Abstract:-c h a r g e c o n t r o l ' i n MOS s t r u c t u r e s f o r t h r e s h o l d s h i f t , a u t o r e g i s t r a t i o n , and complementary w e l l s and 2) d i s t r i b u t i o n cont r o l i n microwave and bipolar structures. Another f e a t u r e t h a t has n o t been e x t e n s i v e l y e x p l o i t e d i s t o combine the advantages o f t h e h i g h r e s o l u t i o n c a p a b i l i t i e s o f e l e c t r i c beam p a t t e r n d e l i n e a t i o n w i t h t h e l o w l a t e r a l s p r e… Show more
“…Introduction of donors and acceptors into semiconductors in thin layers allows the control of their electrical properties in a large variety of electronic devices. Dopants are either diffused from the surface or implanted from ion beams (Chernow et al 1977, Crowder 1973, Dearnuley et al 1973, Mayer et al 1970, Namba 1975. After implantation annealing is required to restore the perfection of the crystal which has been changed during implantation (radiation damage, amorphization) and to electrically activate the charge carriers.…”
Section: A) Measurement Of Dopant Distributions In Semiconductorsmentioning
confidence: 99%
“…After implantation annealing is required to restore the perfection of the crystal which has been changed during implantation (radiation damage, amorphization) and to electrically activate the charge carriers. Implantation distributions can be determined by employing a variety of electrical methods such as Hall effect, differential resistivity, junction depth or capacitance-voltage measurements (Mayer et al 1970). These methods not only use time consuming layer removal but measure only the distribution of the activated implanted atoms.…”
Section: A) Measurement Of Dopant Distributions In Semiconductorsmentioning
The principles and applications of depth profiling by secondary ion mass spectrometry (SIMS) are reviewed. Discussed are the basic physical processes and instrumental factors which influence the shape of depth profiles and which have to be understood or controlled for successful experimental measurements. Microroughness caused by sputtering, atomic mixing by primary beam knock‐on, and sample consumption limit the depth resolution which can be achieved while the chemical effect of ion yield enhancement by reactive species, matrix effects, and preferential sputtering can strongly affect the secondary ion signal. Instrumental effects to be controlled include beam uniformity, sample charging, and beam, and residual gas contamination. High depth resolution and sensitivity are the reasons for a wide variety of applications for SIMS depth profiling. Reviewed are measurements of the range distribution of ions implanted into semiconductors and their redistribution by subsequent annealing, studies of thin films and of oxide layers, diffusion measurements in metals, semiconductors, and minerals, measurements of elemental surface enhancements in airborne particles, and lunar glass spherules, and the search for solar wind implanted ions in lunar crystals.
“…Introduction of donors and acceptors into semiconductors in thin layers allows the control of their electrical properties in a large variety of electronic devices. Dopants are either diffused from the surface or implanted from ion beams (Chernow et al 1977, Crowder 1973, Dearnuley et al 1973, Mayer et al 1970, Namba 1975. After implantation annealing is required to restore the perfection of the crystal which has been changed during implantation (radiation damage, amorphization) and to electrically activate the charge carriers.…”
Section: A) Measurement Of Dopant Distributions In Semiconductorsmentioning
confidence: 99%
“…After implantation annealing is required to restore the perfection of the crystal which has been changed during implantation (radiation damage, amorphization) and to electrically activate the charge carriers. Implantation distributions can be determined by employing a variety of electrical methods such as Hall effect, differential resistivity, junction depth or capacitance-voltage measurements (Mayer et al 1970). These methods not only use time consuming layer removal but measure only the distribution of the activated implanted atoms.…”
Section: A) Measurement Of Dopant Distributions In Semiconductorsmentioning
The principles and applications of depth profiling by secondary ion mass spectrometry (SIMS) are reviewed. Discussed are the basic physical processes and instrumental factors which influence the shape of depth profiles and which have to be understood or controlled for successful experimental measurements. Microroughness caused by sputtering, atomic mixing by primary beam knock‐on, and sample consumption limit the depth resolution which can be achieved while the chemical effect of ion yield enhancement by reactive species, matrix effects, and preferential sputtering can strongly affect the secondary ion signal. Instrumental effects to be controlled include beam uniformity, sample charging, and beam, and residual gas contamination. High depth resolution and sensitivity are the reasons for a wide variety of applications for SIMS depth profiling. Reviewed are measurements of the range distribution of ions implanted into semiconductors and their redistribution by subsequent annealing, studies of thin films and of oxide layers, diffusion measurements in metals, semiconductors, and minerals, measurements of elemental surface enhancements in airborne particles, and lunar glass spherules, and the search for solar wind implanted ions in lunar crystals.
“…Hence, the stoichiometry of a silicon oxide film is given by Two advantages of using Rutherford scattering in place of nuclear reactions are: (i) its relative simplicity (it is not necessary to calculate absolute yields using tabulated cross-section data, since the Rutherford cross sections scale simply wit'h Z $ ) ; 3 ) (ii) a full impurity analysis is also obtained from the one spectrum. The general principles of the technique are described in more detail in references [9] t o [12].…”
It is described how the Rutherford scattering of MeV α‐particles may be used to study the stoichiometry and impurity content of thin silicon oxide films. The relative concentrations of silicon to oxygen can be measured to ≈ 5%, and in the most favourable cases, impurity concentrations as low as ≈1018 ions cm−3 can be measured.
“…Post-growth doping [6] of TMDCs offers an expanded selection of possible dopants compared to the popular method of doping via CVD growth. The technique allows for highly pure, clean and selective substitutional incorporation of dopants [7] and is also compatible with standard semiconductor processing. Ultra-low energy ion implantation is carried out using the ADONIS mass-selected ion beam deposition system at the University of Gottingen [8].…”
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