Is an axizilla possible for di-photon resonance?
Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Kim, Jihn E. [verfasserIn] |
|---|
| Format: |
E-Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
2016transfer abstract |
|---|
| Schlagwörter: |
|---|
| Umfang: |
6 |
|---|
| 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:755 ; year:2016 ; day:10 ; month:04 ; pages:190-195 ; extent:6 |
| Links: |
|---|
| DOI / URN: |
10.1016/j.physletb.2016.02.016 |
|---|
| Katalog-ID: |
ELV014077124 |
|---|
| LEADER | 01000caa a22002652 4500 | ||
|---|---|---|---|
| 001 | ELV014077124 | ||
| 003 | DE-627 | ||
| 005 | 20230625112900.0 | ||
| 007 | cr uuu---uuuuu | ||
| 008 | 180602s2016 xx |||||o 00| ||eng c | ||
| 024 | 7 | |a 10.1016/j.physletb.2016.02.016 |2 doi | |
| 028 | 5 | 2 | |a GBV00000000000204A.pica |
| 035 | |a (DE-627)ELV014077124 | ||
| 035 | |a (ELSEVIER)S0370-2693(16)00112-X | ||
| 040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
| 041 | |a eng | ||
| 082 | 0 | 4 | |a 530 |q DE-600 |
| 082 | 0 | 4 | |a 610 |q VZ |
| 084 | |a 77.50 |2 bkl | ||
| 100 | 1 | |a Kim, Jihn E. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Is an axizilla possible for di-photon resonance? |
| 264 | 1 | |c 2016transfer abstract | |
| 300 | |a 6 | ||
| 336 | |a nicht spezifiziert |b zzz |2 rdacontent | ||
| 337 | |a nicht spezifiziert |b z |2 rdamedia | ||
| 338 | |a nicht spezifiziert |b zu |2 rdacarrier | ||
| 520 | |a Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . | ||
| 520 | |a Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . | ||
| 650 | 7 | |a Heavy quarks |2 Elsevier | |
| 650 | 7 | |a TeV scale pseudoscalars |2 Elsevier | |
| 650 | 7 | |a Axizillas |2 Elsevier | |
| 650 | 7 | |a Di-photon |2 Elsevier | |
| 650 | 7 | |a Discrete symmetry |2 Elsevier | |
| 773 | 0 | 8 | |i Enthalten in |n North-Holland Publ |a Steiner, Genevieve Z. ELSEVIER |t Applying the Go/NoGo processing schema to a visual oddball task in older adults |d 2016 |g Amsterdam |w (DE-627)ELV000151122 |
| 773 | 1 | 8 | |g volume:755 |g year:2016 |g day:10 |g month:04 |g pages:190-195 |g extent:6 |
| 856 | 4 | 0 | |u https://doi.org/10.1016/j.physletb.2016.02.016 |3 Volltext |
| 912 | |a GBV_USEFLAG_U | ||
| 912 | |a GBV_ELV | ||
| 912 | |a SYSFLAG_U | ||
| 912 | |a SSG-OLC-PHA | ||
| 936 | b | k | |a 77.50 |j Psychophysiologie |q VZ |
| 951 | |a AR | ||
| 952 | |d 755 |j 2016 |b 10 |c 0410 |h 190-195 |g 6 | ||
| author_variant |
j e k je jek |
|---|---|
| matchkey_str |
kimjihne:2016----:snxzlaosbeodpoo |
| hierarchy_sort_str |
2016transfer abstract |
| bklnumber |
77.50 |
| publishDate |
2016 |
| allfields |
10.1016/j.physletb.2016.02.016 doi GBV00000000000204A.pica (DE-627)ELV014077124 (ELSEVIER)S0370-2693(16)00112-X DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Kim, Jihn E. verfasserin aut Is an axizilla possible for di-photon resonance? 2016transfer abstract 6 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . Heavy quarks Elsevier TeV scale pseudoscalars Elsevier Axizillas Elsevier Di-photon Elsevier Discrete symmetry Elsevier 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:755 year:2016 day:10 month:04 pages:190-195 extent:6 https://doi.org/10.1016/j.physletb.2016.02.016 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 755 2016 10 0410 190-195 6 |
| spelling |
10.1016/j.physletb.2016.02.016 doi GBV00000000000204A.pica (DE-627)ELV014077124 (ELSEVIER)S0370-2693(16)00112-X DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Kim, Jihn E. verfasserin aut Is an axizilla possible for di-photon resonance? 2016transfer abstract 6 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . Heavy quarks Elsevier TeV scale pseudoscalars Elsevier Axizillas Elsevier Di-photon Elsevier Discrete symmetry Elsevier 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:755 year:2016 day:10 month:04 pages:190-195 extent:6 https://doi.org/10.1016/j.physletb.2016.02.016 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 755 2016 10 0410 190-195 6 |
| allfields_unstemmed |
10.1016/j.physletb.2016.02.016 doi GBV00000000000204A.pica (DE-627)ELV014077124 (ELSEVIER)S0370-2693(16)00112-X DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Kim, Jihn E. verfasserin aut Is an axizilla possible for di-photon resonance? 2016transfer abstract 6 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . Heavy quarks Elsevier TeV scale pseudoscalars Elsevier Axizillas Elsevier Di-photon Elsevier Discrete symmetry Elsevier 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:755 year:2016 day:10 month:04 pages:190-195 extent:6 https://doi.org/10.1016/j.physletb.2016.02.016 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 755 2016 10 0410 190-195 6 |
| allfieldsGer |
10.1016/j.physletb.2016.02.016 doi GBV00000000000204A.pica (DE-627)ELV014077124 (ELSEVIER)S0370-2693(16)00112-X DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Kim, Jihn E. verfasserin aut Is an axizilla possible for di-photon resonance? 2016transfer abstract 6 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . Heavy quarks Elsevier TeV scale pseudoscalars Elsevier Axizillas Elsevier Di-photon Elsevier Discrete symmetry Elsevier 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:755 year:2016 day:10 month:04 pages:190-195 extent:6 https://doi.org/10.1016/j.physletb.2016.02.016 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 755 2016 10 0410 190-195 6 |
| allfieldsSound |
10.1016/j.physletb.2016.02.016 doi GBV00000000000204A.pica (DE-627)ELV014077124 (ELSEVIER)S0370-2693(16)00112-X DE-627 ger DE-627 rakwb eng 530 DE-600 610 VZ 77.50 bkl Kim, Jihn E. verfasserin aut Is an axizilla possible for di-photon resonance? 2016transfer abstract 6 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . Heavy quarks Elsevier TeV scale pseudoscalars Elsevier Axizillas Elsevier Di-photon Elsevier Discrete symmetry Elsevier 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:755 year:2016 day:10 month:04 pages:190-195 extent:6 https://doi.org/10.1016/j.physletb.2016.02.016 Volltext GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA 77.50 Psychophysiologie VZ AR 755 2016 10 0410 190-195 6 |
| language |
English |
| source |
Enthalten in Applying the Go/NoGo processing schema to a visual oddball task in older adults Amsterdam volume:755 year:2016 day:10 month:04 pages:190-195 extent:6 |
| sourceStr |
Enthalten in Applying the Go/NoGo processing schema to a visual oddball task in older adults Amsterdam volume:755 year:2016 day:10 month:04 pages:190-195 extent:6 |
| format_phy_str_mv |
Article |
| bklname |
Psychophysiologie |
| institution |
findex.gbv.de |
| topic_facet |
Heavy quarks TeV scale pseudoscalars Axizillas Di-photon Discrete symmetry |
| dewey-raw |
530 |
| isfreeaccess_bool |
false |
| container_title |
Applying the Go/NoGo processing schema to a visual oddball task in older adults |
| authorswithroles_txt_mv |
Kim, Jihn E. @@aut@@ |
| publishDateDaySort_date |
2016-01-10T00:00:00Z |
| hierarchy_top_id |
ELV000151122 |
| dewey-sort |
3530 |
| id |
ELV014077124 |
| language_de |
englisch |
| fullrecord |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">ELV014077124</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230625112900.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">180602s2016 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1016/j.physletb.2016.02.016</subfield><subfield code="2">doi</subfield></datafield><datafield tag="028" ind1="5" ind2="2"><subfield code="a">GBV00000000000204A.pica</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)ELV014077124</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(ELSEVIER)S0370-2693(16)00112-X</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">DE-600</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">610</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">77.50</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Kim, Jihn E.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Is an axizilla possible for di-photon resonance?</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2016transfer abstract</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">6</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">z</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zu</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 .</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 .</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">Heavy quarks</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">TeV scale pseudoscalars</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">Axizillas</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">Di-photon</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">Discrete symmetry</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="n">North-Holland Publ</subfield><subfield code="a">Steiner, Genevieve Z. ELSEVIER</subfield><subfield code="t">Applying the Go/NoGo processing schema to a visual oddball task in older adults</subfield><subfield code="d">2016</subfield><subfield code="g">Amsterdam</subfield><subfield code="w">(DE-627)ELV000151122</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:755</subfield><subfield code="g">year:2016</subfield><subfield code="g">day:10</subfield><subfield code="g">month:04</subfield><subfield code="g">pages:190-195</subfield><subfield code="g">extent:6</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doi.org/10.1016/j.physletb.2016.02.016</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ELV</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHA</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">77.50</subfield><subfield code="j">Psychophysiologie</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">755</subfield><subfield code="j">2016</subfield><subfield code="b">10</subfield><subfield code="c">0410</subfield><subfield code="h">190-195</subfield><subfield code="g">6</subfield></datafield></record></collection>
|
| author |
Kim, Jihn E. |
| spellingShingle |
Kim, Jihn E. ddc 530 ddc 610 bkl 77.50 Elsevier Heavy quarks Elsevier TeV scale pseudoscalars Elsevier Axizillas Elsevier Di-photon Elsevier Discrete symmetry Is an axizilla possible for di-photon resonance? |
| authorStr |
Kim, Jihn E. |
| ppnlink_with_tag_str_mv |
@@773@@(DE-627)ELV000151122 |
| format |
electronic Article |
| dewey-ones |
530 - Physics 610 - Medicine & health |
| delete_txt_mv |
keep |
| author_role |
aut |
| collection |
elsevier |
| remote_str |
true |
| illustrated |
Not Illustrated |
| topic_title |
530 DE-600 610 VZ 77.50 bkl Is an axizilla possible for di-photon resonance? Heavy quarks Elsevier TeV scale pseudoscalars Elsevier Axizillas Elsevier Di-photon Elsevier Discrete symmetry Elsevier |
| topic |
ddc 530 ddc 610 bkl 77.50 Elsevier Heavy quarks Elsevier TeV scale pseudoscalars Elsevier Axizillas Elsevier Di-photon Elsevier Discrete symmetry |
| topic_unstemmed |
ddc 530 ddc 610 bkl 77.50 Elsevier Heavy quarks Elsevier TeV scale pseudoscalars Elsevier Axizillas Elsevier Di-photon Elsevier Discrete symmetry |
| topic_browse |
ddc 530 ddc 610 bkl 77.50 Elsevier Heavy quarks Elsevier TeV scale pseudoscalars Elsevier Axizillas Elsevier Di-photon Elsevier Discrete symmetry |
| format_facet |
Elektronische Aufsätze Aufsätze Elektronische Ressource |
| format_main_str_mv |
Text Zeitschrift/Artikel |
| carriertype_str_mv |
zu |
| hierarchy_parent_title |
Applying the Go/NoGo processing schema to a visual oddball task in older adults |
| hierarchy_parent_id |
ELV000151122 |
| dewey-tens |
530 - Physics 610 - Medicine & health |
| hierarchy_top_title |
Applying the Go/NoGo processing schema to a visual oddball task in older adults |
| isfreeaccess_txt |
false |
| familylinks_str_mv |
(DE-627)ELV000151122 |
| title |
Is an axizilla possible for di-photon resonance? |
| ctrlnum |
(DE-627)ELV014077124 (ELSEVIER)S0370-2693(16)00112-X |
| title_full |
Is an axizilla possible for di-photon resonance? |
| author_sort |
Kim, Jihn E. |
| journal |
Applying the Go/NoGo processing schema to a visual oddball task in older adults |
| journalStr |
Applying the Go/NoGo processing schema to a visual oddball task in older adults |
| lang_code |
eng |
| isOA_bool |
false |
| dewey-hundreds |
500 - Science 600 - Technology |
| recordtype |
marc |
| publishDateSort |
2016 |
| contenttype_str_mv |
zzz |
| container_start_page |
190 |
| author_browse |
Kim, Jihn E. |
| container_volume |
755 |
| physical |
6 |
| class |
530 DE-600 610 VZ 77.50 bkl |
| format_se |
Elektronische Aufsätze |
| author-letter |
Kim, Jihn E. |
| doi_str_mv |
10.1016/j.physletb.2016.02.016 |
| dewey-full |
530 610 |
| title_sort |
is an axizilla possible for di-photon resonance? |
| title_auth |
Is an axizilla possible for di-photon resonance? |
| abstract |
Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . |
| abstractGer |
Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . |
| abstract_unstemmed |
Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 . |
| collection_details |
GBV_USEFLAG_U GBV_ELV SYSFLAG_U SSG-OLC-PHA |
| title_short |
Is an axizilla possible for di-photon resonance? |
| url |
https://doi.org/10.1016/j.physletb.2016.02.016 |
| remote_bool |
true |
| ppnlink |
ELV000151122 |
| mediatype_str_mv |
z |
| isOA_txt |
false |
| hochschulschrift_bool |
false |
| doi_str |
10.1016/j.physletb.2016.02.016 |
| up_date |
2024-07-06T20:31:06Z |
| _version_ |
1803863055138816000 |
| fullrecord_marcxml |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">ELV014077124</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230625112900.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">180602s2016 xx |||||o 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1016/j.physletb.2016.02.016</subfield><subfield code="2">doi</subfield></datafield><datafield tag="028" ind1="5" ind2="2"><subfield code="a">GBV00000000000204A.pica</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)ELV014077124</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(ELSEVIER)S0370-2693(16)00112-X</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">DE-600</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">610</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">77.50</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Kim, Jihn E.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Is an axizilla possible for di-photon resonance?</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2016transfer abstract</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">6</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">z</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zu</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 .</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Heavy axion-like particles, called axizillas, are simple extensions of the standard model (SM). An axizilla is required not to couple to the quarks, leptons, and Brout–Englert–Higgs doublets of the SM, but couple to the gauge anomalies of the W ± , Z and photon. It is possible to have its branching ratios (BRs) to two photons greater than 10 % and to two Z's less than 10 %. To have a (production cross section) ⋅ (BR to di-photons) at a 10 − 38 cm 2 level, a TeV scale heavy quark Q is required for the gluon–quark fusion process. The decay of Q to axizilla plus quark, and the subsequent decay of the axizilla to two photons can be fitted at the required level of 10 − 38 cm 2 .</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">Heavy quarks</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">TeV scale pseudoscalars</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">Axizillas</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">Di-photon</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="650" ind1=" " ind2="7"><subfield code="a">Discrete symmetry</subfield><subfield code="2">Elsevier</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="n">North-Holland Publ</subfield><subfield code="a">Steiner, Genevieve Z. ELSEVIER</subfield><subfield code="t">Applying the Go/NoGo processing schema to a visual oddball task in older adults</subfield><subfield code="d">2016</subfield><subfield code="g">Amsterdam</subfield><subfield code="w">(DE-627)ELV000151122</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:755</subfield><subfield code="g">year:2016</subfield><subfield code="g">day:10</subfield><subfield code="g">month:04</subfield><subfield code="g">pages:190-195</subfield><subfield code="g">extent:6</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://doi.org/10.1016/j.physletb.2016.02.016</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ELV</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHA</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">77.50</subfield><subfield code="j">Psychophysiologie</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">755</subfield><subfield code="j">2016</subfield><subfield code="b">10</subfield><subfield code="c">0410</subfield><subfield code="h">190-195</subfield><subfield code="g">6</subfield></datafield></record></collection>
|
| score |
7.3995686 |