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P Type , Single Crystal InAs Substrate , 3”, Prime Grade

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    Buy cheap P Type , Single Crystal InAs Substrate , 3”, Prime Grade from wholesalers
    • Buy cheap P Type , Single Crystal InAs Substrate , 3”, Prime Grade from wholesalers

    P Type , Single Crystal InAs 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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    P Type , Single Crystal InAs Substrate , 3”, Prime Grade

    P Type , Single Crystal InAs Substrate , 3”, Prime Grade


    PAM-XIAMEN manufactures high purity single crystal Indium arsenide Wafers for optoelectronics applications. Our standard wafer diameters range from 25.4 mm (1 inch) to 100 mm (6 inches) in size; wafers can be produced in various thicknesses and orientations with polished or unpolished sides and can include dopants. PAM-XIAMEN can produce wide range grades: prime grade, mechanical grade,test grade, dummy grade, technical grade, and optical grade. PAM-XIAMEN also offers materials to customer specifications by request, in addition to custom compositions for commercial and research applications and new proprietary technologies.


    3" InAs Wafer Specification

    ItemSpecifications
    DopantZinc
    Conduction TypeP-type
    Wafer Diameter3"
    Wafer Orientation(100)±0.5°
    Wafer Thickness600±25um
    Primary Flat Length22±2mm
    Secondary Flat Length11±1mm
    Carrier Concentration(1-10)x1017cm-3
    Mobility100-400cm2/V.s
    EPD<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 InAs wafer?

    Indium arsenide is a kind of III-V compound semiconductor material composed of indium and arsenic.It is a silver gray solid with a sphalerite crystal structure at room temperature. The lattice constant is 0.6058nm, and the density is 5.66g/cm (solid) and 5.90g/cm (liquid at melting point). The band structure is a direct transition with a band gap (300K) of 0.45ev. the dissociation pressure of as is only 0.033mpa, and the single crystal can be grown from the melt at atmospheric pressure. The commonly used methods are Hb and LEC. InAs is a kind of semiconductor material which is difficult to purify. The residual carrier concentration is higher than l × 10 / cm, the room temperature electron mobility is 3.3 × 10 ^ 3cm / (V · s), and the hole mobility is 460cm / (V · s). The effective segregation coefficient of sulfur in In and As is close to 1, so it is used as n-type dopant to improve the uniformity of longitudinal carrier concentration distribution. For industrial InAs (s) single crystal, n ≥ 1 × 10 / cm3, μ ≤ 2.0 × 10cm / (V · s), EPD ≤ 5 × 10 / cm3.


    InAs crystal has high electron mobility and mobility ratio (μ E / μ H = 70), low magneto resistance effect and low resistance temperature coefficient. It is an ideal material for manufacturing Hall devices and magneto resistance devices. The emission wavelength of InAs is 3.34 μ M. in GaAs B, InAsPSb and inasb multiple epitaxial materials with lattice matching can be grown on InAs substrate. Lasers and detectors for optical fiber communication at 2-4 μ M band can be manufactured.


    What is a InAs test Wafer?

    Most test wafers are wafers which have fallen out of prime specifications. Test wafers may be used to run marathons, test equipment and for high-end R & D. They are often a cost-effective alternative to prime wafers.

    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 substrate?

    PAM-XIAMEN is proud to offer indium phosphide substrate for all different kinds of projects. If you are looking for InAs wafers, send us enquiry today to learn more about how we can work with you to get you the InAs wafers you need for your next project. Our group team is looking forward to providing both quality products and excellent service for you!

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