equation 104.46 eq:ewh-yukawa-lagrangian
open in the book ·
parts/11-qft-standard-model/06-electroweak-higgs.tex:1611
- part of a statement or proof
Rests on
No declared or derived dependency edges point away from this node yet.
Supports
-
depends_on
proposition 104.61
The couplings are the masses divided by $v$
¶
-
assumes
experiment
The Higgs Boson Discovery
¶
- cites (method) derived bib 08 The ATLAS Experiment at the CERN Large Hadron Collider ¶
- cites (method) derived bib 08 The ATLAS Experiment at the CERN Large Hadron Collider ¶ ↺
- cites (method) derived bib 08 The ATLAS Experiment at the CERN Large Hadron Collider ¶ ↺
- cites (evidence) derived bib 1 Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC ¶
- cites (data) derived bib 1 Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC ¶ ↺
- cites (data) derived bib 1 Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC ¶ ↺
- cites (data) derived bib 1 Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC ¶ ↺
- cites (data) derived bib 1 Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC ¶ ↺
- cites (data) derived bib 1 Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC ¶ ↺
- cites (evidence) derived bib 1 Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC ¶ ↺
- cites (data) derived bib 1 Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC ¶ ↺
- cites (data) derived bib 1 Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC ¶ ↺
- … 128 more
-
depends_on
phenomenon 104.62
The scalar couples in proportion to mass
¶
- tests experiment The Higgs Boson Discovery ¶ ↺
- depends_on phenomenon 113.24 Couplings proportional to mass ¶
-
depends_on
proposition 113.5
One number is unknown, and it is the mass
¶
- depends_on phenomenon 113.17 A new boson near 125 GeV ¶
- depends_on proposition 113.12 Sensitivity is set by ratio, not by rate ¶
-
assumes
experiment
The Higgs Boson Discovery
¶
-
depends_on
proposition 104.42
The sources of custodial violation
¶
-
depends_on
proposition 104.43
The top contribution to $\rho$
¶
-
depends_on
phenomenon 113.6
The weak bosons are massive and the photon is not
¶
- depends_on phenomenon 113.17 A new boson near 125 GeV ¶ ↺
- depends_on phenomenon 103.19 The top mass was known before the top was seen ¶
-
depends_on
phenomenon 113.6
The weak bosons are massive and the photon is not
¶
-
depends_on
proposition 104.43
The top contribution to $\rho$
¶
-
depends_on
theorem 105.25
Number of physical phases
¶
-
depends_on
proposition 105.27
When $CP$ violation is possible
¶
- depends_on proposition 103.30 Area and the Jarlskog invariant ¶
-
depends_on
proposition 105.27
When $CP$ violation is possible
¶
-
depends_on
theorem 104.38
Masses, mixing, and where the CKM matrix comes from
¶
-
depends_on
phenomenon 104.59
A neutral scalar boson exists
¶
- tests experiment The Higgs Boson Discovery ¶ ↺
- depends_on phenomenon 103.10 There are no flavour-changing neutral currents ¶
- depends_on proposition 104.61 The couplings are the masses divided by $v$ ¶ ↺
-
depends_on
phenomenon 104.59
A neutral scalar boson exists
¶
Neighborhood
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Edges
| type | direction | node | provenance | where |
|---|---|---|---|---|
depends_on |
← | The couplings are the masses divided by $v$ | declared | parts/11-qft-standard-model/06-electroweak-higgs.tex:3188 |
depends_on |
← | The sources of custodial violation | declared | parts/11-qft-standard-model/06-electroweak-higgs.tex:1940 |
depends_on |
← | Number of physical phases | declared | parts/11-qft-standard-model/07-discrete-symmetries-cpt.tex:2079 |
depends_on |
← | Masses, mixing, and where the CKM matrix comes from | declared | parts/11-qft-standard-model/06-electroweak-higgs.tex:1674 |