重力波と干渉計型検出器 山元 一広、ちん たん 東京大学 宇宙線研究所

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2013年8月20日 @東京大学 柏キャンパス 第2総合研究棟 重力波と干渉計型検出器 山元 一広、ちん たん 東京大学 宇宙線研究所 At first, thank you for giving a chance talk here. In fact, I have been in Trento in 2002, eight years ago. I am happy because I can visit here again. OK, shall we start ? This is the title of my talk of today. Gravitational wave and detectors. 千葉県夢チャレンジ体験スクール 2013年8月20日 @東京大学 柏キャンパス 第2総合研究棟

1. 重力波 2. 干渉計型検出器 3. 干渉計 Contents この後実際に干渉計に触れる This is the contents. At first, I explain what gravitational wave is. Next, I will show the aims of detection and outline of detectors. At last, I will give recent results in observation and summarize my talk.

1.重力波 重力とは何か ? 全てのものはお互いに引きつけあう 例えば地球と地球の上にあるもの 手を放すと物は落ちる ニュートンの法則 重力とは何か ? 全てのものはお互いに引きつけあう 例えば地球と地球の上にあるもの 手を放すと物は落ちる ニュートンの法則 So, this is the first section, gravitational wave. But what is it ? I 1915, Albert Einstein finished the construction of his famous theory, General theory of Relativity. According to this theory, gravitation is curvature of space-time. In next year, I mean 1916, he predicted the existence of gravitational wave. This wave is the rippled of space-time. アイザック ニュートン (ウィキペディア 英語版)

1.重力波 重力とは何か ? 1915年 アルバート アインシュタイン : 一般相対性理論 “重力は時空(時間と空間)の曲がりである。 物体によって時空は曲がり、その中を進む 物体の軌道が曲がる。” 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) So, this is the first section, gravitational wave. But what is it ? I 1915, Albert Einstein finished the construction of his famous theory, General theory of Relativity. According to this theory, gravitation is curvature of space-time. In next year, I mean 1916, he predicted the existence of gravitational wave. This wave is the rippled of space-time. アルバート アインシュタイン (ウィキペディア 英語版)

1.重力波 重力波とは何か ? 1916年 アルバート アインシュタイン : 重力波 “重力(時空の曲がり)の源となる物体が 激しい運動などをすると時空のさざなみ(重力波) が光と同じ速さで伝わっていく。” 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) So, this is the first section, gravitational wave. But what is it ? I 1915, Albert Einstein finished the construction of his famous theory, General theory of Relativity. According to this theory, gravitation is curvature of space-time. In next year, I mean 1916, he predicted the existence of gravitational wave. This wave is the rippled of space-time. アルバート アインシュタイン (ウィキペディア 英語版)

1.重力波 重力波とは何か 重力波が画面の垂直方向から来ると…. 重力波とは何か 重力波が画面の垂直方向から来ると…. The speed of gravitational wave is the same as that of light. Moreover, it is transverse wave and has two polarizations as like light. This figure shows the polarizations of gravitational wave. These black dots represent free masses. Let us assume that gravitational wave comes along the line which is perpendicular to this screen. The horizontal axis implies time development. Gravitational wave changes the distance between free masses. If distance between them stretches, this length becomes shorter. After that, length becomes the same as the initial one. Next, this axis shrinks and this axis stretches. This polarization is called plus mode. This is called cross mode. http://spacefiles.blogspot.com

1.重力波 重力波を検出する意義 (1)物理的な意義:一般相対性理論の検証 一般相対論による予言で唯一検証されていないもの “アインシュタインからの最後の宿題” (2)天文学的な意義:重力波天文学の創生 重力波から星や宇宙に関する情報を得る 発生後吸収や散乱されずに地球にやってくる The speed of gravitational wave is the same as that of light. Moreover, it is transverse wave and has two polarizations as like light. This figure shows the polarizations of gravitational wave. These black dots represent free masses. Let us assume that gravitational wave comes along the line which is perpendicular to this screen. The horizontal axis implies time development. Gravitational wave changes the distance between free masses. If distance between them stretches, this length becomes shorter. After that, length becomes the same as the initial one. Next, this axis shrinks and this axis stretches. This polarization is called plus mode. This is called cross mode.

1.重力波 (1)物理的な意義:一般相対性理論の検証 一般相対論による予言で唯一検証されていないもの “アインシュタインからの最後の宿題” スイス、ベルンのアインシュタイン博物館の 一般相対性理論の説明より The speed of gravitational wave is the same as that of light. Moreover, it is transverse wave and has two polarizations as like light. This figure shows the polarizations of gravitational wave. These black dots represent free masses. Let us assume that gravitational wave comes along the line which is perpendicular to this screen. The horizontal axis implies time development. Gravitational wave changes the distance between free masses. If distance between them stretches, this length becomes shorter. After that, length becomes the same as the initial one. Next, this axis shrinks and this axis stretches. This polarization is called plus mode. This is called cross mode.

1.重力波 (2)天文学的な意義:重力波天文学の創生 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) (2)天文学的な意義:重力波天文学の創生 The speed of gravitational wave is the same as that of light. Moreover, it is transverse wave and has two polarizations as like light. This figure shows the polarizations of gravitational wave. These black dots represent free masses. Let us assume that gravitational wave comes along the line which is perpendicular to this screen. The horizontal axis implies time development. Gravitational wave changes the distance between free masses. If distance between them stretches, this length becomes shorter. After that, length becomes the same as the initial one. Next, this axis shrinks and this axis stretches. This polarization is called plus mode. This is called cross mode.

1.重力波 (2)天文学的な意義:重力波天文学の創生 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) (2)天文学的な意義:重力波天文学の創生 The speed of gravitational wave is the same as that of light. Moreover, it is transverse wave and has two polarizations as like light. This figure shows the polarizations of gravitational wave. These black dots represent free masses. Let us assume that gravitational wave comes along the line which is perpendicular to this screen. The horizontal axis implies time development. Gravitational wave changes the distance between free masses. If distance between them stretches, this length becomes shorter. After that, length becomes the same as the initial one. Next, this axis shrinks and this axis stretches. This polarization is called plus mode. This is called cross mode.

1.重力波 未だ重力波直接検出は成功していない 散乱や吸収されない、つまり検出しにくい 間接的な証拠 中性子星連星:非常に重くかつ星としてはコンパクト(10km程度) な2つの星が重心の周りを回転 重力波を放出して一回転に要する時間(周期)が 変わる 観測された周期変化が一般相対論の予言と一致 Unfortunately, the interaction of gravitational wave is too weak. Hertz demonstrated the generation and detection of electromagnetic wave and proved the existence of electromagnetic wave. However, artificial generation of gravitational wave is impossible. But how about astronomical events ? They can emit huge energy. Even in such a case, the gravitational wave is so large. The amplitude of gravitational wave is represented by strain, which is the ratio of change of length to length itself. In optimistic case, this value, h, is the order of 10^(-21). This is comparable with the ratio of diameter of hydrogen atom to distance between Sun and Earth. Up to now, nobody has detected gravitational wave. 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日)

1.重力波 周期の変化の観測と計算値の比較 J.M. Weisberg and J.H. Taylor, Moreover, they do not stop the observation ! This is the results of their 30 years observation. The horizontal axis shows years. This is the year of discovery. This is 2005. The vertical axis represents the change of period. Since the first paper in Nature was published in 1979, paper in Nature only shows this region. However, now, we know the results in wider region. These dots are results of observation. This line is the prediction of general relativity. So, measurement and theory are perfectly consistent with each other. J.M. Weisberg and J.H. Taylor, ASP Conference Series, 328 (2005) 25 (arXiv:astro-ph/0407149). 12 12

1.重力波 1993年度 ノーベル物理学賞 ノーベル財団のウェブ 直接検出目指し(次のノーベル賞?)世界各地で検出器を建設開発中 1993年度 ノーベル物理学賞 ノーベル財団のウェブ So, Hulse and Taylor won the Nobel prize in Physics at 1993. 直接検出目指し(次のノーベル賞?)世界各地で検出器を建設開発中

2. 干渉計型重力波検出器 直接検出目指して:方法はいくつかあるが、干渉計が主流 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) Nevertheless, almost all physicists are sure that gravitational wave exists. Why ? Because indirect detection has already done. In 1975, the paper about discovery of binary pulsar was published. The authors are Hulse and Taylor. Pulsar is a kind of neutron star. Neutron star is a compact object. The diameter is in the order of 10 km. However, the mass is comparable with that of Sun. Binary pulsar consists of two neutron stars. Since compact and heavy objects rotates around their center, this binary generates gravitational wave. It implies that it emits energy. So, the period of binary changes. Hulse and Taylor group observed the period and found that its change agree with theoretical prediction by radiation formula of gravitational wave. The first paper of this topic was published in 1979, Nature.

2.干渉計型重力波検出器 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) どのくらい大変? Unfortunately, the interaction of gravitational wave is too weak. Hertz demonstrated the generation and detection of electromagnetic wave and proved the existence of electromagnetic wave. However, artificial generation of gravitational wave is impossible. But how about astronomical events ? They can emit huge energy. Even in such a case, the gravitational wave is so large. The amplitude of gravitational wave is represented by strain, which is the ratio of change of length to length itself. In optimistic case, this value, h, is the order of 10^(-21). This is comparable with the ratio of diameter of hydrogen atom to distance between Sun and Earth. Up to now, nobody has detected gravitational wave.

2.干渉計型重力波検出器 第1世代:検出できず 第2世代:初検出目指して建設開発が進行中 第3世代:本格的な重力波天文学が花開く So, Hulse and Taylor won the Nobel prize in Physics at 1993. 第3世代:本格的な重力波天文学が花開く 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日)

2.干渉計型重力波検出器 (2)天文学的な意義:重力波天文学の創生 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) The speed of gravitational wave is the same as that of light. Moreover, it is transverse wave and has two polarizations as like light. This figure shows the polarizations of gravitational wave. These black dots represent free masses. Let us assume that gravitational wave comes along the line which is perpendicular to this screen. The horizontal axis implies time development. Gravitational wave changes the distance between free masses. If distance between them stretches, this length becomes shorter. After that, length becomes the same as the initial one. Next, this axis shrinks and this axis stretches. This polarization is called plus mode. This is called cross mode.

2.干渉計型重力波検出器 (2)天文学的な意義:重力波天文学の創生 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) The speed of gravitational wave is the same as that of light. Moreover, it is transverse wave and has two polarizations as like light. This figure shows the polarizations of gravitational wave. These black dots represent free masses. Let us assume that gravitational wave comes along the line which is perpendicular to this screen. The horizontal axis implies time development. Gravitational wave changes the distance between free masses. If distance between them stretches, this length becomes shorter. After that, length becomes the same as the initial one. Next, this axis shrinks and this axis stretches. This polarization is called plus mode. This is called cross mode.

2.干渉計型重力波検出器 第2世代:開発中 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) This is the next section, aim of detection. Nobody has detected gravitational wave directly. However, it has already detected indirectly. What is the motivation for direct detection ? There are two kinds of motivation. The first one is in physics. This is the experimental tests for theory of gravitation. The second motivation is related to astronomy. This is the new window for astronomical observation.

2.干渉計型重力波検出器 日本では… 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) OK, at first, I explain the motivation in physics. The details of experimental check are described in this book by Will. I just introduce two kinds of them. The first check is the measurement of speed of gravitational wave. Alternative theories of gravitation predict the difference of speed between gravitational wave and light. So, the measurement of difference is the test of theory of gravitation.

2.干渉計型重力波検出器 KAGRA 岐阜県の 神岡鉱山内に 建設中 地面振動が 小さい (都市近郊の 1/100) 地下にkm スケールの 干渉計を建設する のは初 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) OK, at first, I explain the motivation in physics. The details of experimental check are described in this book by Will. I just introduce two kinds of them. The first check is the measurement of speed of gravitational wave. Alternative theories of gravitation predict the difference of speed between gravitational wave and light. So, the measurement of difference is the test of theory of gravitation.

2.干渉計型重力波検出器 神岡鉱山 カミオカンデや スーパーカミオカンデで 有名 カミオカンデのリーダー 小柴昌俊:2002年度 ノーベル物理学賞 OK, at first, I explain the motivation in physics. The details of experimental check are described in this book by Will. I just introduce two kinds of them. The first check is the measurement of speed of gravitational wave. Alternative theories of gravitation predict the difference of speed between gravitational wave and light. So, the measurement of difference is the test of theory of gravitation.

2.干渉計型重力波検出器 トンネル掘削中 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) The second test is related to polarization. Alternative theories predict the 6 kinds of polarizations. General relativity predicts only two transverse polarizations, this and this. This polarization shows the uniform stretch and shrink. In this three polarizations, this arrow represents the direction of propagation of gravitational wave. So, this polarization is not transverse mode, but longitudinal one. These two mode are mixture of transverse and longitudinal ones.

2.干渉計型重力波検出器 トンネル掘削中 (体積換算で半分完了) トンネル掘削中 (体積換算で半分完了) The second motivation is for astronomy. The detection of gravitational wave opens the new window, gravitational wave astronomy. There are three categories of gravitational wave sources; burst source, periodic source, stochastic source. 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日)

3. 干渉計 直接検出目指して:方法はいくつかあるが、干渉計が主流 安東正樹 重力波望遠鏡KAGRAで見る新しい宇宙の姿 (東大物理学教室談話会 2013年5月31日) Nevertheless, almost all physicists are sure that gravitational wave exists. Why ? Because indirect detection has already done. In 1975, the paper about discovery of binary pulsar was published. The authors are Hulse and Taylor. Pulsar is a kind of neutron star. Neutron star is a compact object. The diameter is in the order of 10 km. However, the mass is comparable with that of Sun. Binary pulsar consists of two neutron stars. Since compact and heavy objects rotates around their center, this binary generates gravitational wave. It implies that it emits energy. So, the period of binary changes. Hulse and Taylor group observed the period and found that its change agree with theoretical prediction by radiation formula of gravitational wave. The first paper of this topic was published in 1979, Nature.

3.干渉計 マイケルソン干渉計 鏡 ビームスプリッター レーザー光源 鏡 光検出器 OK, let’s start discussion about interferometer on Earth. Gravitational wave can change length difference of two arms of Michelson interferometer. It is supposed that gravitational wave comes along the line which is perpendicular to the screen. When this arm length increase, this arm length decrease. Since the length difference changes, the power at photo detector changes. So, we can detect gravitational wave. The target frequency of interferometer on Earth between 10 Hz and 10 kHz. So, frequency band of interferometer is much wider than that of resonator. 光検出器

3.干渉計 (1)レーザー光源から光が出る 鏡 ビームスプリッター レーザー光源 鏡 光検出器 OK, let’s start discussion about interferometer on Earth. Gravitational wave can change length difference of two arms of Michelson interferometer. It is supposed that gravitational wave comes along the line which is perpendicular to the screen. When this arm length increase, this arm length decrease. Since the length difference changes, the power at photo detector changes. So, we can detect gravitational wave. The target frequency of interferometer on Earth between 10 Hz and 10 kHz. So, frequency band of interferometer is much wider than that of resonator. 光検出器

3.干渉計 (2)ビームスプリッターで分けられてそれぞれの腕を進む 鏡 ビームスプリッター レーザー光源 鏡 光検出器 OK, let’s start discussion about interferometer on Earth. Gravitational wave can change length difference of two arms of Michelson interferometer. It is supposed that gravitational wave comes along the line which is perpendicular to the screen. When this arm length increase, this arm length decrease. Since the length difference changes, the power at photo detector changes. So, we can detect gravitational wave. The target frequency of interferometer on Earth between 10 Hz and 10 kHz. So, frequency band of interferometer is much wider than that of resonator. 光検出器

3.干渉計 (3)鏡で反射されて戻る 鏡 ビームスプリッター レーザー光源 鏡 光検出器 OK, let’s start discussion about interferometer on Earth. Gravitational wave can change length difference of two arms of Michelson interferometer. It is supposed that gravitational wave comes along the line which is perpendicular to the screen. When this arm length increase, this arm length decrease. Since the length difference changes, the power at photo detector changes. So, we can detect gravitational wave. The target frequency of interferometer on Earth between 10 Hz and 10 kHz. So, frequency band of interferometer is much wider than that of resonator. 光検出器

3.干渉計 (4)ビームスプリッタで一部反射、一部透過ののち光検出器もしくは 光源へ 鏡 ビームスプリッター レーザー光源 鏡 光検出器 OK, let’s start discussion about interferometer on Earth. Gravitational wave can change length difference of two arms of Michelson interferometer. It is supposed that gravitational wave comes along the line which is perpendicular to the screen. When this arm length increase, this arm length decrease. Since the length difference changes, the power at photo detector changes. So, we can detect gravitational wave. The target frequency of interferometer on Earth between 10 Hz and 10 kHz. So, frequency band of interferometer is much wider than that of resonator. 光検出器

3.干渉計 特に光検出器に注目すると画面上からの光はビームスプリッターを 透過、右からの光は反射されてくる。 鏡 ビームスプリッター レーザー光源 鏡 OK, let’s start discussion about interferometer on Earth. Gravitational wave can change length difference of two arms of Michelson interferometer. It is supposed that gravitational wave comes along the line which is perpendicular to the screen. When this arm length increase, this arm length decrease. Since the length difference changes, the power at photo detector changes. So, we can detect gravitational wave. The target frequency of interferometer on Earth between 10 Hz and 10 kHz. So, frequency band of interferometer is much wider than that of resonator. 光検出器

3.干渉計 (5)光検出器から光の強さに比例した電流が出る。 鏡 ビームスプリッター レーザー光源 鏡 光検出器 電流 OK, let’s start discussion about interferometer on Earth. Gravitational wave can change length difference of two arms of Michelson interferometer. It is supposed that gravitational wave comes along the line which is perpendicular to the screen. When this arm length increase, this arm length decrease. Since the length difference changes, the power at photo detector changes. So, we can detect gravitational wave. The target frequency of interferometer on Earth between 10 Hz and 10 kHz. So, frequency band of interferometer is much wider than that of resonator. 光検出器 電流

3.干渉計 光検出器に来る光 (1)ビームスプリッターで反射され、 画面上の鏡で反射され、 ビームスプリッターを透過した光 (2)ビームスプリッターを透過し、 画面右の鏡で反射され、 ビームスプリッターで反射された光 OK, let’s start discussion about interferometer on Earth. Gravitational wave can change length difference of two arms of Michelson interferometer. It is supposed that gravitational wave comes along the line which is perpendicular to the screen. When this arm length increase, this arm length decrease. Since the length difference changes, the power at photo detector changes. So, we can detect gravitational wave. The target frequency of interferometer on Earth between 10 Hz and 10 kHz. So, frequency band of interferometer is much wider than that of resonator. 光検出器に来る光 (1)と(2)の足し算 光の干渉

3.干渉計 光検出器に来る光 (1)と(2)の足し算 光の干渉 鏡が動くと… 光のタイミングが ずれて光の量が 変わる 一波長 (1/1000ミリメートル!) の鏡の動きも見逃さない。 OK, let’s start discussion about interferometer on Earth. Gravitational wave can change length difference of two arms of Michelson interferometer. It is supposed that gravitational wave comes along the line which is perpendicular to the screen. When this arm length increase, this arm length decrease. Since the length difference changes, the power at photo detector changes. So, we can detect gravitational wave. The target frequency of interferometer on Earth between 10 Hz and 10 kHz. So, frequency band of interferometer is much wider than that of resonator. http://www.miyazaki-gijutsu.com/series4/densi0713.html

3.干渉計 マイケルソン干渉計:腕の長さの差を精密に測定する装置 両方の鏡が同じ方向にずれても検出できない。 OK, let’s start discussion about interferometer on Earth. Gravitational wave can change length difference of two arms of Michelson interferometer. It is supposed that gravitational wave comes along the line which is perpendicular to the screen. When this arm length increase, this arm length decrease. Since the length difference changes, the power at photo detector changes. So, we can detect gravitational wave. The target frequency of interferometer on Earth between 10 Hz and 10 kHz. So, frequency band of interferometer is much wider than that of resonator.

3.干渉計 重力波とは何か 重力波が画面の垂直方向から来ると…. マイケルソン干渉計の腕の長さの差が変わる。 The speed of gravitational wave is the same as that of light. Moreover, it is transverse wave and has two polarizations as like light. This figure shows the polarizations of gravitational wave. These black dots represent free masses. Let us assume that gravitational wave comes along the line which is perpendicular to this screen. The horizontal axis implies time development. Gravitational wave changes the distance between free masses. If distance between them stretches, this length becomes shorter. After that, length becomes the same as the initial one. Next, this axis shrinks and this axis stretches. This polarization is called plus mode. This is called cross mode. マイケルソン干渉計の腕の長さの差が変わる。  マイケルソン干渉計で重力波を検出できる!

3.干渉計 マイケルソン干渉計をさわってみよう! 注意事項 (1)光をのぞきこまない。 (2)光を反射する鏡、ビームスプリッターにはさわらない。 (I)どういう状態だと干渉するのか? (II)重力波の代わりに手で鏡を動かすと?  (III)重力波の代わりに鏡を音楽にのせて動かすと? The speed of gravitational wave is the same as that of light. Moreover, it is transverse wave and has two polarizations as like light. This figure shows the polarizations of gravitational wave. These black dots represent free masses. Let us assume that gravitational wave comes along the line which is perpendicular to this screen. The horizontal axis implies time development. Gravitational wave changes the distance between free masses. If distance between them stretches, this length becomes shorter. After that, length becomes the same as the initial one. Next, this axis shrinks and this axis stretches. This polarization is called plus mode. This is called cross mode.

おわり That’s all. Thank you for your attention.