Pub Date : 1991-08-01DOI: 10.1016/0920-2307(91)90001-4
R. Schreutelkamp, J. Custer, J. R. Liefting, W. X. Lu, F. Saris
{"title":"Pre-amorphization damage in ion-implanted silicon","authors":"R. Schreutelkamp, J. Custer, J. R. Liefting, W. X. Lu, F. Saris","doi":"10.1016/0920-2307(91)90001-4","DOIUrl":"https://doi.org/10.1016/0920-2307(91)90001-4","url":null,"abstract":"","PeriodicalId":100891,"journal":{"name":"Materials Science Reports","volume":"134 1","pages":"275-366"},"PeriodicalIF":0.0,"publicationDate":"1991-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"75783264","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Ion implantation in silicon with doses below the amorphization threshold can lead to the formation of dislocations after high-temperature annealing. We have studied this for implants of 0.1–1 MeV B, Si, P, Ga, As, In, and Sb ions after annealing at 900°C using cross-sectional transmission electron microscopy. Pre-amorphization damage, also called category I dislocations, is observed if the total number of silicon atoms displaced by the implant exceeds a critical value before reaching the threshold dose for amorphization. These dislocations are of interstitial type and result from agglomeration of mobile silicon interstitials. The critical number of displaced Si atoms required for pre-amorphization damage formation increases with the mass of the implanted species and was determined by Rutherford backscattering spectrometry and channeling analysis to range from 1.5 × 1016/cm2 for B ions to (1.5-2) × 1017/cm2 for Sb ions. This increase with mass is attributed to an increasing collision cascade density resulting in a lower fraction of the measured damage being in the form of mobile Si interstitials needed for dislocation formation. In contrast to keV implants, category I defects are observed for high-mass species at MeV energies because the critical number of mobile interstitial silicon atoms is reached prior to the amorphization threshold. The critical number can be used to manipulate secondary defect formation. First, introducing a second damage profile can influence where the secondary defects form. Results are presented for MeV B or As implants in combination with low-energy Si irradiations. Depending on the separate implant parameters the position where secondary defects form can be influenced. Second, a comparison between channeling and random implants of B or P ions in Si(100) wafers shows that higher doses can be reached without formation of secondary defects by channeling implants than by random implants due to the lower amount of damage produced by a channeled ion. In either case, secondary defect formation is observed after high-temperature (900°C) annealing only if the total number of displaced Si atoms exceeds a critical value of ∼ 1.5 × 1016/cm2 and ∼ 5 × 1016/cm2 for the B and P implants, respectively. Third, higher total doses can be introduced without forming secondary defects by repetitive subthreshold implants each followed by an anneal to remove the implant damage. While a single 6 × 1013 In/cm2 implant results in a high density of dislocation loops after annealing, we demonstrate that instead using four separate 1.5 × 1013 In/cm2 implants each followed by an anneal leads to the formation of only a few partial dislocations. Pre-amorphization damage formation and annihilation is shown to influence transient tail diffusion of B. This has been investigated as a function of B implant condition, do
{"title":"Pre-amorphization damage in ion-implanted silicon","authors":"R.J. Schreutelkamp , J.S. Custer, J.R. Liefting, W.X. Lu , F.W. Saris","doi":"10.1016/0920-2307(91)90001-4","DOIUrl":"https://doi.org/10.1016/0920-2307(91)90001-4","url":null,"abstract":"<div><p>Ion implantation in silicon with doses below the amorphization threshold can lead to the formation of dislocations after high-temperature annealing. We have studied this for implants of 0.1–1 MeV B, Si, P, Ga, As, In, and Sb ions after annealing at 900°C using cross-sectional transmission electron microscopy. Pre-amorphization damage, also called category I dislocations, is observed if the total number of silicon atoms displaced by the implant exceeds a critical value before reaching the threshold dose for amorphization. These dislocations are of interstitial type and result from agglomeration of mobile silicon interstitials. The critical number of displaced Si atoms required for pre-amorphization damage formation increases with the mass of the implanted species and was determined by Rutherford backscattering spectrometry and channeling analysis to range from 1.5 × 10<sup>16</sup>/cm<sup>2</sup> for B ions to (1.5-2) × 10<sup>17</sup>/cm<sup>2</sup> for Sb ions. This increase with mass is attributed to an increasing collision cascade density resulting in a lower fraction of the measured damage being in the form of mobile Si interstitials needed for dislocation formation. In contrast to keV implants, category I defects are observed for high-mass species at MeV energies because the critical number of mobile interstitial silicon atoms is reached prior to the amorphization threshold. The critical number can be used to manipulate secondary defect formation. First, introducing a second damage profile can influence where the secondary defects form. Results are presented for MeV B or As implants in combination with low-energy Si irradiations. Depending on the separate implant parameters the position where secondary defects form can be influenced. Second, a comparison between channeling and random implants of B or P ions in Si(100) wafers shows that higher doses can be reached without formation of secondary defects by channeling implants than by random implants due to the lower amount of damage produced by a channeled ion. In either case, secondary defect formation is observed after high-temperature (900°C) annealing only if the total number of displaced Si atoms exceeds a critical value of ∼ 1.5 × 10<sup>16</sup>/cm<sup>2</sup> and ∼ 5 × 10<sup>16</sup>/cm<sup>2</sup> for the B and P implants, respectively. Third, higher total doses can be introduced without forming secondary defects by repetitive subthreshold implants each followed by an anneal to remove the implant damage. While a single 6 × 10<sup>13</sup> In/cm<sup>2</sup> implant results in a high density of dislocation loops after annealing, we demonstrate that instead using four separate 1.5 × 10<sup>13</sup> In/cm<sup>2</sup> implants each followed by an anneal leads to the formation of only a few partial dislocations. Pre-amorphization damage formation and annihilation is shown to influence transient tail diffusion of B. This has been investigated as a function of B implant condition, do","PeriodicalId":100891,"journal":{"name":"Materials Science Reports","volume":"6 7","pages":"Pages 275-366"},"PeriodicalIF":0.0,"publicationDate":"1991-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0920-2307(91)90001-4","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"72288855","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1991-07-01DOI: 10.1016/0920-2307(91)90008-B
James K. Hirvonen
Ion beam technologies have made tremendous gains in the commercial sector over the past two decades. The ion implantation of semiconductors rapidly became an accepted technology in the 1970s because of its ability to produce superior electronic devices or devices unobtainable by any other process. Ion beam modification of non-semiconductor materials for enhancing surface sensitive properties has been actively pursued in the international R&D community since the mid 1970s and continues to find selected industrial applications. This review briefly describes the status of ion implantation, ion beam mixing, and ion cluster beam deposition technologies and the directions in which they are currently being pursued. The hybrid use of ion beams in conjunction with physical vapor deposition, commonly termed ion beam assisted deposition (IBAD), combines many of the attributes of these ion beam treatments and conventional coating technologies. These include high density, superior adhesion, and the ability to produce arbitrarily thick coatings. Perhaps the most important feature of the IBAD technology is the frequently demonstrated ability to control many coatings properties such as morphology, adhesion, stress, as well as stoichiometry. This control is achieved by suitable variation of the relative arrival rates of energetic ions to that of the neutral species, as well as by control of substrate temperature. Many of these energetic ion effects on thin film formation are described and recent examples of research in the areas of: metastable compound formation, optical and electronic coatings, and tribological and corrosion-resistant coatings are presented. The review concludes with a description of pertinent equipment and an assessment of required future research and commercialization possibilities.
{"title":"Ion beam assisted thin film deposition","authors":"James K. Hirvonen","doi":"10.1016/0920-2307(91)90008-B","DOIUrl":"https://doi.org/10.1016/0920-2307(91)90008-B","url":null,"abstract":"<div><p>Ion beam technologies have made tremendous gains in the commercial sector over the past two decades. The ion implantation of semiconductors rapidly became an accepted technology in the 1970s because of its ability to produce superior electronic devices or devices unobtainable by any other process. Ion beam modification of non-semiconductor materials for enhancing surface sensitive properties has been actively pursued in the international R&D community since the mid 1970s and continues to find selected industrial applications. This review briefly describes the status of ion implantation, ion beam mixing, and ion cluster beam deposition technologies and the directions in which they are currently being pursued. The hybrid use of ion beams in conjunction with physical vapor deposition, commonly termed ion beam assisted deposition (IBAD), combines many of the attributes of these ion beam treatments and conventional coating technologies. These include high density, superior adhesion, and the ability to produce arbitrarily thick coatings. Perhaps the most important feature of the IBAD technology is the frequently demonstrated ability to control many coatings properties such as morphology, adhesion, stress, as well as stoichiometry. This control is achieved by suitable variation of the relative arrival rates of energetic ions to that of the neutral species, as well as by control of substrate temperature. Many of these energetic ion effects on thin film formation are described and recent examples of research in the areas of: metastable compound formation, optical and electronic coatings, and tribological and corrosion-resistant coatings are presented. The review concludes with a description of pertinent equipment and an assessment of required future research and commercialization possibilities.</p></div>","PeriodicalId":100891,"journal":{"name":"Materials Science Reports","volume":"6 6","pages":"Pages 215-274"},"PeriodicalIF":0.0,"publicationDate":"1991-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0920-2307(91)90008-B","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"91696322","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1991-04-01DOI: 10.1016/0920-2307(91)90007-A
M. Tamura
Damage formation and annealing behavior in ion-implanted silicon (Si) have been reported in two different regimes. First, the features of generated defects in ion-implanted submicron Si areas are described, particularly emphasizing changes in the spatial distribution of damage with a reduction in pattern sizes into which implantations are carried out. The results are compared with those obtained by focused ion beam (FIB) implantation in Si. The FIB implanted areas are necessarily doped with a high-density ion current 103–106 times higher than that in conventional implantation. Therefore, such a high-dose-rate implantation effect induces situations different from those encountered in the conventional method. Second, damage creation and its characteristic behavior with annealing are described for high-energy (1–3 MeV) ion-implanted Si. Specific annealing behaviors of defects are clarified in the temperature ranges between 500 and 1300°C, based on whether or not buried amorphous layers are formed in the implanted regions. The density reduction and configuration changes of defects between furnace annealing and rapid thermal annealing are compared. Also, the effect of bulk material nature (CZ or FZ) on defect growth is discussed in terms of interactions between oxygen atoms in CZ Si and defects. This interaction phenomenon is useful for gettering of metallic impurities harmful for device performance in Si.
{"title":"Damage formation and annealing of ion implantation in Si","authors":"M. Tamura","doi":"10.1016/0920-2307(91)90007-A","DOIUrl":"10.1016/0920-2307(91)90007-A","url":null,"abstract":"<div><p>Damage formation and annealing behavior in ion-implanted silicon (Si) have been reported in two different regimes. First, the features of generated defects in ion-implanted submicron Si areas are described, particularly emphasizing changes in the spatial distribution of damage with a reduction in pattern sizes into which implantations are carried out. The results are compared with those obtained by focused ion beam (FIB) implantation in Si. The FIB implanted areas are necessarily doped with a high-density ion current 10<sup>3</sup>–10<sup>6</sup> times higher than that in conventional implantation. Therefore, such a high-dose-rate implantation effect induces situations different from those encountered in the conventional method. Second, damage creation and its characteristic behavior with annealing are described for high-energy (1–3 MeV) ion-implanted Si. Specific annealing behaviors of defects are clarified in the temperature ranges between 500 and 1300°C, based on whether or not buried amorphous layers are formed in the implanted regions. The density reduction and configuration changes of defects between furnace annealing and rapid thermal annealing are compared. Also, the effect of bulk material nature (CZ or FZ) on defect growth is discussed in terms of interactions between oxygen atoms in CZ Si and defects. This interaction phenomenon is useful for gettering of metallic impurities harmful for device performance in Si.</p></div>","PeriodicalId":100891,"journal":{"name":"Materials Science Reports","volume":"6 4","pages":"Pages 141-214"},"PeriodicalIF":0.0,"publicationDate":"1991-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0920-2307(91)90007-A","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"79289406","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1991-03-01DOI: 10.1016/0920-2307(91)90004-7
L.J. Chen, K.N. Tu
Epitaxial silicides belong to a special class of silicides which exhibit a definite orientation relationship with respect to the silicon substrate. A silicide is expected to grow epitaxially on silicon if the crystal structures are similar and the lattice mismatch between them is small. The impetus for the study of epitaxial silicides mainly stemmed from several favorable characteristics of epitaxial silicides in comparison with their polycrystalline counterparts. It now appears that almost all transition-metal silicides can be grown epitaxially to a certain extent on silicon. In this report, theories for the epitaxial growth of silicides are first discussed. The formation and characterization of epitaxial silicides by different techniques are described. Epitaxial growth in various metal/Si systems is summarized. Several recent developments in the growth of transition-metal silicides on silicon are described. Factors influencing the growth of epitaxy are examined. Properties and device applications of epitaxial silicides are addressed.
{"title":"Epitaxial growth of transition-metal silicides on silicon","authors":"L.J. Chen, K.N. Tu","doi":"10.1016/0920-2307(91)90004-7","DOIUrl":"10.1016/0920-2307(91)90004-7","url":null,"abstract":"<div><p>Epitaxial silicides belong to a special class of silicides which exhibit a definite orientation relationship with respect to the silicon substrate. A silicide is expected to grow epitaxially on silicon if the crystal structures are similar and the lattice mismatch between them is small. The impetus for the study of epitaxial silicides mainly stemmed from several favorable characteristics of epitaxial silicides in comparison with their polycrystalline counterparts. It now appears that almost all transition-metal silicides can be grown epitaxially to a certain extent on silicon. In this report, theories for the epitaxial growth of silicides are first discussed. The formation and characterization of epitaxial silicides by different techniques are described. Epitaxial growth in various metal/Si systems is summarized. Several recent developments in the growth of transition-metal silicides on silicon are described. Factors influencing the growth of epitaxy are examined. Properties and device applications of epitaxial silicides are addressed.</p></div>","PeriodicalId":100891,"journal":{"name":"Materials Science Reports","volume":"6 2","pages":"Pages 53-140"},"PeriodicalIF":0.0,"publicationDate":"1991-03-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0920-2307(91)90004-7","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"89641638","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1991-02-01DOI: 10.1016/0920-2307(91)90003-6
M. Nastasi, J.W. Mayer
The thermodynamic and kinetic aspects of ion-irradiation-induced phase transformations in intermetallic compounds are reviewed. The different mechanisms for supplying the thermodynamic driving force for such transformations are discussed. The free energy of an irradiated material can be gradually elevated above that of a metastable state by the accumulation of lattice damage through the production of vacancy—interstitial defects, anti-site defects, and dislocations, or quickly elevated by the formation of a thermal spike in the collision cascade. The final state of the irradiated material will ultimately be determined by kinetic constraints in its transformation to lower-energy metastable and equilibrium states.
{"title":"Thermodynamics and kinetics of phase transformations induced by ion irradiation","authors":"M. Nastasi, J.W. Mayer","doi":"10.1016/0920-2307(91)90003-6","DOIUrl":"10.1016/0920-2307(91)90003-6","url":null,"abstract":"<div><p>The thermodynamic and kinetic aspects of ion-irradiation-induced phase transformations in intermetallic compounds are reviewed. The different mechanisms for supplying the thermodynamic driving force for such transformations are discussed. The free energy of an irradiated material can be gradually elevated above that of a metastable state by the accumulation of lattice damage through the production of vacancy—interstitial defects, anti-site defects, and dislocations, or quickly elevated by the formation of a thermal spike in the collision cascade. The final state of the irradiated material will ultimately be determined by kinetic constraints in its transformation to lower-energy metastable and equilibrium states.</p></div>","PeriodicalId":100891,"journal":{"name":"Materials Science Reports","volume":"6 1","pages":"Pages 1-51"},"PeriodicalIF":0.0,"publicationDate":"1991-02-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0920-2307(91)90003-6","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"83706379","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-12-01DOI: 10.1016/0920-2307(90)90003-L
Francesco Priolo, Emanuele Rimini
The ion-beam-induced epitaxial crystallization (IBIEC) and planar amorphization of amorphous Si (a-Si) layers onto single-crystal Si substrates is reviewed. In particular, the dependence of the process on substrate temperature, on substrate orientation and on the energy deposited by the impinging ions into electronic and elastic collisions is treated in detail and discussed. Emphasis is also given to the influence of impurities on IBIEC, where a variety of different phenomena are observed. For instance, fast diffusers, such as Au, are seen to be swept by the moving c-a boundary and present intriguing segregation profiles. Slow diffusers such as As or O, on the other hand, have not enough mobility to move over long-range distances even in the presence of irradiation, but they can strongly modify the kinetics of IBIEC. Dopants such as B, P and As, for example, enhance the ion-induced growth rate by a factor of 2–3, while O retards it. It is also shown that by decreasing the substrate temperature (or by increasing the ion flux) IBIEC can be reversed resulting in a planar layer-by-layer amorphization. This phenomenon evidences the unique non-equilibrium features of ion-assisted phase transitions in silicon which are the result of a dynamic balance between defect production rate and defect annihilation rate. These data are discussed, mainly in comparison with the purely thermally activated growth of a-Si and a possible explanation of the observed phenomena is presented in terms of a simple model. Finally, new possible applications of the phenomenon, such as the ion-induced regrowth of deposited Si layers and of deposited GeSi heterostructures, are illustrated, demonstrating the high potentialities of ion-beam processing in producing epitaxial layers in a non-conventional manner.
{"title":"Ion-beam-induced epitaxial crystallization and amorphization in silicon","authors":"Francesco Priolo, Emanuele Rimini","doi":"10.1016/0920-2307(90)90003-L","DOIUrl":"https://doi.org/10.1016/0920-2307(90)90003-L","url":null,"abstract":"<div><p>The ion-beam-induced epitaxial crystallization (IBIEC) and planar amorphization of amorphous Si (a-Si) layers onto single-crystal Si substrates is reviewed. In particular, the dependence of the process on substrate temperature, on substrate orientation and on the energy deposited by the impinging ions into electronic and elastic collisions is treated in detail and discussed. Emphasis is also given to the influence of impurities on IBIEC, where a variety of different phenomena are observed. For instance, fast diffusers, such as Au, are seen to be swept by the moving c-a boundary and present intriguing segregation profiles. Slow diffusers such as As or O, on the other hand, have not enough mobility to move over long-range distances even in the presence of irradiation, but they can strongly modify the kinetics of IBIEC. Dopants such as B, P and As, for example, enhance the ion-induced growth rate by a factor of 2–3, while O retards it. It is also shown that by decreasing the substrate temperature (or by increasing the ion flux) IBIEC can be reversed resulting in a planar layer-by-layer amorphization. This phenomenon evidences the unique non-equilibrium features of ion-assisted phase transitions in silicon which are the result of a dynamic balance between defect production rate and defect annihilation rate. These data are discussed, mainly in comparison with the purely thermally activated growth of a-Si and a possible explanation of the observed phenomena is presented in terms of a simple model. Finally, new possible applications of the phenomenon, such as the ion-induced regrowth of deposited Si layers and of deposited GeSi heterostructures, are illustrated, demonstrating the high potentialities of ion-beam processing in producing epitaxial layers in a non-conventional manner.</p></div>","PeriodicalId":100891,"journal":{"name":"Materials Science Reports","volume":"5 7","pages":"Pages 321-379"},"PeriodicalIF":0.0,"publicationDate":"1990-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/0920-2307(90)90003-L","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"136850224","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-01-01DOI: 10.1016/S0920-2307(05)80007-6
Yang-Tse Cheng
A thermodynamic approach to atomic diffusion in a thermal spike is reviewed. The approach is based on recent ion mixing experiments which demonstrate the influence of the heat of mixing and the cohesive energy of solids on ion mixing. These thermodynamic effects are assimilated into a phenomenological model of ion mixing. The model is generalized to low-energy ion mixing during sputter depth profiling and is used to elucidate the nature of atomic diffusion in a thermal spike. The onset of radiation-enhanced diffusion in ion mixing is also discussed. A fractal geometry approach to spike formation is presented. An “idealized” collision cascade constructed from the inverse-power potential V(r) ∝ r−1/m (0 < m ≤ 1) is shown to have a fractal tree structure with a fractal dimension D = 1/2m. The same fractal dimension can also be derived from the Winterbon-Sigmund-Sanders (WSS) theory of atomic collisions in solids. The fractal dimension is shown to increase as an actual collision cascade evolves, because of the change of the effective interaction potentials. The concept of “space-filling” fractals is used to specify spikes. The formation of local spikes, their energy densities, the probability of local spikes overlapping, and the time evolution of a collision cascade are also investigated. It is shown that spikes are not expected to form in a single-component solid consisting of elements with atomic number less than 20; many-body collisions have little effect on the formation of spikes; and, the similarity between high-and low-energy ion mixing is the result of the fractal nature of collision cascades.
{"title":"Thermodynamic and fractal geometric aspects of ion-solid interactions","authors":"Yang-Tse Cheng","doi":"10.1016/S0920-2307(05)80007-6","DOIUrl":"10.1016/S0920-2307(05)80007-6","url":null,"abstract":"<div><p>A thermodynamic approach to atomic diffusion in a thermal spike is reviewed. The approach is based on recent ion mixing experiments which demonstrate the influence of the heat of mixing and the cohesive energy of solids on ion mixing. These thermodynamic effects are assimilated into a phenomenological model of ion mixing. The model is generalized to low-energy ion mixing during sputter depth profiling and is used to elucidate the nature of atomic diffusion in a thermal spike. The onset of radiation-enhanced diffusion in ion mixing is also discussed. A fractal geometry approach to spike formation is presented. An “idealized” collision cascade constructed from the inverse-power potential <em>V</em>(<em>r</em>) ∝ <em>r</em><sup>−1/<em>m</em></sup> (0 < <em>m</em> ≤ 1) is shown to have a fractal tree structure with a fractal dimension <em>D</em> = 1/2<em>m</em>. The same fractal dimension can also be derived from the Winterbon-Sigmund-Sanders (WSS) theory of atomic collisions in solids. The fractal dimension is shown to increase as an actual collision cascade evolves, because of the change of the effective interaction potentials. The concept of “space-filling” fractals is used to specify spikes. The formation of local spikes, their energy densities, the probability of local spikes overlapping, and the time evolution of a collision cascade are also investigated. It is shown that spikes are not expected to form in a single-component solid consisting of elements with atomic number less than 20; many-body collisions have little effect on the formation of spikes; and, the similarity between high-and low-energy ion mixing is the result of the fractal nature of collision cascades.</p></div>","PeriodicalId":100891,"journal":{"name":"Materials Science Reports","volume":"5 2","pages":"Pages 45-97"},"PeriodicalIF":0.0,"publicationDate":"1990-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S0920-2307(05)80007-6","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"82933292","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 1990-01-01DOI: 10.1016/S0920-2307(05)80002-7
T.P. Russell
The use of X-ray and neutron reflectivity to study polymers in the condensed state and in solutions is revieved in this article. Basic theoretical and experimental concepts of specular reflectivity are presented. Research in the application of neutron and X-ray reflectivity is discussed along with the relevance of these studies to important issues in polymer science. These include investigations of ordered and disordered homopolymers and block copolymers in solution and in the condensed state. Finally, a discussion of off-specular, diffuse scattering is presented with its potential use in polymer science.
{"title":"X-ray and neutron reflectivity for the investigation of polymers","authors":"T.P. Russell","doi":"10.1016/S0920-2307(05)80002-7","DOIUrl":"10.1016/S0920-2307(05)80002-7","url":null,"abstract":"<div><p>The use of X-ray and neutron reflectivity to study polymers in the condensed state and in solutions is revieved in this article. Basic theoretical and experimental concepts of specular reflectivity are presented. Research in the application of neutron and X-ray reflectivity is discussed along with the relevance of these studies to important issues in polymer science. These include investigations of ordered and disordered homopolymers and block copolymers in solution and in the condensed state. Finally, a discussion of off-specular, diffuse scattering is presented with its potential use in polymer science.</p></div>","PeriodicalId":100891,"journal":{"name":"Materials Science Reports","volume":"5 4","pages":"Pages 171-271"},"PeriodicalIF":0.0,"publicationDate":"1990-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S0920-2307(05)80002-7","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"88159598","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}