WEKO3
アイテム
{"_buckets": {"deposit": "9c84961d-521e-4f34-b922-1950ffbc15d8"}, "_deposit": {"created_by": 1, "id": "8167", "owners": [1], "pid": {"revision_id": 0, "type": "depid", "value": "8167"}, "status": "published"}, "_oai": {"id": "oai:jaxa.repo.nii.ac.jp:00008167", "sets": ["1579", "1891"]}, "author_link": ["45243", "45247", "45245", "45244", "45242", "45246"], "item_5_alternative_title_2": {"attribute_name": "その他のタイトル(英)", "attribute_value_mlt": [{"subitem_alternative_title": "Numerical analysis of energy transmission by phased array lasers"}]}, "item_5_biblio_info_10": {"attribute_name": "書誌情報", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2003-05", "bibliographicIssueDateType": "Issued"}, "bibliographicPageEnd": "85", "bibliographicPageStart": "81", "bibliographic_titles": [{"bibliographic_title": "第22回宇宙エネルギーシンポジウム 平成14年度"}, {"bibliographic_title": "The 22nd ISAS Space Energy Symposium March 12, 2003", "bibliographic_titleLang": "en"}]}]}, "item_5_description_17": {"attribute_name": "抄録(英)", "attribute_value_mlt": [{"subitem_description": "In recent space missions, acquisition of electric power is quite important. Wireless or beaming energy transmissions using a microwave or laser beam have been attracting many interests. Although laser beams are more advantageous in directionality than microwaves, there are mainly two obstacles in constructing a laser transmitter. Firstly, a high power laser beam must be collimated well. Secondly, the high power and lightweight laser facility must be feasible economically. In general, with the increase in power and size of a laser oscillator, it becomes more expensive and difficult to oscillate in a single transverse mode. An arrayed laser is one of the solutions to overcome these obstacles. For the development of an arrayed laser beam system, it is important to know its combined diffraction pattern, and geometric parameters of the array, which strongly influence the pattern, should be optimized. In this paper, a detailed analysis has been performed on coherent combinations of diffraction-limited Gaussian beams. Far-field patterns of rectangular-symmetric arrays were calculated with various geometric parameters such as the number of array elements and the ratio of their pitch to the minimum spot size of an element Delta/w(sub 0). As a result, far-field patterns of arrays were evaluated in terms of a main lobe radius W(sub ML) and an energy fraction of the beam that is contained in the main lobe eta(sub ML). W(sub ML) and eta(sub ML) represent a radius of a receiver and a transmission energy efficiency, respectively. For a constant Delta/w(sub 0), both W(sub ML)/W(sub n) and eta(sub ML) were found insensitive to the number of array elements, where W(sub n) is the radius of a Gaussian beam having emission area equivalent to the array. In other words, a radius of a receiver is independent of the number of array elements but depends on total emission area of the array. This also suggests that an array composed of small diode lasers can be utilized like a large-aperture laser if it has a large total emission area. On the other hand, the dependence on Delta/w(sub 0) was found critical. For any number of array elements, both W(sub ML)/W(sub n) and eta(sub ML) were decreased with Delta/w(sub 0). On the basis of these results, the feasibility of high power energy transmission by phased array lasers has been discussed. 1 GW power can be transmitted from a 5.5 x 5.5 m coherent laser diode array with Delta/w(sub 0) = 2.2 to 11-m-diameter receiver at a distance of 40,000 km with the transmission efficiency of 80 percent. (It was assumed that the transmitter consists of 25,000 x 25,000 laser diodes of the wavelength 808 nm, and the output power of the element laser is 2 W with a 100-micrometer-radius aperture.) If the beams are incoherent, a 200-km-diameter receiver will be required for same conditions. Therefore, coherent combination of laser beams is essential especially for a laser diode array.", "subitem_description_type": "Other"}]}, "item_5_description_32": {"attribute_name": "資料番号", "attribute_value_mlt": [{"subitem_description": "資料番号: AA0045915017", "subitem_description_type": "Other"}]}, "item_5_publisher_8": {"attribute_name": "出版者", "attribute_value_mlt": [{"subitem_publisher": "宇宙科学研究所"}]}, "item_5_publisher_9": {"attribute_name": "出版者(英)", "attribute_value_mlt": [{"subitem_publisher": "The Institute of Space and Astronautical Science (ISAS)"}]}, "item_5_text_20": {"attribute_name": "その他キーワード", "attribute_value_mlt": [{"subitem_text_value": "数値解析"}, {"subitem_text_value": "レーザ、メーザ"}, {"subitem_text_value": "エネルギー生成及び変換"}]}, "item_5_text_35": {"attribute_name": "JAXAカテゴリ", "attribute_value_mlt": [{"subitem_text_value": "JAXAカテゴリ: シンポジウム・研究会"}]}, "item_5_text_36": {"attribute_name": "JAXAカテゴリ2", "attribute_value_mlt": [{"subitem_text_value": "JAXAカテゴリ2: IS"}]}, "item_5_text_42": {"attribute_name": "シンポジウム区分", "attribute_value_mlt": [{"subitem_text_value": "シンポジウム区分: 002"}]}, "item_5_text_43": {"attribute_name": "DSpaceコレクション番号", "attribute_value_mlt": [{"subitem_text_value": "DSpaceコレクション番号: 7"}]}, "item_5_text_6": {"attribute_name": "著者所属", "attribute_value_mlt": [{"subitem_text_value": "東京大学 大学院新領域創成科学研究科"}, {"subitem_text_value": "東京大学 大学院新領域創成科学研究科"}, {"subitem_text_value": "東京大学 大学院工学系研究科"}]}, "item_5_text_7": {"attribute_name": "著者所属(英)", "attribute_value_mlt": [{"subitem_text_language": "en", "subitem_text_value": "University of Tokyo Graduate School of Frontier Sciences"}, {"subitem_text_language": "en", "subitem_text_value": "University of Tokyo Graduate School of Frontier Sciences"}, {"subitem_text_language": "en", "subitem_text_value": "University of Tokyo Graduate School of Engineering"}]}, "item_access_right": {"attribute_name": "アクセス権", "attribute_value_mlt": [{"subitem_access_right": "metadata only access", "subitem_access_right_uri": "http://purl.org/coar/access_right/c_14cb"}]}, "item_creator": {"attribute_name": "著者", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "中川, 樹生"}], "nameIdentifiers": [{"nameIdentifier": "45242", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "小紫, 公也"}], "nameIdentifiers": [{"nameIdentifier": "45243", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "荒川, 義博"}], "nameIdentifiers": [{"nameIdentifier": "45244", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Nakagawa, Tatsuo", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "45245", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Komurasaki, Kimiya", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "45246", "nameIdentifierScheme": "WEKO"}]}, {"creatorNames": [{"creatorName": "Arakawa, Yoshihiro", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "45247", "nameIdentifierScheme": "WEKO"}]}]}, "item_keyword": {"attribute_name": "キーワード", "attribute_value_mlt": [{"subitem_subject": "フェーズドアレイレーザー", "subitem_subject_scheme": "Other"}, {"subitem_subject": "数値解析", "subitem_subject_scheme": "Other"}, {"subitem_subject": "転送効率", "subitem_subject_scheme": "Other"}, {"subitem_subject": "ガラスレーザー", "subitem_subject_scheme": "Other"}, {"subitem_subject": "半導体レーザー", "subitem_subject_scheme": "Other"}, {"subitem_subject": "回折パターン", "subitem_subject_scheme": "Other"}, {"subitem_subject": "コヒーレント光", "subitem_subject_scheme": "Other"}, {"subitem_subject": "光源", "subitem_subject_scheme": "Other"}, {"subitem_subject": "マイクロ波ビーム", "subitem_subject_scheme": "Other"}, {"subitem_subject": "研究開発", "subitem_subject_scheme": "Other"}, {"subitem_subject": "phased array laser", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "numerical analysis", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "transmission efficiency", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "glass laser", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "semiconductor laser", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "diffraction pattern", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "coherent light", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "light source", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "microwave beam", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "research and development", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}]}, "item_language": {"attribute_name": "言語", "attribute_value_mlt": [{"subitem_language": "jpn"}]}, "item_resource_type": {"attribute_name": "資源タイプ", "attribute_value_mlt": [{"resourcetype": "conference paper", "resourceuri": "http://purl.org/coar/resource_type/c_5794"}]}, "item_title": "レーザーアレイによるエネルギー伝送の数値的解析", "item_titles": {"attribute_name": "タイトル", "attribute_value_mlt": [{"subitem_title": "レーザーアレイによるエネルギー伝送の数値的解析"}]}, "item_type_id": "5", "owner": "1", "path": ["1579", "1891"], "permalink_uri": "https://jaxa.repo.nii.ac.jp/records/8167", "pubdate": {"attribute_name": "公開日", "attribute_value": "2015-03-26"}, "publish_date": "2015-03-26", "publish_status": "0", "recid": "8167", "relation": {}, "relation_version_is_last": true, "title": ["レーザーアレイによるエネルギー伝送の数値的解析"], "weko_shared_id": -1}
レーザーアレイによるエネルギー伝送の数値的解析
https://jaxa.repo.nii.ac.jp/records/8167
https://jaxa.repo.nii.ac.jp/records/8167a4cd9e24-1656-489c-9c27-d4d97698e992
Item type | 会議発表論文 / Conference Paper(1) | |||||
---|---|---|---|---|---|---|
公開日 | 2015-03-26 | |||||
タイトル | ||||||
タイトル | レーザーアレイによるエネルギー伝送の数値的解析 | |||||
言語 | ||||||
言語 | jpn | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | フェーズドアレイレーザー | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | 数値解析 | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | 転送効率 | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | ガラスレーザー | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | 半導体レーザー | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | 回折パターン | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | コヒーレント光 | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | 光源 | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | マイクロ波ビーム | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | 研究開発 | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | phased array laser | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | numerical analysis | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | transmission efficiency | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | glass laser | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | semiconductor laser | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | diffraction pattern | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | coherent light | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | light source | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | microwave beam | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | research and development | |||||
資源タイプ | ||||||
資源タイプ識別子 | http://purl.org/coar/resource_type/c_5794 | |||||
資源タイプ | conference paper | |||||
アクセス権 | ||||||
アクセス権 | metadata only access | |||||
アクセス権URI | http://purl.org/coar/access_right/c_14cb | |||||
その他のタイトル(英) | ||||||
その他のタイトル | Numerical analysis of energy transmission by phased array lasers | |||||
著者 |
中川, 樹生
× 中川, 樹生× 小紫, 公也× 荒川, 義博× Nakagawa, Tatsuo× Komurasaki, Kimiya× Arakawa, Yoshihiro |
|||||
著者所属 | ||||||
東京大学 大学院新領域創成科学研究科 | ||||||
著者所属 | ||||||
東京大学 大学院新領域創成科学研究科 | ||||||
著者所属 | ||||||
東京大学 大学院工学系研究科 | ||||||
著者所属(英) | ||||||
en | ||||||
University of Tokyo Graduate School of Frontier Sciences | ||||||
著者所属(英) | ||||||
en | ||||||
University of Tokyo Graduate School of Frontier Sciences | ||||||
著者所属(英) | ||||||
en | ||||||
University of Tokyo Graduate School of Engineering | ||||||
出版者 | ||||||
出版者 | 宇宙科学研究所 | |||||
出版者(英) | ||||||
出版者 | The Institute of Space and Astronautical Science (ISAS) | |||||
書誌情報 |
第22回宇宙エネルギーシンポジウム 平成14年度 en : The 22nd ISAS Space Energy Symposium March 12, 2003 p. 81-85, 発行日 2003-05 |
|||||
抄録(英) | ||||||
内容記述タイプ | Other | |||||
内容記述 | In recent space missions, acquisition of electric power is quite important. Wireless or beaming energy transmissions using a microwave or laser beam have been attracting many interests. Although laser beams are more advantageous in directionality than microwaves, there are mainly two obstacles in constructing a laser transmitter. Firstly, a high power laser beam must be collimated well. Secondly, the high power and lightweight laser facility must be feasible economically. In general, with the increase in power and size of a laser oscillator, it becomes more expensive and difficult to oscillate in a single transverse mode. An arrayed laser is one of the solutions to overcome these obstacles. For the development of an arrayed laser beam system, it is important to know its combined diffraction pattern, and geometric parameters of the array, which strongly influence the pattern, should be optimized. In this paper, a detailed analysis has been performed on coherent combinations of diffraction-limited Gaussian beams. Far-field patterns of rectangular-symmetric arrays were calculated with various geometric parameters such as the number of array elements and the ratio of their pitch to the minimum spot size of an element Delta/w(sub 0). As a result, far-field patterns of arrays were evaluated in terms of a main lobe radius W(sub ML) and an energy fraction of the beam that is contained in the main lobe eta(sub ML). W(sub ML) and eta(sub ML) represent a radius of a receiver and a transmission energy efficiency, respectively. For a constant Delta/w(sub 0), both W(sub ML)/W(sub n) and eta(sub ML) were found insensitive to the number of array elements, where W(sub n) is the radius of a Gaussian beam having emission area equivalent to the array. In other words, a radius of a receiver is independent of the number of array elements but depends on total emission area of the array. This also suggests that an array composed of small diode lasers can be utilized like a large-aperture laser if it has a large total emission area. On the other hand, the dependence on Delta/w(sub 0) was found critical. For any number of array elements, both W(sub ML)/W(sub n) and eta(sub ML) were decreased with Delta/w(sub 0). On the basis of these results, the feasibility of high power energy transmission by phased array lasers has been discussed. 1 GW power can be transmitted from a 5.5 x 5.5 m coherent laser diode array with Delta/w(sub 0) = 2.2 to 11-m-diameter receiver at a distance of 40,000 km with the transmission efficiency of 80 percent. (It was assumed that the transmitter consists of 25,000 x 25,000 laser diodes of the wavelength 808 nm, and the output power of the element laser is 2 W with a 100-micrometer-radius aperture.) If the beams are incoherent, a 200-km-diameter receiver will be required for same conditions. Therefore, coherent combination of laser beams is essential especially for a laser diode array. | |||||
資料番号 | ||||||
内容記述タイプ | Other | |||||
内容記述 | 資料番号: AA0045915017 |