Splitting mass spectra and muon g −2 in Higgs-anomaly mediation
We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high en...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Yin, Wen [verfasserIn] |
|---|
| Format: |
E-Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
2016transfer abstract |
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| Umfang: |
8 |
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| Übergeordnetes Werk: |
Enthalten in: Applying the Go/NoGo processing schema to a visual oddball task in older adults - Steiner, Genevieve Z. ELSEVIER, 2016, Amsterdam |
|---|---|
| Übergeordnetes Werk: |
volume:762 ; year:2016 ; day:10 ; month:11 ; pages:72-79 ; extent:8 |
| Links: |
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| DOI / URN: |
10.1016/j.physletb.2016.09.024 |
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| 520 | |a We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high energy scale with a gravitino mass of ∼ 100 TeV . Due to renormalization group running effects from the Higgs soft masses, the masses of the third generation sfermions become O ( 10 ) TeV at the low energy scale, while the first and second generation sfermion masses are O ( 0.1 - 1 ) TeV , avoiding the tachyonic slepton problem and flavor changing neutral current problem. With the splitting mass spectrum, the muon g − 2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV. Moreover, the third generation Yukawa couplings are expected to be unified in some regions. | ||
| 520 | |a We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high energy scale with a gravitino mass of ∼ 100 TeV . Due to renormalization group running effects from the Higgs soft masses, the masses of the third generation sfermions become O ( 10 ) TeV at the low energy scale, while the first and second generation sfermion masses are O ( 0.1 - 1 ) TeV , avoiding the tachyonic slepton problem and flavor changing neutral current problem. With the splitting mass spectrum, the muon g − 2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV. Moreover, the third generation Yukawa couplings are expected to be unified in some regions. | ||
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10.1016/j.physletb.2016.09.024 doi GBV00000000000205A.pica (DE-627)ELV01408340X (ELSEVIER)S0370-2693(16)30518-4 DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Yin, Wen verfasserin aut Splitting mass spectra and muon g −2 in Higgs-anomaly mediation 2016transfer abstract 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high energy scale with a gravitino mass of ∼ 100 TeV . Due to renormalization group running effects from the Higgs soft masses, the masses of the third generation sfermions become O ( 10 ) TeV at the low energy scale, while the first and second generation sfermion masses are O ( 0.1 - 1 ) TeV , avoiding the tachyonic slepton problem and flavor changing neutral current problem. With the splitting mass spectrum, the muon g − 2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV. Moreover, the third generation Yukawa couplings are expected to be unified in some regions. We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high energy scale with a gravitino mass of ∼ 100 TeV . Due to renormalization group running effects from the Higgs soft masses, the masses of the third generation sfermions become O ( 10 ) TeV at the low energy scale, while the first and second generation sfermion masses are O ( 0.1 - 1 ) TeV , avoiding the tachyonic slepton problem and flavor changing neutral current problem. With the splitting mass spectrum, the muon g − 2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV. Moreover, the third generation Yukawa couplings are expected to be unified in some regions. Yokozaki, Norimi oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:762 year:2016 day:10 month:11 pages:72-79 extent:8 https://doi.org/10.1016/j.physletb.2016.09.024 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 762 2016 10 1110 72-79 8 |
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10.1016/j.physletb.2016.09.024 doi GBV00000000000205A.pica (DE-627)ELV01408340X (ELSEVIER)S0370-2693(16)30518-4 DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Yin, Wen verfasserin aut Splitting mass spectra and muon g −2 in Higgs-anomaly mediation 2016transfer abstract 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high energy scale with a gravitino mass of ∼ 100 TeV . Due to renormalization group running effects from the Higgs soft masses, the masses of the third generation sfermions become O ( 10 ) TeV at the low energy scale, while the first and second generation sfermion masses are O ( 0.1 - 1 ) TeV , avoiding the tachyonic slepton problem and flavor changing neutral current problem. With the splitting mass spectrum, the muon g − 2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV. Moreover, the third generation Yukawa couplings are expected to be unified in some regions. We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high energy scale with a gravitino mass of ∼ 100 TeV . Due to renormalization group running effects from the Higgs soft masses, the masses of the third generation sfermions become O ( 10 ) TeV at the low energy scale, while the first and second generation sfermion masses are O ( 0.1 - 1 ) TeV , avoiding the tachyonic slepton problem and flavor changing neutral current problem. With the splitting mass spectrum, the muon g − 2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV. Moreover, the third generation Yukawa couplings are expected to be unified in some regions. Yokozaki, Norimi oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:762 year:2016 day:10 month:11 pages:72-79 extent:8 https://doi.org/10.1016/j.physletb.2016.09.024 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 762 2016 10 1110 72-79 8 |
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10.1016/j.physletb.2016.09.024 doi GBV00000000000205A.pica (DE-627)ELV01408340X (ELSEVIER)S0370-2693(16)30518-4 DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Yin, Wen verfasserin aut Splitting mass spectra and muon g −2 in Higgs-anomaly mediation 2016transfer abstract 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high energy scale with a gravitino mass of ∼ 100 TeV . Due to renormalization group running effects from the Higgs soft masses, the masses of the third generation sfermions become O ( 10 ) TeV at the low energy scale, while the first and second generation sfermion masses are O ( 0.1 - 1 ) TeV , avoiding the tachyonic slepton problem and flavor changing neutral current problem. With the splitting mass spectrum, the muon g − 2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV. Moreover, the third generation Yukawa couplings are expected to be unified in some regions. We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high energy scale with a gravitino mass of ∼ 100 TeV . Due to renormalization group running effects from the Higgs soft masses, the masses of the third generation sfermions become O ( 10 ) TeV at the low energy scale, while the first and second generation sfermion masses are O ( 0.1 - 1 ) TeV , avoiding the tachyonic slepton problem and flavor changing neutral current problem. With the splitting mass spectrum, the muon g − 2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV. Moreover, the third generation Yukawa couplings are expected to be unified in some regions. Yokozaki, Norimi oth Enthalten in North-Holland Publ Steiner, Genevieve Z. ELSEVIER Applying the Go/NoGo processing schema to a visual oddball task in older adults 2016 Amsterdam (DE-627)ELV000151122 volume:762 year:2016 day:10 month:11 pages:72-79 extent:8 https://doi.org/10.1016/j.physletb.2016.09.024 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 762 2016 10 1110 72-79 8 |
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Splitting mass spectra and muon g −2 in Higgs-anomaly mediation |
| abstract |
We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high energy scale with a gravitino mass of ∼ 100 TeV . Due to renormalization group running effects from the Higgs soft masses, the masses of the third generation sfermions become O ( 10 ) TeV at the low energy scale, while the first and second generation sfermion masses are O ( 0.1 - 1 ) TeV , avoiding the tachyonic slepton problem and flavor changing neutral current problem. With the splitting mass spectrum, the muon g − 2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV. Moreover, the third generation Yukawa couplings are expected to be unified in some regions. |
| abstractGer |
We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high energy scale with a gravitino mass of ∼ 100 TeV . Due to renormalization group running effects from the Higgs soft masses, the masses of the third generation sfermions become O ( 10 ) TeV at the low energy scale, while the first and second generation sfermion masses are O ( 0.1 - 1 ) TeV , avoiding the tachyonic slepton problem and flavor changing neutral current problem. With the splitting mass spectrum, the muon g − 2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV. Moreover, the third generation Yukawa couplings are expected to be unified in some regions. |
| abstract_unstemmed |
We propose a scenario where only the Higgs multiplets have direct couplings to a supersymmetry (SUSY) breaking sector. The standard model matter multiplets as well as the gauge multiples are sequestered from the SUSY breaking sector; therefore, their masses arise via anomaly mediation at the high energy scale with a gravitino mass of ∼ 100 TeV . Due to renormalization group running effects from the Higgs soft masses, the masses of the third generation sfermions become O ( 10 ) TeV at the low energy scale, while the first and second generation sfermion masses are O ( 0.1 - 1 ) TeV , avoiding the tachyonic slepton problem and flavor changing neutral current problem. With the splitting mass spectrum, the muon g − 2 anomaly is explained consistently with the observed Higgs boson mass of 125 GeV. Moreover, the third generation Yukawa couplings are expected to be unified in some regions. |
| collection_details |
GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA |
| title_short |
Splitting mass spectra and muon g −2 in Higgs-anomaly mediation |
| url |
https://doi.org/10.1016/j.physletb.2016.09.024 |
| remote_bool |
true |
| author2 |
Yokozaki, Norimi |
| author2Str |
Yokozaki, Norimi |
| ppnlink |
ELV000151122 |
| mediatype_str_mv |
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| isOA_txt |
false |
| hochschulschrift_bool |
false |
| author2_role |
oth |
| doi_str |
10.1016/j.physletb.2016.09.024 |
| up_date |
2024-07-06T20:35:08.747Z |
| _version_ |
1803863309677494272 |
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| score |
7.401272 |