JP2005195382A - Method and apparatus for generating and irradiating terahertz electromagnetic wave - Google Patents
Method and apparatus for generating and irradiating terahertz electromagnetic wave Download PDFInfo
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- 230000001678 irradiating effect Effects 0.000 title claims abstract description 7
- 238000000034 method Methods 0.000 title claims abstract description 7
- 239000000523 sample Substances 0.000 claims abstract description 25
- 239000013078 crystal Substances 0.000 claims abstract description 24
- 239000000835 fiber Substances 0.000 claims abstract description 18
- 235000013305 food Nutrition 0.000 abstract description 6
- 230000008878 coupling Effects 0.000 abstract description 3
- 238000010168 coupling process Methods 0.000 abstract description 3
- 238000005859 coupling reaction Methods 0.000 abstract description 3
- 239000000126 substance Substances 0.000 abstract 1
- 239000002184 metal Substances 0.000 description 10
- 238000007689 inspection Methods 0.000 description 5
- 230000003287 optical effect Effects 0.000 description 4
- 230000010287 polarization Effects 0.000 description 4
- 229910005543 GaSe Inorganic materials 0.000 description 3
- 238000005259 measurement Methods 0.000 description 3
- 206010028980 Neoplasm Diseases 0.000 description 2
- 239000004698 Polyethylene Substances 0.000 description 2
- XUIMIQQOPSSXEZ-UHFFFAOYSA-N Silicon Chemical compound [Si] XUIMIQQOPSSXEZ-UHFFFAOYSA-N 0.000 description 2
- 210000005252 bulbus oculi Anatomy 0.000 description 2
- 201000011510 cancer Diseases 0.000 description 2
- 230000001427 coherent effect Effects 0.000 description 2
- 238000001514 detection method Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- ZZEMEJKDTZOXOI-UHFFFAOYSA-N digallium;selenium(2-) Chemical compound [Ga+3].[Ga+3].[Se-2].[Se-2].[Se-2] ZZEMEJKDTZOXOI-UHFFFAOYSA-N 0.000 description 2
- -1 polyethylene Polymers 0.000 description 2
- 229920000573 polyethylene Polymers 0.000 description 2
- 229910052710 silicon Inorganic materials 0.000 description 2
- 239000010703 silicon Substances 0.000 description 2
- 229910013641 LiNbO 3 Inorganic materials 0.000 description 1
- 230000005856 abnormality Effects 0.000 description 1
- 210000003323 beak Anatomy 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 230000007547 defect Effects 0.000 description 1
- 239000003365 glass fiber Substances 0.000 description 1
- 239000012535 impurity Substances 0.000 description 1
- 239000004033 plastic Substances 0.000 description 1
- 229920003023 plastic Polymers 0.000 description 1
- 239000004065 semiconductor Substances 0.000 description 1
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- G01N21/35—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light
- G01N21/3581—Investigating relative effect of material at wavelengths characteristic of specific elements or molecules, e.g. atomic absorption spectrometry using infrared light using far infrared light; using Terahertz radiation
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Abstract
Description
本発明はレーザ光源を使ったテラヘルツ帯コヒーレント電磁波発生照射方法及び装置に関する。 The present invention relates to a terahertz band coherent electromagnetic wave generation irradiation method and apparatus using a laser light source.
波長可変レーザを用いて誘電体LiNbO3や半導体GaP結晶などのテラヘルツ電磁波発生用結晶から周波数可変で単一周波数のコヒーレントテラヘルツを発生させることが可能となり、これらをテラヘルツ光源として、生体分子の同定、食品の検査、ガン細胞の検出、IC部品検査などに役立てることができる。すなわち、生体やがん細胞のテラヘルツ共振周波数にあわせて、検体のテラヘルツ帯画像を得る。このため、テラヘルツ電磁波ビームを局所的に照射し、検体を乗せたステージを移動させることにより画像を得ている。Using a wavelength tunable laser, it becomes possible to generate a single-frequency coherent terahertz with a variable frequency from a terahertz electromagnetic wave generating crystal such as a dielectric LiNbO 3 or a semiconductor GaP crystal, and using these as a terahertz light source, It can be used for food inspection, cancer cell detection, IC component inspection, and the like. That is, a terahertz band image of the specimen is obtained in accordance with the terahertz resonance frequency of the living body or cancer cell. For this reason, an image is obtained by locally irradiating a terahertz electromagnetic wave beam and moving the stage on which the specimen is placed.
しかし、店舗内の食品検査や、人体の皮膚、眼球の検査、口内検査などはステージ上の検体を用いての検査ではなく、テラヘルツ波を発生し,受光する携帯可能なプローブを棚の上に置かれている食品に近づけて、あるいは患者の皮膚の患部などに近づけて測定する必要があるがまだこのような携帯可能なテラヘルツ電磁波プローブは知られていない。 However, in-store food inspections, human skin and eyeball inspections, and oral inspections are not performed using specimens on the stage, but a portable probe that generates and receives terahertz waves is placed on the shelf. Although it is necessary to perform measurement close to the food that is placed or close to the affected area of the patient's skin, such a portable terahertz electromagnetic wave probe is not yet known.
従来の画像を得る方法ではポンプ光源として用いるYAGレーザ、信号光源として用いるオプティカルパラメトリックオシレータ(OPO)などは防振台上に置かれたレンズとミラを用いてテラヘルツ電磁波発生用結晶に照射され、二つのレーザの差周波数を有するテラヘルツ電磁波を得ていた。 In a conventional method of obtaining an image, a YAG laser used as a pump light source, an optical parametric oscillator (OPO) used as a signal light source, and the like are irradiated onto a terahertz electromagnetic wave generating crystal using a lens and a mirror placed on a vibration isolator. A terahertz electromagnetic wave having a difference frequency of two lasers was obtained.
また、テラヘルツ電磁波発生用結晶としてGaPを使った場合、二つの入射光の間の微小な角度整合部、出力テラヘルツ波の集光用法物面鏡、テラヘルツ電磁波検出用シリコンボロメータなどで構成され数十cm以上の大きさと微妙な光学系からできていたために定盤上に置かなければならず、携帯は困難であった。 In addition, when GaP is used as a crystal for generating terahertz electromagnetic waves, it consists of a fine angle matching part between two incident lights, a normal mirror for condensing output terahertz waves, a silicon bolometer for detecting terahertz electromagnetic waves, etc. It was difficult to carry because it had to be placed on a surface plate because of its size of more than cm and a delicate optical system.
本発明はこれらの欠点を除き、携帯可能な、小型かつ堅牢で、人の手によって移動させて計測することをを可能にするテラヘルツ電磁波発生照射方法及び装置を提供する。 The present invention eliminates these drawbacks and provides a terahertz electromagnetic wave generating and irradiating method and apparatus that are portable, small and robust, and can be moved and measured by a human hand.
ポンプ光レーザ、信号光レーザはいずれもファイバ結合型にする。波長可変Ybドープファイバレーザ(波長可変範囲1.03μm−1.11μm)はレーザ自体がガラスファイバで構成されており、最適なレーザ光源の一つである。ポンプ光源、信号光源がファイバ結合でない場合はレンズを使ってファイバに導入する。ポンプ光と信号光は通常偏光方向が互いに垂直である。ファイバ入出力型の偏光ビームコンバイナーを使って2つのファイバ出力を1つのファイバ出力へと変換し、テラヘルツ波発生照射部分、すなわちテラヘルツプローブに導入する。 Both the pump light laser and the signal light laser are of the fiber coupling type. The wavelength tunable Yb-doped fiber laser (wavelength tunable range: 1.03 μm to 1.11 μm) is one of the optimum laser light sources because the laser itself is made of glass fiber. If the pump light source and signal light source are not fiber coupled, they are introduced into the fiber using a lens. The polarization directions of the pump light and the signal light are usually perpendicular to each other. Using a fiber input / output type polarization beam combiner, two fiber outputs are converted into one fiber output and introduced into a terahertz wave generating irradiation portion, that is, a terahertz probe.
ポンプ光及び信号光はファイバ先端から放出し直径5mm以下の小型レンズで平行ビームに変換される。直径1mm程度の平行ビームに変換されたポンプ光と信号光はビーム径に見合う小型のテラヘルツ電磁波発生用結晶に導かれほぼ前方方向にテラヘルツ波を発生する。発生したテラヘルツ電磁波は方物面鏡を使わずに直ちにテーパ型金属導波管に導きプローブの先端からテラヘルツ電磁波を放出する。 Pump light and signal light are emitted from the fiber tip and converted into parallel beams by a small lens having a diameter of 5 mm or less. The pump light and the signal light converted into a parallel beam having a diameter of about 1 mm are guided to a small terahertz electromagnetic wave generating crystal corresponding to the beam diameter to generate a terahertz wave in a substantially forward direction. The generated terahertz electromagnetic wave is immediately guided to the tapered metal waveguide without using a plane mirror, and the terahertz electromagnetic wave is emitted from the tip of the probe.
金属導波管の代わりに、ポリエチレンやシリコンでできたレンズを使ってもよい。上記の光学コンポネントである、平行ビーム形成用のレンズ、テラヘルツ電磁波発生用結晶、金属導波管はテラヘルツプローブの軸線から20度以内に配置されているためプローブは携帯に適当な細長い形状を有している。これらのコンポネントは通常のマウントを用いず、一個の金属あるいはプラスティック架台に固着してあり、堅牢であり、携帯移動によって位置ずれを生じない。 A lens made of polyethylene or silicon may be used instead of the metal waveguide. The above-mentioned optical components such as a parallel beam forming lens, a terahertz electromagnetic wave generating crystal, and a metal waveguide are disposed within 20 degrees from the axis of the terahertz probe, so that the probe has an elongated shape suitable for carrying. ing. These components do not use a normal mount, are fixed to a single metal or plastic mount, are robust, and do not shift in position due to mobile movement.
テラヘルツ電磁波を対象とする検体にテラヘルツ電磁波を照射するにはこのプローブを検体に近づけ、検体からの反射テラヘルツ波をおなじ金属導波管へと導き、ビームスプリッタを介して室温で動作するテラヘルツ波検知器に導き反射波強度を計測する。テラヘルツプローブはファイバ結合でポンプ光源、信号光源に接続されているのでポンプ光源、信号光源に対して自由に動かすことが可能である。 In order to irradiate a terahertz electromagnetic wave to a specimen that targets terahertz electromagnetic waves, this probe is brought close to the specimen, the reflected terahertz wave from the specimen is guided to the same metal waveguide, and the terahertz wave that operates at room temperature via a beam splitter is detected. Measure the intensity of the reflected wave. Since the terahertz probe is connected to the pump light source and the signal light source by fiber coupling, the terahertz probe can be freely moved with respect to the pump light source and the signal light source.
本発明によればテラヘルツ波を発生照射検知する部分、すなわちテラヘルツプローブは自由に動かすことができるので、これを携帯して店舗などで食品類に近づけ、あるいは病院において人の皮膚や眼球、口内患部に近づけて、テラヘルツ波を照射し、その反射波強度をおなじプローブで室温で検出できる。これによって、食品の腐敗や、不純物の添加状態、人体皮膚その他の異常を検出することができる。 According to the present invention, the terahertz wave generating and detecting part, that is, the terahertz probe can be moved freely, so that it can be carried close to foods at a store or the like, or a human skin, eyeball, or affected area in the mouth in a hospital The terahertz wave is irradiated close to, and the reflected wave intensity can be detected at room temperature with the same probe. As a result, it is possible to detect food spoilage, the state of added impurities, human skin and other abnormalities.
図1において、二つのファイバ1,2内をそれぞれ伝送されてきたポンプ光と信号光の互いに直交する偏波方向を持つビームを、ファイバ入出力型偏光ビームコンバイナ3を使って1本のファイバ内ビーム4に結合し、細長いテラヘルツプローブ筐体5の末端にある入力端から導入し、直径5mm以下の小型レンズ6によって直径1mm程度の平行ビー厶に変換される。立体状の偏光子7によって互いに垂直な偏光に分離させ、直角プリズム7、偏光子8によって再び二つのビームを結合する。そのビームをテラヘルツ波発生用GaP結晶10に導入する。GaP結晶においてはポンプ光が1.0μmより長波長の場合微小な角度整合が必要である。二つのビームのなす角はテラヘルツ波周波数に比例的に増大するがいずれにしろ微小であり、3THzで35min.程度である。この微小角度を発生させるために偏光子8を所定の微小角度回転させる。偏光子8を極めて小型の回転ステージに乗せれば任意のテラヘルツ周波数で測定できるが、測定周波数があらかじめ分かつている場合はステージを使わないで固定角度を与えることでもよい。他の光学素子及び結晶は全てプローブ筐体に接着あるいはネジ締めにより固定されており、ミラホルダのような大型とならざるを得ないホルダ類は使用していない。 In FIG. 1, a beam having a polarization direction orthogonal to each other of pump light and signal light transmitted through two
一方、位相整合されたテラヘルツ波の発生方向は結晶内で10−20度程度であり、周波数に大きく依存しない。この角度は結晶外に出ると屈折率比だけ大きくなるから、40−60度にも達する。その結果、テラヘルツ波用方物面鏡が複数個必要となり、小型化の障害となる、そこで、これを避けるため、結晶の入力面を図1に示したように出力面にたいして10−20度あらかじめ傾け、その方向から結晶に入射すると、テラヘルツ波ビームは出力面に垂直に近い方向に平行に近いビーム状に出射する。これを図1のように金属導波管11で伝送し、先端の細くしたプローブ先端部分12を検体部分17に近づけてテラヘルツ波を照射する。検体から反射した、テラヘルツ波は再びプローブ先端からビームスプリッタ13を介して室温検知素子DTGSに入射する。発生した電気信号は信号線を通って外部に取り出されるがこの部分は図1では省略してある。筐体は長さ10−20cm,幅5cm、高さ1cm程度であり、携帯することが可能である。 On the other hand, the generation direction of the phase-matched terahertz wave is about 10 to 20 degrees in the crystal and does not greatly depend on the frequency. Since this angle increases by the refractive index ratio when it goes out of the crystal, it reaches 40-60 degrees. As a result, a plurality of terahertz wave plane mirrors are required, which is an obstacle to miniaturization. Therefore, in order to avoid this, the crystal input surface is 10-20 degrees in advance with respect to the output surface as shown in FIG. When tilted and incident on the crystal from that direction, the terahertz wave beam is emitted in a beam shape that is nearly parallel to a direction that is nearly perpendicular to the output surface. This is transmitted through the
テラヘルツ波発生用結晶として複屈折性結晶GaSeを使うと図2のようにポンプ光と信号光、及び発生するテラヘウルツ波は互いに平行となる、この場合、位相整合はGaSe結晶12の複屈折性を利用しておこなわれ、図2ように結晶を垂直入射から傾けることによって行われる。この角度はテラヘルツ周波数によってきまり、最大40度程度である。測定する周波数があらかじめ決まっているときは所定の角度に固定するが周波数をチューニングする必要があるときは小型の回転ステージ上に乗せなければならない。結晶から出たポンプ光と信号光は金属導波管の途中または入り口に設けられたGeやブラックポリエチレンでできた近赤外線フィルタで除去される。出力側の構成は、その他については実施例1と同じである。 When the birefringent crystal GaSe is used as the terahertz wave generating crystal, the pump light and the signal light and the generated terahertz wave are parallel to each other as shown in FIG. 2. In this case, the phase matching causes the birefringence of the
実施例2は実施例1よりコンポネントの数が少ないのでより小型であるが、GaPを使った実施例1に比べてGaSeを使うと出力が充分高くない、また、周波数範囲がGaPの場合最大0.3THz−7THzに対して、GaSeの場合0.3THz−5THzと、より狭い範囲になるという欠点があるので目的によって両者を使い分ける。 The second embodiment is smaller than the first embodiment because the number of components is smaller, but the output is not sufficiently high when using GaSe compared to the first embodiment using GaP, and the maximum is 0 when the frequency range is GaP. In contrast to 3 THz-7 THz, GaSe has a defect of 0.3 THz-5 THz, which is a narrower range.
1…ポンプ光を伝送するファイバ
2…信号光を伝送するファイバ
3…ビームコンバイナ
4…ポンプ光と信号光を伝送するファイバ
5…テラヘルツプローブ筐体
6…小型レンズ
7、8…キュービック偏光子
9…直角プリズム
10…GaP結晶
11…金属導波管
12…金属導波管テーパ部
13…ビームスプリッタ
14…反射テラヘルツ波ビーム
15…金属導波管
16…検知器
17…検体
18…GaSe結晶
19…近赤外線カットフィルタDESCRIPTION OF
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