Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation
Abstract Interaction of the highly localized probe of scanning probe microscopy with solid surfaces with mobile electronic or ionic carriers leads to the redistribution of mobile carriers at the tip surface junction. For small probe biases, this problem is equivalent to the Debye screening, describe...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Fabrikant, V. I. [verfasserIn] Karapetian, E. [verfasserIn] Kalinin, S. V. [verfasserIn] |
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| Format: |
E-Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2019 |
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| Schlagwörter: |
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| Übergeordnetes Werk: |
Enthalten in: Journal of engineering mathematics - Dordrecht [u.a.] : Springer Science + Business Media B.V, 1967, 115(2019), 1 vom: Apr., Seite 141-156 |
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| Übergeordnetes Werk: |
volume:115 ; year:2019 ; number:1 ; month:04 ; pages:141-156 |
| Links: |
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| DOI / URN: |
10.1007/s10665-019-09996-4 |
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| Katalog-ID: |
SPR012324167 |
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| 245 | 1 | 0 | |a Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation |
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| 520 | |a Abstract Interaction of the highly localized probe of scanning probe microscopy with solid surfaces with mobile electronic or ionic carriers leads to the redistribution of mobile carriers at the tip surface junction. For small probe biases, this problem is equivalent to the Debye screening, described by Klein–Gordon (K–G) integral equation. Here, an exact solution to the K–G equation is derived for the case of a circle in the form of a convergent series expansion of the solution, which is effective for relatively small values of the inverse Debye length, k. Also, a reasonably accurate solution is derived for large values of parameter k by using the method of collocation. A surprisingly simple asymptotic solution is derived for very large values of k, which is valid for the arbitrary right-hand side of the equation. The same methods can be used for the case of elliptic domain. | ||
| 650 | 4 | |a Exact solution |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Integral equations |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Klein–Gordon |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Potential theory |7 (dpeaa)DE-He213 | |
| 650 | 4 | |a Series expansion |7 (dpeaa)DE-He213 | |
| 700 | 1 | |a Karapetian, E. |e verfasserin |4 aut | |
| 700 | 1 | |a Kalinin, S. V. |e verfasserin |4 aut | |
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10.1007/s10665-019-09996-4 doi (DE-627)SPR012324167 (SPR)s10665-019-09996-4-e DE-627 ger DE-627 rakwb eng 510 ASE 31.80 bkl 50.03 bkl Fabrikant, V. I. verfasserin aut Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Interaction of the highly localized probe of scanning probe microscopy with solid surfaces with mobile electronic or ionic carriers leads to the redistribution of mobile carriers at the tip surface junction. For small probe biases, this problem is equivalent to the Debye screening, described by Klein–Gordon (K–G) integral equation. Here, an exact solution to the K–G equation is derived for the case of a circle in the form of a convergent series expansion of the solution, which is effective for relatively small values of the inverse Debye length, k. Also, a reasonably accurate solution is derived for large values of parameter k by using the method of collocation. A surprisingly simple asymptotic solution is derived for very large values of k, which is valid for the arbitrary right-hand side of the equation. The same methods can be used for the case of elliptic domain. Exact solution (dpeaa)DE-He213 Integral equations (dpeaa)DE-He213 Klein–Gordon (dpeaa)DE-He213 Potential theory (dpeaa)DE-He213 Series expansion (dpeaa)DE-He213 Karapetian, E. verfasserin aut Kalinin, S. V. verfasserin aut Enthalten in Journal of engineering mathematics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1967 115(2019), 1 vom: Apr., Seite 141-156 (DE-627)270937552 (DE-600)1478716-7 1573-2703 nnns volume:115 year:2019 number:1 month:04 pages:141-156 https://dx.doi.org/10.1007/s10665-019-09996-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 31.80 ASE 50.03 ASE AR 115 2019 1 04 141-156 |
| spelling |
10.1007/s10665-019-09996-4 doi (DE-627)SPR012324167 (SPR)s10665-019-09996-4-e DE-627 ger DE-627 rakwb eng 510 ASE 31.80 bkl 50.03 bkl Fabrikant, V. I. verfasserin aut Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Interaction of the highly localized probe of scanning probe microscopy with solid surfaces with mobile electronic or ionic carriers leads to the redistribution of mobile carriers at the tip surface junction. For small probe biases, this problem is equivalent to the Debye screening, described by Klein–Gordon (K–G) integral equation. Here, an exact solution to the K–G equation is derived for the case of a circle in the form of a convergent series expansion of the solution, which is effective for relatively small values of the inverse Debye length, k. Also, a reasonably accurate solution is derived for large values of parameter k by using the method of collocation. A surprisingly simple asymptotic solution is derived for very large values of k, which is valid for the arbitrary right-hand side of the equation. The same methods can be used for the case of elliptic domain. Exact solution (dpeaa)DE-He213 Integral equations (dpeaa)DE-He213 Klein–Gordon (dpeaa)DE-He213 Potential theory (dpeaa)DE-He213 Series expansion (dpeaa)DE-He213 Karapetian, E. verfasserin aut Kalinin, S. V. verfasserin aut Enthalten in Journal of engineering mathematics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1967 115(2019), 1 vom: Apr., Seite 141-156 (DE-627)270937552 (DE-600)1478716-7 1573-2703 nnns volume:115 year:2019 number:1 month:04 pages:141-156 https://dx.doi.org/10.1007/s10665-019-09996-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 31.80 ASE 50.03 ASE AR 115 2019 1 04 141-156 |
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10.1007/s10665-019-09996-4 doi (DE-627)SPR012324167 (SPR)s10665-019-09996-4-e DE-627 ger DE-627 rakwb eng 510 ASE 31.80 bkl 50.03 bkl Fabrikant, V. I. verfasserin aut Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Interaction of the highly localized probe of scanning probe microscopy with solid surfaces with mobile electronic or ionic carriers leads to the redistribution of mobile carriers at the tip surface junction. For small probe biases, this problem is equivalent to the Debye screening, described by Klein–Gordon (K–G) integral equation. Here, an exact solution to the K–G equation is derived for the case of a circle in the form of a convergent series expansion of the solution, which is effective for relatively small values of the inverse Debye length, k. Also, a reasonably accurate solution is derived for large values of parameter k by using the method of collocation. A surprisingly simple asymptotic solution is derived for very large values of k, which is valid for the arbitrary right-hand side of the equation. The same methods can be used for the case of elliptic domain. Exact solution (dpeaa)DE-He213 Integral equations (dpeaa)DE-He213 Klein–Gordon (dpeaa)DE-He213 Potential theory (dpeaa)DE-He213 Series expansion (dpeaa)DE-He213 Karapetian, E. verfasserin aut Kalinin, S. V. verfasserin aut Enthalten in Journal of engineering mathematics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1967 115(2019), 1 vom: Apr., Seite 141-156 (DE-627)270937552 (DE-600)1478716-7 1573-2703 nnns volume:115 year:2019 number:1 month:04 pages:141-156 https://dx.doi.org/10.1007/s10665-019-09996-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 31.80 ASE 50.03 ASE AR 115 2019 1 04 141-156 |
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10.1007/s10665-019-09996-4 doi (DE-627)SPR012324167 (SPR)s10665-019-09996-4-e DE-627 ger DE-627 rakwb eng 510 ASE 31.80 bkl 50.03 bkl Fabrikant, V. I. verfasserin aut Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation 2019 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Interaction of the highly localized probe of scanning probe microscopy with solid surfaces with mobile electronic or ionic carriers leads to the redistribution of mobile carriers at the tip surface junction. For small probe biases, this problem is equivalent to the Debye screening, described by Klein–Gordon (K–G) integral equation. Here, an exact solution to the K–G equation is derived for the case of a circle in the form of a convergent series expansion of the solution, which is effective for relatively small values of the inverse Debye length, k. Also, a reasonably accurate solution is derived for large values of parameter k by using the method of collocation. A surprisingly simple asymptotic solution is derived for very large values of k, which is valid for the arbitrary right-hand side of the equation. The same methods can be used for the case of elliptic domain. Exact solution (dpeaa)DE-He213 Integral equations (dpeaa)DE-He213 Klein–Gordon (dpeaa)DE-He213 Potential theory (dpeaa)DE-He213 Series expansion (dpeaa)DE-He213 Karapetian, E. verfasserin aut Kalinin, S. V. verfasserin aut Enthalten in Journal of engineering mathematics Dordrecht [u.a.] : Springer Science + Business Media B.V, 1967 115(2019), 1 vom: Apr., Seite 141-156 (DE-627)270937552 (DE-600)1478716-7 1573-2703 nnns volume:115 year:2019 number:1 month:04 pages:141-156 https://dx.doi.org/10.1007/s10665-019-09996-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER SSG-OPC-MAT SSG-OPC-ASE GBV_ILN_11 GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_63 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_150 GBV_ILN_151 GBV_ILN_152 GBV_ILN_161 GBV_ILN_170 GBV_ILN_171 GBV_ILN_187 GBV_ILN_213 GBV_ILN_224 GBV_ILN_230 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_636 GBV_ILN_702 GBV_ILN_2001 GBV_ILN_2003 GBV_ILN_2004 GBV_ILN_2005 GBV_ILN_2006 GBV_ILN_2007 GBV_ILN_2009 GBV_ILN_2010 GBV_ILN_2011 GBV_ILN_2014 GBV_ILN_2015 GBV_ILN_2020 GBV_ILN_2021 GBV_ILN_2025 GBV_ILN_2026 GBV_ILN_2027 GBV_ILN_2031 GBV_ILN_2034 GBV_ILN_2037 GBV_ILN_2038 GBV_ILN_2039 GBV_ILN_2044 GBV_ILN_2048 GBV_ILN_2049 GBV_ILN_2050 GBV_ILN_2055 GBV_ILN_2057 GBV_ILN_2059 GBV_ILN_2061 GBV_ILN_2064 GBV_ILN_2065 GBV_ILN_2068 GBV_ILN_2070 GBV_ILN_2086 GBV_ILN_2088 GBV_ILN_2093 GBV_ILN_2106 GBV_ILN_2107 GBV_ILN_2108 GBV_ILN_2110 GBV_ILN_2111 GBV_ILN_2112 GBV_ILN_2113 GBV_ILN_2116 GBV_ILN_2118 GBV_ILN_2119 GBV_ILN_2122 GBV_ILN_2129 GBV_ILN_2143 GBV_ILN_2144 GBV_ILN_2147 GBV_ILN_2148 GBV_ILN_2152 GBV_ILN_2153 GBV_ILN_2188 GBV_ILN_2190 GBV_ILN_2232 GBV_ILN_2336 GBV_ILN_2446 GBV_ILN_2470 GBV_ILN_2472 GBV_ILN_2507 GBV_ILN_2522 GBV_ILN_2548 GBV_ILN_4035 GBV_ILN_4037 GBV_ILN_4046 GBV_ILN_4112 GBV_ILN_4125 GBV_ILN_4242 GBV_ILN_4246 GBV_ILN_4249 GBV_ILN_4251 GBV_ILN_4305 GBV_ILN_4306 GBV_ILN_4307 GBV_ILN_4313 GBV_ILN_4322 GBV_ILN_4323 GBV_ILN_4324 GBV_ILN_4325 GBV_ILN_4326 GBV_ILN_4328 GBV_ILN_4333 GBV_ILN_4334 GBV_ILN_4335 GBV_ILN_4336 GBV_ILN_4338 GBV_ILN_4393 GBV_ILN_4700 31.80 ASE 50.03 ASE AR 115 2019 1 04 141-156 |
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| author |
Fabrikant, V. I. |
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Fabrikant, V. I. ddc 510 bkl 31.80 bkl 50.03 misc Exact solution misc Integral equations misc Klein–Gordon misc Potential theory misc Series expansion Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation |
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510 ASE 31.80 bkl 50.03 bkl Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation Exact solution (dpeaa)DE-He213 Integral equations (dpeaa)DE-He213 Klein–Gordon (dpeaa)DE-He213 Potential theory (dpeaa)DE-He213 Series expansion (dpeaa)DE-He213 |
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ddc 510 bkl 31.80 bkl 50.03 misc Exact solution misc Integral equations misc Klein–Gordon misc Potential theory misc Series expansion |
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ddc 510 bkl 31.80 bkl 50.03 misc Exact solution misc Integral equations misc Klein–Gordon misc Potential theory misc Series expansion |
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ddc 510 bkl 31.80 bkl 50.03 misc Exact solution misc Integral equations misc Klein–Gordon misc Potential theory misc Series expansion |
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Elektronische Aufsätze Aufsätze Elektronische Ressource |
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Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation |
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Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation |
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Fabrikant, V. I. |
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Journal of engineering mathematics |
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Fabrikant, V. I. Karapetian, E. Kalinin, S. V. |
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Fabrikant, V. I. |
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exact, approximate and asymptotic solutions of the klein–gordon integral equation |
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Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation |
| abstract |
Abstract Interaction of the highly localized probe of scanning probe microscopy with solid surfaces with mobile electronic or ionic carriers leads to the redistribution of mobile carriers at the tip surface junction. For small probe biases, this problem is equivalent to the Debye screening, described by Klein–Gordon (K–G) integral equation. Here, an exact solution to the K–G equation is derived for the case of a circle in the form of a convergent series expansion of the solution, which is effective for relatively small values of the inverse Debye length, k. Also, a reasonably accurate solution is derived for large values of parameter k by using the method of collocation. A surprisingly simple asymptotic solution is derived for very large values of k, which is valid for the arbitrary right-hand side of the equation. The same methods can be used for the case of elliptic domain. |
| abstractGer |
Abstract Interaction of the highly localized probe of scanning probe microscopy with solid surfaces with mobile electronic or ionic carriers leads to the redistribution of mobile carriers at the tip surface junction. For small probe biases, this problem is equivalent to the Debye screening, described by Klein–Gordon (K–G) integral equation. Here, an exact solution to the K–G equation is derived for the case of a circle in the form of a convergent series expansion of the solution, which is effective for relatively small values of the inverse Debye length, k. Also, a reasonably accurate solution is derived for large values of parameter k by using the method of collocation. A surprisingly simple asymptotic solution is derived for very large values of k, which is valid for the arbitrary right-hand side of the equation. The same methods can be used for the case of elliptic domain. |
| abstract_unstemmed |
Abstract Interaction of the highly localized probe of scanning probe microscopy with solid surfaces with mobile electronic or ionic carriers leads to the redistribution of mobile carriers at the tip surface junction. For small probe biases, this problem is equivalent to the Debye screening, described by Klein–Gordon (K–G) integral equation. Here, an exact solution to the K–G equation is derived for the case of a circle in the form of a convergent series expansion of the solution, which is effective for relatively small values of the inverse Debye length, k. Also, a reasonably accurate solution is derived for large values of parameter k by using the method of collocation. A surprisingly simple asymptotic solution is derived for very large values of k, which is valid for the arbitrary right-hand side of the equation. The same methods can be used for the case of elliptic domain. |
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Exact, approximate and asymptotic solutions of the Klein–Gordon integral equation |
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https://dx.doi.org/10.1007/s10665-019-09996-4 |
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Karapetian, E. Kalinin, S. V. |
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Karapetian, E. Kalinin, S. V. |
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| doi_str |
10.1007/s10665-019-09996-4 |
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2024-07-04T02:41:26.731Z |
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code="a">50.03</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">115</subfield><subfield code="j">2019</subfield><subfield code="e">1</subfield><subfield code="c">04</subfield><subfield code="h">141-156</subfield></datafield></record></collection>
|
| score |
7.40189 |