1994
DOI: 10.1103/physrevb.49.5291
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Electrical studies on H-implanted silicon

Abstract: Electrical properties of high-dose (1.6X 10' at./cm') H+-implanted B-doped silicon have been investigated using transient capacitance spectroscopy, capacitance-voltage, and spreading resistance profiling.The role of hydrogen is twofold: to interact with the defects created by ion implantation, modifying their electrical properties, and to neutralize the shallow-acceptor dopants. The evolution of the defects responsible for the deep levels and the depth of the neutralized region have been investigated after iso… Show more

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Cited by 24 publications
(16 citation statements)
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“…We have gained direct knowledge of the behaviour of hydrogen in ion-implanted crystalline silicon from a long series of studies started in 1989 and carried out by employing experimental techniques like secondary ion mass spectrometry (SIMS) [13 to 151, multiplecrystal X-ray diffraction (XRD) [ 131, channeling Rutherford back-scattering spectrometry (RBS) [13 to 191, elastic recoil detection analysis (ERDA) [15,191, transmission electron microscopy (TEM) [13 to 15, 17 to 191, spectroscopic ellipsometry [20], spreading resistance (SR) [21], deep level transient spectroscopy (DLTS) [21], positron annihilation technique (PAT) [22], and photoluminescence (PL) [23]; by simulating the imparted damage by means of MARLOWE and TRIM (transport of ion in matters) codes ([18] and [19], respectively); and by developing new methods for the analysis of channeling RBS spectra [18, 241. With these techniques we have studied the effects of the implanation energy E , fluence @, and temperature Tmp,, and of the subsequent annealing process (temperature T,,, and duration t,,,) on the physico-chemical properties of the hydrogen-implanted Si : H layer; the attention was mainly concentrated on lightly doped silicon implanted at low energy (15.5 keV) and high fluence (1.6 x 1OI6 cm-').…”
Section: Introductionmentioning
confidence: 99%
“…We have gained direct knowledge of the behaviour of hydrogen in ion-implanted crystalline silicon from a long series of studies started in 1989 and carried out by employing experimental techniques like secondary ion mass spectrometry (SIMS) [13 to 151, multiplecrystal X-ray diffraction (XRD) [ 131, channeling Rutherford back-scattering spectrometry (RBS) [13 to 191, elastic recoil detection analysis (ERDA) [15,191, transmission electron microscopy (TEM) [13 to 15, 17 to 191, spectroscopic ellipsometry [20], spreading resistance (SR) [21], deep level transient spectroscopy (DLTS) [21], positron annihilation technique (PAT) [22], and photoluminescence (PL) [23]; by simulating the imparted damage by means of MARLOWE and TRIM (transport of ion in matters) codes ([18] and [19], respectively); and by developing new methods for the analysis of channeling RBS spectra [18, 241. With these techniques we have studied the effects of the implanation energy E , fluence @, and temperature Tmp,, and of the subsequent annealing process (temperature T,,, and duration t,,,) on the physico-chemical properties of the hydrogen-implanted Si : H layer; the attention was mainly concentrated on lightly doped silicon implanted at low energy (15.5 keV) and high fluence (1.6 x 1OI6 cm-').…”
Section: Introductionmentioning
confidence: 99%
“…12 For higher temperatures the carriers quantum confinement is probably eliminated by nanoblisters coarsening ͑giving detectable bubbles͒ and the passivation of nonradiative recombination centers decreases, due to the H loss. Nanoblisters cannot be resolved by TEM and their existence can only be detected through the measurement of the displacement field they cause within the Si lattice.…”
mentioning
confidence: 99%
“…Furthermore, chemically active implanted species such as H can neutralize dopants, thereby causing strong changes in the electrical property of crystalline silicon. 25 The low mobility of carriers in the implanted region effectively limits diffusion of excited electrons away from the vicinity of the ion track. Most of the electronic energy lost by the incident ions is stored locally as potential energy in trapped excitons ͑localized electron-hole pairs͒.…”
Section: Discussionmentioning
confidence: 99%