Diffraction from a moving grating
Abstract A first-principles tutorial account is given for the diffraction of either light or free, non-relativistic, massive particles from a moving grating. Discussion on the properties of the moving grating including non-reciprocity is followed by considering both Raman-Nath (thin grating) diffrac...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Bahabad, Alon [verfasserIn] |
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| Format: |
Artikel |
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| Sprache: |
Englisch |
| Erschienen: |
2013 |
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| Schlagwörter: |
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| Anmerkung: |
© Springer Science+Business Media New York 2013 |
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| Übergeordnetes Werk: |
Enthalten in: Optical and quantum electronics - Springer US, 1975, 46(2013), 8 vom: 16. Nov., Seite 1065-1077 |
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| Übergeordnetes Werk: |
volume:46 ; year:2013 ; number:8 ; day:16 ; month:11 ; pages:1065-1077 |
| Links: |
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| DOI / URN: |
10.1007/s11082-013-9825-7 |
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| Katalog-ID: |
OLC2081990156 |
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| 520 | |a Abstract A first-principles tutorial account is given for the diffraction of either light or free, non-relativistic, massive particles from a moving grating. Discussion on the properties of the moving grating including non-reciprocity is followed by considering both Raman-Nath (thin grating) diffraction and Bragg (thick grating) diffraction in either transmission or reflection geometry. Use of four-momentum conservation with dispersion relations yield the angles of diffraction. The increase in the angle of diffraction for grazing incident by using a moving grating relative to using a static grating is calculated. It is shown that this increase is possible only for Raman-Nath geometry. | ||
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10.1007/s11082-013-9825-7 doi (DE-627)OLC2081990156 (DE-He213)s11082-013-9825-7-p DE-627 ger DE-627 rakwb eng 500 620 VZ Bahabad, Alon verfasserin aut Diffraction from a moving grating 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2013 Abstract A first-principles tutorial account is given for the diffraction of either light or free, non-relativistic, massive particles from a moving grating. Discussion on the properties of the moving grating including non-reciprocity is followed by considering both Raman-Nath (thin grating) diffraction and Bragg (thick grating) diffraction in either transmission or reflection geometry. Use of four-momentum conservation with dispersion relations yield the angles of diffraction. The increase in the angle of diffraction for grazing incident by using a moving grating relative to using a static grating is calculated. It is shown that this increase is possible only for Raman-Nath geometry. Optical diffraction Material diffraction Physical optics Enthalten in Optical and quantum electronics Springer US, 1975 46(2013), 8 vom: 16. Nov., Seite 1065-1077 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:46 year:2013 number:8 day:16 month:11 pages:1065-1077 https://doi.org/10.1007/s11082-013-9825-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 GBV_ILN_4700 AR 46 2013 8 16 11 1065-1077 |
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10.1007/s11082-013-9825-7 doi (DE-627)OLC2081990156 (DE-He213)s11082-013-9825-7-p DE-627 ger DE-627 rakwb eng 500 620 VZ Bahabad, Alon verfasserin aut Diffraction from a moving grating 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2013 Abstract A first-principles tutorial account is given for the diffraction of either light or free, non-relativistic, massive particles from a moving grating. Discussion on the properties of the moving grating including non-reciprocity is followed by considering both Raman-Nath (thin grating) diffraction and Bragg (thick grating) diffraction in either transmission or reflection geometry. Use of four-momentum conservation with dispersion relations yield the angles of diffraction. The increase in the angle of diffraction for grazing incident by using a moving grating relative to using a static grating is calculated. It is shown that this increase is possible only for Raman-Nath geometry. Optical diffraction Material diffraction Physical optics Enthalten in Optical and quantum electronics Springer US, 1975 46(2013), 8 vom: 16. Nov., Seite 1065-1077 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:46 year:2013 number:8 day:16 month:11 pages:1065-1077 https://doi.org/10.1007/s11082-013-9825-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 GBV_ILN_4700 AR 46 2013 8 16 11 1065-1077 |
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10.1007/s11082-013-9825-7 doi (DE-627)OLC2081990156 (DE-He213)s11082-013-9825-7-p DE-627 ger DE-627 rakwb eng 500 620 VZ Bahabad, Alon verfasserin aut Diffraction from a moving grating 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2013 Abstract A first-principles tutorial account is given for the diffraction of either light or free, non-relativistic, massive particles from a moving grating. Discussion on the properties of the moving grating including non-reciprocity is followed by considering both Raman-Nath (thin grating) diffraction and Bragg (thick grating) diffraction in either transmission or reflection geometry. Use of four-momentum conservation with dispersion relations yield the angles of diffraction. The increase in the angle of diffraction for grazing incident by using a moving grating relative to using a static grating is calculated. It is shown that this increase is possible only for Raman-Nath geometry. Optical diffraction Material diffraction Physical optics Enthalten in Optical and quantum electronics Springer US, 1975 46(2013), 8 vom: 16. Nov., Seite 1065-1077 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:46 year:2013 number:8 day:16 month:11 pages:1065-1077 https://doi.org/10.1007/s11082-013-9825-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 GBV_ILN_4700 AR 46 2013 8 16 11 1065-1077 |
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10.1007/s11082-013-9825-7 doi (DE-627)OLC2081990156 (DE-He213)s11082-013-9825-7-p DE-627 ger DE-627 rakwb eng 500 620 VZ Bahabad, Alon verfasserin aut Diffraction from a moving grating 2013 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer Science+Business Media New York 2013 Abstract A first-principles tutorial account is given for the diffraction of either light or free, non-relativistic, massive particles from a moving grating. Discussion on the properties of the moving grating including non-reciprocity is followed by considering both Raman-Nath (thin grating) diffraction and Bragg (thick grating) diffraction in either transmission or reflection geometry. Use of four-momentum conservation with dispersion relations yield the angles of diffraction. The increase in the angle of diffraction for grazing incident by using a moving grating relative to using a static grating is calculated. It is shown that this increase is possible only for Raman-Nath geometry. Optical diffraction Material diffraction Physical optics Enthalten in Optical and quantum electronics Springer US, 1975 46(2013), 8 vom: 16. Nov., Seite 1065-1077 (DE-627)129419540 (DE-600)189950-8 (DE-576)014796139 0306-8919 nnns volume:46 year:2013 number:8 day:16 month:11 pages:1065-1077 https://doi.org/10.1007/s11082-013-9825-7 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-TEC SSG-OLC-PHY GBV_ILN_22 GBV_ILN_70 GBV_ILN_150 GBV_ILN_4700 AR 46 2013 8 16 11 1065-1077 |
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Abstract A first-principles tutorial account is given for the diffraction of either light or free, non-relativistic, massive particles from a moving grating. Discussion on the properties of the moving grating including non-reciprocity is followed by considering both Raman-Nath (thin grating) diffraction and Bragg (thick grating) diffraction in either transmission or reflection geometry. Use of four-momentum conservation with dispersion relations yield the angles of diffraction. The increase in the angle of diffraction for grazing incident by using a moving grating relative to using a static grating is calculated. It is shown that this increase is possible only for Raman-Nath geometry. © Springer Science+Business Media New York 2013 |
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Abstract A first-principles tutorial account is given for the diffraction of either light or free, non-relativistic, massive particles from a moving grating. Discussion on the properties of the moving grating including non-reciprocity is followed by considering both Raman-Nath (thin grating) diffraction and Bragg (thick grating) diffraction in either transmission or reflection geometry. Use of four-momentum conservation with dispersion relations yield the angles of diffraction. The increase in the angle of diffraction for grazing incident by using a moving grating relative to using a static grating is calculated. It is shown that this increase is possible only for Raman-Nath geometry. © Springer Science+Business Media New York 2013 |
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Abstract A first-principles tutorial account is given for the diffraction of either light or free, non-relativistic, massive particles from a moving grating. Discussion on the properties of the moving grating including non-reciprocity is followed by considering both Raman-Nath (thin grating) diffraction and Bragg (thick grating) diffraction in either transmission or reflection geometry. Use of four-momentum conservation with dispersion relations yield the angles of diffraction. The increase in the angle of diffraction for grazing incident by using a moving grating relative to using a static grating is calculated. It is shown that this increase is possible only for Raman-Nath geometry. © Springer Science+Business Media New York 2013 |
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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">OLC2081990156</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230503233848.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">230228s2013 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s11082-013-9825-7</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2081990156</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s11082-013-9825-7-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">500</subfield><subfield code="a">620</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Bahabad, Alon</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Diffraction from a moving grating</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2013</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">© Springer Science+Business Media New York 2013</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract A first-principles tutorial account is given for the diffraction of either light or free, non-relativistic, massive particles from a moving grating. Discussion on the properties of the moving grating including non-reciprocity is followed by considering both Raman-Nath (thin grating) diffraction and Bragg (thick grating) diffraction in either transmission or reflection geometry. Use of four-momentum conservation with dispersion relations yield the angles of diffraction. The increase in the angle of diffraction for grazing incident by using a moving grating relative to using a static grating is calculated. It is shown that this increase is possible only for Raman-Nath geometry.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Optical diffraction</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Material diffraction</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Physical optics</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Optical and quantum electronics</subfield><subfield code="d">Springer US, 1975</subfield><subfield code="g">46(2013), 8 vom: 16. Nov., Seite 1065-1077</subfield><subfield code="w">(DE-627)129419540</subfield><subfield code="w">(DE-600)189950-8</subfield><subfield code="w">(DE-576)014796139</subfield><subfield code="x">0306-8919</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:46</subfield><subfield code="g">year:2013</subfield><subfield code="g">number:8</subfield><subfield code="g">day:16</subfield><subfield code="g">month:11</subfield><subfield code="g">pages:1065-1077</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/s11082-013-9825-7</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-TEC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_150</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4700</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">46</subfield><subfield code="j">2013</subfield><subfield code="e">8</subfield><subfield code="b">16</subfield><subfield code="c">11</subfield><subfield code="h">1065-1077</subfield></datafield></record></collection>
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