Angle of arrival estimation using spectral interferometry
Identifieur interne :
003A90 ( PascalFrancis/Curation );
précédent :
003A89;
suivant :
003A91
Angle of arrival estimation using spectral interferometry
Auteurs : Z. W. Barber [
États-Unis] ;
C. Harrington [
États-Unis] ;
C. W. Thiel [
États-Unis] ;
W. R. Babbitt [
États-Unis] ;
R. Krishna Mohan [
États-Unis]
Source :
-
Journal of luminescence [ 0022-2313 ] ; 2010.
RBID : Pascal:10-0355002
Descripteurs français
- Pascal (Inist)
- Traitement signal,
Holographie,
Etude théorique,
Méthode analytique,
Interféromètre Mach Zehnder,
Interférométrie optique,
Hyperfréquence,
Composé ternaire,
Grenat aluminium yttrium,
Temps retard,
Angle arrivée,
YAG,
Y3Al5O12,
Al O Y,
0760L,
4240,
Système réseau en phase.
English descriptors
- KwdEn :
- Analytical method,
Arrival angle,
Holography,
Light interferometry,
Mach-Zehnder interferometers,
Microwave radiation,
Phased-array systems,
Signal processing,
Ternary compounds,
Theoretical study,
Time delay,
YAG.
Abstract
We have developed a correlative signal processing concept based on a Mach-Zehnder interferometer and spatial-spectral (S2) materials that enables direct mapping of RF spectral phase as well as power spectral recording. This configuration can be used for precise frequency resolved time delay estimation between signals received by a phased antenna array system that in turn could be utilized to estimate the angle of arrival. We present an analytical theoretical model and a proof-of-principle demonstration of the concept of time difference of arrival estimation with a cryogenically cooled Tm:YAG crystal that operates on microwave signals modulated onto a stabilized optical carrier at 793 nm.
| pA |
| A01 | 01 | 1 | | @0 0022-2313 |
|---|
| A02 | 01 | | | @0 JLUMA8 |
|---|
| A03 | | 1 | | @0 J. lumin. |
|---|
| A05 | | | | @2 130 |
|---|
| A06 | | | | @2 9 |
|---|
| A08 | 01 | 1 | ENG | @1 Angle of arrival estimation using spectral interferometry |
|---|
| A09 | 01 | 1 | ENG | @1 Special Issue based on the Proceedings of the Tenth International Meeting on Hole Burning, Single Molecule, and Related Spectroscopies: Science and Applications (HBSM 2009), Palm cove, Australia, June 22-27, 2009. Issue dedicated to Ivan Lorgeré and Oliver Guillot-Noël |
|---|
| A11 | 01 | 1 | | @1 BARBER (Z. W.) |
|---|
| A11 | 02 | 1 | | @1 HARRINGTON (C.) |
|---|
| A11 | 03 | 1 | | @1 THIEL (C. W.) |
|---|
| A11 | 04 | 1 | | @1 BABBITT (W. R.) |
|---|
| A11 | 05 | 1 | | @1 KRISHNA MOHAN (R.) |
|---|
| A12 | 01 | 1 | | @1 CHANELIERE (Thierry) @9 ed. |
|---|
| A12 | 02 | 1 | | @1 SELLARS (Matt J.) @9 ed. |
|---|
| A12 | 03 | 1 | | @1 MANSON (Neil B.) @9 ed. |
|---|
| A14 | 01 | | | @1 Spectrum Lab, Montana State University @2 Bozeman, MT 59717 @3 USA @Z 1 aut. @Z 2 aut. @Z 3 aut. @Z 4 aut. @Z 5 aut. |
|---|
| A15 | 01 | | | @1 Laboratoire Aimé Cotton, CNRS-UPR 3321, Univ. Paris-Sud, Bât. 505 @2 91405 Orsay @3 FRA @Z 1 aut. |
|---|
| A15 | 02 | | | @1 Laser Physics Centre, Research School of Physics and Engineering, The Australian National University @2 Canberra, ACT 0200 @3 AUS @Z 2 aut. @Z 3 aut. |
|---|
| A20 | | | | @1 1614-1618 |
|---|
| A21 | | | | @1 2010 |
|---|
| A23 | 01 | | | @0 ENG |
|---|
| A43 | 01 | | | @1 INIST @2 14666 @5 354000193752120100 |
|---|
| A44 | | | | @0 0000 @1 © 2010 INIST-CNRS. All rights reserved. |
|---|
| A45 | | | | @0 12 ref. |
|---|
| A47 | 01 | 1 | | @0 10-0355002 |
|---|
| A60 | | | | @1 P @2 C |
|---|
| A61 | | | | @0 A |
|---|
| A64 | 01 | 1 | | @0 Journal of luminescence |
|---|
| A66 | 01 | | | @0 NLD |
|---|
| C01 | 01 | | ENG | @0 We have developed a correlative signal processing concept based on a Mach-Zehnder interferometer and spatial-spectral (S2) materials that enables direct mapping of RF spectral phase as well as power spectral recording. This configuration can be used for precise frequency resolved time delay estimation between signals received by a phased antenna array system that in turn could be utilized to estimate the angle of arrival. We present an analytical theoretical model and a proof-of-principle demonstration of the concept of time difference of arrival estimation with a cryogenically cooled Tm:YAG crystal that operates on microwave signals modulated onto a stabilized optical carrier at 793 nm. |
|---|
| C02 | 01 | 3 | | @0 001B00G60L |
|---|
| C02 | 02 | 3 | | @0 001B40B40 |
|---|
| C03 | 01 | 3 | FRE | @0 Traitement signal @5 03 |
|---|
| C03 | 01 | 3 | ENG | @0 Signal processing @5 03 |
|---|
| C03 | 02 | 3 | FRE | @0 Holographie @5 19 |
|---|
| C03 | 02 | 3 | ENG | @0 Holography @5 19 |
|---|
| C03 | 03 | 3 | FRE | @0 Etude théorique @5 21 |
|---|
| C03 | 03 | 3 | ENG | @0 Theoretical study @5 21 |
|---|
| C03 | 04 | X | FRE | @0 Méthode analytique @5 23 |
|---|
| C03 | 04 | X | ENG | @0 Analytical method @5 23 |
|---|
| C03 | 04 | X | SPA | @0 Método analítico @5 23 |
|---|
| C03 | 05 | 3 | FRE | @0 Interféromètre Mach Zehnder @5 30 |
|---|
| C03 | 05 | 3 | ENG | @0 Mach-Zehnder interferometers @5 30 |
|---|
| C03 | 06 | 3 | FRE | @0 Interférométrie optique @5 31 |
|---|
| C03 | 06 | 3 | ENG | @0 Light interferometry @5 31 |
|---|
| C03 | 07 | 3 | FRE | @0 Hyperfréquence @5 37 |
|---|
| C03 | 07 | 3 | ENG | @0 Microwave radiation @5 37 |
|---|
| C03 | 08 | 3 | FRE | @0 Composé ternaire @5 50 |
|---|
| C03 | 08 | 3 | ENG | @0 Ternary compounds @5 50 |
|---|
| C03 | 09 | 3 | FRE | @0 Grenat aluminium yttrium @5 51 |
|---|
| C03 | 09 | 3 | ENG | @0 YAG @5 51 |
|---|
| C03 | 10 | 3 | FRE | @0 Temps retard @5 61 |
|---|
| C03 | 10 | 3 | ENG | @0 Time delay @5 61 |
|---|
| C03 | 11 | X | FRE | @0 Angle arrivée @5 62 |
|---|
| C03 | 11 | X | ENG | @0 Arrival angle @5 62 |
|---|
| C03 | 11 | X | SPA | @0 Angulo llegada @5 62 |
|---|
| C03 | 12 | 3 | FRE | @0 YAG @4 INC @5 71 |
|---|
| C03 | 13 | 3 | FRE | @0 Y3Al5O12 @4 INC @5 72 |
|---|
| C03 | 14 | 3 | FRE | @0 Al O Y @4 INC @5 75 |
|---|
| C03 | 15 | 3 | FRE | @0 0760L @4 INC @5 83 |
|---|
| C03 | 16 | 3 | FRE | @0 4240 @4 INC @5 84 |
|---|
| C03 | 17 | 3 | FRE | @0 Système réseau en phase @4 CD @5 96 |
|---|
| C03 | 17 | 3 | ENG | @0 Phased-array systems @4 CD @5 96 |
|---|
| N21 | | | | @1 228 |
|---|
|
|---|
| pR |
| A30 | 01 | 1 | ENG | @1 International Conference on Hole Burning, Single Molecule, and Related Spectroscopies: Science and Applications (HBSM 2009) @2 10 @3 Palm Cove AUS @4 2009-06-22 |
|---|
|
|---|
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Le document en format XML
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<author><name sortKey="Barber, Z W" sort="Barber, Z W" uniqKey="Barber Z" first="Z. W." last="Barber">Z. W. Barber</name>
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<s2>Bozeman, MT 59717</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
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</affiliation><author><name sortKey="Harrington, C" sort="Harrington, C" uniqKey="Harrington C" first="C." last="Harrington">C. Harrington</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Spectrum Lab, Montana State University</s1>
<s2>Bozeman, MT 59717</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><country>États-Unis</country>
</affiliation><author><name sortKey="Thiel, C W" sort="Thiel, C W" uniqKey="Thiel C" first="C. W." last="Thiel">C. W. Thiel</name>
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<s3>USA</s3>
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<sZ>3 aut.</sZ>
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</inist:fA14><country>États-Unis</country>
</affiliation><author><name sortKey="Babbitt, W R" sort="Babbitt, W R" uniqKey="Babbitt W" first="W. R." last="Babbitt">W. R. Babbitt</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Spectrum Lab, Montana State University</s1>
<s2>Bozeman, MT 59717</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
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</affiliation><author><name sortKey="Krishna Mohan, R" sort="Krishna Mohan, R" uniqKey="Krishna Mohan R" first="R." last="Krishna Mohan">R. Krishna Mohan</name>
<affiliation wicri:level="1"><inist:fA14 i1="01"><s1>Spectrum Lab, Montana State University</s1>
<s2>Bozeman, MT 59717</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</inist:fA14><country>États-Unis</country>
</affiliation><series><title level="j" type="main">Journal of luminescence</title>
<title level="j" type="abbreviated">J. lumin.</title>
<idno type="ISSN">0022-2313</idno>
<imprint><date when="2010">2010</date>
</imprint><seriesStmt><title level="j" type="main">Journal of luminescence</title>
<title level="j" type="abbreviated">J. lumin.</title>
<idno type="ISSN">0022-2313</idno>
</seriesStmt><profileDesc><textClass><keywords scheme="KwdEn" xml:lang="en"><term>Analytical method</term>
<term>Arrival angle</term>
<term>Holography</term>
<term>Light interferometry</term>
<term>Mach-Zehnder interferometers</term>
<term>Microwave radiation</term>
<term>Phased-array systems</term>
<term>Signal processing</term>
<term>Ternary compounds</term>
<term>Theoretical study</term>
<term>Time delay</term>
<term>YAG</term>
</keywords><keywords scheme="Pascal" xml:lang="fr"><term>Traitement signal</term>
<term>Holographie</term>
<term>Etude théorique</term>
<term>Méthode analytique</term>
<term>Interféromètre Mach Zehnder</term>
<term>Interférométrie optique</term>
<term>Hyperfréquence</term>
<term>Composé ternaire</term>
<term>Grenat aluminium yttrium</term>
<term>Temps retard</term>
<term>Angle arrivée</term>
<term>YAG</term>
<term>Y3Al5O12</term>
<term>Al O Y</term>
<term>0760L</term>
<term>4240</term>
<term>Système réseau en phase</term>
</keywords><front><div type="abstract" xml:lang="en">We have developed a correlative signal processing concept based on a Mach-Zehnder interferometer and spatial-spectral (S2) materials that enables direct mapping of RF spectral phase as well as power spectral recording. This configuration can be used for precise frequency resolved time delay estimation between signals received by a phased antenna array system that in turn could be utilized to estimate the angle of arrival. We present an analytical theoretical model and a proof-of-principle demonstration of the concept of time difference of arrival estimation with a cryogenically cooled Tm:YAG crystal that operates on microwave signals modulated onto a stabilized optical carrier at 793 nm.</div>
</front><inist><standard h6="B"><pA><fA01 i1="01" i2="1"><s0>0022-2313</s0>
</fA01><fA02 i1="01"><s0>JLUMA8</s0>
</fA02><fA03 i2="1"><s0>J. lumin.</s0>
</fA03><fA05><s2>130</s2>
</fA05><fA08 i1="01" i2="1" l="ENG"><s1>Angle of arrival estimation using spectral interferometry</s1>
</fA08><fA09 i1="01" i2="1" l="ENG"><s1>Special Issue based on the Proceedings of the Tenth International Meeting on Hole Burning, Single Molecule, and Related Spectroscopies: Science and Applications (HBSM 2009), Palm cove, Australia, June 22-27, 2009. Issue dedicated to Ivan Lorgeré and Oliver Guillot-Noël</s1>
</fA09><fA11 i1="01" i2="1"><s1>BARBER (Z. W.)</s1>
</fA11><fA11 i1="02" i2="1"><s1>HARRINGTON (C.)</s1>
</fA11><fA11 i1="03" i2="1"><s1>THIEL (C. W.)</s1>
</fA11><fA11 i1="04" i2="1"><s1>BABBITT (W. R.)</s1>
</fA11><fA11 i1="05" i2="1"><s1>KRISHNA MOHAN (R.)</s1>
</fA11><fA12 i1="01" i2="1"><s1>CHANELIERE (Thierry)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="02" i2="1"><s1>SELLARS (Matt J.)</s1>
<s9>ed.</s9>
</fA12><fA12 i1="03" i2="1"><s1>MANSON (Neil B.)</s1>
<s9>ed.</s9>
</fA12><fA14 i1="01"><s1>Spectrum Lab, Montana State University</s1>
<s2>Bozeman, MT 59717</s2>
<s3>USA</s3>
<sZ>1 aut.</sZ>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
<sZ>4 aut.</sZ>
<sZ>5 aut.</sZ>
</fA14><fA15 i1="01"><s1>Laboratoire Aimé Cotton, CNRS-UPR 3321, Univ. Paris-Sud, Bât. 505</s1>
<s2>91405 Orsay</s2>
<s3>FRA</s3>
<sZ>1 aut.</sZ>
</fA15><fA15 i1="02"><s1>Laser Physics Centre, Research School of Physics and Engineering, The Australian National University</s1>
<s2>Canberra, ACT 0200</s2>
<s3>AUS</s3>
<sZ>2 aut.</sZ>
<sZ>3 aut.</sZ>
</fA15><fA20><s1>1614-1618</s1>
</fA20><fA21><s1>2010</s1>
</fA21><fA23 i1="01"><s0>ENG</s0>
</fA23><fA43 i1="01"><s1>INIST</s1>
<s2>14666</s2>
<s5>354000193752120100</s5>
</fA43><fA44><s0>0000</s0>
<s1>© 2010 INIST-CNRS. All rights reserved.</s1>
</fA44><fA45><s0>12 ref.</s0>
</fA45><fA47 i1="01" i2="1"><s0>10-0355002</s0>
</fA47><fA60><s1>P</s1>
<s2>C</s2>
</fA60><fA64 i1="01" i2="1"><s0>Journal of luminescence</s0>
</fA64><fA66 i1="01"><s0>NLD</s0>
</fA66><fC01 i1="01" l="ENG"><s0>We have developed a correlative signal processing concept based on a Mach-Zehnder interferometer and spatial-spectral (S2) materials that enables direct mapping of RF spectral phase as well as power spectral recording. This configuration can be used for precise frequency resolved time delay estimation between signals received by a phased antenna array system that in turn could be utilized to estimate the angle of arrival. We present an analytical theoretical model and a proof-of-principle demonstration of the concept of time difference of arrival estimation with a cryogenically cooled Tm:YAG crystal that operates on microwave signals modulated onto a stabilized optical carrier at 793 nm.</s0>
</fC01><fC02 i1="01" i2="3"><s0>001B00G60L</s0>
</fC02><fC02 i1="02" i2="3"><s0>001B40B40</s0>
</fC02><fC03 i1="01" i2="3" l="FRE"><s0>Traitement signal</s0>
<s5>03</s5>
</fC03><fC03 i1="01" i2="3" l="ENG"><s0>Signal processing</s0>
<s5>03</s5>
</fC03><fC03 i1="02" i2="3" l="FRE"><s0>Holographie</s0>
<s5>19</s5>
</fC03><fC03 i1="02" i2="3" l="ENG"><s0>Holography</s0>
<s5>19</s5>
</fC03><fC03 i1="03" i2="3" l="FRE"><s0>Etude théorique</s0>
<s5>21</s5>
</fC03><fC03 i1="03" i2="3" l="ENG"><s0>Theoretical study</s0>
<s5>21</s5>
</fC03><fC03 i1="04" i2="X" l="FRE"><s0>Méthode analytique</s0>
<s5>23</s5>
</fC03><fC03 i1="04" i2="X" l="ENG"><s0>Analytical method</s0>
<s5>23</s5>
</fC03><fC03 i1="04" i2="X" l="SPA"><s0>Método analítico</s0>
<s5>23</s5>
</fC03><fC03 i1="05" i2="3" l="FRE"><s0>Interféromètre Mach Zehnder</s0>
<s5>30</s5>
</fC03><fC03 i1="05" i2="3" l="ENG"><s0>Mach-Zehnder interferometers</s0>
<s5>30</s5>
</fC03><fC03 i1="06" i2="3" l="FRE"><s0>Interférométrie optique</s0>
<s5>31</s5>
</fC03><fC03 i1="06" i2="3" l="ENG"><s0>Light interferometry</s0>
<s5>31</s5>
</fC03><fC03 i1="07" i2="3" l="FRE"><s0>Hyperfréquence</s0>
<s5>37</s5>
</fC03><fC03 i1="07" i2="3" l="ENG"><s0>Microwave radiation</s0>
<s5>37</s5>
</fC03><fC03 i1="08" i2="3" l="FRE"><s0>Composé ternaire</s0>
<s5>50</s5>
</fC03><fC03 i1="08" i2="3" l="ENG"><s0>Ternary compounds</s0>
<s5>50</s5>
</fC03><fC03 i1="09" i2="3" l="FRE"><s0>Grenat aluminium yttrium</s0>
<s5>51</s5>
</fC03><fC03 i1="09" i2="3" l="ENG"><s0>YAG</s0>
<s5>51</s5>
</fC03><fC03 i1="10" i2="3" l="FRE"><s0>Temps retard</s0>
<s5>61</s5>
</fC03><fC03 i1="10" i2="3" l="ENG"><s0>Time delay</s0>
<s5>61</s5>
</fC03><fC03 i1="11" i2="X" l="FRE"><s0>Angle arrivée</s0>
<s5>62</s5>
</fC03><fC03 i1="11" i2="X" l="ENG"><s0>Arrival angle</s0>
<s5>62</s5>
</fC03><fC03 i1="11" i2="X" l="SPA"><s0>Angulo llegada</s0>
<s5>62</s5>
</fC03><fC03 i1="12" i2="3" l="FRE"><s0>YAG</s0>
<s4>INC</s4>
<s5>71</s5>
</fC03><fC03 i1="13" i2="3" l="FRE"><s0>Y3Al5O12</s0>
<s4>INC</s4>
<s5>72</s5>
</fC03><fC03 i1="14" i2="3" l="FRE"><s0>Al O Y</s0>
<s4>INC</s4>
<s5>75</s5>
</fC03><fC03 i1="15" i2="3" l="FRE"><s0>0760L</s0>
<s4>INC</s4>
<s5>83</s5>
</fC03><fC03 i1="16" i2="3" l="FRE"><s0>4240</s0>
<s4>INC</s4>
<s5>84</s5>
</fC03><fC03 i1="17" i2="3" l="FRE"><s0>Système réseau en phase</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03><fC03 i1="17" i2="3" l="ENG"><s0>Phased-array systems</s0>
<s4>CD</s4>
<s5>96</s5>
</fC03><fN21><s1>228</s1>
</fN21><pR><fA30 i1="01" i2="1" l="ENG"><s1>International Conference on Hole Burning, Single Molecule, and Related Spectroscopies: Science and Applications (HBSM 2009)</s1>
<s2>10</s2>
<s3>Palm Cove AUS</s3>
<s4>2009-06-22</s4>
</fA30>
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