Magnetic response of split ring resonator metamaterials: From effective medium dispersion to photonic band gaps
Abstract On systematically investigating the electromagnetic response of periodic split-ring resonator (SRR) metamaterials as a function of the size-to-wavelength (a/λ) ratio, we find that the stop bands due to the geometric resonances of the SRR weaken with increasing (a/λ) ratio, and are eventuall...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
CHAKRABARTI, SANGEETA [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2012 |
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| Schlagwörter: |
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| Anmerkung: |
© Indian Academy of Sciences 2012 |
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| Übergeordnetes Werk: |
Enthalten in: Pramāna - Springer-Verlag, 1973, 78(2012), 3 vom: 17. Feb., Seite 483-492 |
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| Übergeordnetes Werk: |
volume:78 ; year:2012 ; number:3 ; day:17 ; month:02 ; pages:483-492 |
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10.1007/s12043-011-0241-x |
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| 520 | |a Abstract On systematically investigating the electromagnetic response of periodic split-ring resonator (SRR) metamaterials as a function of the size-to-wavelength (a/λ) ratio, we find that the stop bands due to the geometric resonances of the SRR weaken with increasing (a/λ) ratio, and are eventually replaced by stop bands due to Bragg scattering. Our study traces the behaviour of SRR-based metamaterials as the resonance frequency increases and the wavelength of the radiation finally becomes comparable to the size of the unit cell of the metamaterial. In the intermediate stages, the dispersion of the SRR metamaterial can still be described as due to a localized magnetic resonances while Bragg scattering finally becomes the dominant phenomenon as a/λ∼1/2. | ||
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10.1007/s12043-011-0241-x doi (DE-627)OLC2076058494 (DE-He213)s12043-011-0241-x-p DE-627 ger DE-627 rakwb eng 530 VZ CHAKRABARTI, SANGEETA verfasserin aut Magnetic response of split ring resonator metamaterials: From effective medium dispersion to photonic band gaps 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2012 Abstract On systematically investigating the electromagnetic response of periodic split-ring resonator (SRR) metamaterials as a function of the size-to-wavelength (a/λ) ratio, we find that the stop bands due to the geometric resonances of the SRR weaken with increasing (a/λ) ratio, and are eventually replaced by stop bands due to Bragg scattering. Our study traces the behaviour of SRR-based metamaterials as the resonance frequency increases and the wavelength of the radiation finally becomes comparable to the size of the unit cell of the metamaterial. In the intermediate stages, the dispersion of the SRR metamaterial can still be described as due to a localized magnetic resonances while Bragg scattering finally becomes the dominant phenomenon as a/λ∼1/2. Metamaterials split-ring resonators magnetic resonance RAMAKRISHNA, S ANANTHA aut Enthalten in Pramāna Springer-Verlag, 1973 78(2012), 3 vom: 17. Feb., Seite 483-492 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:78 year:2012 number:3 day:17 month:02 pages:483-492 https://doi.org/10.1007/s12043-011-0241-x lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 78 2012 3 17 02 483-492 |
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10.1007/s12043-011-0241-x doi (DE-627)OLC2076058494 (DE-He213)s12043-011-0241-x-p DE-627 ger DE-627 rakwb eng 530 VZ CHAKRABARTI, SANGEETA verfasserin aut Magnetic response of split ring resonator metamaterials: From effective medium dispersion to photonic band gaps 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2012 Abstract On systematically investigating the electromagnetic response of periodic split-ring resonator (SRR) metamaterials as a function of the size-to-wavelength (a/λ) ratio, we find that the stop bands due to the geometric resonances of the SRR weaken with increasing (a/λ) ratio, and are eventually replaced by stop bands due to Bragg scattering. Our study traces the behaviour of SRR-based metamaterials as the resonance frequency increases and the wavelength of the radiation finally becomes comparable to the size of the unit cell of the metamaterial. In the intermediate stages, the dispersion of the SRR metamaterial can still be described as due to a localized magnetic resonances while Bragg scattering finally becomes the dominant phenomenon as a/λ∼1/2. Metamaterials split-ring resonators magnetic resonance RAMAKRISHNA, S ANANTHA aut Enthalten in Pramāna Springer-Verlag, 1973 78(2012), 3 vom: 17. Feb., Seite 483-492 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:78 year:2012 number:3 day:17 month:02 pages:483-492 https://doi.org/10.1007/s12043-011-0241-x lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 78 2012 3 17 02 483-492 |
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10.1007/s12043-011-0241-x doi (DE-627)OLC2076058494 (DE-He213)s12043-011-0241-x-p DE-627 ger DE-627 rakwb eng 530 VZ CHAKRABARTI, SANGEETA verfasserin aut Magnetic response of split ring resonator metamaterials: From effective medium dispersion to photonic band gaps 2012 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Indian Academy of Sciences 2012 Abstract On systematically investigating the electromagnetic response of periodic split-ring resonator (SRR) metamaterials as a function of the size-to-wavelength (a/λ) ratio, we find that the stop bands due to the geometric resonances of the SRR weaken with increasing (a/λ) ratio, and are eventually replaced by stop bands due to Bragg scattering. Our study traces the behaviour of SRR-based metamaterials as the resonance frequency increases and the wavelength of the radiation finally becomes comparable to the size of the unit cell of the metamaterial. In the intermediate stages, the dispersion of the SRR metamaterial can still be described as due to a localized magnetic resonances while Bragg scattering finally becomes the dominant phenomenon as a/λ∼1/2. Metamaterials split-ring resonators magnetic resonance RAMAKRISHNA, S ANANTHA aut Enthalten in Pramāna Springer-Verlag, 1973 78(2012), 3 vom: 17. Feb., Seite 483-492 (DE-627)129403342 (DE-600)186949-8 (DE-576)014785102 0304-4289 nnns volume:78 year:2012 number:3 day:17 month:02 pages:483-492 https://doi.org/10.1007/s12043-011-0241-x lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_70 AR 78 2012 3 17 02 483-492 |
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Abstract On systematically investigating the electromagnetic response of periodic split-ring resonator (SRR) metamaterials as a function of the size-to-wavelength (a/λ) ratio, we find that the stop bands due to the geometric resonances of the SRR weaken with increasing (a/λ) ratio, and are eventually replaced by stop bands due to Bragg scattering. Our study traces the behaviour of SRR-based metamaterials as the resonance frequency increases and the wavelength of the radiation finally becomes comparable to the size of the unit cell of the metamaterial. In the intermediate stages, the dispersion of the SRR metamaterial can still be described as due to a localized magnetic resonances while Bragg scattering finally becomes the dominant phenomenon as a/λ∼1/2. © Indian Academy of Sciences 2012 |
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Abstract On systematically investigating the electromagnetic response of periodic split-ring resonator (SRR) metamaterials as a function of the size-to-wavelength (a/λ) ratio, we find that the stop bands due to the geometric resonances of the SRR weaken with increasing (a/λ) ratio, and are eventually replaced by stop bands due to Bragg scattering. Our study traces the behaviour of SRR-based metamaterials as the resonance frequency increases and the wavelength of the radiation finally becomes comparable to the size of the unit cell of the metamaterial. In the intermediate stages, the dispersion of the SRR metamaterial can still be described as due to a localized magnetic resonances while Bragg scattering finally becomes the dominant phenomenon as a/λ∼1/2. © Indian Academy of Sciences 2012 |
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Abstract On systematically investigating the electromagnetic response of periodic split-ring resonator (SRR) metamaterials as a function of the size-to-wavelength (a/λ) ratio, we find that the stop bands due to the geometric resonances of the SRR weaken with increasing (a/λ) ratio, and are eventually replaced by stop bands due to Bragg scattering. Our study traces the behaviour of SRR-based metamaterials as the resonance frequency increases and the wavelength of the radiation finally becomes comparable to the size of the unit cell of the metamaterial. In the intermediate stages, the dispersion of the SRR metamaterial can still be described as due to a localized magnetic resonances while Bragg scattering finally becomes the dominant phenomenon as a/λ∼1/2. © Indian Academy of Sciences 2012 |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2076058494</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230402042933.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s2012 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s12043-011-0241-x</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2076058494</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s12043-011-0241-x-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">CHAKRABARTI, SANGEETA</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Magnetic response of split ring resonator metamaterials: From effective medium dispersion to photonic band gaps</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2012</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Indian Academy of Sciences 2012</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract On systematically investigating the electromagnetic response of periodic split-ring resonator (SRR) metamaterials as a function of the size-to-wavelength (a/λ) ratio, we find that the stop bands due to the geometric resonances of the SRR weaken with increasing (a/λ) ratio, and are eventually replaced by stop bands due to Bragg scattering. Our study traces the behaviour of SRR-based metamaterials as the resonance frequency increases and the wavelength of the radiation finally becomes comparable to the size of the unit cell of the metamaterial. In the intermediate stages, the dispersion of the SRR metamaterial can still be described as due to a localized magnetic resonances while Bragg scattering finally becomes the dominant phenomenon as a/λ∼1/2.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Metamaterials</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">split-ring resonators</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">magnetic resonance</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">RAMAKRISHNA, S ANANTHA</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Pramāna</subfield><subfield code="d">Springer-Verlag, 1973</subfield><subfield code="g">78(2012), 3 vom: 17. 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