Cálculo del ancho de línea de la resonancia ferromagnética (FMR) en películas ultradelgadas
En este trabajo se empleó un formalismo clásico para determinar los anchos de línea de la resonancia ferromagnética (FMR) en una película ultradelgada. Como resultado, se derivó una expresión analítica para el campo magnético efectivo del sistema propuesto. Se llevó a cabo la expansión en serie de F...
- Autores:
-
Ortiz Olarte, Brayan De Jesús
- Tipo de recurso:
- Trabajo de grado de pregrado
- Fecha de publicación:
- 2024
- Institución:
- Universidad de Córdoba
- Repositorio:
- Repositorio Institucional Unicórdoba
- Idioma:
- spa
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- oai:repositorio.unicordoba.edu.co:ucordoba/8574
- Acceso en línea:
- https://repositorio.unicordoba.edu.co/handle/ucordoba/8574
https://repositorio.unicordoba.edu.co
- Palabra clave:
- Resonancia ferromagnética
Ancho de línea
Dinámica de magnetización
Ferromagnetic resonance
Line width
Magnetization dynamics
- Rights
- openAccess
- License
- Copyright Universidad de Córdoba, 2024
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Cálculo del ancho de línea de la resonancia ferromagnética (FMR) en películas ultradelgadas |
| title |
Cálculo del ancho de línea de la resonancia ferromagnética (FMR) en películas ultradelgadas |
| spellingShingle |
Cálculo del ancho de línea de la resonancia ferromagnética (FMR) en películas ultradelgadas Resonancia ferromagnética Ancho de línea Dinámica de magnetización Ferromagnetic resonance Line width Magnetization dynamics |
| title_short |
Cálculo del ancho de línea de la resonancia ferromagnética (FMR) en películas ultradelgadas |
| title_full |
Cálculo del ancho de línea de la resonancia ferromagnética (FMR) en películas ultradelgadas |
| title_fullStr |
Cálculo del ancho de línea de la resonancia ferromagnética (FMR) en películas ultradelgadas |
| title_full_unstemmed |
Cálculo del ancho de línea de la resonancia ferromagnética (FMR) en películas ultradelgadas |
| title_sort |
Cálculo del ancho de línea de la resonancia ferromagnética (FMR) en películas ultradelgadas |
| dc.creator.fl_str_mv |
Ortiz Olarte, Brayan De Jesús |
| dc.contributor.advisor.none.fl_str_mv |
López Ortiz, Javier |
| dc.contributor.author.none.fl_str_mv |
Ortiz Olarte, Brayan De Jesús |
| dc.contributor.jury.none.fl_str_mv |
Rosbel Jiménez Narváez Franklin Peniche Blanquicet |
| dc.subject.proposal.spa.fl_str_mv |
Resonancia ferromagnética Ancho de línea Dinámica de magnetización |
| topic |
Resonancia ferromagnética Ancho de línea Dinámica de magnetización Ferromagnetic resonance Line width Magnetization dynamics |
| dc.subject.keywords.eng.fl_str_mv |
Ferromagnetic resonance Line width Magnetization dynamics |
| description |
En este trabajo se empleó un formalismo clásico para determinar los anchos de línea de la resonancia ferromagnética (FMR) en una película ultradelgada. Como resultado, se derivó una expresión analítica para el campo magnético efectivo del sistema propuesto. Se llevó a cabo la expansión en serie de Fourier de los campos magnéticos y la magnetización. Asimismo, se calcularon las componentes dinámicas del campo magnético efectivo en función del vector de onda. Subsecuentemente, se determinaron las componentes del tensor de susceptibilidad magnética transversal. Finalmente, se estableció la relación de dispersión para el sistema. |
| publishDate |
2024 |
| dc.date.accessioned.none.fl_str_mv |
2024-08-21T14:30:30Z |
| dc.date.available.none.fl_str_mv |
2024-08-21T14:30:30Z |
| dc.date.issued.none.fl_str_mv |
2024-08-19 |
| dc.type.none.fl_str_mv |
Trabajo de grado - Pregrado |
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info:eu-repo/semantics/bachelorThesis |
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http://purl.org/coar/resource_type/c_7a1f |
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info:eu-repo/semantics/acceptedVersion |
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http://purl.org/coar/resource_type/c_7a1f |
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acceptedVersion |
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https://repositorio.unicordoba.edu.co/handle/ucordoba/8574 |
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Universidad de Córdoba |
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Repositorio Universidad de Córdoba |
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https://repositorio.unicordoba.edu.co |
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https://repositorio.unicordoba.edu.co/handle/ucordoba/8574 https://repositorio.unicordoba.edu.co |
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Universidad de Córdoba Repositorio Universidad de Córdoba |
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spa |
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spa |
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[1] C. Kittel, Excitation of Spin Waves in a Ferromagnet by a Uniform rf Field, Phys. Rev. 110, 1295, 1958, Vol. 110, No. 6, https://doi.org/10.1103/PhysRev.110.1295. [2] P. E. Wigen, C. F. Kooi, and M. R. Shanabarger, Bull. Am, Linewidths in Ferromagnetic Thin Films, J. Appl. Phys, 1963, Vol. 8, No. 248, https://doi.org/10.1063/1.1713481 [3] A. M. Portis, Appl. Phys, 1963, Letters 2, No. 69. [4] J. T. Davies, Effect of Nonuniform Magnetization on the Spin-Wave Spectrum in Thin Ferromagnetic Films, J. Appl. Phys, 1964, Vol. 35, No. 3, https://doi.org/10.1063/1.1713482. [5] O. G. Vendik, B. A. Kalinikos, and D. N. Chartorizhski, Instability of spin waves in tangentially magnetized ferromagnetic films, Soviet Phys. Solid State, vol. 19, p. 222, 1977. [6] D. D. Stancil, Magnetostatic waves in non-uniform bias fields including exchange effects, IEEE Trans. Mag., vol. MAG-16, p. 1153, 1980. [7] R. F. Sooho, Microwave Magnetics, New York: Harper and Row, 1985. [8] L. Landau and L. Lifshitz, Phys. Zeit. Sowjetunion, vol. 8, p. 153, 1935. [9] T. A. Gilbert, Equation of motion of magnetization, Armor Research Foundation, Chicago, IL, Tech. Rep. 11, January 1955. [10] C. E. Patton, Microwave resonance and relaxation in Magnetic Oxides, D. J. Craik, Ed. London, U.K.:Wiley, 1975, ch. 10, pp. 575–648. [11] Daniel D. Stancil Anil Prabhakar, Spin Waves Theory and Applications, 2008. [12] V. L. Safonov, Tensor form of magnetization damping, J. Appl. Phys., vol. 91, pp. 8653–8655, 2002. [13] D. J. Twisselmann and R. D. McMichael, Intrinsic damping and intentional ferromagnetic resonance broadening in thin Permalloy films, J. Appl. Phys., vol. 93, pp. 6903–6905, 2003. [14] R. D. McMichael, D. J. Twisselmann, and A. Kunz, Localized ferromagnetic resonance in inhomogeneous thin films, Phys. Rev. Lett., vol.90, pp. 227 601–227 601, 2003, https: //doi.org/10.1103/PhysRevLett.90.227601. [15] E. Schlomann, Inhomogeneous broadening of ferromagnetic resonance lines, Phys. Rev., vol. 182, pp. 632–645, 1969. [16] E. Schlomann, Ferromagnetic resonance in polycrystals, J. Phys. Radium, vol.20, pp. 327–332, 1959. [17] C. Chappert, K. L. Dang, P. Beauvillain, H. Hurdequint, and D. Renard, Ferromagnetic resonance studies of very thin cobalt films on a gold substrate, Phys. Rev. B, Condens. Matter, vol. 34, pp. 3192–3197, 1986. [18] S. Mizukami, Y. Ando, and T. Miyazaki, Ferromagnetic resonance linewidth for NM/80NiFe/NM films (NM = Cu, Ta, Pd and Pt), J. Magn. Magn. Mater., vol. 226–230, pp. 1640–1642, 2001. [19] W. Platow, A. N. Anisimov, G. L. Dunifer,M. Farle, and K. Baberschke, Correlations between ferromagnetic-resonance linewidths and sample quality in the study of metallic ultrathin films Phys. Rev. B, Condens. Matter, vol. 58, pp. 5611–5621, 1998. [20] B. Heinrich and J. F. Cochran, FMR linebroadening in metals due to two-magnon scattering, J. Appl. Phys., vol. 57, pp. 3690–3692, 1985. [21] T. D. Rossing, Resonance linewidth and anisotropy variation in thin films, J. Appl. Phys., vol. 34, pp. 995–995, 1963. [22] Q. H. F. Vrehen, Absorption and dispersion in porous and anisotropic polycrystalline ferrites at microwave frequencies, J. Appl. Phys., vol. 40, pp. 1849–1860, 1969. [23] Q. H. F. Vrehen, A. B. van Groenou, and J. G. M. de Lau, Relaxation of ferromagnetic precession by excitation of spin-waves in a polycrystalline ferrite Solid State Commun., vol. 7, pp. 117–121, 1969. [24] R. D. McMichael, M. D. Stiles, P. J. Chen, andW. F. Egelhoff, Jr., Ferromagnetic resonance linewidth in thin films coupled to NiO, J. Appl. Phys., vol. 83, no. 11, pp. 7037–7039, 1998, http://dx.doi.org/10.1063/1.367725. [25] B. A. Kalinikos and A. N. Slavin, Theory of dipole-exchange spin wave spectrum for ferromagnetic films with mixed exchange boundary conditions, J. Phys. C, Solid State Phys., vol. 19, pp. 7013–7033, 1986, 10.1088/0022-3719/19/35/014. [26] K. J. Harte, Theory of magnetization ripple in ferromagnetic films, J. Appl. Phys., vol. 39, no. 3, pp. 1503–1524, 1968, https://doi.org/10.1063/1.1656388. [27] M. J. Hurben and C. E. Patton, Theory of two magnon scattering microwave relaxation and ferromagnetic resonance linewidth in magnetic thin films, J. Appl. Phys., vol. 83, no. 8, pp. 4344–4365, 1998, https://doi.org/10.1063/1.367194. [28] A. M. Clogston, H. Suhl, L. R. Walker, and P. W. Anderson, Ferromagnetic resonance line width in insulating materials, J. Phys. Chem. Solids, vol. 1, pp. 129–136, 1956, https: //doi.org/10.1016/0022-3697(56)90019-1. [29] J. F. Cochran, R. W. Qiao, and B. Heinrich, Two-magnon contribution to the ferromagnetic resonance linewidth in amorphous ferromagnetic metals Phys. Rev. B, Condens. Matter, vol. 39, pp. 4399–4408, 1989, https://doi.org/10.1103/PhysRevB.39.4399. [30] H. B. Callen, Fluctuation, Relaxation and Resonance in Magnetic Systems, Edinburgh, U.K.: Oliver and Boyd, 1962, ch. 4, pp. 69–85. [31] M. Sparks, Ferromagnetic Relaxation Theory . Advanced Physics Monograph Series. New York: McGraw–Hill, 1964. [32] M. Sparks, Ferromagnetic resonance in thin films. II. Theory of linewidths Phys. Rev. B, Condens. Matter, vol. 1, pp. 3856–3869, 1970, https://doi.org/10.1103/PhysRevB.1. 3856. |
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López Ortiz, Javier43bf1c65-9afe-408f-b549-298eb1c5d895-1Ortiz Olarte, Brayan De Jesús5db83e46-e293-4a61-8df3-304452dde5ac-1Rosbel Jiménez Narváez7df0b95b-ca1f-4e13-8367-3d9a963476d0-1Franklin Peniche Blanquicet2ce76096-fcd1-4393-9779-6ab5cee5624e-12024-08-21T14:30:30Z2024-08-21T14:30:30Z2024-08-19https://repositorio.unicordoba.edu.co/handle/ucordoba/8574Universidad de CórdobaRepositorio Universidad de Córdobahttps://repositorio.unicordoba.edu.coEn este trabajo se empleó un formalismo clásico para determinar los anchos de línea de la resonancia ferromagnética (FMR) en una película ultradelgada. Como resultado, se derivó una expresión analítica para el campo magnético efectivo del sistema propuesto. Se llevó a cabo la expansión en serie de Fourier de los campos magnéticos y la magnetización. Asimismo, se calcularon las componentes dinámicas del campo magnético efectivo en función del vector de onda. Subsecuentemente, se determinaron las componentes del tensor de susceptibilidad magnética transversal. Finalmente, se estableció la relación de dispersión para el sistema.1. Introducción ...................................................................................................... 72. Tensor de susceptibilidad .............................................................................. 92.1. Ecuación de movimiento para la magnetización ...................................... 92.2. Susceptibilidad sin intercambio ni anisotropía ........................................ 122.3. Susceptibilidad con intercambio y anisotropía ........................................ 162.4. Amortiguación magnética ........................................................................... 213. Modos normales de ondas de espines ....................................................... 394. Teoría cuántica de dos magnones ............................................................... 465. Modelo clásico de dos magnones ................................................................ 546. Conclusiones ................................................................................................... 617. Referencias bibliográficas ............................................................................. 63PregradoFísico(a)Trabajos de Investigación y/o Extensiónapplication/pdfspaUniversidad de CórdobaFacultad de Ciencias BásicasMontería, Córdoba, ColombiaFísicaCopyright Universidad de Córdoba, 2024https://creativecommons.org/licenses/by-nc-nd/4.0/Atribución-NoComercial-SinDerivadas 4.0 Internacional (CC BY-NC-ND 4.0)info:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2https://repositorio.unicordoba.edu.coCálculo del ancho de línea de la resonancia ferromagnética (FMR) en películas ultradelgadasTrabajo de grado - Pregradoinfo:eu-repo/semantics/bachelorThesishttp://purl.org/coar/resource_type/c_7a1finfo:eu-repo/semantics/acceptedVersion[1] C. Kittel, Excitation of Spin Waves in a Ferromagnet by a Uniform rf Field, Phys. Rev. 110, 1295, 1958, Vol. 110, No. 6, https://doi.org/10.1103/PhysRev.110.1295.[2] P. E. Wigen, C. F. Kooi, and M. R. Shanabarger, Bull. Am, Linewidths in Ferromagnetic Thin Films, J. Appl. Phys, 1963, Vol. 8, No. 248, https://doi.org/10.1063/1.1713481[3] A. M. Portis, Appl. Phys, 1963, Letters 2, No. 69.[4] J. T. Davies, Effect of Nonuniform Magnetization on the Spin-Wave Spectrum in Thin Ferromagnetic Films, J. Appl. Phys, 1964, Vol. 35, No. 3, https://doi.org/10.1063/1.1713482.[5] O. G. Vendik, B. A. Kalinikos, and D. N. Chartorizhski, Instability of spin waves in tangentially magnetized ferromagnetic films, Soviet Phys. Solid State, vol. 19, p. 222, 1977.[6] D. D. Stancil, Magnetostatic waves in non-uniform bias fields including exchange effects, IEEE Trans. Mag., vol. MAG-16, p. 1153, 1980.[7] R. F. Sooho, Microwave Magnetics, New York: Harper and Row, 1985.[8] L. Landau and L. Lifshitz, Phys. Zeit. Sowjetunion, vol. 8, p. 153, 1935.[9] T. A. Gilbert, Equation of motion of magnetization, Armor Research Foundation, Chicago, IL, Tech. Rep. 11, January 1955.[10] C. E. Patton, Microwave resonance and relaxation in Magnetic Oxides, D. J. Craik, Ed. London, U.K.:Wiley, 1975, ch. 10, pp. 575–648.[11] Daniel D. Stancil Anil Prabhakar, Spin Waves Theory and Applications, 2008.[12] V. L. Safonov, Tensor form of magnetization damping, J. Appl. Phys., vol. 91, pp. 8653–8655, 2002.[13] D. J. Twisselmann and R. D. McMichael, Intrinsic damping and intentional ferromagnetic resonance broadening in thin Permalloy films, J. Appl. Phys., vol. 93, pp. 6903–6905, 2003.[14] R. D. McMichael, D. J. Twisselmann, and A. Kunz, Localized ferromagnetic resonance in inhomogeneous thin films, Phys. Rev. Lett., vol.90, pp. 227 601–227 601, 2003, https: //doi.org/10.1103/PhysRevLett.90.227601.[15] E. Schlomann, Inhomogeneous broadening of ferromagnetic resonance lines, Phys. Rev., vol. 182, pp. 632–645, 1969.[16] E. Schlomann, Ferromagnetic resonance in polycrystals, J. Phys. Radium, vol.20, pp. 327–332, 1959.[17] C. Chappert, K. L. Dang, P. Beauvillain, H. Hurdequint, and D. Renard, Ferromagnetic resonance studies of very thin cobalt films on a gold substrate, Phys. Rev. B, Condens. Matter, vol. 34, pp. 3192–3197, 1986.[18] S. Mizukami, Y. Ando, and T. Miyazaki, Ferromagnetic resonance linewidth for NM/80NiFe/NM films (NM = Cu, Ta, Pd and Pt), J. Magn. Magn. Mater., vol. 226–230, pp. 1640–1642, 2001.[19] W. Platow, A. N. Anisimov, G. L. Dunifer,M. Farle, and K. Baberschke, Correlations between ferromagnetic-resonance linewidths and sample quality in the study of metallic ultrathin films Phys. Rev. B, Condens. Matter, vol. 58, pp. 5611–5621, 1998.[20] B. Heinrich and J. F. Cochran, FMR linebroadening in metals due to two-magnon scattering, J. Appl. Phys., vol. 57, pp. 3690–3692, 1985.[21] T. D. Rossing, Resonance linewidth and anisotropy variation in thin films, J. Appl. Phys., vol. 34, pp. 995–995, 1963.[22] Q. H. F. Vrehen, Absorption and dispersion in porous and anisotropic polycrystalline ferrites at microwave frequencies, J. Appl. Phys., vol. 40, pp. 1849–1860, 1969.[23] Q. H. F. Vrehen, A. B. van Groenou, and J. G. M. de Lau, Relaxation of ferromagnetic precession by excitation of spin-waves in a polycrystalline ferrite Solid State Commun., vol. 7, pp. 117–121, 1969.[24] R. D. McMichael, M. D. Stiles, P. J. Chen, andW. F. Egelhoff, Jr., Ferromagnetic resonance linewidth in thin films coupled to NiO, J. Appl. Phys., vol. 83, no. 11, pp. 7037–7039, 1998, http://dx.doi.org/10.1063/1.367725.[25] B. A. Kalinikos and A. N. Slavin, Theory of dipole-exchange spin wave spectrum for ferromagnetic films with mixed exchange boundary conditions, J. Phys. C, Solid State Phys., vol. 19, pp. 7013–7033, 1986, 10.1088/0022-3719/19/35/014.[26] K. J. Harte, Theory of magnetization ripple in ferromagnetic films, J. Appl. Phys., vol. 39, no. 3, pp. 1503–1524, 1968, https://doi.org/10.1063/1.1656388.[27] M. J. Hurben and C. E. Patton, Theory of two magnon scattering microwave relaxation and ferromagnetic resonance linewidth in magnetic thin films, J. Appl. Phys., vol. 83, no. 8, pp. 4344–4365, 1998, https://doi.org/10.1063/1.367194.[28] A. M. Clogston, H. Suhl, L. R. Walker, and P. W. Anderson, Ferromagnetic resonance line width in insulating materials, J. Phys. Chem. Solids, vol. 1, pp. 129–136, 1956, https: //doi.org/10.1016/0022-3697(56)90019-1.[29] J. F. Cochran, R. W. Qiao, and B. Heinrich, Two-magnon contribution to the ferromagnetic resonance linewidth in amorphous ferromagnetic metals Phys. Rev. B, Condens. Matter, vol. 39, pp. 4399–4408, 1989, https://doi.org/10.1103/PhysRevB.39.4399.[30] H. B. Callen, Fluctuation, Relaxation and Resonance in Magnetic Systems, Edinburgh, U.K.: Oliver and Boyd, 1962, ch. 4, pp. 69–85.[31] M. Sparks, Ferromagnetic Relaxation Theory . Advanced Physics Monograph Series. New York: McGraw–Hill, 1964.[32] M. Sparks, Ferromagnetic resonance in thin films. II. Theory of linewidths Phys. Rev. B, Condens. Matter, vol. 1, pp. 3856–3869, 1970, https://doi.org/10.1103/PhysRevB.1. 3856.Resonancia ferromagnéticaAncho de líneaDinámica de magnetizaciónFerromagnetic resonanceLine widthMagnetization dynamicsPublicationORIGINALOrtizOlarteBrayanDeJesus.pdfOrtizOlarteBrayanDeJesus.pdfapplication/pdf584814https://repositorio.unicordoba.edu.co/bitstreams/90b3a6f1-1124-4aab-9d53-3091849ff8e7/downloadc66b7c2664fca36128ee687e56c8c984MD51Formato de autorización.pdfFormato de autorización.pdfapplication/pdf568165https://repositorio.unicordoba.edu.co/bitstreams/6a4db229-a34c-4bd0-95fc-039e26534555/download0a03f82807b78c14a65af4a77378e5b5MD52LICENSElicense.txtlicense.txttext/plain; charset=utf-815543https://repositorio.unicordoba.edu.co/bitstreams/d73656a7-9a10-408c-8ce8-e9af12a2a272/download73a5432e0b76442b22b026844140d683MD53TEXTOrtizOlarteBrayanDeJesus.pdf.txtOrtizOlarteBrayanDeJesus.pdf.txtExtracted 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