2004
DOI: 10.1016/j.jcrysgro.2004.03.049
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Low-resistance n-type polycrystalline InAs grown by molecular beam epitaxy

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Cited by 12 publications
(13 citation statements)
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“…The resistivity increases significantly from 26 Ω μm for the 63 nm template opening to 64 Ω μm for the 315 nm opening. This is attributed to an increasing number of grain boundaries in polycrystalline InAs grown in the larger openings which results in more electron trapping and scattering. , We see little change in resistivity with temperature, indicating that the mobility is limited by charged impurity scattering as opposed to phonons …”
mentioning
confidence: 75%
See 1 more Smart Citation
“…The resistivity increases significantly from 26 Ω μm for the 63 nm template opening to 64 Ω μm for the 315 nm opening. This is attributed to an increasing number of grain boundaries in polycrystalline InAs grown in the larger openings which results in more electron trapping and scattering. , We see little change in resistivity with temperature, indicating that the mobility is limited by charged impurity scattering as opposed to phonons …”
mentioning
confidence: 75%
“…This is attributed to an increasing number of grain boundaries in polycrystalline InAs grown in the larger openings which results in more electron trapping and scattering. 23,24 We see little change in resistivity with temperature, indicating that the mobility is limited by charged impurity scattering as opposed to phonons. 25 A crude estimation of the carrier concentration can be obtained by = × × n q…”
mentioning
confidence: 86%
“…Because the emitter regrowth is fully epitaxial, it is possible to grow highly conductive materials such as n ++ InP and n ++ InGaAs in contrast to our previous work on polycrystalline emitter regrowth. 7 For doping levels of N D =2ϫ 10 19 cm −3 in InGaAs and InP, Hall measurements on separate samples show electron mobilities of 1900 and 600 cm 2 / V s, respectively. Therefore esh =20 ⍀ / sq.…”
Section: Transistor Designmentioning
confidence: 98%
“…For InP HBTs, the only prior work on emitter regrowth has focused on polycrystalline InAs. [5][6][7] Here we present the first fully epitaxial regrown-emitter InP HBTs. Figure 1 shows a schematic cross-section of the regrownemitter HBT.…”
Section: Introductionmentioning
confidence: 99%
“…Presently, the highest quality devices are all generated via wafer bonding and epitaxial transfer approaches. Direct growth approaches often suffer from low material quality due to the formation of nanocrystalline materials or defects if grown on highly mismatched substrates. Most monolithic material integration schemes for back-end compatible materials result in polycrystalline films with maximum reported mobilities on the order of 100 cm 2 /(V s). Templated liquid phase (TLP) growth has been shown to be a promising route toward growth of crystalline semiconductors on nonepitaxial substrates, overcoming the limitations of standard vapor phase growth techniques with typical mobilities 2–5 times higher than other monolithic integration schemes.…”
Section: Introductionmentioning
confidence: 99%