
At 77 K

1.5·104 V cm-1 < F < 3·104 V cm-13·104 V cm-1 < F < 6·104 V cm-1
βo = 4.7·105 cm-1;βo = 4.5·106 cm-1;
Fpo = 0.85·105 V cm-1.Fpo = 1.54·105 V cm-1

Generation rate g versus electric field for relatively low fields, T = 77 K.
Solid line shows result of calculation.
Experimental results: open and full circles -undoped InAs,
open triangles - compensated InAs.
Breakdown voltage and breakdown field versus doping density for an abrupt p-n junction, 77 K.

Recombination Parameters

Pure n-type material (no =2·10-15cm-3)
The longest lifetime of holesτp ~ 3·10-6 s
Diffusion length LpLp ~ 10 - 20 µm.
Pure p-type material
The longest lifetime of electronsτn ~ 3·10-8 s
Diffusion length LnLn ~ 30 - 60 µm

Characteristic surface recombination rates (cm s-1) 102 - 104.

Radiative recombination coefficient

77 K1.2·10-9 cm3s-1
298 K1.1·10-10 cm3s-1

Auger coefficient

300 K2.2·10-27cm3s-1

Are You Looking for an InAs Wafer?

PAM-XIAMEN is your go-to place for everything wafers, including InAs wafers, as we have been doing it for almost 30 years! Enquire us today to learn more about the wafers that we offer and how we can help you with your next project. Our group team is looking forward to providing both quality products and excellent service for you!

Product Tags:

indium arsenide wafer

  

3 inch wafer

  
Quality N Type , InAs( Indium Arsenide ) Substrate , 3”, Prime Grade for sale
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