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Undoped , Indium Antimonide Substrate , 3”, Prime Grade

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    Buy cheap Undoped , Indium Antimonide Substrate , 3”, Prime Grade from wholesalers
     
    Buy cheap Undoped , Indium Antimonide Substrate , 3”, Prime Grade from wholesalers
    • Buy cheap Undoped , Indium Antimonide Substrate , 3”, Prime Grade from wholesalers

    Undoped , Indium Antimonide Substrate , 3”, Prime Grade

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    Brand Name : PAM-XIAMEN
    Payment Terms : T/T
    Supply Ability : 10,000 wafers/month
    Delivery Time : 5-50 working days
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    Undoped , Indium Antimonide Substrate , 3”, Prime Grade

    Undoped, Indium Antimonide Substrate, 3”, Prime Grade

    PAM-XIAMEN offers InSb wafer – Indium Antimonide which are grown by LEC(Liquid Encapsulated Czochralski) as epi-ready or mechanical grade with n type, p type or undoped in different orientation(111)or(100).Indium antimonide (InSb) is a crystalline compound made from the elements indium (In) and antimony (Sb). It is a narrow-gap semiconductor material from the III-V group used in infrared detectors, including thermal imaging cameras, FLIR systems, infrared homing missile guidance systems, and in infrared astronomy. The indium antimonide detectors are sensitive between 1–5 µm wavelengths.


    Undoped, Indium Antimonide Substrate, 3”, Prime Grade

    Wafer Specification
    ItemSpecifications
    Wafer Diameter

    3″76.2±0.4mm

    Crystal Orientation

    3″(111)AorB±0.1°

    Thickness

    3″ 800or900±25um

    Primary flat length

    3″22±2mm

    Secondary flat length

    3″11±1mm

    Surface FinishP/E, P/P
    PackageEpi-Ready,Single wafer container or CF cassette

    Electrical and Doping Specification
    Conduction Typen-type
    DopantUndoped
    EPD cm-2≤50
    Mobility cm² V-1s-1≥4*105
    Carrier Concentration cm-35*1013-3*1014

    Electrical properties of InSb Wafer

    Band structure and carrier concentration of InSb Wafer include Basic Parameters,Mobility and Hall Effect,Transport Properties in High Electric Fields,Impact Ionization
    ,Recombination Parameters


    Basic Parameters
    Mobility and Hall Effect
    Transport Properties in High Electric Fields
    Impact Ionization
    Recombination Parameters

    Basic Parameters

    Breakdown field≈103 V cm-1
    Mobility Electrons≤7.7·104 cm2V-1s-1
    Mobility Holes≤850 cm2V-1s-1
    Diffusion coefficient Electrons≤2·103 cm2s-1
    Diffusion coefficient Holes≤22 cm2s-1
    Electron thermal velocity9.8·105 m s-1
    Hole thermal velocity1.8·105 m s-1

    Mobility and Hall Effect

    Electron Hall mobility versus temperature for different doping levels and different compensation ratios

    CurveNd (cm-3)θ = Na/Nd
    1.3.85·10140.5
    2.8.5·10140.88
    3.9.5·10140.98
    4.1.35·10150.99

    Electron mobility versus temperature (high temperatures).
    Solid line is theoretical calculation for electron-drift mobility.
    Experimental data are Hall mobilities.

    For pure n-InSb at T ≥ 200K:
    µnH≈7.7·104(T/300)-1.66 (cm2 V-1 s-1).

    Electron mobility versus electron concentration. T = 300 K
    Electron mobility versus electron concentration. T = 77 K
    The electron Hall factor versus carrier concentration. T = 77 K

    Maximal electron mobility for pure n-InSb
    77 K1.2·106 cm2V-1s-1
    300 K7.7·104 cm2V-1s-1
    Maximal electron mobility for InSb grown on GaAs substrate
    77K1.5·105 cm2V-1s-1 (no= 2.2·1015 cm-3)
    300 K7.0·104 cm2V-1s-1 (no= 2.0·1016 cm-3)
    Maximal electron mobility for InSb grown on InP substrate
    77 K1.1·105 cm2V-1s-1
    300 K7.0·104 cm2V-1s-1

    Hole Hall mobility versus temperature for different hole concentrations.
    po (cm-3):
    1. 8·1014;
    2. 3.15·1018;
    3. 2.5·1019;

    For pure p-InSb at T > 60K:
    µpH≈850(T/300)-1.8 (cm2V-1s-1)

    Hall mobility versus hole concentrations:
    1. 77 K
    2. 290K
    The hole Hall factor versus carrier concentration, 77 K

    Transport Properties in High Electric Fields

    Field dependence of the electron drift velocity, 77 K.
    Solid lines is the Monte Carlo calculation.
    Points are experimental data.
    Field dependence of the electron drift velocity, 77 K.
    Solid lines is the Monte Carlo calculation.
    Points are experimental data.
    Fraction of electrons in the L-valley as a function of electric field F, 77K
    Frequency dependence of the efficiency in LSA mode
    Fo = F + F1sin(2π·ft):
    Fo= 2.5 kV cm-1

    Impact Ionization

    The dependence of generation rate for electrons gn versus electric field F, 300 K

    For 300 K, for 30 V/cm < F < 300 V/cm:

    gn(F) = 126·F2exp(F/160) (s-1),

    where F is in V cm-1.

    The dependence of generation rate for electrons gn versus electric field F, 77 K
    The dependence of ionization rates for electrons αi versus the electric field F, T=78 K
    The dependence of generation rate for holes gp versus the electric field F, T =77K

    Recombination Parameters

    For pure InSb at T≥250K lifetime of carrier (electrons and holes) is determined by Auger recombination:
    τn = τp ≈1/C ni2,
    where C≈5·10-26 cm-6 s-1 is the Auger coefficient.
    ni is the intrinsic carrier concentration.

    For T = 300 Kτn = τp≈5·10-8 s
    For T = 77K
    n-type: the lifetime of holesτp ~ 10-6 s
    p-type: the lifetime of electronsτn ~ 10-10 s

    Temperature dependence of surface recombination velocity for p-InSb.
    Temperature dependence of surface recombination velocity for n-InSb.

    Radiative recombination coefficient~5·10-11 cm3s-1
    Auger coefficient~5·10-26 cm6s-1

    Are You Looking for an InSb Wafer?

    PAM-XIAMEN is your go-to place for everything wafers, including InSb 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!

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