{"title":"违反同位旋衰变Ds*→Dsπ0和中间介子环辐射衰变Ds*→Dsγ的联合研究","authors":"Jun Wang, Qiang Zhao","doi":"10.1103/physrevd.111.096007","DOIUrl":null,"url":null,"abstract":"We carry out a combined study of the isospin-violating decay D</a:mi></a:mrow>s</a:mi></a:mrow>*</a:mo></a:mrow></a:msubsup>→</a:mo>D</a:mi></a:mrow>s</a:mi></a:mrow></a:msub>π</a:mi></a:mrow>0</a:mn></a:mrow></a:msup></a:mrow></a:math> and radiative decay <d:math xmlns:d=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><d:msubsup><d:mi>D</d:mi><d:mi>s</d:mi><d:mo>*</d:mo></d:msubsup><d:mo stretchy=\"false\">→</d:mo><d:msub><d:mi>D</d:mi><d:mi>s</d:mi></d:msub><d:mi>γ</d:mi></d:math> in an effective Lagrangian approach by taking into account the corrections from the one-loop transitions. By distinguishing the transition mechanisms of the long-distance interactions through the intermediate meson loops from the short-distance interactions through the <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mi>η</g:mi><g:mo>−</g:mo><g:msup><g:mi>π</g:mi><g:mn>0</g:mn></g:msup></g:math> mixing at the tree level, the isospin-violating decay <i:math xmlns:i=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><i:msubsup><i:mi>D</i:mi><i:mi>s</i:mi><i:mo>*</i:mo></i:msubsup><i:mo stretchy=\"false\">→</i:mo><i:msub><i:mi>D</i:mi><i:mi>s</i:mi></i:msub><i:msup><i:mi>π</i:mi><i:mn>0</i:mn></i:msup></i:math> can be well constrained. In our approach, the higher-order corrections to the isospin-violating effects can involve the intermediate <l:math xmlns:l=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><l:msup><l:mi>D</l:mi><l:mrow><l:mo stretchy=\"false\">(</l:mo><l:mo>*</l:mo><l:mo stretchy=\"false\">)</l:mo></l:mrow></l:msup></l:math> and <p:math xmlns:p=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><p:msup><p:mi>K</p:mi><p:mrow><p:mo stretchy=\"false\">(</p:mo><p:mo>*</p:mo><p:mo stretchy=\"false\">)</p:mo></p:mrow></p:msup></p:math> scatterings. We find that the contributions from the destructive interference of intermediate meson loops via <t:math xmlns:t=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><t:mrow><t:msup><t:mrow><t:mi>D</t:mi></t:mrow><t:mrow><t:mo stretchy=\"false\">(</t:mo><t:mo>*</t:mo><t:mo stretchy=\"false\">)</t:mo><t:mn>0</t:mn></t:mrow></t:msup><t:mo stretchy=\"false\">(</t:mo><t:mi>c</t:mi><t:mover accent=\"true\"><t:mrow><t:mi>u</t:mi></t:mrow><t:mrow><t:mo stretchy=\"false\">¯</t:mo></t:mrow></t:mover><t:mo stretchy=\"false\">)</t:mo><t:msup><t:mrow><t:mi>K</t:mi></t:mrow><t:mrow><t:mo stretchy=\"false\">(</t:mo><t:mo>*</t:mo><t:mo stretchy=\"false\">)</t:mo><t:mo>+</t:mo></t:mrow></t:msup><t:mo stretchy=\"false\">(</t:mo><t:mi>u</t:mi><t:mover accent=\"true\"><t:mrow><t:mi>s</t:mi></t:mrow><t:mrow><t:mo stretchy=\"false\">¯</t:mo></t:mrow></t:mover><t:mo stretchy=\"false\">)</t:mo></t:mrow></t:math> and <hb:math xmlns:hb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><hb:mrow><hb:msup><hb:mrow><hb:mi>D</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\"false\">(</hb:mo><hb:mo>*</hb:mo><hb:mo stretchy=\"false\">)</hb:mo><hb:mo>+</hb:mo></hb:mrow></hb:msup><hb:mo stretchy=\"false\">(</hb:mo><hb:mi>c</hb:mi><hb:mover accent=\"true\"><hb:mrow><hb:mi>d</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\"false\">¯</hb:mo></hb:mrow></hb:mover><hb:mo stretchy=\"false\">)</hb:mo><hb:msup><hb:mrow><hb:mi>K</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\"false\">(</hb:mo><hb:mo>*</hb:mo><hb:mo stretchy=\"false\">)</hb:mo><hb:mn>0</hb:mn></hb:mrow></hb:msup><hb:mo stretchy=\"false\">(</hb:mo><hb:mi>d</hb:mi><hb:mover accent=\"true\"><hb:mrow><hb:mi>s</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\"false\">¯</hb:mo></hb:mrow></hb:mover><hb:mo stretchy=\"false\">)</hb:mo></hb:mrow></hb:math> rescatterings are significant. Within the commonly accepted UV cutoff range, we obtain the partial decay width <vb:math xmlns:vb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><vb:mrow><vb:mi mathvariant=\"normal\">Γ</vb:mi><vb:mo stretchy=\"false\">[</vb:mo><vb:msubsup><vb:mrow><vb:mi>D</vb:mi></vb:mrow><vb:mrow><vb:mi>s</vb:mi></vb:mrow><vb:mrow><vb:mo>*</vb:mo></vb:mrow></vb:msubsup><vb:mo stretchy=\"false\">→</vb:mo><vb:msub><vb:mrow><vb:mi>D</vb:mi></vb:mrow><vb:mrow><vb:mi>s</vb:mi></vb:mrow></vb:msub><vb:msup><vb:mrow><vb:mi>π</vb:mi></vb:mrow><vb:mrow><vb:mn>0</vb:mn></vb:mrow></vb:msup><vb:mo stretchy=\"false\">]</vb:mo><vb:mo>=</vb:mo><vb:msubsup><vb:mrow><vb:mn>9.92</vb:mn></vb:mrow><vb:mrow><vb:mo>−</vb:mo><vb:mn>0.66</vb:mn></vb:mrow><vb:mrow><vb:mo>+</vb:mo><vb:mn>0.76</vb:mn></vb:mrow></vb:msubsup><vb:mtext> </vb:mtext><vb:mtext> </vb:mtext><vb:mi>eV</vb:mi></vb:mrow></vb:math>. This approach allows us to describe the <bc:math xmlns:bc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><bc:msubsup><bc:mi>D</bc:mi><bc:mi>s</bc:mi><bc:mo>*</bc:mo></bc:msubsup></bc:math> radiative decay in the same framework via the vector-meson-dominance model. We demonstrate that both the tree-level and one-loop transitions can be self-consistently determined if we adopt the experimental data for the branching ratio fraction of <dc:math xmlns:dc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><dc:msubsup><dc:mi>D</dc:mi><dc:mi>s</dc:mi><dc:mo>*</dc:mo></dc:msubsup><dc:mo stretchy=\"false\">→</dc:mo><dc:msub><dc:mi>D</dc:mi><dc:mi>s</dc:mi></dc:msub><dc:msup><dc:mi>π</dc:mi><dc:mn>0</dc:mn></dc:msup></dc:math> to <gc:math xmlns:gc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><gc:msubsup><gc:mi>D</gc:mi><gc:mi>s</gc:mi><gc:mo>*</gc:mo></gc:msubsup><gc:mo stretchy=\"false\">→</gc:mo><gc:msub><gc:mi>D</gc:mi><gc:mi>s</gc:mi></gc:msub><gc:mi>γ</gc:mi></gc:math>. It then leads to a reliable estimate of the total decay width of <jc:math xmlns:jc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jc:msubsup><jc:mi>D</jc:mi><jc:mi>s</jc:mi><jc:mo>*</jc:mo></jc:msubsup></jc:math>, i.e., <lc:math xmlns:lc=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><lc:mrow><lc:msub><lc:mrow><lc:mi mathvariant=\"normal\">Γ</lc:mi></lc:mrow><lc:mrow><lc:mtext>total</lc:mtext></lc:mrow></lc:msub><lc:mo stretchy=\"false\">(</lc:mo><lc:msubsup><lc:mrow><lc:mi>D</lc:mi></lc:mrow><lc:mrow><lc:mi>s</lc:mi></lc:mrow><lc:mrow><lc:mo>*</lc:mo><lc:mo>+</lc:mo></lc:mrow></lc:msubsup><lc:mo stretchy=\"false\">)</lc:mo><lc:mo>=</lc:mo><lc:mn>17</lc:mn><lc:msubsup><lc:mrow><lc:mn>0</lc:mn></lc:mrow><lc:mrow><lc:mo>−</lc:mo><lc:mn>12</lc:mn></lc:mrow><lc:mrow><lc:mo>+</lc:mo><lc:mn>13</lc:mn></lc:mrow></lc:msubsup><lc:mtext> </lc:mtext><lc:mtext> </lc:mtext><lc:mi>eV</lc:mi></lc:mrow></lc:math>. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20167,"journal":{"name":"Physical Review D","volume":"25 1","pages":""},"PeriodicalIF":5.3000,"publicationDate":"2025-05-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Combined study of the isospin-violating decay Ds*→Dsπ0 and radiative decay Ds*→Dsγ with intermediate meson loops\",\"authors\":\"Jun Wang, Qiang Zhao\",\"doi\":\"10.1103/physrevd.111.096007\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We carry out a combined study of the isospin-violating decay D</a:mi></a:mrow>s</a:mi></a:mrow>*</a:mo></a:mrow></a:msubsup>→</a:mo>D</a:mi></a:mrow>s</a:mi></a:mrow></a:msub>π</a:mi></a:mrow>0</a:mn></a:mrow></a:msup></a:mrow></a:math> and radiative decay <d:math xmlns:d=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><d:msubsup><d:mi>D</d:mi><d:mi>s</d:mi><d:mo>*</d:mo></d:msubsup><d:mo stretchy=\\\"false\\\">→</d:mo><d:msub><d:mi>D</d:mi><d:mi>s</d:mi></d:msub><d:mi>γ</d:mi></d:math> in an effective Lagrangian approach by taking into account the corrections from the one-loop transitions. By distinguishing the transition mechanisms of the long-distance interactions through the intermediate meson loops from the short-distance interactions through the <g:math xmlns:g=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><g:mi>η</g:mi><g:mo>−</g:mo><g:msup><g:mi>π</g:mi><g:mn>0</g:mn></g:msup></g:math> mixing at the tree level, the isospin-violating decay <i:math xmlns:i=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><i:msubsup><i:mi>D</i:mi><i:mi>s</i:mi><i:mo>*</i:mo></i:msubsup><i:mo stretchy=\\\"false\\\">→</i:mo><i:msub><i:mi>D</i:mi><i:mi>s</i:mi></i:msub><i:msup><i:mi>π</i:mi><i:mn>0</i:mn></i:msup></i:math> can be well constrained. In our approach, the higher-order corrections to the isospin-violating effects can involve the intermediate <l:math xmlns:l=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><l:msup><l:mi>D</l:mi><l:mrow><l:mo stretchy=\\\"false\\\">(</l:mo><l:mo>*</l:mo><l:mo stretchy=\\\"false\\\">)</l:mo></l:mrow></l:msup></l:math> and <p:math xmlns:p=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><p:msup><p:mi>K</p:mi><p:mrow><p:mo stretchy=\\\"false\\\">(</p:mo><p:mo>*</p:mo><p:mo stretchy=\\\"false\\\">)</p:mo></p:mrow></p:msup></p:math> scatterings. We find that the contributions from the destructive interference of intermediate meson loops via <t:math xmlns:t=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><t:mrow><t:msup><t:mrow><t:mi>D</t:mi></t:mrow><t:mrow><t:mo stretchy=\\\"false\\\">(</t:mo><t:mo>*</t:mo><t:mo stretchy=\\\"false\\\">)</t:mo><t:mn>0</t:mn></t:mrow></t:msup><t:mo stretchy=\\\"false\\\">(</t:mo><t:mi>c</t:mi><t:mover accent=\\\"true\\\"><t:mrow><t:mi>u</t:mi></t:mrow><t:mrow><t:mo stretchy=\\\"false\\\">¯</t:mo></t:mrow></t:mover><t:mo stretchy=\\\"false\\\">)</t:mo><t:msup><t:mrow><t:mi>K</t:mi></t:mrow><t:mrow><t:mo stretchy=\\\"false\\\">(</t:mo><t:mo>*</t:mo><t:mo stretchy=\\\"false\\\">)</t:mo><t:mo>+</t:mo></t:mrow></t:msup><t:mo stretchy=\\\"false\\\">(</t:mo><t:mi>u</t:mi><t:mover accent=\\\"true\\\"><t:mrow><t:mi>s</t:mi></t:mrow><t:mrow><t:mo stretchy=\\\"false\\\">¯</t:mo></t:mrow></t:mover><t:mo stretchy=\\\"false\\\">)</t:mo></t:mrow></t:math> and <hb:math xmlns:hb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><hb:mrow><hb:msup><hb:mrow><hb:mi>D</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\\\"false\\\">(</hb:mo><hb:mo>*</hb:mo><hb:mo stretchy=\\\"false\\\">)</hb:mo><hb:mo>+</hb:mo></hb:mrow></hb:msup><hb:mo stretchy=\\\"false\\\">(</hb:mo><hb:mi>c</hb:mi><hb:mover accent=\\\"true\\\"><hb:mrow><hb:mi>d</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\\\"false\\\">¯</hb:mo></hb:mrow></hb:mover><hb:mo stretchy=\\\"false\\\">)</hb:mo><hb:msup><hb:mrow><hb:mi>K</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\\\"false\\\">(</hb:mo><hb:mo>*</hb:mo><hb:mo stretchy=\\\"false\\\">)</hb:mo><hb:mn>0</hb:mn></hb:mrow></hb:msup><hb:mo stretchy=\\\"false\\\">(</hb:mo><hb:mi>d</hb:mi><hb:mover accent=\\\"true\\\"><hb:mrow><hb:mi>s</hb:mi></hb:mrow><hb:mrow><hb:mo stretchy=\\\"false\\\">¯</hb:mo></hb:mrow></hb:mover><hb:mo stretchy=\\\"false\\\">)</hb:mo></hb:mrow></hb:math> rescatterings are significant. Within the commonly accepted UV cutoff range, we obtain the partial decay width <vb:math xmlns:vb=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><vb:mrow><vb:mi mathvariant=\\\"normal\\\">Γ</vb:mi><vb:mo stretchy=\\\"false\\\">[</vb:mo><vb:msubsup><vb:mrow><vb:mi>D</vb:mi></vb:mrow><vb:mrow><vb:mi>s</vb:mi></vb:mrow><vb:mrow><vb:mo>*</vb:mo></vb:mrow></vb:msubsup><vb:mo stretchy=\\\"false\\\">→</vb:mo><vb:msub><vb:mrow><vb:mi>D</vb:mi></vb:mrow><vb:mrow><vb:mi>s</vb:mi></vb:mrow></vb:msub><vb:msup><vb:mrow><vb:mi>π</vb:mi></vb:mrow><vb:mrow><vb:mn>0</vb:mn></vb:mrow></vb:msup><vb:mo stretchy=\\\"false\\\">]</vb:mo><vb:mo>=</vb:mo><vb:msubsup><vb:mrow><vb:mn>9.92</vb:mn></vb:mrow><vb:mrow><vb:mo>−</vb:mo><vb:mn>0.66</vb:mn></vb:mrow><vb:mrow><vb:mo>+</vb:mo><vb:mn>0.76</vb:mn></vb:mrow></vb:msubsup><vb:mtext> </vb:mtext><vb:mtext> </vb:mtext><vb:mi>eV</vb:mi></vb:mrow></vb:math>. This approach allows us to describe the <bc:math xmlns:bc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><bc:msubsup><bc:mi>D</bc:mi><bc:mi>s</bc:mi><bc:mo>*</bc:mo></bc:msubsup></bc:math> radiative decay in the same framework via the vector-meson-dominance model. We demonstrate that both the tree-level and one-loop transitions can be self-consistently determined if we adopt the experimental data for the branching ratio fraction of <dc:math xmlns:dc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><dc:msubsup><dc:mi>D</dc:mi><dc:mi>s</dc:mi><dc:mo>*</dc:mo></dc:msubsup><dc:mo stretchy=\\\"false\\\">→</dc:mo><dc:msub><dc:mi>D</dc:mi><dc:mi>s</dc:mi></dc:msub><dc:msup><dc:mi>π</dc:mi><dc:mn>0</dc:mn></dc:msup></dc:math> to <gc:math xmlns:gc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><gc:msubsup><gc:mi>D</gc:mi><gc:mi>s</gc:mi><gc:mo>*</gc:mo></gc:msubsup><gc:mo stretchy=\\\"false\\\">→</gc:mo><gc:msub><gc:mi>D</gc:mi><gc:mi>s</gc:mi></gc:msub><gc:mi>γ</gc:mi></gc:math>. It then leads to a reliable estimate of the total decay width of <jc:math xmlns:jc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><jc:msubsup><jc:mi>D</jc:mi><jc:mi>s</jc:mi><jc:mo>*</jc:mo></jc:msubsup></jc:math>, i.e., <lc:math xmlns:lc=\\\"http://www.w3.org/1998/Math/MathML\\\" display=\\\"inline\\\"><lc:mrow><lc:msub><lc:mrow><lc:mi mathvariant=\\\"normal\\\">Γ</lc:mi></lc:mrow><lc:mrow><lc:mtext>total</lc:mtext></lc:mrow></lc:msub><lc:mo stretchy=\\\"false\\\">(</lc:mo><lc:msubsup><lc:mrow><lc:mi>D</lc:mi></lc:mrow><lc:mrow><lc:mi>s</lc:mi></lc:mrow><lc:mrow><lc:mo>*</lc:mo><lc:mo>+</lc:mo></lc:mrow></lc:msubsup><lc:mo stretchy=\\\"false\\\">)</lc:mo><lc:mo>=</lc:mo><lc:mn>17</lc:mn><lc:msubsup><lc:mrow><lc:mn>0</lc:mn></lc:mrow><lc:mrow><lc:mo>−</lc:mo><lc:mn>12</lc:mn></lc:mrow><lc:mrow><lc:mo>+</lc:mo><lc:mn>13</lc:mn></lc:mrow></lc:msubsup><lc:mtext> </lc:mtext><lc:mtext> </lc:mtext><lc:mi>eV</lc:mi></lc:mrow></lc:math>. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>\",\"PeriodicalId\":20167,\"journal\":{\"name\":\"Physical Review D\",\"volume\":\"25 1\",\"pages\":\"\"},\"PeriodicalIF\":5.3000,\"publicationDate\":\"2025-05-07\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Physical Review D\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1103/physrevd.111.096007\",\"RegionNum\":2,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"Physics and Astronomy\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review D","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevd.111.096007","RegionNum":2,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"Physics and Astronomy","Score":null,"Total":0}
Combined study of the isospin-violating decay Ds*→Dsπ0 and radiative decay Ds*→Dsγ with intermediate meson loops
We carry out a combined study of the isospin-violating decay Ds*→Dsπ0 and radiative decay Ds*→Dsγ in an effective Lagrangian approach by taking into account the corrections from the one-loop transitions. By distinguishing the transition mechanisms of the long-distance interactions through the intermediate meson loops from the short-distance interactions through the η−π0 mixing at the tree level, the isospin-violating decay Ds*→Dsπ0 can be well constrained. In our approach, the higher-order corrections to the isospin-violating effects can involve the intermediate D(*) and K(*) scatterings. We find that the contributions from the destructive interference of intermediate meson loops via D(*)0(cu¯)K(*)+(us¯) and D(*)+(cd¯)K(*)0(ds¯) rescatterings are significant. Within the commonly accepted UV cutoff range, we obtain the partial decay width Γ[Ds*→Dsπ0]=9.92−0.66+0.76eV. This approach allows us to describe the Ds* radiative decay in the same framework via the vector-meson-dominance model. We demonstrate that both the tree-level and one-loop transitions can be self-consistently determined if we adopt the experimental data for the branching ratio fraction of Ds*→Dsπ0 to Ds*→Dsγ. It then leads to a reliable estimate of the total decay width of Ds*, i.e., Γtotal(Ds*+)=170−12+13eV. Published by the American Physical Society2025
期刊介绍:
Physical Review D (PRD) is a leading journal in elementary particle physics, field theory, gravitation, and cosmology and is one of the top-cited journals in high-energy physics.
PRD covers experimental and theoretical results in all aspects of particle physics, field theory, gravitation and cosmology, including:
Particle physics experiments,
Electroweak interactions,
Strong interactions,
Lattice field theories, lattice QCD,
Beyond the standard model physics,
Phenomenological aspects of field theory, general methods,
Gravity, cosmology, cosmic rays,
Astrophysics and astroparticle physics,
General relativity,
Formal aspects of field theory, field theory in curved space,
String theory, quantum gravity, gauge/gravity duality.