アンテナアレイファクターによる電波画像処理とその応用
小 林 弘 一
• • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • •
(2020 年 7 月 31
• • • • • • • • • •
Imaging Technology of Electromagnetic Wave by Using Antenna Array-Factor and
its Application
Hirokazu Kobayashi
Electromagnetic Information System Laboratory,
Department of Electronics and Information Systems Engineering
Abstract
• •
The array factor (AF) describes the electromagnetic radiation characteristic of an array of numerous small antenna
elements; the antenna composed of these plural elements is called an array antenna. The AF concept can be applied not
only to antenna characteristic theory but also to the image processing method discussed in this paper. Synthetic aperture
radar (SAR) is a typical imaging method for microwaves. In this method, the transmitting and receiving antennae are
moved in a wide area to generate an equivalent large antenna, and the reflected signal is processed to obtain an image
with high resolution based on the beam with higher sharpness. In general, SAR systems tend to be large and have
advantages for distant targets such as satellite SAR and earth mapping.
On the other hand, AF theory superposes the signals received from each element in consideration of the path
difference, which is the phase variation between the transmitting and receiving elements via the target scatterer.
Therefore, unlike SAR, a focal point of the array can be obtained, allowing short-range targets to be imaged with high
resolution. However, both methods are equivalent for image processing through Fourier theory. In this paper, the authors
will review previously published articles and discuss various applications and future prospects, such as equivalent
complex-permittivity measurements, wall-through radar, and near-field to far-field transformation methods.
キ ー ワ ー ド ;
ア レ イ フ ァ ク タ ー
, レ ー ダ 画 像 , ア レ イ ア ン テ ナ , 合 成 開 口 レ ー ダ , 誘 電 率 計 測 ,
壁透過レーダ
, 近傍電磁界遠方変換, 幾何光学解説理論, MIMO レーダ
Keyword;
Array-factor, radar imaging, array antenna, synthetic aperture radar, focusing, permittivity measurement,
wall-through radar, near-field to far-field transformation, geometrical theory of diffraction (GTD), MIMO
radar.
アンテナアレイファクターによる電波画像処理とその応用
小 林 弘 一
• • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • • •
(2020 年 7 月 31
• • • • • • • • • •
Imaging Technology of Electromagnetic Wave by Using Antenna Array-Factor and
its Application
Hirokazu Kobayashi
Electromagnetic Information System Laboratory,
Department of Electronics and Information Systems Engineering
Abstract
• •
The array factor (AF) describes the electromagnetic radiation characteristic of an array of numerous small antenna
elements; the antenna composed of these plural elements is called an array antenna. The AF concept can be applied not
only to antenna characteristic theory but also to the image processing method discussed in this paper. Synthetic aperture
radar (SAR) is a typical imaging method for microwaves. In this method, the transmitting and receiving antennae are
moved in a wide area to generate an equivalent large antenna, and the reflected signal is processed to obtain an image
with high resolution based on the beam with higher sharpness. In general, SAR systems tend to be large and have
advantages for distant targets such as satellite SAR and earth mapping.
On the other hand, AF theory superposes the signals received from each element in consideration of the path
difference, which is the phase variation between the transmitting and receiving elements via the target scatterer.
Therefore, unlike SAR, a focal point of the array can be obtained, allowing short-range targets to be imaged with high
resolution. However, both methods are equivalent for image processing through Fourier theory. In this paper, the authors
will review previously published articles and discuss various applications and future prospects, such as equivalent
complex-permittivity measurements, wall-through radar, and near-field to far-field transformation methods.
キ ー ワ ー ド ;
ア レ イ フ ァ ク タ ー
, レ ー ダ 画 像 , ア レ イ ア ン テ ナ , 合 成 開 口 レ ー ダ , 誘 電 率 計 測 ,
壁透過レーダ
, 近傍電磁界遠方変換, 幾何光学解説理論, MIMO レーダ
Keyword;
Array-factor, radar imaging, array antenna, synthetic aperture radar, focusing, permittivity measurement,
wall-through radar, near-field to far-field transformation, geometrical theory of diffraction (GTD), MIMO
radar.
電子情報システム工学科,波動情報システム研究室
(2020 年 7 月 31 日受理)
Osaka Institute of Technology Vol. 65, No. 1(2020)pp. 21〜42
1.·͕͖͑ ΞϨΠϑΝΫλʔ(Array-Factor:AF)ͱɺిؾతʹ খ͞ͳΞϯςφ(ૉࢠΞϯςφͱݺΜͰ͍Δ)Λෳݸ ྻͨ͠ͱ͖ͷΞϯςφશମ͕࡞Δ์ࣹಛੑΛࢦ͢ɻ࣮ࡍ ͜ͷAFʹ֤ૉࢠͷࢦੑΛॏͤͨ͞ͷ͕ΞϨΠΞ ϯςφͷ࠷ऴ์ࣹύλʔϯͱͳΔɻ͜ͷΞϨΠΞϯςφ ͷ֤ૉࢠͷҐ૬ࠩΛ͋ΔΞϧΰϦζϜͰੜ͢ΔͱɺAF ίϯϑΥʔϚϧΞϨΠΛؚΉిࢠࠪͷϏʔϜϑΥʔ Ϛʔͱͯ͠ݟΔ͜ͱ͕Ͱ͖Δ͠[1]ɺ֤ૉࢠʹॏΈΛ͚ Δ͜ͱͰΞμϓςΟϒͳॲཧՄೳͱͳΔɻ·ͨɺۙ ݯͱͯ͠AFΛଊ͑ΔͱԕํมͷΞϧΰϦζϜʹԠ ༻Ͱ͖Δ[2]ɻAF֤ૉࢠͷԆҐ૬ͷͱͳΔͷͰɺ ͜͜Ͱओʹٞ͢Δిը૾ॲཧͷՄೳੑ͋Δ[3,4]ɻ ຊͰɺಋମฏ൘ͳͲͷ୯७ͳλʔήοτʹΑΔࣹ ࢄཚʹର͠ɺۙքΛؚΉͦͷཧܭࢉΛ༻͍ͨը ૾ॲཧ͓Αͼ࣮ଌ֬ೝʹ͍ͭͯɺࠓ·Ͱͷஶऀͷจݙ Λ·ͱΊΔܗͰٞ͠ɺࠓޙͷݚڀൃలͷࢿͱ͍ͨ͠ɻ ͳ͓ɺ࣮ଌσʔλʹΑΔը૾͚ͩͰͳ͘ܭࢉཧͰγ ϛϡϨʔγϣϯ͕Ͱ͖Δͱ͍͏͜ͱɺص্Ͱ֬ೝ࡞ ۀ͕Ͱ͖Δͱ͍͏͜ͱΛҙຯ͠ɺ༷ʑͳύϥϝʔλͷ࠷ దԽΛਤΔ͜ͱ͕ՄೳͱͳΔɻ લड़ͷΞϨΠΞϯςφʹΑΔϨʔμը૾ͷߟ͑ํɺ ૹ৴Ξϯςφɺඪମɺͦͯ͠ड৴ΞϯςφؒͷҐ૬ ใͱরࣹྖҬͷඪ͔ΒͷཧతͳΤίʔ৴߸ͷ Ґ૬ใͷ૬ؔੑΛΈΔํ๏Ͱ͋Δɻ͜ͷ૬ؔੑ؆୯ ͳҐ૬ͷڃܭࢉͰߦ͏͜ͱ͕Ͱ͖ɺ݁Ռ͕ղೳͷ ্ʹͭͳ͕ΔҰछͷ߹։ޱॲཧͱΈͳ͢͜ͱ͕Ͱ͖Δɻ ిΛૹ৴͠ɺͦͷΤίʔΛड৴͢ΔͨΊʹɺΞϨΠ ͷ֤ૉࢠΛશͯ༻ҙ͢Δඞཁͳ͍ɻλʔήοτͱϨʔ μͷҐஔ͕ؔ૬ରతʹݻఆ͞Ε͍ͯΔɺ͋Δ͍ॲཧ ϨʔτͰ΄΅Ҡಈ͍ͯ͠ͳ͍ɺͳͲ͕ԾఆͰ͖Δͱɺ1 ݸͷΞϯςφΛػցతʹࠪͯ͠Α͍ɻ·ͨɺૹड৴ Ξϯςφճ࿏ͷෳࡶ͞Λආ͚ΔͨΊɺผʑʹ༻ҙ͢Δ ํ͕ଌఆܥ؆୯ʹͳΔɻྫ͑ɺ൚༻ͷωοτϫʔΫ ΞφϥΠβͳͲΛૹ৴ݯ͓Αͼड৴ܥʹ༻͍Δ߹ɺૹ ड৴ͷΞΠιϨʔγϣϯΛऔΔͨΊʹૹ৴ͱड৴ͷΞϯ ςφΛۭؒతʹ͢ߏՄೳͰ͋Δɻ·ͨҠಈ͢Δૹ ৴ͷҐஔ࠲ඪͱड৴ͷͦΕҧ͍ͬͯͯΑ͘ɺૹ৴ϙ Πϯτͷํ͕ड৴ΑΓগͳ͍ߏίετޮ͕ߴ͍ ͱࢥΘΕΔɻ͜ͷΑ͏ʹߟ͑ΔͱɺAFʹΑΔը૾ॲཧ ݱࡏपͱͳ͍ͬͯΔMIMO(Multiple-input multiple output)ϨʔμͱجຊతʹՁͰ͋Δ͜ͱ͕͔Δɻ ຊͷ༰ҎԼͷΑ͏ʹͳ͍ͬͯΔɻઌ߲ͣ࣍Ͱ AFͷఆࣜΛߦ͍ɺΞϯςφϏʔϜΛిࢠతʹࠪ͢Δ ϑΣʔζυΞϨΠΞϯςφΛྫʹͱͬͯɺAFͷجຊతͳ ߟ͑ํΛड़Δɻଓ͘3.߲ͰɺۙڑλʔήοτΛҙ ࣝͯ͠ΞϨΠͷযԽΛߦ͍ɺ4.߲Ͱɺ͜ͷযԽAF ΛͬͨϨʔμը૾ʹ͍ͭͯٞ͢Δɻ5.߲Ͱɺը૾ ͷཧݕ౼Λߦ͏ͨΊɺλʔήοτ͕ಋମετϦοϓͷ ͱ͖ͷUniform Asymptotic Theory(UAT)ͱPhysical
Optics(PO)ʹΑΔఆࣜԽߦ͍ɺ6.߲Ͱ2ຕͷετϦο ϓΛަͤͨ͞ίʔφʔϦϑϨΫλʔϞσϧͷ࣮ଌͱܭ ࢉͷൺֱݕ౼Λߦ͏ɻଓ͚ͯɺ7.߲ͰΞϯςφϏʔϜΛ ߟྀͨ͠ͱ͖ͷը૾ධՁɺ8.߲Ͱ༠ిମฏ൘͕͋Δ ߹ͷը૾ݕ౼Λٞ͢Δɻ༠ిମฏ൘นಁաϨʔμͱ ͯ͠ݟͳ͢͜ͱ͕Ͱ͖Δɻͦͯ͠ɺ༠ిମฏ൘ͷ༗ແʹ Αͬͯը૾ͷੜҐஔ͕มԽ͢Δ͜ͱΛԠ༻͢Δͱɺฏ ൘ͷՁ༠ిΛධՁ͢Δ͜ͱ͕Ͱ͖Δɻ͜ͷٞΛ9. ߲ͱ10.߲Ͱߦ͏ɻ·ͨ1.Ͱɺجຊύϥϝʔλͷ มԽʹΑΔը૾γϛϡϨʔγϣϯ݁ՌΛఏࣔͯ͠Δɻ 2.ΞϨΠϑΝΫλʔͷఆࣜͱϏʔϜࠪ ࠓɺෳͷݯ͕ܗ͢Δి࣓քʹରͯ͠ɺͦͷݯΛ ͱͯ͠ଊ͑ํੑͷ์ࣹύλʔϯΛԾఆ͢Δɻͦͯ͠ɺ ֤ݯʢΞϯςφʣͦͷҐஔͰڅిͷҐ૬ಉ͡Ͱ͋ Δͱͯ͠ɺԕํͰͷి࣓քΛ֤Ξϯςφͷ࠲ඪʹΑΔҐ ૬ࠩҟΛߟྀͨ͠ಈͷ୯७ͳॏͶ߹ͤͰදݱ͢Δɻ ݯྻ࠲ඪ͕ฏ໘ͷ߹ɺAFFourierڃͱಉ͡ܗͱ ͳΔɻ࣮ࡍͷ֤Ξϯςφࢦੑ͕͋ΔͷͰɺ͜ΕΛAF ʹॏͤ͞ΔͱɺΞϨΠશମͷ߹์ࣹύλʔϯ͕ܭࢉ Ͱ͖ΔɻͨͩɺΞϯςφؒͷۭؒ૬ޓ݁߹Λແࢹ͍ͯ͠ ΔͷͰɺ݅ʹΑ࣮ͬͯࡍͱ߹Θͳ͍߹ൃੜ͢Δɻ ্ͯ͞ड़ͷΑ͏ʹɺۭؒͷҙ࠲ඪʹݯ͕ݽཱ ͯ͠ྻ͞Ε͍ͯΔͱ͖ͷAFɺݯͷҐ૬ͦͷҐஔ ࠲ඪʹґଘ͍ͯ͠ΔͷͰɺٿ࠲ඪͷ֯มΛ(θ, ϕ)ͱ ͯ͠ɺ୯७ʹ f (θ, ϕ) =∑anexp{jk(xnu + ynv + zncos θ)} (1) Ͱ༩͑Δ͜ͱ͕Ͱ͖Δɻ͜͜Ͱɺ(xn, yn, zn)n൪ૉ
ࢠͷ3࣍ݩۭؒ࠲ඪ(u = sin θ cos ϕ, v = sin θ sin ϕ)Ͱ͋
Γɺk = 2π/λΛࢦ͢ɻ·ͨɺan֤ૉࢠͷෳૉৼ ෯Ͱ͋Δɻ͜ͷ؆ܿͳجຊࣜঢ়ͷ์ࣹݯͷू߹͕ԕ ํͰͭ͘Δ์ࣹքΛද͍ͯ͠Δ͕ɺ࣮ࡍଘࡏ͍ͯ͠Δͱ ࢥΘΕΔ֤Ξϯςφૉࢠؒͷి࣓քతͳ૬ޓ݁߹ແࢹ ͍ͯ͠Δɻਤ11࣍ݩͷִؒϦχΞΞϨΠʹฏ໘ ͕ೖࣹͨ͠ͱ͖ɺ֤ૉࢠʹྭى͞ΕΔҐ૬ࠩΛࣔͨ͠
1.·͕͖͑ ΞϨΠϑΝΫλʔ(Array-Factor:AF)ͱɺిؾతʹ খ͞ͳΞϯςφ(ૉࢠΞϯςφͱݺΜͰ͍Δ)Λෳݸ ྻͨ͠ͱ͖ͷΞϯςφશମ͕࡞Δ์ࣹಛੑΛࢦ͢ɻ࣮ࡍ ͜ͷAFʹ֤ૉࢠͷࢦੑΛॏͤͨ͞ͷ͕ΞϨΠΞ ϯςφͷ࠷ऴ์ࣹύλʔϯͱͳΔɻ͜ͷΞϨΠΞϯςφ ͷ֤ૉࢠͷҐ૬ࠩΛ͋ΔΞϧΰϦζϜͰੜ͢ΔͱɺAF ίϯϑΥʔϚϧΞϨΠΛؚΉిࢠࠪͷϏʔϜϑΥʔ Ϛʔͱͯ͠ݟΔ͜ͱ͕Ͱ͖Δ͠[1]ɺ֤ૉࢠʹॏΈΛ͚ Δ͜ͱͰΞμϓςΟϒͳॲཧՄೳͱͳΔɻ·ͨɺۙ ݯͱͯ͠AFΛଊ͑ΔͱԕํมͷΞϧΰϦζϜʹԠ ༻Ͱ͖Δ[2]ɻAF֤ૉࢠͷԆҐ૬ͷͱͳΔͷͰɺ ͜͜Ͱओʹٞ͢Δిը૾ॲཧͷՄೳੑ͋Δ[3,4]ɻ ຊͰɺಋମฏ൘ͳͲͷ୯७ͳλʔήοτʹΑΔࣹ ࢄཚʹର͠ɺۙքΛؚΉͦͷཧܭࢉΛ༻͍ͨը ૾ॲཧ͓Αͼ࣮ଌ֬ೝʹ͍ͭͯɺࠓ·Ͱͷஶऀͷจݙ Λ·ͱΊΔܗͰٞ͠ɺࠓޙͷݚڀൃలͷࢿͱ͍ͨ͠ɻ ͳ͓ɺ࣮ଌσʔλʹΑΔը૾͚ͩͰͳ͘ܭࢉཧͰγ ϛϡϨʔγϣϯ͕Ͱ͖Δͱ͍͏͜ͱɺص্Ͱ֬ೝ࡞ ۀ͕Ͱ͖Δͱ͍͏͜ͱΛҙຯ͠ɺ༷ʑͳύϥϝʔλͷ࠷ దԽΛਤΔ͜ͱ͕ՄೳͱͳΔɻ લड़ͷΞϨΠΞϯςφʹΑΔϨʔμը૾ͷߟ͑ํɺ ૹ৴Ξϯςφɺඪମɺͦͯ͠ड৴ΞϯςφؒͷҐ૬ ใͱরࣹྖҬͷඪ͔ΒͷཧతͳΤίʔ৴߸ͷ Ґ૬ใͷ૬ؔੑΛΈΔํ๏Ͱ͋Δɻ͜ͷ૬ؔੑ؆୯ ͳҐ૬ͷڃܭࢉͰߦ͏͜ͱ͕Ͱ͖ɺ݁Ռ͕ղೳͷ ্ʹͭͳ͕ΔҰछͷ߹։ޱॲཧͱΈͳ͢͜ͱ͕Ͱ͖Δɻ ిΛૹ৴͠ɺͦͷΤίʔΛड৴͢ΔͨΊʹɺΞϨΠ ͷ֤ૉࢠΛશͯ༻ҙ͢Δඞཁͳ͍ɻλʔήοτͱϨʔ μͷҐஔ͕ؔ૬ରతʹݻఆ͞Ε͍ͯΔɺ͋Δ͍ॲཧ ϨʔτͰ΄΅Ҡಈ͍ͯ͠ͳ͍ɺͳͲ͕ԾఆͰ͖Δͱɺ1 ݸͷΞϯςφΛػցతʹࠪͯ͠Α͍ɻ·ͨɺૹड৴ Ξϯςφճ࿏ͷෳࡶ͞Λආ͚ΔͨΊɺผʑʹ༻ҙ͢Δ ํ͕ଌఆܥ؆୯ʹͳΔɻྫ͑ɺ൚༻ͷωοτϫʔΫ ΞφϥΠβͳͲΛૹ৴ݯ͓Αͼड৴ܥʹ༻͍Δ߹ɺૹ ड৴ͷΞΠιϨʔγϣϯΛऔΔͨΊʹૹ৴ͱड৴ͷΞϯ ςφΛۭؒతʹ͢ߏՄೳͰ͋Δɻ·ͨҠಈ͢Δૹ ৴ͷҐஔ࠲ඪͱड৴ͷͦΕҧ͍ͬͯͯΑ͘ɺૹ৴ϙ Πϯτͷํ͕ड৴ΑΓগͳ͍ߏίετޮ͕ߴ͍ ͱࢥΘΕΔɻ͜ͷΑ͏ʹߟ͑ΔͱɺAFʹΑΔը૾ॲཧ ݱࡏपͱͳ͍ͬͯΔMIMO(Multiple-input multiple output)ϨʔμͱجຊతʹՁͰ͋Δ͜ͱ͕͔Δɻ ຊͷ༰ҎԼͷΑ͏ʹͳ͍ͬͯΔɻઌ߲ͣ࣍Ͱ AFͷఆࣜΛߦ͍ɺΞϯςφϏʔϜΛిࢠతʹࠪ͢Δ ϑΣʔζυΞϨΠΞϯςφΛྫʹͱͬͯɺAFͷجຊతͳ ߟ͑ํΛड़Δɻଓ͘3.߲ͰɺۙڑλʔήοτΛҙ ࣝͯ͠ΞϨΠͷযԽΛߦ͍ɺ4.߲Ͱɺ͜ͷযԽAF ΛͬͨϨʔμը૾ʹ͍ͭͯٞ͢Δɻ5.߲Ͱɺը૾ ͷཧݕ౼Λߦ͏ͨΊɺλʔήοτ͕ಋମετϦοϓͷ ͱ͖ͷUniform Asymptotic Theory(UAT)ͱPhysical
Optics(PO)ʹΑΔఆࣜԽߦ͍ɺ6.߲Ͱ2ຕͷετϦο ϓΛަͤͨ͞ίʔφʔϦϑϨΫλʔϞσϧͷ࣮ଌͱܭ ࢉͷൺֱݕ౼Λߦ͏ɻଓ͚ͯɺ7.߲ͰΞϯςφϏʔϜΛ ߟྀͨ͠ͱ͖ͷը૾ධՁɺ8.߲Ͱ༠ిମฏ൘͕͋Δ ߹ͷը૾ݕ౼Λٞ͢Δɻ༠ిମฏ൘นಁաϨʔμͱ ͯ͠ݟͳ͢͜ͱ͕Ͱ͖Δɻͦͯ͠ɺ༠ిମฏ൘ͷ༗ແʹ Αͬͯը૾ͷੜҐஔ͕มԽ͢Δ͜ͱΛԠ༻͢Δͱɺฏ ൘ͷՁ༠ిΛධՁ͢Δ͜ͱ͕Ͱ͖Δɻ͜ͷٞΛ9. ߲ͱ10.߲Ͱߦ͏ɻ·ͨ1.Ͱɺجຊύϥϝʔλͷ มԽʹΑΔը૾γϛϡϨʔγϣϯ݁ՌΛఏࣔͯ͠Δɻ 2.ΞϨΠϑΝΫλʔͷఆࣜͱϏʔϜࠪ ࠓɺෳͷݯ͕ܗ͢Δి࣓քʹରͯ͠ɺͦͷݯΛ ͱͯ͠ଊ͑ํੑͷ์ࣹύλʔϯΛԾఆ͢Δɻͦͯ͠ɺ ֤ݯʢΞϯςφʣͦͷҐஔͰڅిͷҐ૬ಉ͡Ͱ͋ Δͱͯ͠ɺԕํͰͷి࣓քΛ֤Ξϯςφͷ࠲ඪʹΑΔҐ ૬ࠩҟΛߟྀͨ͠ಈͷ୯७ͳॏͶ߹ͤͰදݱ͢Δɻ ݯྻ࠲ඪ͕ฏ໘ͷ߹ɺAFFourierڃͱಉ͡ܗͱ ͳΔɻ࣮ࡍͷ֤Ξϯςφࢦੑ͕͋ΔͷͰɺ͜ΕΛAF ʹॏͤ͞ΔͱɺΞϨΠશମͷ߹์ࣹύλʔϯ͕ܭࢉ Ͱ͖ΔɻͨͩɺΞϯςφؒͷۭؒ૬ޓ݁߹Λແࢹ͍ͯ͠ ΔͷͰɺ݅ʹΑ࣮ͬͯࡍͱ߹Θͳ͍߹ൃੜ͢Δɻ ্ͯ͞ड़ͷΑ͏ʹɺۭؒͷҙ࠲ඪʹݯ͕ݽཱ ͯ͠ྻ͞Ε͍ͯΔͱ͖ͷAFɺݯͷҐ૬ͦͷҐஔ ࠲ඪʹґଘ͍ͯ͠ΔͷͰɺٿ࠲ඪͷ֯มΛ(θ, ϕ)ͱ ͯ͠ɺ୯७ʹ f (θ, ϕ) =∑anexp{jk(xnu + ynv + zncos θ)} (1) Ͱ༩͑Δ͜ͱ͕Ͱ͖Δɻ͜͜Ͱɺ(xn, yn, zn)n൪ૉ
ࢠͷ3࣍ݩۭؒ࠲ඪ(u = sin θ cos ϕ, v = sin θ sin ϕ)Ͱ͋
Γɺk = 2π/λΛࢦ͢ɻ·ͨɺan֤ૉࢠͷෳૉৼ ෯Ͱ͋Δɻ͜ͷ؆ܿͳجຊࣜঢ়ͷ์ࣹݯͷू߹͕ԕ ํͰͭ͘Δ์ࣹքΛද͍ͯ͠Δ͕ɺ࣮ࡍଘࡏ͍ͯ͠Δͱ ࢥΘΕΔ֤Ξϯςφૉࢠؒͷి࣓քతͳ૬ޓ݁߹ແࢹ ͍ͯ͠Δɻਤ11࣍ݩͷִؒϦχΞΞϨΠʹฏ໘ ͕ೖࣹͨ͠ͱ͖ɺ֤ૉࢠʹྭى͞ΕΔҐ૬ࠩΛࣔͨ͠ ਤ-1 ฏ໘রࣹ࣌ͷִؒΞϨΠૉࢠʹ༠ى͞ ΕΔҐ૬ࠩ
Fig.1 Phase differences induced in equi-pitched array elements as plane wave incident.
ͷͰ͋Γɺ͜ΕΒͷड৴ʑ߸ͷΛͱͬͯΞϨΠΞϯςφ ͷड৴ʑ߸ग़ྗͱ͢Δɻҩྍը૾Ͱɺ͜ͷߟ͑Λ ʮԆͨ͠ෳ৴߸ͷҐ૬ʯͱ͍͏ҙຯͰɺDelay and Sum Beamforming(DAS)ͱݺΜͰ͍Δ[5]ɻͳ͓ɺ্ड़ ์ࣹքͱ͍͏ૹ৴ܥͰఆࣜԽ͍ͯ͠Δ͕ɺฏ໘͕Ξ ϨΠ໘ʹࣼΊʹೖࣹ͢Δͱͯ͠ٻΊͯಉ݁͡ՌͱͳΔɻ ୈ(1) ࣜͷෳૉৼ෯ an ʹ͢Δͱɺ͜ΕΛॏΈ ؔͱ֤ͯ͠ૉࢠͷड৴ʑ߸ʹಠཱͯ͠ࢪ͢͜ͱʹΑ Γɺ֤छͷదԠܕΞϨΠॲཧ͕ՄೳͱͳΔɻͦͷॲཧΞ ϧΰϦζϜͷද͕֨MUSIC(MUltiple SIgnal
Clas-sification) ๏Ͱ͋Γɺి౸དྷํͷධՁ͋Δ͍
ׯ ব ํ ͷ ψ ϧ ܗ ͳ Ͳ ͕ ظ Ͱ ͖ Δ ख ๏ Ͱ ͋ Δɻ͜ͷΞμϓςΟϒΞϯςφॲཧͱަपଟॏ ׂ:OFDM(Orthogonal Frequency Division Multiplex-ing)ͳͲͷมௐٕज़ΛΈ߹ͤͯɺۙMIMOγεςϜ ͕Μʹݚڀ͞Ε͍ͯΔͷपͷ௨ΓͰ͋Δɻ͜Ε ૹड৴ͰΞϨΠΞϯςφΛߏ͠ɺ௨৴࣭Λ্ͤ͞ Δ͜ͱΛతͱ͍ͯ͠ΔεϚʔτΞϯςφٕज़ͷҰͭͱ ݴΘΕ͍ͯΔ[6,7] ɻૹ৴ిྗ͓ΑͼଳҬ෯͚ͩʹґଘ ͠ͳ͍Ͱɺෳͷൖ࿏ΛؚΊͯใྔ͋Δ͍௨৴ڑ Λվળ͢ΔํࣜͰ͋ΓɺݪཧతʹϨʔμγεςϜʹ Ԡ༻͕ظͰ͖Δɻ·ͨୈ(1)ࣜͷҐ૬߲ʹ͢Δͱɺ ݶఆ͞ΕۭͨؒͰϏʔϜͷࢦํΛҙʹมԽͤ͞ Δ͜ͱ͕Ͱ͖ΔɻϚΠΫϩଳ(RF)Ͱ͜ΕΛߦ͏ʹɺ ઢ࿏ΛΓସ͑ΔҠ૬σόΠε͕ඞཁͱͳΔɻલड़ͷ ΞμϓςΟϒॲཧͰɺϕʔεόϯυۙลͰσδλϧత ʹॏΈͷෳૉॲཧՄೳͰ͋Δɻ ͞Βʹจݙ[2] Ͱใࠂ͞Ε͍ͯΔΑ͏ʹɺAFͷ ݯΛۙքͰͷి࣓քσʔλͱ͢Δͱɺ͜Ε͕ͦͷ·· ԕํքʹม͞ΕΔɻલड़ͨ͠AFΛٻΊΔߟ͑ํ͔Β͠ ͯવͷؼ݁Ͱ͋Δɻۙి࣓քΛԕํʹม͢Δʹɺ ਤ-2 ࡾ֯ྻͷฏ໘ΞϨΠ
Fig.2 Planar array in triangular placed elements.
ฏ໘εϖΫτϥϜల։๏ͱ͍͏ݫີͳཧʹج͖ͮม ࣜΛఆࣜԽ͍ͯͨ͠ɻಛʹฏ໘ঢ়ʹऔಘͨۙ͠ք ݁ՌతʹFourierมͷܗͰԕํք͕ٻΊΒΕΔͷͰɺ औಘͨۙ͠σʔλΛ୯ʹFFT͢Εԕํք͕ಘΒΕΔ ͜ͱྑ͘ΒΕ͍ͯΔɻҰํɺԁࠪ͋Δ͍ٿ໘ ࠪͰBesselؔͳͲͷಛघ͕ؔඞཁͰ͋Γɺԕํ քʹม͢Δʹॏ͍࡞ۀͱͳ͍ͬͯͨɻ͔͠͠ɺࣜ(1) ͚ͩʹجͮ͘AFͷํ๏ͰɺΞϯςφͷԕํք͋Δ͍ ͖݅ͰϨʔμஅ໘ੵͷԕํք͕༰қʹٻΊΒΕΔɻ Ҏ্ͷΑ͏ʹΞϯςφܥΛࢄԽͯ͠औΓѻ͏ͱɺ্ ه(1)ࣜͷ֤ύϥϝʔλΛॴͷྔʹಠཱͯ͠ૢ࡞Ͱ͖ ΔͷͰɺతʹԠ༷ͯ͡ʑͳԠ༻͕ߟ͑ΒΕΔɻຊͰ ɺ͜ͷɺAFʹΑΔฏқͳը૾ॲཧʹ͍ͭͯɺλʔήο τϞσϧͷۙքΛجʹجຊతͳݕ౼Λߦ͏ɻ͜ͷը૾ ॲཧɺԻྖҬͰͷΞμϓςΟϒͳॲཧΛΘͤͨ ҩྍؔ࿈Ͱͷ[8]ɺ͋Δ͍ϚΠΫϩྖҬͰͷ දۙลͷۚଐମͷϨʔμը૾ʹΑΔࣝผ[9] ͳͲʹ ΄΅ಉ͡ߟ͑ํͰԠ༻͞Ε͍ͯΔɻ ͳ͓MUSIC๏ͳͲͰɺݻ༗ΛѻͬͨΓαϒΞϨΠ Խͯͦ͠ͷͱ͖ͷ౷ܭΛ༻͍ͨΓ͢ΔͷͰɺߦྻʹΑ ΔϕΫτϧද͕ࣔศརͰ͋ΓɺࢀߟॻΛؚΉଟ͘ͷจݙ Ͱߦྻදࣔͱͳ͍ͬͯΔɻ͔͠͠ຊͰͦ͜·Ͱཱ ͪೖΒͳ͍ͷͰɺ͔Γқ͍εΧϥʔදࣔͷ··ٞ͢ Δ͜ͱʹ͢Δɻ ্ͯ͞هAFΛཧղ͢ΔͨΊʹɺϑΣʔζυΞϨΠΞϯ ςφ(Ґ૬ܕిࢠࠪΞϯςφ)Λ೦಄ʹAFͷ۩ମతͳ දࣔʹ͍͓ͭͯٞͯ͘͠ɻલड़ͷϦχΞΞϨΠΛ2࣍
ݩʹ֦ுͨ͠ϓϥφΞϨΠΛਤ2ʹࣔ͢ɻૉࢠྻҰ ൠੑΛ࣋ͨͨ͢Ίɺx࣠ํʹִஈ͕δx͚ͩͣΕͨࡾ֯ ྻͱ͢Δɻ͜ͷૉࢠ࠲ඪΛͦͷ··ୈ(1)ࣜʹೖ͢ ΕɺΞϨΠͷ์ࣹಛੑ(AF)͕ٻΊΒΕΔɻిࢠతͳ ϏʔϜࠪΛҙࣝ͢Δͱɺ֤ૉࢠʹڅి͢ΔྭৼҐ૬ ಠ੍ཱͯ͠ޚͰ͖ΔΑ͏ʹ͓ͯ͘͠ඞཁ͕͋Δɻ͜ͷΑ ͏ͳిࢠϏʔϜࠪํࣜͷΞϯςφΛϑΣʔζυΞϨΠ ͱݺΜͰ͓ΓɺຆͲͷγεςϜҐ૬ΛՄมͤ͞Δσό ΠεͰ͋ΔҠ૬ثΛ࠾༻͍ͯ͠Δɻ֤ૉࢠͷ͜ͷҐ૬Λ Ͳ͏ͷΑ͏ʹઃఆ͢ΕΑ͍͔ɺ͜ΕHuygensͷݪཧ ΑΓͪʹ༠ಋͰ͖ΔɻϏʔϜΛ͚͍ͨํʹ֤ૉࢠ ͔Βͷ์ࣹքͷҐ૬ΛͣΒͤΑ͍ɻ͜ͷج४ΞϨΠ ์ࣹքͷҐ૬໘͕ϏʔϜํͱਨʹͳΔΑ͏ʹҠ૬ ثΛۦಈ͢Δ͜ͱͰ͋Δ[1]ɻࠓɺΞϨΠ։ޱ͕(x, y) ໘ʹଘࡏ͠ɺzํΛϏʔϜࢦํͱ͢Δɻ֤ૉࢠɺ ਤ2ʹࣔ͢Α͏ʹm, n = 1, 2,· · · ͱͯ͠ɺنଇతʹࡾ֯ ྻ͞Ε͍ͯΔɻ͜ͷͱ͖ɺૉࢠͷ࠲ඪ xm= dx{m−1}+δx· mod(n, 2), yn={n − 1} dy (2) Ͱද͞ΕΔɻ্ࣜͰmod(a, b)a/b ͷ༨ΓΛද͓ͯ͠ Γɺmod(n, 2)0͔1ʹͳΔɻૉࢠִؒxͱyํ Ͱ֤ʑdx, dyͱ͍ͯ͠Δɻ૬ޓ݁߹Λߟ͑ͳ͍߹ɺ(1) ࣜͷ ∑ ∑m·∑n ͱͰ͖ΔͷͰɺ࣍ࣜͷΑ͏ʹ มܗͰ͖Δɻ f (θ, ϕ) = M ∑ m=1 N ∑ n=1 amnexp(jψmn), ψmn= k{dx(m−1)+δx·mod(n, 2)} u+kdy(n−1)v. (3)
͜͜Ͱɺ(u, v) = (sin θ cos ϕ, sin θ sin ϕ)ٿ࠲ඪͱ֯ ࠲ඪͷมҼࢠͰ͋ΓɺM, N ֤ʑm, nͷ࠷େͰ ͋ΔɻϏʔϜΛ(u0, v0)ʹ͚͍ͨ߹ɺͭ·ΓϑΣʔ ζυΞϨΠγεςϜͰͷϏʔϜࠪͰɺ(u, v) Λ (u− u0, v− v0) Ͱஔ͖͑ΕΑ͍ɻ͜ΕAF͕։ޱ ͷFourierมͱͳ͍ͬͯΔ͜ͱʹؾ͚ɺ༰қ ʹཧղͰ͖Δઢܗܥͷجຊੑ࣭Ͱ͋Δɻ૬ޓ݁߹ͷӨڹ Λແࢹ͍ͯ͠ΔͷͰҐ૬Ͱ͖ɺamnamn= aman ͱͰ͖Δɻैͬͯɺ(3)ࣜ f (u, v) = M ∑ m=1 amexp{j(αm+βm)}· N ∑ n=1 anexp{(jαn+βn)} , αm= k{dx(m− 1) + δx· mod(n, 2)} u, αn= kdy(n− 1)v, βm=−k {dx(m− 1) + δx· mod(n, 2)} u0, βn=−kdy(n− 1)v0 (4) ͱཧ͞ΕΔɻ͜Ε͕ϏʔϜࠪ(u0, v0)ΛؚΊ֤ͨૉ ࢠͷྭৼ͖͢Ґ૬Ͱ͋Γɺݱଘ͢Δେܕ͔Βখܕ ʹࢸΔଟ͘ͷϑΣʔζυΞϨΠγεςϜɺ͜ͷ୯७ͳ ͔ࣜΒۦಈ͖͢Ґ૬ྔΛܭࢉ͍ͯ͠Δɻ ֤ૉࢠ͔Βͷ໘ͷแབྷઢʹ૬͢ΔҐ૬໘ʹର͠ ͯɺϏʔϜਨʹࢦ͢Δɻ͜ΕHuygensͷݪཧ͔ Βࣔࠦ͞ΕΔɻ֤ૉࢠͷҐ૬ΛԿΒ͔ͷΞϧΰϦζϜͰ ੍ޚ͢Δͱɺ์ࣹύλʔϯʹψϧੜͰ͖ɺϏʔϜͱψ ϧΛಠཱͯࠪ͢͠Δ͜ͱߟ͑ΒΕΔɻ·ͨɺϏʔϜ ͷిྗ෯͋Δ͍αΠυϩʔϒঢ়گʹԠͯ͡ม͑ Δ͜ͱ͕Ͱ͖Δɻ͜ͷΑ͏ͳ์ࣹύλʔϯ੍ޚΛҰׅ͠ ͯߦͳ͏ٕज़ΛϏʔϜϑΥʔϛϯάͱ͍͏͕ɺRF৴߸Λ ϕʔεόϯυ৴߸ʹมͯ͠σδλϧσʔλͱͯ͠ѻ͏ ͜ͱͰɺ৴߸ॲཧͱͷ߹ੑ͕࣮ݱͰ͖Δɻ͜ΕΛσδ λϧϏʔϜϑΥʔϛϯά(DBF)ͱݺΜͰ͍ΔɻDBFʹड ৴ʑ߸ͷS/NൺͷใΛՃ͑ΔͱɺΞϯςφ͕ࣗతʹ ׯবΛආ͚ΔΑ͏ͳΞϧΰϦζϜ͕ߟ͑ΒΕΔɻ͜Ε ͕લड़ͷΞμϓςΟϒΞϯςφͰ͋ΓɺۙɺA/Dมث (Analogue-digital converter)ͱίϯϐϡʔλͷߴ ԽΛഎܠʹ࣮༻Խ͞Εͭͭ͋Δॲཧٕज़Ͱ͋Δɻ ԁܗ(Ϧϯά)ΞϨΠɺ͋Δ͍ͦΕΛଟஈʹॏͶͨԁ ΞϨΠʹରͯ͠ɺ(1)ࣜͷجຊ͔ࣜΒAFͷผͷදࣔ ͕ࣜ༠ಋͰ͖ΔɻಛʹۙքͷԕํมͰɺଌఆਫ਼ ΛߴΊΔͨΊฏ໘ࠪΑΓดۭͨؒ͡Λͭ͘Δԁ ࠪͷํ͕·͍͜͠ͱ͕ଟ͍ɻ͜ͷͱ͖ͷมΞϧΰϦ ζϜʹAFΛ༻͍ɺϓϩʔϏϯά༻ͷΞϯςφࢦੑΛߟ ྀͨ͠ܭࢉޮͷྑ͍ද͕ࣔࣜٻΊΒΕΔ[2]ɻҩྍ ͚ͷը૾ॲཧͰɺԻଳͰͷϦϯάΞϨΠํࣜ ଟ͘࠾༻͞Ε͍ͯΔΑ͏Ͱ͋Δɻ ۙɺϨʔμը૾ͷੳʹภใΛԠ༻ͨ͠ཧ͕Ϧ ϞʔτηϯγϯάͰਫ਼ྗతʹݚڀ͞Ε͍ͯΔ[10]ɻ ͜ΕϨʔμʹΑͬͯੜ͞Εͨը૾ͷதʹࢄཚମʹԠ ͍ͯ͡Ζ͍Ζͷภؚ͕·Ε͓ͯΓɺඪࣝผΛ తͱͯ͠ɺಘΒΕͨϨʔμը૾͔ΒภใʹԠͯ͡࠶ ղ͢Δٕज़Ͱ͋Δɻྫ͑ɺւ໘͋Δ͍໘ͳͲฏ ໘ঢ়ͷλʔήοτ͔Β1ճͷද໘ࣹɺϏϧσΟϯά ͳͲͷίʔφʔঢ়ͷମ͔Β2ճͷμϒϧࣹɺྛ ͳͲԞߦ͖·Ͱߟྀͨ͠ମੵࢄཚ͕ओମͱͳΔ͜ͱ͕ ͔͍ͬͯΔɻैͬͯɺͦΕʹԠͯ͡ಘΒΕͨը૾ͷࢄ ཚߦྻΛ࠶ղ͢Δ͜ͱͰɺྨࣝผ͕ՄೳͱͳΔɻຊ ॻͷΑ͏ͳܭࢉཧͰλʔήοτͱภํΛҙʹ ઃఆͰ͖ΔͷͰɺશภใΛؚΜͩը૾ͷγϛϡϨʔ γϣϯՄೳͰ͋Δɻ
ݩʹ֦ுͨ͠ϓϥφΞϨΠΛਤ2ʹࣔ͢ɻૉࢠྻҰ ൠੑΛ࣋ͨͨ͢Ίɺx࣠ํʹִஈ͕δx͚ͩͣΕͨࡾ֯ ྻͱ͢Δɻ͜ͷૉࢠ࠲ඪΛͦͷ··ୈ(1)ࣜʹೖ͢ ΕɺΞϨΠͷ์ࣹಛੑ(AF)͕ٻΊΒΕΔɻిࢠతͳ ϏʔϜࠪΛҙࣝ͢Δͱɺ֤ૉࢠʹڅి͢ΔྭৼҐ૬ ಠ੍ཱͯ͠ޚͰ͖ΔΑ͏ʹ͓ͯ͘͠ඞཁ͕͋Δɻ͜ͷΑ ͏ͳిࢠϏʔϜࠪํࣜͷΞϯςφΛϑΣʔζυΞϨΠ ͱݺΜͰ͓ΓɺຆͲͷγεςϜҐ૬ΛՄมͤ͞Δσό ΠεͰ͋ΔҠ૬ثΛ࠾༻͍ͯ͠Δɻ֤ૉࢠͷ͜ͷҐ૬Λ Ͳ͏ͷΑ͏ʹઃఆ͢ΕΑ͍͔ɺ͜ΕHuygensͷݪཧ ΑΓͪʹ༠ಋͰ͖ΔɻϏʔϜΛ͚͍ͨํʹ֤ૉࢠ ͔Βͷ์ࣹքͷҐ૬ΛͣΒͤΑ͍ɻ͜ͷج४ΞϨΠ ์ࣹքͷҐ૬໘͕ϏʔϜํͱਨʹͳΔΑ͏ʹҠ૬ ثΛۦಈ͢Δ͜ͱͰ͋Δ[1]ɻࠓɺΞϨΠ։ޱ͕(x, y) ໘ʹଘࡏ͠ɺzํΛϏʔϜࢦํͱ͢Δɻ֤ૉࢠɺ ਤ2ʹࣔ͢Α͏ʹm, n = 1, 2,· · · ͱͯ͠ɺنଇతʹࡾ֯ ྻ͞Ε͍ͯΔɻ͜ͷͱ͖ɺૉࢠͷ࠲ඪ xm= dx{m−1}+δx· mod(n, 2), yn={n − 1} dy (2) Ͱද͞ΕΔɻ্ࣜͰmod(a, b)a/b ͷ༨ΓΛද͓ͯ͠ Γɺmod(n, 2)0͔1ʹͳΔɻૉࢠִؒxͱyํ Ͱ֤ʑdx, dyͱ͍ͯ͠Δɻ૬ޓ݁߹Λߟ͑ͳ͍߹ɺ(1) ࣜͷ ∑ ∑m·∑n ͱͰ͖ΔͷͰɺ࣍ࣜͷΑ͏ʹ มܗͰ͖Δɻ f (θ, ϕ) = M ∑ m=1 N ∑ n=1 amnexp(jψmn), ψmn= k{dx(m−1)+δx·mod(n, 2)} u+kdy(n−1)v. (3)
͜͜Ͱɺ(u, v) = (sin θ cos ϕ, sin θ sin ϕ)ٿ࠲ඪͱ֯ ࠲ඪͷมҼࢠͰ͋ΓɺM, N ֤ʑm, nͷ࠷େͰ ͋ΔɻϏʔϜΛ(u0, v0)ʹ͚͍ͨ߹ɺͭ·ΓϑΣʔ ζυΞϨΠγεςϜͰͷϏʔϜࠪͰɺ(u, v) Λ (u− u0, v− v0) Ͱஔ͖͑ΕΑ͍ɻ͜ΕAF͕։ޱ ͷFourierมͱͳ͍ͬͯΔ͜ͱʹؾ͚ɺ༰қ ʹཧղͰ͖Δઢܗܥͷجຊੑ࣭Ͱ͋Δɻ૬ޓ݁߹ͷӨڹ Λແࢹ͍ͯ͠ΔͷͰҐ૬Ͱ͖ɺamnamn= aman ͱͰ͖Δɻैͬͯɺ(3)ࣜ f (u, v) = M ∑ m=1 amexp{j(αm+βm)}· N ∑ n=1 anexp{(jαn+βn)} , αm= k{dx(m− 1) + δx· mod(n, 2)} u, αn= kdy(n− 1)v, βm=−k {dx(m− 1) + δx· mod(n, 2)} u0, βn=−kdy(n− 1)v0 (4) ͱཧ͞ΕΔɻ͜Ε͕ϏʔϜࠪ(u0, v0)ΛؚΊ֤ͨૉ ࢠͷྭৼ͖͢Ґ૬Ͱ͋Γɺݱଘ͢Δେܕ͔Βখܕ ʹࢸΔଟ͘ͷϑΣʔζυΞϨΠγεςϜɺ͜ͷ୯७ͳ ͔ࣜΒۦಈ͖͢Ґ૬ྔΛܭࢉ͍ͯ͠Δɻ ֤ૉࢠ͔Βͷ໘ͷแབྷઢʹ૬͢ΔҐ૬໘ʹର͠ ͯɺϏʔϜਨʹࢦ͢Δɻ͜ΕHuygensͷݪཧ͔ Βࣔࠦ͞ΕΔɻ֤ૉࢠͷҐ૬ΛԿΒ͔ͷΞϧΰϦζϜͰ ੍ޚ͢Δͱɺ์ࣹύλʔϯʹψϧੜͰ͖ɺϏʔϜͱψ ϧΛಠཱͯࠪ͢͠Δ͜ͱߟ͑ΒΕΔɻ·ͨɺϏʔϜ ͷిྗ෯͋Δ͍αΠυϩʔϒঢ়گʹԠͯ͡ม͑ Δ͜ͱ͕Ͱ͖Δɻ͜ͷΑ͏ͳ์ࣹύλʔϯ੍ޚΛҰׅ͠ ͯߦͳ͏ٕज़ΛϏʔϜϑΥʔϛϯάͱ͍͏͕ɺRF৴߸Λ ϕʔεόϯυ৴߸ʹมͯ͠σδλϧσʔλͱͯ͠ѻ͏ ͜ͱͰɺ৴߸ॲཧͱͷ߹ੑ͕࣮ݱͰ͖Δɻ͜ΕΛσδ λϧϏʔϜϑΥʔϛϯά(DBF)ͱݺΜͰ͍ΔɻDBFʹड ৴ʑ߸ͷS/NൺͷใΛՃ͑ΔͱɺΞϯςφ͕ࣗతʹ ׯবΛආ͚ΔΑ͏ͳΞϧΰϦζϜ͕ߟ͑ΒΕΔɻ͜Ε ͕લड़ͷΞμϓςΟϒΞϯςφͰ͋ΓɺۙɺA/Dมث (Analogue-digital converter)ͱίϯϐϡʔλͷߴ ԽΛഎܠʹ࣮༻Խ͞Εͭͭ͋Δॲཧٕज़Ͱ͋Δɻ ԁܗ(Ϧϯά)ΞϨΠɺ͋Δ͍ͦΕΛଟஈʹॏͶͨԁ ΞϨΠʹରͯ͠ɺ(1)ࣜͷجຊ͔ࣜΒAFͷผͷදࣔ ͕ࣜ༠ಋͰ͖ΔɻಛʹۙքͷԕํมͰɺଌఆਫ਼ ΛߴΊΔͨΊฏ໘ࠪΑΓดۭͨؒ͡Λͭ͘Δԁ ࠪͷํ͕·͍͜͠ͱ͕ଟ͍ɻ͜ͷͱ͖ͷมΞϧΰϦ ζϜʹAFΛ༻͍ɺϓϩʔϏϯά༻ͷΞϯςφࢦੑΛߟ ྀͨ͠ܭࢉޮͷྑ͍ද͕ࣔࣜٻΊΒΕΔ[2]ɻҩྍ ͚ͷը૾ॲཧͰɺԻଳͰͷϦϯάΞϨΠํࣜ ଟ͘࠾༻͞Ε͍ͯΔΑ͏Ͱ͋Δɻ ۙɺϨʔμը૾ͷੳʹภใΛԠ༻ͨ͠ཧ͕Ϧ ϞʔτηϯγϯάͰਫ਼ྗతʹݚڀ͞Ε͍ͯΔ[10]ɻ ͜ΕϨʔμʹΑͬͯੜ͞Εͨը૾ͷதʹࢄཚମʹԠ ͍ͯ͡Ζ͍Ζͷภؚ͕·Ε͓ͯΓɺඪࣝผΛ తͱͯ͠ɺಘΒΕͨϨʔμը૾͔ΒภใʹԠͯ͡࠶ ղ͢Δٕज़Ͱ͋Δɻྫ͑ɺւ໘͋Δ͍໘ͳͲฏ ໘ঢ়ͷλʔήοτ͔Β1ճͷද໘ࣹɺϏϧσΟϯά ͳͲͷίʔφʔঢ়ͷମ͔Β2ճͷμϒϧࣹɺྛ ͳͲԞߦ͖·Ͱߟྀͨ͠ମੵࢄཚ͕ओମͱͳΔ͜ͱ͕ ͔͍ͬͯΔɻैͬͯɺͦΕʹԠͯ͡ಘΒΕͨը૾ͷࢄ ཚߦྻΛ࠶ղ͢Δ͜ͱͰɺྨࣝผ͕ՄೳͱͳΔɻຊ ॻͷΑ͏ͳܭࢉཧͰλʔήοτͱภํΛҙʹ ઃఆͰ͖ΔͷͰɺશภใΛؚΜͩը૾ͷγϛϡϨʔ γϣϯՄೳͰ͋Δɻ 3.ΞϨΠͷযԽʹΑΔϨʔμը૾ ਫಓɺཕͳͲͷதຒઃͷ୳ࠪʹɺλʔήο τͷը૾σʔλ͕ਖ਼֬Ͱ͋Εࣝผఆͷ֬େ͖͘ ্͢ΔɻಈʹΑΔը૾ԽॲཧͷͰɺখதن ͷݻఆΞϯςφղೳ͕͍͜ͱ͋ΓɺۭؒతʹҠ ಈͤ͞Ձతʹେ͖ͳ։ޱΛಘͯղೳΛ͋͛Δ߹։ ޱॲཧ(SAR)Λجʹͨ͠ํ๏͕͘ීٴ͍ͯ͠Δɻ͜͜ Ͱɺຊ֨తͳSARͰߦ͏ΞδϚεѹॖ͓ΑͼϨϯδѹ ॖ(ύϧεѹॖ) ͷΑ͏ͳϋʔυͱιϑτΣΞʹؔΘ ΔॲཧͰͳ͘ɺ؆қͳϋʔυͱલड़ͷAFཧʹΑΔॲ ཧ๏ʹ͍ͭͯٞ͢Δɻಈͷը૾ॲཧʹຊ֨తͳSAR ॲཧΛ࠾༻͢ΔͱɺϨʔμͷϋʔυΣΞͦͷॲཧʹ ߹Θͤͯઃܭ͠ͳ͚ΕͳΒͳ͍ɻҰํɺAFΛૹड৴Խ ͠ɺఆͨ͠λʔήοτͷ࠲ඪΛݩʹλʔήοτΤίʔ ͷҐ૬ͱൺֱ͢Δ͜ͱͰɺλʔήοτ࠲ඪͷۙลͰͷ ૬ؔੑ͕ධՁͰ͖Δɻ͜ͷ୯७ͳ֓೦ʹΑΔͱɺϨʔμ ͷϋʔυ͓ΑͼιϑτΣΞඇৗʹγϯϓϧͳߏͱ ͳΔɻͨͩ͠রࣹྖҬશൠΛը૾ॲཧ͢Δ߹ɺԾఆ͠ ͨඪͷ࠲ඪશҬͰܭࢉ͢Δඞཁ͕͋ΔͷͰܭࢉ࣌ ؒίετͷ͕͋Δɻ͔͠͠ɺ࠷ۙͷPCͰେ͖ͳ ͱͳΒͳ͍ͱ༧͍ͯ͠Δɻͨͩ͜ͷཧ༝ͷͨΊɺ
AFʹΑΔযԽը૾(Array-Factor Focusing: AFF)
ͷԠ༻ൣғɺൺֱతۙڑͷখྖҬͷը૾ॲཧʹ࠷ద Ͱ͋ΔͱࢥΘΕΔɻ લड़ͷ͘ΞϨΠʹΑΔϨʔμը૾ͷߟ͑ํɺ࣮ଌ ৴߸ͷҐ૬ใͱরࣹྖҬͷඪ͔ΒͷཧతͳΤ ίʔ৴߸ͷҐ૬ใͷ૬ؔੑΛΈΔํ๏Ͱ͋Δɻ͜ͷ૬ ؔੑ؆୯ͳҐ૬ͷڃܭࢉͰߦ͏͜ͱ͕Ͱ͖ɺ݁Ռ͕ ղೳͷ্ʹͭͳ͕ΔҰछͷ߹։ޱॲཧͱΈͳ͢͜ ͱ͕Ͱ͖ΔɻిΛૹ৴͠ɺͦͷΤίʔΛड৴͢ΔͨΊ ʹɺΞϨΠͷ֤ૉࢠΛશͯ༻ҙ͢Δඞཁͳ͍ɻλʔ ήοτͱϨʔμͷҐஔ͕ؔ૬ରతʹݻఆ͞Ε͍ͯΔɺ͋ Δ͍ॲཧϨʔτͰ΄΅Ҡಈ͍ͯ͠ͳ͍ɺͳͲ͕Ծఆ Ͱ͖Δͱɺ1ݸͷΞϯςφΛػցతʹࠪͯ͠Α͍ɻ· ͨɺૹड৴Ξϯςφճ࿏ͷෳࡶ͞Λආ͚ΔͨΊɺผʑʹ ༻ҙ͢Δํ͕ଌఆܥ؆୯ʹͳΔɻྫ͑ɺ൚༻ͷωο τϫʔΫΞφϥΠβͳͲΛૹ৴ݯ͓Αͼड৴ܥʹ༻͍Δ ߹ɺૹड৴ͷΞΠιϨʔγϣϯΛऔΔͨΊʹૹ৴ͱड ৴ͷΞϯςφΛۭؒతʹ͢ߏՄೳͰ͋Δɻ·ͨҠ ಈ͢Δૹ৴ͷҐஔ࠲ඪͱड৴ͷͦΕҧ͍ͬͯͯΑ ͘ɺૹ৴ϙΠϯτͷํ͕ड৴ΑΓগͳ͍ߏίετ ޮ͕ߴ͍ͱࢥΘΕΔɻ ͯ͞ɺΞϨΠͷجຊࣜ(1)Λ͏গ͠ৄ͘͠ݟΔͨΊ ʹɺը૾σʔλΛҙࣝͨ͠Ґஔ࠲ඪมͷࢄཚքϞσϧ Λ࣍ࣜͰ༩͑Δɻ es(x, z) = M ∑ m=1 Am· δ(r − rm). (5) ͜͜Ͱɺr, rm֤ʑݯͱ؍ଌͷҐஔϕΫτϧͰ͋ ΓɺDiracͷDeltaؔδ(r− rm)͕͍ΘΏΔը૾ͷϐ Ϋηϧ࠲ඪʹରԠ͍ͯ͠Δͱߟ͑ΒΕΔɻδ(r− rm) FourierมཧΑΓ δ(r−rm) = ∫ ∞ −∞ exp{−j(k·rm}·exp{j(k·r)}dk (6) ͱۙࣅͰ͖Δ[11]ɻͭ·ΓϕΫτϧۭؒkͰͷࢄཚ քΛEs(k)ͱ͢Δͱɺ͜ΕΛٯFourierมͨ͠ͷ͕ ্ࣜʹͳΔɻैͬͯɺ͜ΕΛ͞ΒʹFourierม͢Δͱɺ Es(k) = M ∑ m=1 Amexp{−j(k · rm)} (7) ͕ಘΒΕΔɻ্ࣜͰྫ͑ɺx− z໘Ͱͷը૾(z Ϩ ϯδํ)rm= (xm, zm), r = (x, z), k = (kx, kz)ͱͳ Δɻୈ(7)ࣜϨʔμͰಘΒΕΔड৴σʔλͷܗͱͳͬ ͓ͯΓɺୈ(1)ࣜͷAFͱྨࣅͨ͠දࣔࣜͱͳ͍ͬͯΔɻ ͭ·Γɺୈ(1)ࣜ͋Δ͍(7)ࣜΛجʹۙλʔήοτ ͷযԽͱૹड৴Խૢ࡞Λߦ͑ɺλʔήοτ࠲ඪͷը ૾σʔλ͕ಘΒΕΔ͜ͱʹͳΔɻ্ड़ͷࢄཚମΛෳͷ ঢ়ମͱͯ͠ѻ͏ํ๏ɺؔ(point spread function)ͱͯ͘͠༻͍ΒΕ͍ͯΔۙࣅղ๏Ͱ͋Δɻ ঢ়ମʹΑΔࢄཚಈ؆୯ʹදݱͰ͖ΔͷͰɺߟ͑ ͍ͯΔରମͷද໘࠲ඪΛෳͷͰͳͧΒ͑ɺ͜Ε Βͷ͔ΒͷҐ૬ࠩΛߟྀ͢Δ͚ͩͰ߹ࢄཚΛ༰қ ʹධՁͰ͖Δ͜ͱʹͳΔɻ ΞϨΠ֤ૉࢠͰͷԆҐ૬Λߟ͢ΔͨΊʹɺਫฏ ໘ͷ֯ํɺํҐͱڑ͓Αͼߴ͞ํͷ࠲ඪΛ ֯࠲ඪܥ(x, y, z)Ͱද͢͜ͱΛߟ͑Δɻਤ3ʹࣔ͢ Α͏ʹɺm ൪ʹ͓͚Δૹ৴Ξϯςφͷ࠲ඪΛrt m= (xt m, ymt , zmt) ͱ͠ɺn൪ʹ͓͚Δड৴Ξϯςφͷ ࠲ඪΛrr n= (xrn, ynr, znr) ͱ͢ΔɻҰํɺը૾σʔλ ͷมͱͳΔඪࢄཚͷ࠲ඪΛrp= (xp, yp, zp) ͱ ද͢ɻ͜͜ͰrҐஔϕΫτϧΛද͍ͯ͠Δɻm൪ ͷૹ৴Ξϯςφ͔Βͷ৴߸ɺযͱԾఆ͢Δඪ ͷ࠲ඪ(xp, yp, zp)Ͱࣹࢄཚͨ͠ޙɺn൪ͷड৴Ξ ϯςφʹΔɻ͜ͷͱ͖ͷޫֶతͳܦ࿏ɺ͜ΕΛ rmn(xp, yp, zp)ͱ͢Δͱɺ rmn(xp, yp, zp)=|rp− rtm| + |rrn− rp|
ਤ-3 AFযԽʹΑΔϨʔμߏ(ҙ: ਤ2
ͷ൪߸m, nͱऔΓํ͕ҟͳΔ)
Fig.3 Radar configuration in AF focusing. Note the different m, n from Fig.2.
={(xtm− xp)2+ (ymt − yp)2+ (ztm− zp)2} 1 2 +{(xrn− xp)2+ (ynr− yp)2+ (znr− zp)2} 1 2 (8) ͱܭࢉ͞ΕΔɻkΛߟྀ͢ΔͱɺҐ૬ܦ࿏krmn ʹࢉ͞ΕΔɻฏ໘Λ݅ͱͯ͠ఆࣜԽ͞ΕͨAFୈ (1)ࣜʹର͠ɺ(8)ࣜۙྖҬΛҙࣝͨ͠যԽૢ࡞ (focusing)ʹ૬͢Δɻ 4.AFFʹΑΔը૾Խͷఆࣜ લ߲ͰΞϨΠͷযԽʹର͢Δߟ͑ํ(AF Focus-ing:AFF)ʹ͍ͭͯٞͨ͠ɻ͜͜ͰɺϨʔμͷप ಛੑΛߟྀͯ͠ը૾ΛಘΔͨΊͷ۩ମతͳॲཧ๏ʹ͍ͭ ͯɺਤ3Λࢀর͠ͳ͕Βٞ͢Δɻ Ϩʔμͷૹ৴पʹ࿈ଓܗ(CW)Λఆ͠ɺप Λεςοϓঢ়ʹҾͤ͞Δɻεςοϓঢ়ʹҾ͢Δͷ ɺଌఆثͷಛੑΛߟྀͯ͠ͷ͜ͱͰ͋Γɺͦͷεςο ϓ෯ɺपͷύϥϝʔλʹΑΓ୯ௐ૿Ճؔʹ͍ۙ ܗͰҾͯ͠ྑ͍ɻΞϨΠͷm൪ͷૹ৴Ξϯςφ ͔Βૹ৴ͯ͠n൪ͷड৴ΞϯςφͰܭଌ͞Εͨℓ൪ ͷεςοϓप fℓ Ͱͷड৴ڧΛPℓmn(fℓ, rmn)ͱ ͢Δɻ͜ͷͱ͖ɺλʔήοτ࠲ඪrpΛը૾ྖҬͰͷม r(x, y, z)ʹஔ͖͑Δͱɺલ߲(7)ࣜͰݟͨΑ͏ʹɺ Ϩʔμલํͷి࣓քڧɺ͢ͳΘͪϨʔμը૾ Q0(r)= 1 LM N L ∑ ℓ=1 M ∑ m=1 N ∑ n=1 Pℓmn(fℓ, rmn) · exp {jkℓrmn(xp, yp, zp)} = 1 LM N L ∑ ℓ=1 M ∑ m=1 N ∑ n=1 Pℓmn(fℓ, rmn) · exp { j2πfℓ c rmn(xp, yp, zp) } · exp(jϕℓ) (9) ͰධՁͰ͖Δͱߟ͑ΒΕΔɻ͜͜ͰɺL, M, N ֤ʑૹ ৴Ξϯςφɺड৴ΞϯςφɺपεςοϓͰ͋ ΓɺkℓޫΛcͱͯ͠ɺkℓ= 2πfℓ/cΛ͍ͬͯ ΔɻϨϯδํͷղೳ͕ଳҬ෯ʹґଘ͢Δ͜ͱɺલ ग़ͷpsfʹΑͬͯ༰қʹ͕ؔࣜ༠ಋͰ͖Δ͕ɺ͜͜Ͱ ࢴ໘ͷ߹ͰׂѪ͢ΔɻPℓmn(fℓ, rmn)ड৴ΞϨΠ Ͱड৴͢ΔిྗͰ͋Γɺ(1)ࣜͷෳૉৼ෯anΞϨΠΞ ϯςφརಘʹ૬͢Δɻ͜ͷड৴ిྗܭଌͷࡍʹඪ४ λʔήοτͷपಛੑσ(fℓ)Ͱߍਖ਼͓ͯ͘͜͠ͱ͕ ·͍͠ɻ·ͨɺҐ૬ϕℓ ଌఆγεςϜ͋Δ͍Ϩʔμ ܥͷ෦ԆྔͰ͋ΓɺϨʔμͷηοςΟϯά࣌ʹಋମ ٿͳͲͷඪ४ߍਖ਼λʔήοτͰ͜ͷྔΛิਖ਼͢Εྑ͍ɻ ্ࣜͷ࠲ඪؔΛมr = (x, y, z)ͱͯ͠ඳը͢Ε ɺରྖҬͷը૾σʔλɺ͔͠తʹΑͬͯ3࣍ ݩը૾͕ಘΒΕΔ͜ͱʹͳΔɻ Ҏ্ͷΑ͏ʹAFFը૾ɺड৴ʑ߸ͱରྖҬͷؔ࿈ ੑɺͭ·Γ݁ͼ͖ͭͷ߹͍ΛҐ૬ͷ߹ੑͱͯ͠දݱ ͨ͠ͷͱݟΔ͜ͱ͕Ͱ͖Δɻ͜ΕλʔήοτྖҬΛ ࠪ͢Δr࠲ඪͱλʔήοτ࠲ඪrp ͷࠩr− rp͕ඇৗ ʹখ͍͞ΛͱΔλʔήοτۙͰɺQ(rp)࠷ڧ͘ ͳΓۭؒεϖΫτϥϜͷϐʔΫΛఄ͢ΔɻAFΛͬͨΞ ϯςφϏʔϜࠪͷදࣔࣜ(7)Λݟ͔ͯΔΑ͏ʹɺ ϐʔΫϏʔϜࠪํ(u0, v0)ʹͳ͍ͬͯΔɻ(9) ࣜAFͱશ͘ಉ͡ߟ͑ʹج͍͍ͮͯΔɻҰํɺධՁࣜ Q(rp)ૹड৴ΞϨΠૉࢠͱपͷपظؔ(ࢦ) ͱͳ͍ͬͯΔɻैͬͯύϥϝʔλͷ݅ʹΑͬͯɺ͍ ΘΏΔۭؒతͳᐆດੑ(ambiguity)͕ൃੜ͢Δɻ͜Ε AFཧͰݴ͏άϨʔςΟϯάϩʔϒ(grating-lobe)ɺ FourierཧͰݴ͑ΤΠϦΞε(aliasing)ͷ͜ͱͰ ͋Γɺ࣮ࡍͷΞϨΠϨʔμͷઃܭ࣌ʹ͜ͷᐆດੑΛආ ͚ΔΑ͏ʹҙ͢Δඞཁ͕͋Δɻͳ͓ɺQ0(rp)ʹ࣮ଌ Λ༻͍Δ߹͜ͷ··Ͱྑ͍͕ɺΑΓਖ਼֬ͳܭࢉγ ϛϡϨʔγϣϯʹΞϯςφͷࢦੑʹΑΔڧมԽΛ ߟྀ͠ͳ͚ΕͳΒͳ͍ɻ͜Εޙͷ߲Ͱߟ͢Δ͜ͱ ʹ͠Α͏ɻ ୈ(9)ࣜҰ༷ͳۭؒʹλʔήοτ͕ݽཱͯ͠ஔ͔ Εͨͱ͖ͷදࣔࣜͰ͋ΔɻதͳͲͷຒઃ͋Δ͍น ಁաͳͲΛҙࣝ͢Δͱɺෳͷҟछഔ࣭ͷ༠ిͷҧ͍ ʹґଘ͢Δܦ࿏ࠩΛߟྀ͢Δ͜ͱඞཁͱͳΔɻ͜Εʹ
ਤ-3 AFযԽʹΑΔϨʔμߏ(ҙ: ਤ2
ͷ൪߸m, nͱऔΓํ͕ҟͳΔ)
Fig.3 Radar configuration in AF focusing. Note the different m, n from Fig.2.
={(xtm− xp)2+ (ymt − yp)2+ (ztm− zp)2} 1 2 +{(xrn− xp)2+ (ynr− yp)2+ (znr− zp)2} 1 2 (8) ͱܭࢉ͞ΕΔɻkΛߟྀ͢ΔͱɺҐ૬ܦ࿏krmn ʹࢉ͞ΕΔɻฏ໘Λ݅ͱͯ͠ఆࣜԽ͞ΕͨAFୈ (1)ࣜʹର͠ɺ(8)ࣜۙྖҬΛҙࣝͨ͠যԽૢ࡞ (focusing)ʹ૬͢Δɻ 4.AFFʹΑΔը૾Խͷఆࣜ લ߲ͰΞϨΠͷযԽʹର͢Δߟ͑ํ(AF Focus-ing:AFF)ʹ͍ͭͯٞͨ͠ɻ͜͜ͰɺϨʔμͷप ಛੑΛߟྀͯ͠ը૾ΛಘΔͨΊͷ۩ମతͳॲཧ๏ʹ͍ͭ ͯɺਤ3Λࢀর͠ͳ͕Βٞ͢Δɻ Ϩʔμͷૹ৴पʹ࿈ଓܗ(CW)Λఆ͠ɺप Λεςοϓঢ়ʹҾͤ͞Δɻεςοϓঢ়ʹҾ͢Δͷ ɺଌఆثͷಛੑΛߟྀͯ͠ͷ͜ͱͰ͋Γɺͦͷεςο ϓ෯ɺपͷύϥϝʔλʹΑΓ୯ௐ૿Ճؔʹ͍ۙ ܗͰҾͯ͠ྑ͍ɻΞϨΠͷm൪ͷૹ৴Ξϯςφ ͔Βૹ৴ͯ͠n൪ͷड৴ΞϯςφͰܭଌ͞Εͨℓ൪ ͷεςοϓप fℓ Ͱͷड৴ڧΛPℓmn(fℓ, rmn)ͱ ͢Δɻ͜ͷͱ͖ɺλʔήοτ࠲ඪrpΛը૾ྖҬͰͷม r(x, y, z)ʹஔ͖͑Δͱɺલ߲(7)ࣜͰݟͨΑ͏ʹɺ Ϩʔμલํͷి࣓քڧɺ͢ͳΘͪϨʔμը૾ Q0(r)= 1 LM N L ∑ ℓ=1 M ∑ m=1 N ∑ n=1 Pℓmn(fℓ, rmn) · exp {jkℓrmn(xp, yp, zp)} = 1 LM N L ∑ ℓ=1 M ∑ m=1 N ∑ n=1 Pℓmn(fℓ, rmn) · exp { j2πfℓ c rmn(xp, yp, zp) } · exp(jϕℓ) (9) ͰධՁͰ͖Δͱߟ͑ΒΕΔɻ͜͜ͰɺL, M, N ֤ʑૹ ৴Ξϯςφɺड৴ΞϯςφɺपεςοϓͰ͋ ΓɺkℓޫΛcͱͯ͠ɺkℓ= 2πfℓ/cΛ͍ͬͯ ΔɻϨϯδํͷղೳ͕ଳҬ෯ʹґଘ͢Δ͜ͱɺલ ग़ͷpsfʹΑͬͯ༰қʹ͕ؔࣜ༠ಋͰ͖Δ͕ɺ͜͜Ͱ ࢴ໘ͷ߹ͰׂѪ͢ΔɻPℓmn(fℓ, rmn)ड৴ΞϨΠ Ͱड৴͢ΔిྗͰ͋Γɺ(1)ࣜͷෳૉৼ෯anΞϨΠΞ ϯςφརಘʹ૬͢Δɻ͜ͷड৴ిྗܭଌͷࡍʹඪ४ λʔήοτͷपಛੑσ(fℓ)Ͱߍਖ਼͓ͯ͘͜͠ͱ͕ ·͍͠ɻ·ͨɺҐ૬ϕℓ ଌఆγεςϜ͋Δ͍Ϩʔμ ܥͷ෦ԆྔͰ͋ΓɺϨʔμͷηοςΟϯά࣌ʹಋମ ٿͳͲͷඪ४ߍਖ਼λʔήοτͰ͜ͷྔΛิਖ਼͢Εྑ͍ɻ ্ࣜͷ࠲ඪؔΛมr = (x, y, z)ͱͯ͠ඳը͢Ε ɺରྖҬͷը૾σʔλɺ͔͠తʹΑͬͯ3࣍ ݩը૾͕ಘΒΕΔ͜ͱʹͳΔɻ Ҏ্ͷΑ͏ʹAFFը૾ɺड৴ʑ߸ͱରྖҬͷؔ࿈ ੑɺͭ·Γ݁ͼ͖ͭͷ߹͍ΛҐ૬ͷ߹ੑͱͯ͠දݱ ͨ͠ͷͱݟΔ͜ͱ͕Ͱ͖Δɻ͜ΕλʔήοτྖҬΛ ࠪ͢Δr࠲ඪͱλʔήοτ࠲ඪrpͷࠩr− rp͕ඇৗ ʹখ͍͞ΛͱΔλʔήοτۙͰɺQ(rp)࠷ڧ͘ ͳΓۭؒεϖΫτϥϜͷϐʔΫΛఄ͢ΔɻAFΛͬͨΞ ϯςφϏʔϜࠪͷදࣔࣜ(7)Λݟ͔ͯΔΑ͏ʹɺ ϐʔΫϏʔϜࠪํ(u0, v0)ʹͳ͍ͬͯΔɻ(9) ࣜAFͱશ͘ಉ͡ߟ͑ʹج͍͍ͮͯΔɻҰํɺධՁࣜ Q(rp)ૹड৴ΞϨΠૉࢠͱपͷपظؔ(ࢦ) ͱͳ͍ͬͯΔɻैͬͯύϥϝʔλͷ݅ʹΑͬͯɺ͍ ΘΏΔۭؒతͳᐆດੑ(ambiguity)͕ൃੜ͢Δɻ͜Ε AFཧͰݴ͏άϨʔςΟϯάϩʔϒ(grating-lobe)ɺ FourierཧͰݴ͑ΤΠϦΞε(aliasing)ͷ͜ͱͰ ͋Γɺ࣮ࡍͷΞϨΠϨʔμͷઃܭ࣌ʹ͜ͷᐆດੑΛආ ͚ΔΑ͏ʹҙ͢Δඞཁ͕͋Δɻͳ͓ɺQ0(rp)ʹ࣮ଌ Λ༻͍Δ߹͜ͷ··Ͱྑ͍͕ɺΑΓਖ਼֬ͳܭࢉγ ϛϡϨʔγϣϯʹΞϯςφͷࢦੑʹΑΔڧมԽΛ ߟྀ͠ͳ͚ΕͳΒͳ͍ɻ͜Εޙͷ߲Ͱߟ͢Δ͜ͱ ʹ͠Α͏ɻ ୈ(9)ࣜҰ༷ͳۭؒʹλʔήοτ͕ݽཱͯ͠ஔ͔ Εͨͱ͖ͷදࣔࣜͰ͋ΔɻதͳͲͷຒઃ͋Δ͍น ಁաͳͲΛҙࣝ͢Δͱɺෳͷҟछഔ࣭ͷ༠ిͷҧ͍ ʹґଘ͢Δܦ࿏ࠩΛߟྀ͢Δ͜ͱඞཁͱͳΔɻ͜Εʹ ؔͯ͠ɺ༠ిਪఆ๏ʹབྷΊͯޙड़͍ͯ͠ΔɻL, M, N ͷ࣮ࡍతͳλʔήοτ·ͰͷڑɺΞϯςφִؒ ͱࠪ෯ɺϨϯδํͷղೳʹґଘ͢Δ͕ɺ3-7m Ε ͨরࣹྖҬ্ͷۚଐମݕग़Ϩʔμʹ͓͍ͯɺपൺଳ Ҭ͕20%ɺΞϯςφִؒ10cmɺΞϨΠ։ޱ2m ఔ Ͱͷ࣮ଌྫ͕ใࠂ͞Ε͍ͯΔ[12]ɻ·ͨɺযԽը૾ ͷॲཧաఔ͔ΒਪଌͰ͖ΔΑ͏ʹɺ(9)ࣜฏ໘ΞϨ ΠͷFourierڃͷܗͱͳ͍ͬͯΔͷͰɺΫϩεϨϯδ ը૾ղೳ։ޱʹґଘ͢ΔϏʔϜ෯ͷ΄Ͳͱͳ Δ͜ͱ͕༧͞ΕΔɻ นಁա͋Δ͍ຒઃݕ༻ͷηϯαʔͰɺϨʔμ ͱλʔήοτؒʹෆཁͷো͕ଘࡏ͢Δɻ͜ΕॴҦ Ϋϥολ(clutter)ͱݟ၏͢͜ͱ͕Ͱ͖Δɻଟ༠ిମ ΛಁաนͷϞσϧͱ͢ΔͱɺࣹͱಁաΛड৴ʑ ߸ʹऔΓೖΕͯͦͷଘࡏΛߟྀͰ͖ΔɻAFFʹΑΔϨʔ μը૾ɺͱΓΘ͚ۙڑʹ͓͍ͯ༗ӹͰ͋Δɻಁա ͷೖࣹ֯ґଘੑ͓Αͼपґଘੑ͕ɺͲͷఔը૾ ͷ࣭ʹӨڹΛ༩͑Δ͔ॏཁͳ֬ೝࣄ߲Ͱ͋Γɺ͜Εʹ ͍ͭͯޙͷ߲Ͱٞ͢Δɻશ࣮ͯଌͰݕ౼͢Δͱ࣌ؒ తίετେͳͷͱͳΔͷͰɺγϛϡϨʔγϣϯϞσ ϧཱ͕֬Ͱ͖Εص্ݕ౼͕ՄೳͱͳΔɻ߹։ޱϨʔ μը૾SARͱͷൺֱɺ͋Δ͍λʔήοτΛ୯७ͳ2࣍ ݩͰϞσϦϯάͨ͠ͱ͖ͷزԿޫֶճંཧ(GTD)͓Α ͼҰ༷ۙཧ(UAT)ʹΑΔۙքγϛϡϨʔγϣϯͳ Ͳ͕طʹஶऀʹΑͬͯใࠂ͞Ε͓ͯΓɺ͜ΕΛ߲࣍Ͱ ߟ͢Δ[13-15]ɻ 5.UATͱPOཧϞσϧͰͷಋମετϦοϓʹΑΔࢄཚ ͜͜Ͱɺૹड৴ΞϨΠϑΥʔΧγϯάʹΑΔϨʔμ ը૾ॲཧ(AFF)Λߟ͢ΔͨΊɺಋମετϦοϓΛλʔ ήοτϞσϧͱͯ͠औΓ্͛ΔɻετϦοϓͱ2࣍ݩ ͷଳঢ়ͷബ͍ಋମฏ൘ͷ͜ͱͰ͋Γɺ͜ΕʹΑΔࢄཚք ཧޫֶ๏(PO)ͳͲΛ༻͍ͯ༰қʹԕํք͕ٻΊΒ Εɺ݁ՌɺετϦοϓ෯͓Αͼ֯(u or v)ͷੵ ΛҾͱ͢ΔsincؔͰ༩͑ΒΕΔɻ͔͠͠ɺ͜͜Ͱͷ ϨʔμߏಛʹۙྖҬΛҙ͍ࣝͯ͠ΔͷͰɺۙࢄཚ քͷܭࢉ͕Մೳͳද͕ࣔࣜϙΠϯτͱͳΔɻͦ͜ͰɺUAT ͳͲͷޫઢཧʹΑͬͯۙքΛධՁ͢Δ͜ͱʹ͢Δɻ ਤ4ʹࣔ͢Α͏ʹɺετϦοϓ y ࣠ํʹҰ༷Ͱ (−a ≥ x ≥ a, y = 0)ʹஔ͔Ε͍ͯΔͱ͢Δɻઢݯr0 Λ දΘ͢ͷʹɺετϦοϓͷதԝ(ݪ)ɺ͓Αͼx < 0ͱ x > 0ʹ͋ΔೋͭͷΤοδ1,2Λத৺ʹʑۃ࠲ඪΛ༻ ͍ͯ(d, ϕ0), (d1, ϕ01), (d2, ϕ02)ͱ͢Δɻ؍ଌಉ༷ ਤ-4 ಋମετϦοϓʹΑΔճંɿ؍ଌͱݯ࠲ඪ
Fig.4 Diffraction of a line source by conducting strip: coordinates of observation and source.
ਤ-5 ಋମετϦοϓʹΑΔઢݯͷۙࢄཚ ք, ্:ిྲྀݯ E-ภ,Լ:࣓ྲྀݯ H-ภ
Fig.5 Scattering near-field of a line source by a conducting strip: upper:E-wave, lower: H-wave.
ʹ(ρ, ϕ), (ρ1, ϕ1), (ρ2, ϕ2)ͱද͢ɻಉਤͰɺӄӨڥ
ք(Shadow Boundary)ΛSBͱه͍ͯ͠Δɻฏ໘ʹΑ
Δి࣓քΛ
ਤ-6 ಋମετϦοϓʹର͢ΔUAT๏ͱPO๏ͷ ܭࢉൺֱ
Fig.6 AFF image by UAT and PO.
ͱ͢Δͱɺ͜Ε͕2ຕॏͳͬͨετϦοϓͰɺ ut(r) = uthp(ρ1, ϕ1) + uthp(ρ2, ϕ2)− uext(r), uext(r) = U ( cosϕ 2 ) ·[ui(ℓi)− ur(ℓr)] (11) ͱͳΔɻ͜͜ͰɺU (·)HeavisideͷεςοϓؔͰ͋ Δɻ্ࣜʹΑΔۙքܭࢉ݁ՌΛਤ5ʹࣔ͢ɻઢݯ ݪ͔Βy = 10λ, x = 0ͷڑʹஔ͔Ε͓ͯΓɺݪʹஔ ͔Εͨ෯3λͷετϦοϓͷۙͰͷి࣓քͰ͋Δ(λ: )ɻಉਤͰ্ଆ͕E-(ిྲྀݯ)ɺԼଆ͕H-(࣓ྲྀݯ) ͷ߹Ͱ͋Γɺਤதͷx্࣠ʹॻ͔Ε͍ͯΔଠઢ͕ετ ϦοϓҐஔΛ͍ࣔͯ͠Δɻ֤ʑͷภͷڥք݅΄΅ ຬ͞Ε͍ͯΔ͜ͱ͕͔Δɻ ಋମετϦοϓPO๏ͰύλʔϯΛ༧ଌͰ͖Δɻ͠ ͔͠લड़ͷΑ͏ʹɺۙͰͷύλʔϯධՁʹֶతͳ ࠔੑ͕͏ɻ͜͜Ͱɺ্ࣜͰ༩͑ΒΕΔUATۙք ͱPOʹΑΔԕํքͰͷϞσϦϯάͰͲͷΑ͏ͳ͕ࠩੜ͡ Δ͔Λ֬ೝ͢ΔͨΊɺಉ͡ύϥϝʔλͷετϦοϓʹର ͢ΔܭࢉൺֱΛਤ6ʹࣔͯ͋͠Δɻେ͖ͳҧ͍͕ൃੜ͠ ͍ͯΔ͜ͱ͕ཧղͰ͖Δɻಉ͡Ϟσϧʹର͠ɺୈ(11)ࣜ ʹΑΔࢄཚքΛ(9)ࣜͷPℓmnͱͯ͠ɺQ(rp)ͷઈର Λͦͷ··2࣍ݩ͓Αͼ3࣍ݩදࣔͨ͠ͷ͕ਤ7Ͱ͋ Δɻૉࢠִؒ1.6λͰ։ޱ16ૉࢠͷΞϯςφΞϨΠͷ தԝ͔ΒڑRʹஔͨ͠෯2a = 4λ (= 30cm)ͷΞϯ ςφʹਖ਼ର(S = 0)ͨ͠ετϦοϓʹE-ภͷిΛ রࣹͨ͠߹Ͱ͋Γɺಉ(a)R = 68λɺ(b)137λ ͷҐஔ͔Βૹड৴͍ͯ͠ΔɻൺଳҬ෯34%Ͱ͋Δɻ͜ ͷγϛϡϨʔγϣϯߏͰ1Ҏ্ͷૉࢠִؒͱ͠ (a) R = 68λ (b) R = 137λ ਤ-7 AFF 2,3࣍ݩը૾:ετϦοϓ෯ 2a = 4λ, E-ภ
Fig.7 AFF images:strip width 2a = 4λ, E-wave.
͍ͯΔͷͰɺAzํʹάϨʔςΟϯάϩʔϒ͕ൃੜ͢ ΔɻಉਤͰɺͦͷը૾ͷൣғʹଘࡏ͍ͯ͠ͳ͍ɻ
ਤ-6 ಋମετϦοϓʹର͢ΔUAT๏ͱPO๏ͷ ܭࢉൺֱ
Fig.6 AFF image by UAT and PO.
ͱ͢Δͱɺ͜Ε͕2ຕॏͳͬͨετϦοϓͰɺ ut(r) = uthp(ρ1, ϕ1) + uthp(ρ2, ϕ2)− uext(r), uext(r) = U ( cosϕ 2 ) ·[ui(ℓi)− ur(ℓr)] (11) ͱͳΔɻ͜͜ͰɺU (·)HeavisideͷεςοϓؔͰ͋ Δɻ্ࣜʹΑΔۙքܭࢉ݁ՌΛਤ5ʹࣔ͢ɻઢݯ ݪ͔Βy = 10λ, x = 0ͷڑʹஔ͔Ε͓ͯΓɺݪʹஔ ͔Εͨ෯3λͷετϦοϓͷۙͰͷి࣓քͰ͋Δ(λ: )ɻಉਤͰ্ଆ͕E-(ిྲྀݯ)ɺԼଆ͕H-(࣓ྲྀݯ) ͷ߹Ͱ͋Γɺਤதͷx্࣠ʹॻ͔Ε͍ͯΔଠઢ͕ετ ϦοϓҐஔΛ͍ࣔͯ͠Δɻ֤ʑͷภͷڥք݅΄΅ ຬ͞Ε͍ͯΔ͜ͱ͕͔Δɻ ಋମετϦοϓPO๏ͰύλʔϯΛ༧ଌͰ͖Δɻ͠ ͔͠લड़ͷΑ͏ʹɺۙͰͷύλʔϯධՁʹֶతͳ ࠔੑ͕͏ɻ͜͜Ͱɺ্ࣜͰ༩͑ΒΕΔUATۙք ͱPOʹΑΔԕํքͰͷϞσϦϯάͰͲͷΑ͏ͳ͕ࠩੜ͡ Δ͔Λ֬ೝ͢ΔͨΊɺಉ͡ύϥϝʔλͷετϦοϓʹର ͢ΔܭࢉൺֱΛਤ6ʹࣔͯ͋͠Δɻେ͖ͳҧ͍͕ൃੜ͠ ͍ͯΔ͜ͱ͕ཧղͰ͖Δɻಉ͡Ϟσϧʹର͠ɺୈ(11)ࣜ ʹΑΔࢄཚքΛ(9)ࣜͷPℓmnͱͯ͠ɺQ(rp)ͷઈର Λͦͷ··2࣍ݩ͓Αͼ3࣍ݩදࣔͨ͠ͷ͕ਤ7Ͱ͋ Δɻૉࢠִؒ1.6λͰ։ޱ16ૉࢠͷΞϯςφΞϨΠͷ தԝ͔ΒڑRʹஔͨ͠෯2a = 4λ (= 30cm)ͷΞϯ ςφʹਖ਼ର(S = 0)ͨ͠ετϦοϓʹE-ภͷిΛ রࣹͨ͠߹Ͱ͋Γɺಉ(a)R = 68λɺ(b)137λ ͷҐஔ͔Βૹड৴͍ͯ͠ΔɻൺଳҬ෯34%Ͱ͋Δɻ͜ ͷγϛϡϨʔγϣϯߏͰ1Ҏ্ͷૉࢠִؒͱ͠ (a) R = 68λ (b) R = 137λ ਤ-7 AFF 2,3࣍ݩը૾:ετϦοϓ෯ 2a = 4λ, E-ภ
Fig.7 AFF images:strip width 2a = 4λ, E-wave.
͍ͯΔͷͰɺAzํʹάϨʔςΟϯάϩʔϒ͕ൃੜ͢ ΔɻಉਤͰɺͦͷը૾ͷൣғʹଘࡏ͍ͯ͠ͳ͍ɻ (a) S = 0 (b) S = 13.7λ ਤ-8 AFF 2,3 ࣍ݩը૾: ετϦοϓ෯ 2a = 4λ, R = 68λ, H-ภ
Fig.8 AFF images:strip width 2a = 4λ, R = 68λ, H-wave. ಋମετϦοϓͷཧࣜ2࣍ݩϞσϧͰ͋Δɻैͬ ͯɺετϦοϓͷॎํͷมԽແࢹ͢Δ͜ͱʹͳΔ͕ɺ ετϦοϓͷ෯(ԣ)ํʹΞϯςφΛ1࣍ݩࠪͯ͠ ͍ΔͷͰɺ͜ͷӨڹۇগͱࢥΘΕΔɻͭ·Γɺ࣮ଌͷ ࡍʹՄೳͳݶΓετϦοϓͷॎํͷ͕͞େ͖͍ۚ ଐฏ൘Λ࠾༻͢Δ͜ͱ͕ϙΠϯτͱͳΔɻ ਤ8ετϦοϓ෯2a = 4λͰH-ภɺڑR = 68λ ͷ߹Ͱ͋Δɻಉ(a)ਤ7ͱಉ͡։ޱΛͭΞϨΠ ͱετϦοϓ͕ਖ਼ର͍ͯ͠Δ ͱ͖ɺ(b)ΞϨΠͱετ Ϧοϓͷத৺͕֤ʑS = 13.7λ͚ͩAzํʹΦϑηο τ͍ͯ͠Δͱ͖ͷ2, 3࣍ݩϓϩοτͰ͋Δɻಉ(b)ਤ (a)ͷ࠷େʹର͢Δ૬ରͰϓϩοτ͓ͯ͠Γɺࣼ ΊํʹΦϑηοτ͚ͨͩ͠Ϩϕϧ͕ݮ͍ͯ͠Δɻ ಉਤΑΓετϦοϓͷΤοδʹΑΔճંͷӨڹ͕ಡΈ औΕΔɻͳ͓ɺ7,8ୈ(9)ࣜͷQ0(rp)Λͦͷ··ϓ ϩοτ͍ͯ͠ΔͷͰɺૉࢠΞϯςφͷࢦੑํੑͷ ··Ͱ͋Δɻ Ҏ্ɺAFΛԠ༻ͨ͠Ұछͷ߹։ޱॲཧ๏AFFʹ͍ͭ ͯٞͨ͠ɻϞσϧͱͯ͠ετϦοϓͷۙքΛͬͯ γϛϡϨʔγϣϯΛߦ͕ͬͨɺ͜ΕϨʔμͷઃܭɺλʔ ήοτΛؚΉγϛϡϨʔγϣϯͳͲʹର͢Δࣄલݕ౼ͱ ͯ͠Ԡ༻Ͱ͖ΔͷͰɺͦͷҙٛେ͖͍ɻ3࣍ݩλʔ ήοτͷۙքܭࢉ͕Ͱ͖Δͱɺภղੳ͋Δ͍Ϋϩ εϨϯδํͷը૾ॲཧղੳՄೳͱͳΔɻ ࠷ޙʹલ߲ͱಉ͡ϞσϧΛͬͯɺAFFͱSAR ʹΑ ΔϨʔμը૾Λൺֱ͢Δɻਤ9 Ξϯςφ։ޱͱλʔ ήοτ(ετϦοϓதԝ) ؒͷڑR Λύϥϝʔλͱ ͯ͠ཧܭࢉͨ݁͠ՌͰ͋Δɻಉਤʹࣔ͢Α͏ʹɺR = 0.3 (0.4λ), 1.0, 2.0, 5.0, 10.0, 20.0 [m]ͱมԽ͍ͤͯ͞ Δɻ͜ͷ߹ɺR = 0.3 [m]ۙքྖҬɺR = 2 [m]Ҏ ԕԕํքྖҬʹଐ͢ΔɻۙྖҬͰͷSARը૾AFF ʹൺͯը૾ͷ࣭͕ྼԽ͍ͯ͠ΔɻSARը૾جຊ తʹૹड৴͕ಉۭؒ͡ʹҐஔ͢ΔϞϊελςοΫܕͰ ͋ΓɺҰํɺAFFૹड৴͕ҟͳΔҐஔͰಈ࡞͢ΔόΠ ελςοΫ(MIMO)Ͱ͋Δɻ͜ͷͨΊɺۙڑͰͷϑΥʔ ΧγϯάAFFͷํ͕༏Ε͍ͯΔɻ͔͠͠ɺಉਤͰ ͔ΔΑ͏ʹɺԕํྖҬͰSARͷํ͕ը૾ͷ࣭͕ྑ͍͜ ͱ͕ಡΈऔΕΔɻ͜ͷཧతͳൺֱݕ౼ࠓޙߦ͏͜ͱ ʹ͍ͨ͠ɻ 6. 2໘ίʔφʔϦϑϨΫλͷཧܭࢉͱ࣮ଌʹΑΔϨʔ μը૾ɹ ͜͜Ͱਤ10ʹࣔ͢Α͏ͳ2ຕͷฏ൘Λަͤͨ͞2 ໘ίʔφʔϦϑϨΫλʹΑΔAFFը૾ʹ͍ͭͯٞ͢Δɻ ͜ͷࢄཚମͷϞσϧલ߲ͷετϦοϓΛ2ݸΈ߹Θ
ਤ-9 UATʹΑΔετϦοϓϞσϧͷAFFͱSARը૾ͷཧܭࢉ
Fig.9 AFF and SAR images by UAT strip model.
ͤͨͷͰ͋ΓɺετϦοϓಉ༷2࣍ݩମͱͯ͠ѻ͏ ͜ͱ͕Ͱ͖Δɻ1ճ͋Δ͍2ճͷࣹɺࣹ͕ӄ Өڥքͷ֎ଆʹ͋Δͷ͔ଆʹ͋Δͷ͔ʹґଘ͢Δɻਤ 11 σ2D(ρ) = 2πρ E(ρ)· E∗(ρ) E(0)· E∗(0) (12) Ͱ ఆ ٛ ͞ Ε Δ ۙ Ͱ ͷ 2 ࣍ ݩ Ϩ ʔ μ அ ໘ ੵ (Radar Cross-Section:RCS)Λܭࢉͨ͠E-ภͷ݁ՌͰ͋Δɻ ௨ৗͷRCSρ→ ∞ͷԕํͰධՁ͞ΕΔɻܭࢉ͓Αͼ ࣮ݧʹ༻͍ͨฏ൘ͷҰลͷ͞5λͰ͋Γɺઢݯ͓ Αͼ؍ଌͱؒڑΛ֤ʑd, ρͱͯ͠ಉਤʹهࡌ ͍ͯ͠Δɻਤதʹ͋Δه߸ͰA→ B → CͱͳΔʹै͍ ి࣓քͷ૬ఆཧ͕ݟΒΕɺ؍ଌρ͕ԕํͱͳΔʹै ͍ύλʔϯͷมԽ࠷খͱͳΔ͜ͱ͕͔Δ(ਤதه߸ D)ɻͳ͓ɺUATʹΑΔ͜ͷܭࢉ݁Ռݫີղͱൺֱ͠ ্΄΅ಉ݁͡Ռͱͳ͍ͬͯΔ͜ͱΛ֬ೝ͍ͯ͠Δɻ ਤ12ਤ11ͱಉ͡ύϥϝʔλͷ2໘ίʔφʔϦϑϨ ΫλΛλʔήοτͱ࣮ͯ͠ଌͨ͠߹ͷAFFʹΑΔϨʔ μը૾Ͱ͋Δɻಉਤࠨཧܭࢉը૾ɺӈ࣮ଌը૾Ͱ ͋ΓɺภE-ภͰ͋ΔɻUATʹΑΔۙքϞσϧΛ ͍ͬͯΔͷͰɺೋͭͷedgeʹΑΔճંͷঢ়گ͕ԿΕ ਤ-10 2໘ίʔφʔϦϑϨΫλͷUATʹΑΔϞ σϦϯά
Fig.10 UAT model for 2-face corner-reflector.
ͷը૾͔ΒಡΈऔΕΔɻͳ͓ɺ࣮ଌʹΑΔը૾Ͱɺ Azํʹத৺Ґஔ͕ͣΕ͍ͯΔ͕Ξϯςφ։ޱͱλʔ ήοτͷத৺͕Φϑηοτ͍ͯ͠ΔͨΊͰ͋Δɻ 7.ΞϯςφϏʔϜΛߟྀͨ͠ͱ͖ͷը૾ධՁ ࠓ·Ͱͷཧը૾ͷܭࢉʹΞϯςφύλʔϯΛແࢦ ੑͱͯ͠ѻ͍ͬͯͨɻ͔࣮͠͠ࡍͷΞϯςφϏʔϜ ࢦੑ͕ଘࡏ͠ɺλʔήοτۭؒʹরࣹͨ͠ͱ͖ɺ͋Δ ͍λʔήοτ͔ΒͷࢄཚΛड৴͢Δͱ͖ʹɺϏʔϜ ʹΑΔॏΈ͕ൃੜ͢ΔɻAFF๏ͰόΠελςοΫͰΞ
ਤ-9 UATʹΑΔετϦοϓϞσϧͷAFFͱSARը૾ͷཧܭࢉ
Fig.9 AFF and SAR images by UAT strip model.
ͤͨͷͰ͋ΓɺετϦοϓಉ༷2࣍ݩମͱͯ͠ѻ͏ ͜ͱ͕Ͱ͖Δɻ1ճ͋Δ͍2ճͷࣹɺࣹ͕ӄ Өڥքͷ֎ଆʹ͋Δͷ͔ଆʹ͋Δͷ͔ʹґଘ͢Δɻਤ 11 σ2D(ρ) = 2πρ E(ρ)· E∗(ρ) E(0)· E∗(0) (12) Ͱ ఆ ٛ ͞ Ε Δ ۙ Ͱ ͷ 2 ࣍ ݩ Ϩ ʔ μ அ ໘ ੵ (Radar Cross-Section:RCS)Λܭࢉͨ͠E-ภͷ݁ՌͰ͋Δɻ ௨ৗͷRCSρ→ ∞ͷԕํͰධՁ͞ΕΔɻܭࢉ͓Αͼ ࣮ݧʹ༻͍ͨฏ൘ͷҰลͷ͞5λͰ͋Γɺઢݯ͓ Αͼ؍ଌͱؒڑΛ֤ʑd, ρͱͯ͠ಉਤʹهࡌ ͍ͯ͠Δɻਤதʹ͋Δه߸ͰA→ B → CͱͳΔʹै͍ ి࣓քͷ૬ఆཧ͕ݟΒΕɺ؍ଌρ͕ԕํͱͳΔʹै ͍ύλʔϯͷมԽ࠷খͱͳΔ͜ͱ͕͔Δ(ਤதه߸ D)ɻͳ͓ɺUATʹΑΔ͜ͷܭࢉ݁Ռݫີղͱൺֱ͠ ্΄΅ಉ݁͡Ռͱͳ͍ͬͯΔ͜ͱΛ֬ೝ͍ͯ͠Δɻ ਤ12ਤ11ͱಉ͡ύϥϝʔλͷ2໘ίʔφʔϦϑϨ ΫλΛλʔήοτͱ࣮ͯ͠ଌͨ͠߹ͷAFFʹΑΔϨʔ μը૾Ͱ͋Δɻಉਤࠨཧܭࢉը૾ɺӈ࣮ଌը૾Ͱ ͋ΓɺภE-ภͰ͋ΔɻUATʹΑΔۙքϞσϧΛ ͍ͬͯΔͷͰɺೋͭͷedgeʹΑΔճંͷঢ়گ͕ԿΕ ਤ-10 2໘ίʔφʔϦϑϨΫλͷUATʹΑΔϞ σϦϯά
Fig.10 UAT model for 2-face corner-reflector.
ͷը૾͔ΒಡΈऔΕΔɻͳ͓ɺ࣮ଌʹΑΔը૾Ͱɺ Azํʹத৺Ґஔ͕ͣΕ͍ͯΔ͕Ξϯςφ։ޱͱλʔ ήοτͷத৺͕Φϑηοτ͍ͯ͠ΔͨΊͰ͋Δɻ 7.ΞϯςφϏʔϜΛߟྀͨ͠ͱ͖ͷը૾ධՁ ࠓ·Ͱͷཧը૾ͷܭࢉʹΞϯςφύλʔϯΛແࢦ ੑͱͯ͠ѻ͍ͬͯͨɻ͔࣮͠͠ࡍͷΞϯςφϏʔϜ ࢦੑ͕ଘࡏ͠ɺλʔήοτۭؒʹরࣹͨ͠ͱ͖ɺ͋Δ ͍λʔήοτ͔ΒͷࢄཚΛड৴͢Δͱ͖ʹɺϏʔϜ ʹΑΔॏΈ͕ൃੜ͢ΔɻAFF๏ͰόΠελςοΫͰΞ ਤ-11 2໘ίʔφʔϦϑϨΫλͷۙόΠελςΟοΫRCSܭࢉύλʔϯ
Fig.11 Near-field patterns for 2-face corner-reflector.
ਤ-12 2໘ίʔφʔϦϑϨΫλͷUATʹΑΔϞ
σϦϯάͱ࣮ଌ
Fig.12 UAT theory and measurement for 2-face cor-ner reflector. ϨΠ։ޱ্ͰͷฏۉԽ͕ਤΕΔͱࢥΘΕΔ͕ɺएׯͷӨ ڹੜ͡Δͱ༧͍ͯ͠Δɻ·ͨવͳ͕ΒɺΞϯςφ རಘͷपಛੑಛʹϨϯδํͰͷը૾ͷۉҰੑʹ ӨڹΛ༩͑ΔͷͰɺ͜ͷಛੑѲͭͭ͠ը૾࠶ੜͷࡍ ʹิঈ͓ͯ͘͠ඞཁ͕͋Δɻ ૹड৴ΞϯςφͷۭؒύλʔϯಛੑΛؚΜͩΞϯςφ རಘΛ֤ʑGt ℓmn(fℓ, rmn), Grℓmn(fℓ, rmn)ͱ͢Δͱɺઌ ͷ(9)ࣜ࣍ͷΑ͏ʹमਖ਼͞ΕΔɻ Q1(r) = Gtℓmn(fℓ, rmn)· Grℓmn(fℓ, rmn)· Q0(r). (13) Ξϯςφࢦੑύλʔϯλʔήοτ͔Βͷࢄཚిྗʹ ॏΈͷΑ͏ʹ࡞༻͢ΔͷͰɺಛʹۙྖҬͰແࢹͰ͖ ͳ͍ิਖ਼ͱͳΔ͜ͱ͕༧͞ΕΔɻ ࣮ଌͰ༻͍ͨΞϯςφͷܭࢉύλʔϯʹؔ͠ɺਤ13ʹ ͦͷॾݩΛࣔ͢ɻܭࢉจݙ[14]ʹৄड़͞Ε͍ͯΔ։ ޱ๏ʹΑΔ݁ՌͰ͋Γɺ࣮ଌͱྑ͘Ұக͍ͯ͠Δ ͜ͱ͕͔Δɻ͜ͷܭࢉύλʔϯΛAFFը૾ʹద༻ͨ͠
ਤ-13 ࣮ଌʹ༻ۣͨ͠ܗϗʔϯΞϯςφͷཧͱ࣮ଌύλʔϯ
Fig.13 Theoretical and measurement patterns of horn antenna for AFF measurement.
ਤ-14 ϨʔμAFFը૾ʹର͢ΔΞϯςφϏʔϜͷӨڹ
Fig.14 Antenna beam effect to AFF radar imaging.
݁Ռ͕ਤ14Ͱ͋Δɻλʔήοτ෯30[cm]ͷಋମετ ϦοϓͰ͋Γɺಉਤࠨ͕ਤ13ͷΞϯςφϏʔϜΛߟྀ͠ ͨAFFը૾Ͱ͋Δɻߟྀ͠ͳ͍߹ͱͷ͕ࠩ͋·Γେ͖ ͘ͳ͍ͷͰɺਤ14ͷதԝͱӈʹ֤ʑAzํͱRangeํ ͷஅ໘ͰͷࠩΛࣔ͢ɻಉਤͰେ͖ͳҧ͍ݟΒΕͳ ͍͕ɺΞϨΠ։ޱ͕λʔήοτʹൺͯେ͖͍߹ɺ ͋Δ͍ΞϨΠͱλʔήοτؒڑ͕ൺֱత͍߹ʹ ݦஶͳ͕ࠩൃੜͯ͘͠Δͱ༧͍ͯ͠Δɻܭࢉγϛϡ ϨʔγϣϯͰಉจݙͷཧࣜΛΘͣʹɺਖ਼ݭ ͔GaussϏʔϜͰۙࣅ͢ΔͷܭࢉίετΛߟྀͨ͠ํ ๏Ͱ͋Δɻ ͳ͓ɺ্هΞϯςφϏʔϜิਖ਼ܭࢉ্ͰͷͰ ͋Γɺ࣮ࡍͷܭଌͰطʹ࣮͞ΕͨΞϯςφͷϏʔϜ ͷॏΈ͕ड৴σʔλʹؚ·Ε͍ͯΔͷͰɺߟྀ͢Δඞཁ ͳ͍ɻ 8.นಁաϨʔμͱͯ͠ͷAFFཧ นಁա͋Δ͍ຒઃݕ༻ͷηϯαͰɺϨʔμͱ λʔήοτؒʹෆཁͷো͕ଘࡏ͢Δɻ͜ΕॴҦΫ ϥολͱͯ͠ݟ၏͢͜ͱͰ͖Δɻஶऀ͕طʹൃදͯ͠ ͍Δଟ༠ిମΛಁաนͷϞσϧͱ͢Δͱɺࣹͱಁ աΛड৴ʑ߸ʹऔΓೖΕΔ͜ͱ͕Ͱ͖ɺͦͷଘࡏΛ ධՁͰ͖Δ[14,16] ɻAFFʹΑΔϨʔμը૾ۙڑʹ ͓͍ͯ༗ӹͰ͋Δ͜ͱલ߲·ͰͰ֬ೝ͍ͯ͠Δɻैͬ ͯɺಁաͷೖࣹ֯ґଘੑ͓Αͼपґଘੑ͕Ͳͷ ఔը૾ͷ࣭ʹӨڹΛ༩͑Δ͔ɺॏཁͳ֬ೝࣄ߲Ͱ͋ Δɻશ࣮ͯଌͰݕ౼͢Δͱ࣌ؒతίετେͳͷͱ
ਤ-13 ࣮ଌʹ༻ۣͨ͠ܗϗʔϯΞϯςφͷཧͱ࣮ଌύλʔϯ
Fig.13 Theoretical and measurement patterns of horn antenna for AFF measurement.
ਤ-14 ϨʔμAFFը૾ʹର͢ΔΞϯςφϏʔϜͷӨڹ
Fig.14 Antenna beam effect to AFF radar imaging.
݁Ռ͕ਤ14Ͱ͋Δɻλʔήοτ෯30[cm]ͷಋମετ ϦοϓͰ͋Γɺಉਤࠨ͕ਤ13ͷΞϯςφϏʔϜΛߟྀ͠ ͨAFFը૾Ͱ͋Δɻߟྀ͠ͳ͍߹ͱͷ͕ࠩ͋·Γେ͖ ͘ͳ͍ͷͰɺਤ14ͷதԝͱӈʹ֤ʑAzํͱRangeํ ͷஅ໘ͰͷࠩΛࣔ͢ɻಉਤͰେ͖ͳҧ͍ݟΒΕͳ ͍͕ɺΞϨΠ։ޱ͕λʔήοτʹൺͯେ͖͍߹ɺ ͋Δ͍ΞϨΠͱλʔήοτؒڑ͕ൺֱత͍߹ʹ ݦஶͳ͕ࠩൃੜͯ͘͠Δͱ༧͍ͯ͠Δɻܭࢉγϛϡ ϨʔγϣϯͰಉจݙͷཧࣜΛΘͣʹɺਖ਼ݭ ͔GaussϏʔϜͰۙࣅ͢ΔͷܭࢉίετΛߟྀͨ͠ํ ๏Ͱ͋Δɻ ͳ͓ɺ্هΞϯςφϏʔϜิਖ਼ܭࢉ্ͰͷͰ ͋Γɺ࣮ࡍͷܭଌͰطʹ࣮͞ΕͨΞϯςφͷϏʔϜ ͷॏΈ͕ड৴σʔλʹؚ·Ε͍ͯΔͷͰɺߟྀ͢Δඞཁ ͳ͍ɻ 8.นಁաϨʔμͱͯ͠ͷAFFཧ นಁա͋Δ͍ຒઃݕ༻ͷηϯαͰɺϨʔμͱ λʔήοτؒʹෆཁͷো͕ଘࡏ͢Δɻ͜ΕॴҦΫ ϥολͱͯ͠ݟ၏͢͜ͱͰ͖Δɻஶऀ͕طʹൃදͯ͠ ͍Δଟ༠ిମΛಁաนͷϞσϧͱ͢Δͱɺࣹͱಁ աΛड৴ʑ߸ʹऔΓೖΕΔ͜ͱ͕Ͱ͖ɺͦͷଘࡏΛ ධՁͰ͖Δ[14,16] ɻAFFʹΑΔϨʔμը૾ۙڑʹ ͓͍ͯ༗ӹͰ͋Δ͜ͱલ߲·ͰͰ֬ೝ͍ͯ͠Δɻैͬ ͯɺಁաͷೖࣹ֯ґଘੑ͓Αͼपґଘੑ͕Ͳͷ ఔը૾ͷ࣭ʹӨڹΛ༩͑Δ͔ɺॏཁͳ֬ೝࣄ߲Ͱ͋ Δɻશ࣮ͯଌͰݕ౼͢Δͱ࣌ؒతίετେͳͷͱ ͳΔͷͰɺ͜͜Ͱఏࣔ͢ΔΑ͏ʹγϛϡϨʔγϣϯϞσ ϧཱ͕֬Ͱ͖Εص্ݕ౼͕ՄೳͱͳΓɺ͜ͷͷݚ ڀଅਐʹد༩Ͱ͖Δɻ ࠓɺนΛଟͷ༠ిମฏ൘ͱͯ͠ѻ͏ͱɺಈ͜ΕΒ ͷ෦Ͱଟॏͷࣹͱಁաͷޙɺಈͷਐߦํʹ࠷ ऴͷಁաΛͬͯλʔήοτʹൖ͢ΔɻҰํɺΞ ϨΠͷૹड৴ਵ࣌มΘΔͷͰɺ͜ͷଟฏ൘ͷೖ ࣹ֯ݻఆ͞Ε͍ͯͳ͍ɻ͜ͷͱ͖ɺҰͭʹͳΔͷ ͕༠ిମͰͷಈͷԆྔͰ͋Δɻλʔήοτͱਖ਼ର ͍ͯ͠Δͱ͖Λج४ͱ͢ΔͱɺͦΕҎ֎ͷೖࣹ֯ΛҎͯ ೖࣹ͢ΔಈৗʹԆ͍ͯ͠ΔɻۙྖҬͰͷϨʔμ ηϯαͰɺ͜ͷԆྔ͔ͳΓେ͖͘ͳΔ߹͋Δ ͱ༧͞ΕΔɻಛʹɺΞϨΠ։ޱ͕λʔήοτؒڑ ΑΓେ͖͘ɺೖࣹ͕֯ेΛ͑Δ߹ͷԆྔڑ ʹࢉͯ͠ηϯνϝʔτϧͷΦʔμʔͱͳΔɻຊ߲Ͱ ɺଟͷ༠ిମฏ൘ʹΑΔҐ૬ԆΛܭࢉ͢Δ؆୯ͳ දࣔࣜΛSnellͷ๏ଇΛ༻͍ͯ༠ಋ͓ͯ͘͠ɻ લड़ͷҐ૬Ԇྔܦ࿏ʹஔ͖͔͑ͯߟ͑Δͱ ͔Γқ͍ɻ༠ిͱಁ࣓ͷҟͳΔഔ࣭ͷڥքͰɺ
Snellͷ๏ଇk1sin θ1= k2sin θ2ཱ͕͢Δɻk1, k2
֤ʑͷഔ࣭தͰͷͰ͋Γɺഔ࣭ߏఆ(ε, µ)ͱ
k = ω√εµ (ω = 2πf, f : पεϖΫτϥϜ)ͷ͕ؔ
͋Δɻ༠ిମฏ൘͕N ͋Δ߹ɺ֤༠ిମΛஞ࣍࿈ଓ ͤ͞Δ͜ͱʹΑΓ
k1sin θ1= k2sin θ2=· · · = kisin θi=· · ·
= kNsin θN, i = 1, 2,· · · , N (14) ͳΔ͕ؔࣜಘΒΕΔɻॳظͱͳΔೖࣹ֯θ1͕༩͑Β ΕΕɺi൪ͷͷೖࣹ֯༰қʹܭࢉͰ͖Δɻࠓɺ֤ ͷްΈΛziͱ͢ΔͱɺN શ෦Λൖ͢Δಁաͷޫ ֶతͳܦ࿏DࡾฏํͷఆཧΑΓ༰қʹ࣍ࣜͰ༩͑Β ΕΔɻ D = N ∑ i=1 kizi·(ki2− k12sin2θ1)−1/2. (15) Ξϯςφͷ࠲ඪɺͭ·ΓݯͷҐஔ(x0, y0, z0)ͱ࠷ऴͷ ಁաͱͳΔ؍ଌ࠲ඪ(x, y, z)্ࣜͷؔΛຬͨ͞ͳ ͚ΕͳΒͳ͍ɻ͜ΕΑΓɺೖࣹ֯ɺݯ࠲ඪͦͯ͠؍ ଌ࠲ඪ͜ͷ2͕ܾͭ·ΕΓͷ1ͭࣗಈతʹٻ ΊΕΔɻ͜ͷؔΛಈతʹҠಈ͢Δૹड৴Ξϯςφͦ͠ ͯλʔήοτؒͷܦ࿏ิਖ਼ʹద༻ͯ͠ɺ༠ిମͷ ൖಈͷޫֶܦ࿏Λิਖ਼͢ΕΑ͍ɻো͕ଘࡏ͠ ͍ͯΔͨΊʹ༨ʹൃੜ͍ͯ͠Δ૯ܦ࿏(15)ࣜΛߟ ྀ͢Δͱɺ݁ہɺઌͷ(13)ࣜ Q(r) = Tt ℓmn(fℓ, rmn) exp{jkDt(rtm, r,N ) } ·Tℓmnr (fℓ, rmn) exp{jkDr(rrn, r,N )} · Q1(r) = 1 LM N L ∑ ℓ=1 M ∑ m=1 N ∑ n=1 ·Tt ℓmn(fℓ, rmn) exp{jkD(rtm, r,N ) } ·Tr ℓmn(fℓ, rmn) exp{jkD(rrn, r,N )} ·Gt ℓmn(fℓ, rmn)· Grℓmn(fℓ, rmn)· Pℓmn(fℓ, rmn) · exp { j2πfℓ c rmn(xp, yp, zp) } · exp(jϕℓ) (16) ͷ Α ͏ ʹ म ਖ਼ Ͱ ͖ Δ ɻ͜ ͜ Ͱ ɺDt(r m, r,N ) ͱ Dr(r n, r,N )֤ʑૹ৴ଆͱλʔήοτଆ͔Βೖࣹ͠ ͨͱ͖ͷN ͷ༠ిମนʹΑΔૠೖܦ࿏Λද͓ͯ͠ ΓɺTt ℓmn(fℓ, rmn), Tℓmnr (fℓ, rmn)จݙ[17] Ͱݫີʹ ఆࣜԽ͍ͯ͠ΔN ༠ిମʹΑΔಁաͰ͋Γɺ֤ʑ ૹ৴ଆ͔Βೖࣹͨ͠ͱ͖ͱλʔήοτଆ͔Βೖࣹͨ͠ͱ ͖ͷͰ͋Δɻ·ͨɺGt ℓmn(fℓ, rmn), Grℓmn(fℓ, rmn) ֤ʑૹ৴ͱड৴Ξϯςφͷۭؒύλʔϯ(རಘ)ಛੑͰ ͋Γɺ͜Ε͕λʔήοτ͔ΒͷࢄཚిྗʹॏΈͷΑ͏ʹ ࡞༻͢ΔͷͰɺಛʹۙྖҬͰແࢹͰ͖ͳ͍ิਖ਼ͱͳ Δ͜ͱ͕༧Ͱ͖Δɻ 9.1ͷน͕͋Δͱ͖ͷAFF࣮ଌͱ༠ిܭଌԠ༻ɹ ਤ15ް͞6 cmͷίϯΫϦʔτนΛஔ͍ͯ͠Δ࣮ ݧܥΛࣔͨ͠ͷͰ͋ΔɻϨʔμॾݩಉਤʹΑΔɻΞ ϯςφͱλʔήοτؒڑ100cmɺΞϨΠ։ޱͱε τϦοϓ෯֤ʑ90, 22cmͰ͋Δɻਤ16ίϯΫϦʔ τͷൺ༠ిΛεr= 5.4ͱͨ͠ͱ͖ͷAFFը૾Ͱ͋Δɻ ͜ͷਤͰγεςϜԆྔejϕℓ ͷิਖ਼લͳͷͰɺϨϯδ ํ127cmͷͱ͜Ζʹλʔήοτத৺͕දΕ͍ͯΔɻ͜ ͷ༠ిͷܾఆʹؔͯ͠ޙड़͢Δɻิਖ਼ޙͷը૾ए ׯվળ͞Ε͍ͯΔͷ͕͔Δ͕ɺৄ͘͠ݟΔͨΊɺ͜ͷ அ໘มԽΛΫϩεϨϯδ(Az)ํͱϨϯδํͰࣔ͠ ͨͷ͕ਤ17Ͱ͋Δɻ༧͞Εͨ௨Γɺิਖ਼Λߦ͏ͱத৺ ෦ΑΓपล෦ͷํͰͦͷޮՌ͕໌֬ʹݟΒΕΔ͜ͱ͕ ͔Δɻࠓճͷ࣮ݧ1ͷ߹Ͱ͋Δ͕ɺޙͰ3ͷ ߹ௐΔɻͳ͓ɺ্هϞϧλϧίϯΫϦʔτͷൺ༠ ిน͕ແ͍ͱ͖ͷλʔήοτը૾ͷϐʔΫ͋Δ͍ த৺࠲ඪͱน͕͋Δͱ͖ͷͦΕΛൺֱ͠ɺλʔήοτ શମͷը૾ΛϨϯδํʹҠಈͤͯ͞ɺ༠ిΛٯࢉ͠ ͯٻΊ͍ͯΔɻ͜ͷΑ͏ʹՁతͳ༠ిͷܭଌ͕Մೳ ͱͳΔͷͰɺ͜ͷߟ͑Ԡ༻্ඇৗʹॏཁͰ͋ΔɻҎԼ ͜Εʹ͍͓ͭͯٞͯ͘͠ɻ
ਤ-15 ίϯΫϦʔτนʹΑΔಁա࣮ݧ(ฏ໘ਤ): ܦ࿏ิਖ਼ͷ༗ޮੑ֬ೝ
Fig.15 Transmission measurement of a concrete wall (plan view): Effectiveness of length compensation.
ਤ-16 1ܦ࿏ิਖ਼ͷ༗ແʹΑΔ࣮ଌAFFը૾ൺֱ, ࠨɿίϯΫϦʔτน͕ແ͍߹, தɿ1ίϯΫ
Ϧʔτนɺܦ࿏ແิਖ਼, ӈɿܦ࿏ิਖ਼͋Γ
Fig.16 AFF iage comparison, left: no wall, middle: with a concrete wall, no compensation, right: after compensation. ༠ిͷܭଌಉ࣠ઢ࿏ɺಋɺۭಎڞৼثͳͲͷ ૹઢ࿏Λར༻ͯ͠༠ిମ࣮લޙͷมԽΑΓߦ͏ํ ๏ɺۭͦͯؒ͠ͰͷࣹͷมԽ͔ΒٻΊΔํ๏͕ ͋Δɻલऀਖ਼֬ͳ༠ి͕ٻΊΒΕΔ͕ɺۭؒʹ ͍ͯ͠Δେ͖ͳମͳͲʹෆదͰ͋Δɻޙऀͷۭؒఆ ࡏ๏ɺిٵऩମͷࣹଌఆʹྑ͘༻͍ΒΕΔ ۭؒఆࡏ๏Ͱ͋Δ͕ɺࣹͷS/Nൺ͕ෆ҆ఆʹͳ Δɺ͋Δ͍ࣹ͕ΞϯςφϘΞαΠτํͷϏʔ Ϝۙ࣠ʹґଘ͍ͯ͠Δɺͦͯ͠ͷ༠ిٻΊΒΕ ͳ͍ͳͲͷ͕ܽ͋Δɻ͜͜Ͱͷը૾γϑτʹΑΔํ๏
(Image Shifting Method: ISMͱԾশ͢Δ)ը૾ੜ
ॲཧAFF๏ͷੜతͳܭଌ๏ͱͯ͠ɺྛͳͲͷۭؒ ʹࢄͨ͠ମͷՁతͳ༠ిΛͦΕͳΓͷ҆ఆͨ͠ ܭଌਫ਼͕ظͰ͖Δɻ ਤ161ίϯΫϦʔτนͷ߹Ͱ͋Δ͕ɺ͜ͷ1 ͷίϯΫϦʔτͷ྆ଆʹผͷ࣭ͷ༠ిମฏ൘ΛுΓ ͚ͨ3ͷนͷ߹ʹಉ͡Α͏ʹɺISMͰՁతͳ༠ ిΛٻΊΔΞϧΰϦζϜ͕ՄೳͰ͋Δɻ͜ͷ2८ͷܭ ଌํ๏ɺนಁաϨʔμʹԠ༻Ͱ͖ΔՄೳੑ͕͋Δɻ ෆಛఆͷนͷ(Ձత)ͳ༠ి͓ΑͼްΈະͰ͋Δ ͜ͱ͕ҰൠతͰ͋Δɻͦ͜Ͱɺ1ճͷܭଌͰରΛ ଌΓɺ2ճͷܭଌͰ͜ͷରʹ༧Ί༻ҙͨ͠༠ి
ਤ-15 ίϯΫϦʔτนʹΑΔಁա࣮ݧ(ฏ໘ਤ): ܦ࿏ิਖ਼ͷ༗ޮੑ֬ೝ
Fig.15 Transmission measurement of a concrete wall (plan view): Effectiveness of length compensation.
ਤ-16 1ܦ࿏ิਖ਼ͷ༗ແʹΑΔ࣮ଌAFFը૾ൺֱ, ࠨɿίϯΫϦʔτน͕ແ͍߹, தɿ1ίϯΫ
Ϧʔτนɺܦ࿏ແิਖ਼, ӈɿܦ࿏ิਖ਼͋Γ
Fig.16 AFF iage comparison, left: no wall, middle: with a concrete wall, no compensation, right: after compensation. ༠ిͷܭଌಉ࣠ઢ࿏ɺಋɺۭಎڞৼثͳͲͷ ૹઢ࿏Λར༻ͯ͠༠ిମ࣮લޙͷมԽΑΓߦ͏ํ ๏ɺۭͦͯؒ͠ͰͷࣹͷมԽ͔ΒٻΊΔํ๏͕ ͋Δɻલऀਖ਼֬ͳ༠ి͕ٻΊΒΕΔ͕ɺۭؒʹ ͍ͯ͠Δେ͖ͳମͳͲʹෆదͰ͋Δɻޙऀͷۭؒఆ ࡏ๏ɺిٵऩମͷࣹଌఆʹྑ͘༻͍ΒΕΔ ۭؒఆࡏ๏Ͱ͋Δ͕ɺࣹͷS/Nൺ͕ෆ҆ఆʹͳ Δɺ͋Δ͍ࣹ͕ΞϯςφϘΞαΠτํͷϏʔ Ϝۙ࣠ʹґଘ͍ͯ͠Δɺͦͯ͠ͷ༠ిٻΊΒΕ ͳ͍ͳͲͷ͕ܽ͋Δɻ͜͜Ͱͷը૾γϑτʹΑΔํ๏
(Image Shifting Method: ISMͱԾশ͢Δ)ը૾ੜ
ॲཧAFF๏ͷੜతͳܭଌ๏ͱͯ͠ɺྛͳͲͷۭؒ ʹࢄͨ͠ମͷՁతͳ༠ిΛͦΕͳΓͷ҆ఆͨ͠ ܭଌਫ਼͕ظͰ͖Δɻ ਤ161ίϯΫϦʔτนͷ߹Ͱ͋Δ͕ɺ͜ͷ1 ͷίϯΫϦʔτͷ྆ଆʹผͷ࣭ͷ༠ిମฏ൘ΛுΓ ͚ͨ3ͷนͷ߹ʹಉ͡Α͏ʹɺISMͰՁతͳ༠ ిΛٻΊΔΞϧΰϦζϜ͕ՄೳͰ͋Δɻ͜ͷ2८ͷܭ ଌํ๏ɺนಁաϨʔμʹԠ༻Ͱ͖ΔՄೳੑ͕͋Δɻ ෆಛఆͷนͷ(Ձత)ͳ༠ి͓ΑͼްΈະͰ͋Δ ͜ͱ͕ҰൠతͰ͋Δɻͦ͜Ͱɺ1ճͷܭଌͰରΛ ଌΓɺ2ճͷܭଌͰ͜ͷରʹ༧Ί༻ҙͨ͠༠ి ਤ-17 ը૾ϐʔΫϨϕϧͰͷ֤ओํͷஅ໘ม Խ: 1(εr= 5.4), ্:ΫϩεϨϯδํ, Լ: Ϩϯδํ
Fig.17 Variation of cross-section at image peak-level, upper: cross-range direction, lower: range direction. ͱްΈ͕طͷฏ൘ΛషΓ͚ͯܭଌ͢ΔɻಘΒΕͨը ૾ͷը૾γϑτྔΛิਖ਼͢Εɺର(น)ͷՁతͳ ༠ిͱްΈ͕ධՁͰ͖Δ͜ͱʹͳΔɻ͜ͷͱ͖ͷਖ਼֬ ͳܭࢉʹඞཁͳͷલड़ͷଟ༠ిମฏ൘ʹΑΔཧͱ ܦ࿏ิਖ਼(AFF)ΞϧΰϦζϜͰ͋Δ͕ɺ͜͜Ͱۙࣅ తͰ͋Δ͕࣮༻తͳࢉग़๏ʹ͍ͭͯޙड़͢Δɻ ͯ͞ɺΞϯςφҐஔΛݻఆͨ͠௨ৗͷϨʔμࠪͷ ߹ɺͦͷࣹ৴߸ͷதʹૠೖҐ૬ใؚ͕·Ε͓ͯΓɺ ্ड़ͷૢ࡞͕ՄೳͰ͋Δɻ͜͜Ͱड़Δը૾ใΛͬ ͯ༠ి͋Δ͍ްΈΛܭଌ͢Δͱɺඇৗʹ҆ఆͨ͠S/N ൺͰܭଌͰ͖Δͱ͍͏ͷ͕ϙΠϯτͰ͋Δɻಛʹύϧε ϨʔμͷߴͳϨʔμΛΘͳͯ͘ྑ͘ɺAzํͷ ҐஔಛఆͰ͖Δͱ͍͏ͷେ͖ͳϝϦοτͰ͋Δɻෳ ૉ༠ిͷڏ෦ɺนͷ༗ແʹΑΔड৴ిྗྔΛൺֱ͢ Δ͜ͱͰࢉग़Ͱ͖Δɻนʹরࣹࣹͨ͠ిྗߟྀͰ ͖ͳ͍͕ɺଟฏ൘ͷཧͰڏ෦ͷΛ͍ٻΊΔ͜ ͱ͕Ͱ͖Δ[4,14]ɻޙड़ͷΑ͏ʹɺਤ16ͷίϯΫϦʔ τͷྫʹద༻͢Δͱɺεr= 5.4−j0.29ͱͳͬͨɻ ܦ࿏ิਖ਼(AFF)ʹࡍͯ͠ͷཧഎܠͱISM๏ʹΑ ΔఆࣜԽΛ؆୯ʹ·ͱΊ͓ͯ͘ɻ༠ి͕εɺಁ࣓ ͕µͷഔ࣭தͷv = 1/√εµɺਅۭதޫ c = 1/√ε0µ0Ͱ༩͑ΒΕΔɻൺ༠ిεr= ε/ε0ͱൺಁ࣓ µr= µ/µ0Λఆٛ͢Δͱɺഔ࣭தͷಈͷඇ࣓ ੑମഔ࣭Λఆ͠(µr= 1)ɺ v =√1 εµ = c √ε r (17) ͱͳΔɻ͜ͷͱ͖ɺഔ࣭தͷ k = ω v = √ε r ω c = n ω c (18) Ͱ༩͑ΒΕΔɻnਅۭ͔Βഔ࣭ͷಁաΠϯσοΫε n = √εrͰ͋ΔɻҰํɺ࠲ඪzͷਖ਼ͷํʹਐΉ༠ిମ ͷಈ Ez= E0e−αzej(ωt−βz), jk = α + jβ (19) Ͱද͞ΕΔɻαΛݮਰఆɺβΛҐ૬ఆͱݺΜͰ͍Δɻ ഔ࣭Λແଛࣦͱ͢Δͱɺk = βͱͳΔɻ Ҏ্͔Β໌Β͔ͳΑ͏ʹɺഔ࣭தͷಈ(19)ࣜΑΓ ∆ϕ = k0√εrz0− k0z0= k0(√εr− 1)z0 (20) ͚ͩܦ࿏͕৳ு͢Δɻ͜Ε͕ը૾ੜ࣌ͷҐஔγϑτ ྔ∆ϕ/k0ʹରԠ͢Δɻ্ࣜͰz0༠ిମোͷްΈ Ͱ͋ΔɻҐ૬ૠೖʹࢉ͢Εɺը૾্ͰLͷҐஔγ ϑτʹର͠ɺ∆ϕ = k0L = k0(√εr− 1)z0 ͚ͩͷҐ૬͕ܦ ࿏ͷยಓ(1-way)ʹՃ͞Εͨ͜ͱʹͳΔɻ͜ΕΑΓ εr= (L z0 + 1 )2 ≥ 1 (21) ͱ͍͏؆୯ͳධՁ͕ࣜಋ͔ΕΔɻಘΒΕͨը૾͔Βλʔ ήοτͷҠಈྔLΛԿΒ͔ͷํ๏ͰٻΊΔࡍɺͦͷಡΈ औΓޡࠩΛ±∆Lͱ͢Δͱɺ(21)ࣜ∆Lͷୈ1߲·Ͱ ͯ͠ɺ εr → εr±√εr· ∆L z0 (22) ͱද͞ΕΔɻ͜ΕΑΓɺz0͕૬ରతʹେ͖͍ఔͦͷޡࠩ ͷӨڹԼ͠ɺ√εrͷେ͖͕͞େ͖͍ͱ͖ఔͦͷӨڹ ͕େ͖͘ͳΔ͜ͱ͕͔Δɻ ਤ16ͷ࣮ݧྫͰɺطྔͰ͋Δ༠ిମްΈ͕z0= 6 cmɺը૾্ͷҐஔγϑτྔ͕L = 8 cmͷ߹ɺεr= 5.4͕ ਪఆ͞ΕΔɻಡΈऔΓޡࠩΛ±0.5cmͱ͢Δͱɺ(22)ࣜ ΑΓຌͦ∆εr=±0.2ͷޡ͕ࠩଳ͢Δ͜ͱʹͳΔɻͳ ͓ɺϚΠΫϩճ࿏ཧͰ͍͏ಉ࣠Ϟʔυ(TEM mode) ͷมԽ͔Β༠ిΛܭଌ͢Δಉ࣠๏ʹͯಉίϯΫϦʔ
ਤ-18 ࣮ݧʹ༻͍ͨίϯΫϦʔτน
Fig.18 Concrete wall for measurement.
ਤ-19 3ܦ࿏ิਖ਼ͷ༗ແʹΑΔAFFը૾ൺ
ֱ: ࣮ଌ, ੴߣϘʔυεr = 4.0), ্:ແิਖ਼,
Լ:ิਖ਼
Fig.19 3-layered AFF image, upper: no compensa-tion, lower:with length compensation.
τΛܭଌ͢Δͱɺεr= 5.1ͱͳͬͨɻจݙ[9] Ͱυϥ ΠίϯΫϦʔτͷൺ༠ిεr= 4͔Β10Ͱ͋Δͱه ࡌ͞Ε͍ͯΔɻ 10.3ͷน͕͋Δͱ͖ͷ࣮ଌྫ͓Αͼٞɹ ࣮ଌͷ࠷ޙͷྫͱͯ͠ɺ3ίϯΫϦʔτͷ߹Λࣔ ͢ɻਤ18࣮ݧʹ༻͍ͨ1(ࠨ)ͱ3ίϯΫϦʔτ นͷࣸਅͰ͋Δɻ3นίϯΫϦʔταϯϓϧͷ྆ଆ ʹް͞9.6mmͷੴߣϘʔυΛுΓ͚͍ͯΔɻ͜ͷͱ͖ औಘͨ͠AFFը૾Λਤ19,20ʹࣔ͢ɻલਤAFFը૾ɺ ਤ-20 ը૾ϐʔΫϨϕϧͰͷ֤ओํͷஅ໘ม Խ, ্:ΫϩεϨϯδํ, Լ:Ϩϯδํ
Fig.20 Variation of cross-section in peal-level of 3 layered AFF image, upper: cross-range di-rection, lower:range direction.
ޙਤஅ໘ڧͰ͋ΔɻੴߣϘʔυͷްΈ9.6mmࣄલ ʹܭଌͯ͠طͰ͋Δ͕ɺ༠ిෆ໌Ͱ͋ΔɻίΞ෦ ͷίϯΫϦʔτͷްΈͱൺ༠ిલड़ͷ6.0ͱධՁ εr= 5.4Ͱ͋Δɻ͜ΕΒͷใͱAFFը૾ͷҠಈྔΛલ ड़ଟ༠ిମͷཧʹద༻͠ɺ྆นͷੴߣϘʔυͷ༠ి Λࢉग़͢Δͱɺεr= 4.0ͱͳͬͨɻҰൠͷڭՊॻʹੴ ߣϘʔυͷ༠ిυϥΠίϯΫϦʔτͱ΄΅ಉ͡ͱͳ Δεr= 5લޙͱ͍ΘΕ͍ͯΔɻ นಁաϨʔμͳͲͷԠ༻ঢ়گΛ૾͢ΔͱɺนͷްΈ ͱ͔༠ిະͰ͋Δɻ্͔͠͠هͷࣄ࣮Λ༻͍Δ ͱɺ͜ͷະՁతͳ1ݸͷ༠ిମฏ൘ͱͯ͠ܭଌ Ͱ͖ΔՄೳੑ͕͋Δɻͭ·Γɺطͷ༠ిମฏ൘Λนʹ షΓ͚ͯɺషΓ͚લͱൺֱ͢ΕΑ͍͜ͱʹͳΔɻ େ͖ͳ༠ిͱްΈͷͰ͋Δɻ͜Εʹؔ͠؆ ୯ͳߟΛߦ͏ɻ ࠓɺۭؾߟ͑ͳ͍Ͱน͕N ͋Δͱ͢Δɻ֤ͷ ڥքͰෳࡶͳಈͷࣹ͓Αͼ۶ં͕༧ݟ͞ΕΔ͕ɺ ֤ͷૠೖҐ૬Λۙࣅతʹk0√εiziͰ༩͑Δɻεiͱzi i൪ͷͷൺ༠ిͱްΈͰ͋Δɻ͜Εʹ๏ઢ͔Βଌͬ