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Two kinds of systems have been investigated. One is with a tree-level \ngluon propagator (model A) and the other is with the lattice-QCD based (LQB) gluon \npropagator (model B). We have found that 2¢T =0 =3:43kBTc in model B (¢:energy \n\np=pF \ngap, kB:Boltzmann constant, Tc:critical temperature). This value is very close to the \nfamous BCS result, which is 2Δ = 3:52kBTc. We have found that the coherence length \n(´) is not affected by T in 2SC, while Δ decreases as T increases and vanishes at Tc. In \naddition, we have found that the Cooper pair wave function c(p) is not affected by T , \napart from normalization constant. With these results, the second-order phase transition \nbetween 2SC and a normal quark matter, which is considered to be quark-gluon plasma, \ncan be characterized by the constant spatial structure and decrease in the coherent Cooper \npair number with increased T . The quark density of the 2SC has been found to be in a \nrealistic region for compact star core. The value of η in 2SC is shorter than the averaged \ninterquark density (d). The small size of the Cooper pair suggests that they are tightly \nbound and rather bosonic. Therefore, it is natural that we expect the realizability of \nquark Bose-Einstein condensation phase. Some of our results, the larger ¢, higher Tc, \nwider μ region and shorter η in model B suggest that the LQB gluon propagator induces \nstronger quark-quark interaction than the tree-level one.", "subitem_description_language": "en", "subitem_description_type": "Abstract"}]}, "item_10002_identifier_registration": {"attribute_name": "ID登録", "attribute_value_mlt": [{"subitem_identifier_reg_text": "10.18933/00000105", "subitem_identifier_reg_type": "JaLC"}]}, "item_10002_publisher_8": {"attribute_name": "出版者", "attribute_value_mlt": [{"subitem_publisher": "了德寺大学"}]}, "item_10002_relation_12": {"attribute_name": "論文ID(NAID)", "attribute_value_mlt": [{"subitem_relation_type": "isIdenticalTo", "subitem_relation_type_id": {"subitem_relation_type_id_text": "40019349469", "subitem_relation_type_select": "NAID"}}]}, "item_10002_source_id_11": {"attribute_name": "書誌レコードID", "attribute_value_mlt": [{"subitem_source_identifier": "AA12217741", "subitem_source_identifier_type": "NCID"}]}, "item_10002_source_id_9": {"attribute_name": "ISSN", "attribute_value_mlt": [{"subitem_source_identifier": "1881-9796", "subitem_source_identifier_type": "PISSN"}]}, "item_10002_version_type_20": {"attribute_name": "著者版フラグ", "attribute_value_mlt": [{"subitem_version_resource": "http://purl.org/coar/version/c_970fb48d4fbd8a85", "subitem_version_type": "VoR"}]}, "item_creator": {"attribute_name": "著者", "attribute_type": "creator", "attribute_value_mlt": [{"creatorNames": [{"creatorName": "木内, 一佳志", "creatorNameLang": "ja"}, {"creatorName": "キウチ, ヒヨシ", "creatorNameLang": "ja-Kana"}, {"creatorName": "KIUCHI, Hiyoshi", "creatorNameLang": "en"}], "nameIdentifiers": [{"nameIdentifier": "176", "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": "2016-05-17"}], "displaytype": "detail", "download_preview_message": "", "file_order": 0, "filename": "2012_01_5.pdf", "filesize": [{"value": "977.7 kB"}], "format": "application/pdf", "future_date_message": "", "is_thumbnail": false, "licensetype": "license_11", "mimetype": "application/pdf", "size": 977700.0, "url": {"label": "量子色力学類似有効理論に於けるカラー超伝導体の熱力学", "url": "https://ryotokuji-u.repo.nii.ac.jp/record/127/files/2012_01_5.pdf"}, "version_id": "c37e652d-35f0-4c70-92e1-03abac36fdc7"}]}, "item_keyword": {"attribute_name": "キーワード", "attribute_value_mlt": [{"subitem_subject": "有限温度", "subitem_subject_scheme": "Other"}, {"subitem_subject": "熱力学", "subitem_subject_scheme": "Other"}, {"subitem_subject": "カラー超伝導体", "subitem_subject_scheme": "Other"}, {"subitem_subject": "QCD類似理論", "subitem_subject_scheme": "Other"}, {"subitem_subject": "クーパー対", "subitem_subject_scheme": "Other"}, {"subitem_subject": "thermodynamics", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "color superconductor", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "QCD-like theory", "subitem_subject_language": "en", "subitem_subject_scheme": "Other"}, {"subitem_subject": "Cooper pair", "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": "departmental bulletin paper", "resourceuri": "http://purl.org/coar/resource_type/c_6501"}]}, "item_title": "量子色力学類似有効理論に於けるカラー超伝導体の熱力学", "item_titles": {"attribute_name": "タイトル", "attribute_value_mlt": [{"subitem_title": "量子色力学類似有効理論に於けるカラー超伝導体の熱力学", "subitem_title_language": "ja"}, {"subitem_title": "Thermodynamics of Color Superconductor in a QCD-like Effective Theory", "subitem_title_language": "en"}]}, "item_type_id": "10002", "owner": "8", "path": ["12"], "permalink_uri": "https://doi.org/10.18933/00000105", "pubdate": {"attribute_name": "PubDate", "attribute_value": "2016-05-17"}, "publish_date": "2016-05-17", "publish_status": "0", "recid": "127", "relation": {}, "relation_version_is_last": true, "title": ["量子色力学類似有効理論に於けるカラー超伝導体の熱力学"], "weko_shared_id": -1}
量子色力学類似有効理論に於けるカラー超伝導体の熱力学
https://doi.org/10.18933/00000105
https://doi.org/10.18933/000001050b125323-8399-4198-8b04-12a379915e38
名前 / ファイル | ライセンス | アクション |
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Item type | 紀要論文 / Departmental Bulletin Paper(1) | |||||
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公開日 | 2016-05-17 | |||||
タイトル | ||||||
言語 | ja | |||||
タイトル | 量子色力学類似有効理論に於けるカラー超伝導体の熱力学 | |||||
タイトル | ||||||
言語 | en | |||||
タイトル | Thermodynamics of Color Superconductor in a QCD-like Effective Theory | |||||
言語 | ||||||
言語 | jpn | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | 有限温度 | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | 熱力学 | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | カラー超伝導体 | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | QCD類似理論 | |||||
キーワード | ||||||
主題Scheme | Other | |||||
主題 | クーパー対 | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | thermodynamics | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | color superconductor | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | QCD-like theory | |||||
キーワード | ||||||
言語 | en | |||||
主題Scheme | Other | |||||
主題 | Cooper pair | |||||
資源タイプ | ||||||
資源タイプ識別子 | http://purl.org/coar/resource_type/c_6501 | |||||
資源タイプ | departmental bulletin paper | |||||
ID登録 | ||||||
ID登録 | 10.18933/00000105 | |||||
ID登録タイプ | JaLC | |||||
その他(別言語等)のタイトル | ||||||
その他のタイトル | Thermodynamics of Color Superconductor in a QCD-like Effective Theory | |||||
言語 | en | |||||
著者 |
木内, 一佳志
× 木内, 一佳志 |
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抄録 | ||||||
内容記述タイプ | Abstract | |||||
内容記述 | クォークとグルオンの物理系は、低温・低密度では、カイラル対称性の破れたハドロン相と なっているが、高温、若しくは高密度では、カイラル対称性が回復し、クォーク・グルオン・ プラズマ相(QGP) あるいは、カラー超伝導相などとなる。 今回われわれは、有限温度および密度に於いて、2フレーバーカラー超伝導体(2SC) の熱力学を 量子色力学類似有効理論を用いて調べた。中等度のクォーク密度領域に於いて2¢T =0 =3:43kBTc p=pF という結果を得た(¢:ギャップエネルギー, pF :フェルミ運動量、kB:ボルツマン定数, Tc:臨界温 度)。この値は、通常の電子系の超伝導での結果(2Δ = 3:52kBTc) と略同じである。クォーク・ クーパー対の波動関数は規格化定数を別にすれば、温度に依存せず、対のコヒーレンス長は、 臨界温度まで略一定であることが判明した。 一方、エネルギーギャップは、温度の上昇と共 に減少し、臨界温度で零となる。従って、2SC からQGP への2 次相転移は、クォーク・クー パー対の空間構造の不変性と対の減少によって特徴付けられることが判った。 |
|||||
言語 | ja | |||||
抄録 | ||||||
内容記述タイプ | Abstract | |||||
内容記述 | We have investigated the thermodynamics of two-flavor color superconductor (2SC) at finite temperature (T) and quark chemical potential (1) within the framework of a QCD-like effective theory, in which an asymptotically free momentum-dependent running coupling is used. Two kinds of systems have been investigated. One is with a tree-level gluon propagator (model A) and the other is with the lattice-QCD based (LQB) gluon propagator (model B). We have found that 2¢T =0 =3:43kBTc in model B (¢:energy p=pF gap, kB:Boltzmann constant, Tc:critical temperature). This value is very close to the famous BCS result, which is 2Δ = 3:52kBTc. We have found that the coherence length (´) is not affected by T in 2SC, while Δ decreases as T increases and vanishes at Tc. In addition, we have found that the Cooper pair wave function c(p) is not affected by T , apart from normalization constant. With these results, the second-order phase transition between 2SC and a normal quark matter, which is considered to be quark-gluon plasma, can be characterized by the constant spatial structure and decrease in the coherent Cooper pair number with increased T . The quark density of the 2SC has been found to be in a realistic region for compact star core. The value of η in 2SC is shorter than the averaged interquark density (d). The small size of the Cooper pair suggests that they are tightly bound and rather bosonic. Therefore, it is natural that we expect the realizability of quark Bose-Einstein condensation phase. Some of our results, the larger ¢, higher Tc, wider μ region and shorter η in model B suggest that the LQB gluon propagator induces stronger quark-quark interaction than the tree-level one. |
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言語 | en | |||||
書誌情報 |
了德寺大学研究紀要 en : The Bulletin of Ryotokuji University 号 6, p. 11-30, 発行日 2012 |
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出版者 | ||||||
出版者 | 了德寺大学 | |||||
ISSN | ||||||
収録物識別子タイプ | PISSN | |||||
収録物識別子 | 1881-9796 | |||||
書誌レコードID | ||||||
収録物識別子タイプ | NCID | |||||
収録物識別子 | AA12217741 | |||||
論文ID(NAID) | ||||||
関連タイプ | isIdenticalTo | |||||
識別子タイプ | NAID | |||||
関連識別子 | 40019349469 | |||||
著者版フラグ | ||||||
出版タイプ | VoR | |||||
出版タイプResource | http://purl.org/coar/version/c_970fb48d4fbd8a85 |