ログイン
言語:

WEKO3

  • トップ
  • ランキング
To
lat lon distance
To

Field does not validate



インデックスリンク

インデックスツリー

メールアドレスを入力してください。

WEKO

One fine body…

WEKO

One fine body…

アイテム

{"_buckets": {"deposit": "c5c51168-85a5-415b-bbe6-f7ffadb3850d"}, "_deposit": {"created_by": 21, "id": "4065", "owners": [21], "pid": {"revision_id": 0, "type": "depid", "value": "4065"}, "status": "published"}, "_oai": {"id": "oai:ir.soken.ac.jp:00004065", "sets": ["16"]}, "author_link": ["2244", "2246", "2245"], "item_1_biblio_info_21": {"attribute_name": "書誌情報(ソート用)", "attribute_value_mlt": [{"bibliographicIssueDates": {"bibliographicIssueDate": "2013-03-31", "bibliographicIssueDateType": "Issued"}, "bibliographic_titles": [{}]}]}, "item_1_creator_2": {"attribute_name": "著者名", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "岡澤, 晋"}], "nameIdentifiers": [{"nameIdentifier": "2244", "nameIdentifierScheme": "WEKO"}]}]}, "item_1_creator_3": {"attribute_name": "フリガナ", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "オカザワ, ススム"}], "nameIdentifiers": [{"nameIdentifier": "2245", "nameIdentifierScheme": "WEKO"}]}]}, "item_1_date_granted_11": {"attribute_name": "学位授与年月日", "attribute_value_mlt": [{"subitem_dategranted": "2013-03-22"}]}, "item_1_degree_grantor_5": {"attribute_name": "学位授与機関", "attribute_value_mlt": [{"subitem_degreegrantor": [{"subitem_degreegrantor_name": "総合研究大学院大学"}]}]}, "item_1_degree_name_6": {"attribute_name": "学位名", "attribute_value_mlt": [{"subitem_degreename": "博士(理学)"}]}, "item_1_description_1": {"attribute_name": "ID", "attribute_value_mlt": [{"subitem_description": "2013020", "subitem_description_type": "Other"}]}, "item_1_description_12": {"attribute_name": "要旨", "attribute_value_mlt": [{"subitem_description": "We examine non-equilibrium aspects of the black hole thermodynamics by applying the non-equilibrium fluctuation theorems developed in the statistical physics. In particular, we consider a scalar field in a black hole background.\nWe derive the stochastic equations, i.e. the Langevin equation and the Fokker-Planck equations for a scalar field in a black hole background within the 0→ limit with the Hawking temperature πκ2/ fixed. By applying the fluctuation theorems to these effective equations of motion, we can derive the generalized second law of black hole thermodynamics, a linear response theorem of an energy flow and its non-linear generalizations as corollaries. We further investigate quantum corrections of the membrane paradigm.\nWe introduce infinitely many variables between the horizon and the stretched horizon and consider them as environmental variables. By integrating them, we can show that the variable at the stretched horizon behaves stochastically with a noise term. Though the environmental variables are living outside of the horizon, they can encode information in the black hole through choosing the Kruskal vacuum with the regularity condition at the horizon. In this sense, the integration of the environmental variables corresponds to integrating hidden variables in the horizon.\nThe system of the scalar field behaves stochastically due to the absorption of energy into the black hole and emission of the Hawking radiation from the black hole horizon. The dissipation comes from the classical causal property of the horizon; the black hole horizon absorbs matter and, once they fall in, they cannot come out. On the other hand, the noise term comes from the Hawking radiation, which is essentially quantum mechanical and, hence, we need to quantize the system in a black hole background in an appropriate way.\nThe thesis is organized as follows. In section 2, we briefly review the stochastic approach to thermodynamic systems, the Langevin equation and the Fokker-Planck equation. An important property of the stochastic equation is that it violates the time reversal symmetry which can be measured by an entropy increase in the path integral. In the next section 3, the fluctuation theorem for a stochastic system is reviewed. It relates the entropy increasing and decreasing probabilities. From the fluctuation theorem, the Jarzynski equality is derived. In addition, we explain the fluctuation theorem for a steady state and derivations of non-linear generalizations of the Green-Kubo formula. In section 4, we derive an effective stochastic equation of a scalar field in a black hole background. In\nderiving the Langevin equation, the quantum property of the vacuum with the regularity condition at the horizon is very important, which is first explained. We then introduce a set of discretized equations of a scalar field near the black hole horizon, and integrate the variables between the horizon and the stretched horizon. The integration leads to an effective stochastic equation for a variable at the stretched horizon. This has the same spirit as deriving a Langevin equation of a system in contact with a thermal bath. In section 5, we apply the fluctuation theorem to a scalar field in a black hole background. We consider two different situations. In the first case, we put a scalar field and a black hole in a box with an insulating wall. By applying the fluctuation theorem, we can derive a relation connecting entropy decreasing probabilities with increasing ones. From this, the generalized second law of black hole thermodynamics can be derived. In the second case, the wall is assumed to be in contact with a thermal bath of a different temperature which is slightly lower than the Hawking temperature of the black hole. Then there is an energy flow from the black hole to the wall. By applying the steady state fluctuation theorem to it, a linear response theorem of an energy flow to the temperature difference and its non-linear generalizations can be obtained. In section 6, we extend the idea of the membrane paradigm. The equations of the classical membrane paradigm are essentially determined by the regularity condition. We further put the effect of the Hawking radiation to it.\nIn the appendix A, we review a derivation of the path integral form of the Fokker-Planck equation. In the appendix B, we review an example of the exact solution of the Fokker-Planck equation. In the appendix C, we will discuss the relation between the noise correlation and the flux of the Hawking radiation.", "subitem_description_type": "Other"}]}, "item_1_description_7": {"attribute_name": "学位記番号", "attribute_value_mlt": [{"subitem_description": "総研大甲第1588号 ", "subitem_description_type": "Other"}]}, "item_1_select_14": {"attribute_name": "所蔵", "attribute_value_mlt": [{"subitem_select_item": "有"}]}, "item_1_select_16": {"attribute_name": "複写", "attribute_value_mlt": [{"subitem_select_item": "全文公開可"}]}, "item_1_select_17": {"attribute_name": "公開状況", "attribute_value_mlt": [{"subitem_select_item": "application/pdf"}]}, "item_1_select_8": {"attribute_name": "研究科", "attribute_value_mlt": [{"subitem_select_item": "高エネルギー加速器科学研究科"}]}, "item_1_select_9": {"attribute_name": "専攻", "attribute_value_mlt": [{"subitem_select_item": "14 素粒子原子核専攻"}]}, "item_1_text_10": {"attribute_name": "学位授与年度", "attribute_value_mlt": [{"subitem_text_value": "2012"}]}, "item_creator": {"attribute_name": "著者", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "OKAZAWA, Susumu ", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "2246", "nameIdentifierScheme": "WEKO"}]}]}, "item_files": {"attribute_name": "ファイル情報", "attribute_type": "file", "attribute_value_mlt": [{"accessrole": "open_date", "date": [{"dateType": "Available", "dateValue": "2016-02-26"}], "displaytype": "simple", "download_preview_message": "", "file_order": 0, "filename": "甲1588_要旨.pdf", "filesize": [{"value": "261.7 kB"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_11", "mimetype": "application/pdf", "size": 261700.0, "url": {"label": "要旨・審査要旨", "url": "https://ir.soken.ac.jp/record/4065/files/甲1588_要旨.pdf"}, "version_id": "6aefab81-d097-4366-a605-af15e0bba766"}, {"accessrole": "open_date", "date": [{"dateType": "Available", "dateValue": "2016-02-17"}], "displaytype": "simple", "download_preview_message": "", "file_order": 1, "filename": "甲1588_本文.pdf", "filesize": [{"value": "526.5 kB"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_11", "mimetype": "application/pdf", "size": 526500.0, "url": {"label": "本文", "url": "https://ir.soken.ac.jp/record/4065/files/甲1588_本文.pdf"}, "version_id": "b4fbbdc4-8254-4517-a3d6-140ed2a05531"}]}, "item_language": {"attribute_name": "言語", "attribute_value_mlt": [{"subitem_language": "eng"}]}, "item_resource_type": {"attribute_name": "資源タイプ", "attribute_value_mlt": [{"resourcetype": "thesis", "resourceuri": "http://purl.org/coar/resource_type/c_46ec"}]}, "item_title": "Non-equilibrium Aspects of the Black Hole Thermodynamics", "item_titles": {"attribute_name": "タイトル", "attribute_value_mlt": [{"subitem_title": "Non-equilibrium Aspects of the Black Hole Thermodynamics"}, {"subitem_title": "Non-equilibrium Aspects of the Black Hole Thermodynamics", "subitem_title_language": "en"}]}, "item_type_id": "1", "owner": "21", "path": ["16"], "permalink_uri": "https://ir.soken.ac.jp/records/4065", "pubdate": {"attribute_name": "公開日", "attribute_value": "2013-11-15"}, "publish_date": "2013-11-15", "publish_status": "0", "recid": "4065", "relation": {}, "relation_version_is_last": true, "title": ["Non-equilibrium Aspects of the Black Hole Thermodynamics"], "weko_shared_id": 21}
  1. 020 学位論文
  2. 高エネルギー加速器科学研究科
  3. 14 素粒子原子核専攻

Non-equilibrium Aspects of the Black Hole Thermodynamics

https://ir.soken.ac.jp/records/4065
https://ir.soken.ac.jp/records/4065
22705dd0-517d-4307-a916-411fc79d6f16
名前 / ファイル ライセンス アクション
甲1588_要旨.pdf 要旨・審査要旨 (261.7 kB)
甲1588_本文.pdf 本文 (526.5 kB)
Item type 学位論文 / Thesis or Dissertation(1)
公開日 2013-11-15
タイトル
タイトル Non-equilibrium Aspects of the Black Hole Thermodynamics
タイトル
言語 en
タイトル Non-equilibrium Aspects of the Black Hole Thermodynamics
言語
言語 eng
資源タイプ
資源タイプ識別子 http://purl.org/coar/resource_type/c_46ec
資源タイプ thesis
著者名 岡澤, 晋

× 岡澤, 晋

WEKO 2244

岡澤, 晋

Search repository
フリガナ オカザワ, ススム

× オカザワ, ススム

WEKO 2245

オカザワ, ススム

Search repository
著者 OKAZAWA, Susumu

× OKAZAWA, Susumu

WEKO 2246

en OKAZAWA, Susumu

Search repository
学位授与機関
学位授与機関名 総合研究大学院大学
学位名
学位名 博士(理学)
学位記番号
内容記述タイプ Other
内容記述 総研大甲第1588号
研究科
値 高エネルギー加速器科学研究科
専攻
値 14 素粒子原子核専攻
学位授与年月日
学位授与年月日 2013-03-22
学位授与年度
2012
要旨
内容記述タイプ Other
内容記述 We examine non-equilibrium aspects of the black hole thermodynamics by applying the non-equilibrium fluctuation theorems developed in the statistical physics. In particular, we consider a scalar field in a black hole background.
We derive the stochastic equations, i.e. the Langevin equation and the Fokker-Planck equations for a scalar field in a black hole background within the 0→ limit with the Hawking temperature πκ2/ fixed. By applying the fluctuation theorems to these effective equations of motion, we can derive the generalized second law of black hole thermodynamics, a linear response theorem of an energy flow and its non-linear generalizations as corollaries. We further investigate quantum corrections of the membrane paradigm.
We introduce infinitely many variables between the horizon and the stretched horizon and consider them as environmental variables. By integrating them, we can show that the variable at the stretched horizon behaves stochastically with a noise term. Though the environmental variables are living outside of the horizon, they can encode information in the black hole through choosing the Kruskal vacuum with the regularity condition at the horizon. In this sense, the integration of the environmental variables corresponds to integrating hidden variables in the horizon.
The system of the scalar field behaves stochastically due to the absorption of energy into the black hole and emission of the Hawking radiation from the black hole horizon. The dissipation comes from the classical causal property of the horizon; the black hole horizon absorbs matter and, once they fall in, they cannot come out. On the other hand, the noise term comes from the Hawking radiation, which is essentially quantum mechanical and, hence, we need to quantize the system in a black hole background in an appropriate way.
The thesis is organized as follows. In section 2, we briefly review the stochastic approach to thermodynamic systems, the Langevin equation and the Fokker-Planck equation. An important property of the stochastic equation is that it violates the time reversal symmetry which can be measured by an entropy increase in the path integral. In the next section 3, the fluctuation theorem for a stochastic system is reviewed. It relates the entropy increasing and decreasing probabilities. From the fluctuation theorem, the Jarzynski equality is derived. In addition, we explain the fluctuation theorem for a steady state and derivations of non-linear generalizations of the Green-Kubo formula. In section 4, we derive an effective stochastic equation of a scalar field in a black hole background. In
deriving the Langevin equation, the quantum property of the vacuum with the regularity condition at the horizon is very important, which is first explained. We then introduce a set of discretized equations of a scalar field near the black hole horizon, and integrate the variables between the horizon and the stretched horizon. The integration leads to an effective stochastic equation for a variable at the stretched horizon. This has the same spirit as deriving a Langevin equation of a system in contact with a thermal bath. In section 5, we apply the fluctuation theorem to a scalar field in a black hole background. We consider two different situations. In the first case, we put a scalar field and a black hole in a box with an insulating wall. By applying the fluctuation theorem, we can derive a relation connecting entropy decreasing probabilities with increasing ones. From this, the generalized second law of black hole thermodynamics can be derived. In the second case, the wall is assumed to be in contact with a thermal bath of a different temperature which is slightly lower than the Hawking temperature of the black hole. Then there is an energy flow from the black hole to the wall. By applying the steady state fluctuation theorem to it, a linear response theorem of an energy flow to the temperature difference and its non-linear generalizations can be obtained. In section 6, we extend the idea of the membrane paradigm. The equations of the classical membrane paradigm are essentially determined by the regularity condition. We further put the effect of the Hawking radiation to it.
In the appendix A, we review a derivation of the path integral form of the Fokker-Planck equation. In the appendix B, we review an example of the exact solution of the Fokker-Planck equation. In the appendix C, we will discuss the relation between the noise correlation and the flux of the Hawking radiation.
所蔵
値 有
戻る
0
views
See details
Views

Versions

Ver.1 2023-06-20 15:15:56.777052
Show All versions

Share

Mendeley Twitter Facebook Print Addthis

Cite as

エクスポート

OAI-PMH
  • OAI-PMH JPCOAR
  • OAI-PMH DublinCore
  • OAI-PMH DDI
Other Formats
  • JSON
  • BIBTEX

Confirm


Powered by WEKO3


Powered by WEKO3