REVIEW
Higgs Boson Mass, Proton Decay, Naturalness and Constraints of LHC and Planck Data
High Energy Physics - Phenomenology · Submitted 29 Mar 2013 · 85 references
Pith's verdict: The Higgs-mass sensitivity of the p → ν̄K+ lifetime is the real result and it holds up; the naturalness claim in s6 is close to a tautology of the fine-tuning measure the authors chose.
T0 · AI review
Why Pith says this
Highlight any text to comment on it.
Referee report
The paper
The paper claims
In supergravity unified models the 126 GeV Higgs mass implies multi-TeV sfermions, making the p to anti-neutrino K+ lifetime extremely sensitive to the Higgs mass and shifting naturalness arguments toward a several-TeV SUSY scale.
The reading
Extended reading notes
Core claim
The paper's load-bearing assertion, from abstract:s2, is that over the allowed parameter space of supergravity unified models the proton lifetime for p to anti-neutrino K+ is highly sensitive to the Higgs boson mass, with a few-GeV shift changing the lifetime by as much as two orders of magnitude or more. If correct, this ties a measured quantity (the Higgs mass) to an unmeasured one (the proton lifetime) tightly enough that a future proton decay signal or null result would constrain the SUSY spectrum, and it makes the p to anti-neutrino K+ channel the priority target for next-generation detectors.
Load-bearing premise
The absolute proton lifetime, and therefore the proton-stability fine-tuning factor F_pd = 4e33 yr divided by the predicted lifetime (Eq. 24), is normalized by an effective Higgs triplet mass M_eff_H3/M_G that the authors choose by hand as 10, 25, or 50 (Sec. III, discussion around Eq. 9 and the Fig. 2 and Fig. 3 captions). The paper is explicit that it does not commit to a GUT structure and that M_eff_H3 can be made much larger than the GUT scale. Because F_pd is defined as a ratio to the experimental limit, the choice of M_eff_H3 directly sets the naturalness conclusion, so the claim that combined fine tuning favors several-TeV scalars rests on a knob rather than on a derived quantity.
Original abstract
A Higgs boson mass $\sim 126$ GeV as determined by the LHC data requires a large loop correction which in turn implies a large sfermion mass. Implication of this result for the stability of the proton in supersymmetric grand unified theories is examined including other experiments constraints along with the most recent result on cold dark matter from Planck. It is shown that over the allowed parameter space of supergravity unified models, proton lifetime is highly sensitive to the Higgs boson mass and a few GeV shift in its mass can change the proton decay lifetime for the mode $p\to \bar \nu K^+$ by as much as two orders of magnitude or more. An analysis is also given on the nature of radiative breaking of the electroweak symmetry in view of the high Higgs boson, and it is shown that most of the parameter space of universal and non-universal supergravity unified models lies on the Hyperbolic Branch of radiative breaking of the electroweak symmetry, while the Ellipsoidal Branch and the Focal Point regions are highly depleted and contain only a very small region of the allowed parameter space. Also discussed are the naturalness criteria when the proton stability constraints along with the electroweak symmetry breaking are considered together. It is shown that under the assumed naturalness criteria the overall fine tuning is improved for larger values of the scalar mass with the inclusion of the proton stability constraint. Thus the naturalness criteria including proton stability along with electroweak symmetry breaking constraints tend to favor the weak scale of SUSY in the several TeV region. Implications for the discovery of supersymmetry in view of the high Higgs mass are briefly discussed.
The compiled record
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
The abstract, sentence by sentence
A Higgs boson mass $\sim 126$ GeV as determined by the LHC data requires a large loop correction which in turn implies a large sfermion mass. Implication of this result for the stability of the proton in supersymmetric grand unified theories is examined including other experiments constraints along with the most recent result on cold dark matter from Planck. It is shown that over the allowed parameter space of supergravity unified models, proton lifetime is highly sensitive to the Higgs boson mass and a few GeV shift in its mass can change the proton decay lifetime for the mode $p\to \bar \nu K^+$ by as much as two orders of magnitude or more. An analysis is also given on the nature of radiative breaking of the electroweak symmetry in view of the high Higgs boson, and it is shown that most of the parameter space of universal and non-universal supergravity unified models lies on the Hyperbolic Branch of radiative breaking of the electroweak symmetry, while the Ellipsoidal Branch and the Focal Point regions are highly depleted and contain only a very small region of the allowed parameter space. Also discussed are the naturalness criteria when the proton stability constraints along with the electroweak symmetry breaking are considered together. It is shown that under the assumed naturalness criteria the overall fine tuning is improved for larger values of the scalar mass with the inclusion of the proton stability constraint. Thus the naturalness criteria including proton stability along with electroweak symmetry breaking constraints tend to favor the weak scale of SUSY in the several TeV region. Implications for the discovery of supersymmetry in view of the high Higgs mass are briefly discussed.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A Higgs boson mass $\sim 126$ GeV as determined by the LHC data requires a large loop correction which in turn implies a large sfermion mass. | background 0.41 | 0.18 | 0.10 | asserted 0.98 |
| s1 | Implication of this result for the stability of the proton in supersymmetric grand unified theories is examined including other experiments constraints along with the most recent result on cold dark matter from Planck. | contribution 0.95 | 0.65 | 0.05 | asserted 0.51 |
| s2 | It is shown that over the allowed parameter space of supergravity unified models, proton lifetime is highly sensitive to the Higgs boson mass and a few GeV shift in its mass can change the proton decay lifetime for the mode $p\to \bar \nu K^+$ by as much as two orders of magnitude or more. | result 1.00 | 0.85 | 0.23 | asserted 1.00 |
| s3 | An analysis is also given on the nature of radiative breaking of the electroweak symmetry in view of the high Higgs boson, and it is shown that most of the parameter space of universal and non-universal supergravity unified models lies on the Hyperbolic Branch of radiative breaking of the electroweak symmetry, while the Ellipsoidal Branch and the Focal Point regions are highly depleted and contain only a very small region of the allowed parameter space. | result 0.95 | 0.89 | 0.12 | asserted 1.00 |
| s4 | Also discussed are the naturalness criteria when the proton stability constraints along with the electroweak symmetry breaking are considered together. | contribution 0.99 | 0.60 | 0.05 | unclear 0.72 |
| s5 | It is shown that under the assumed naturalness criteria the overall fine tuning is improved for larger values of the scalar mass with the inclusion of the proton stability constraint. | result 0.96 | 0.88 | 0.15 | asserted 1.00 |
| s6 | Thus the naturalness criteria including proton stability along with electroweak symmetry breaking constraints tend to favor the weak scale of SUSY in the several TeV region. | interpretation 0.79 | 0.84 | 0.54 | asserted 0.72 |
| s7 | Implications for the discovery of supersymmetry in view of the high Higgs mass are briefly discussed. | interpretation 0.83 | 0.42 | 0.04 | unclear 0.96 |
What was examined, and what was not
- arXiv listing abstract v1
- full text
- figures and tables
- references and citing sentences
- relations to other papers
- P abstract
- S sections
- T body sentences
- C citations
- R cross-paper relations
Figures
Figures reproduced from arXiv:1303.7472 by the authors.
References
How the literature uses it
32 arXiv papers cite this in 44 sentences
Papers citing it · 37 sentences without a confident label
Uses its method or tool 1 paper
-
In this case a more appropriate object to consider is a composite fine tuning $F$ defined by [ref] [equation] An analysis of fine tunings defined by <ref>, <ref> and <ref> is given in Fig. 8 of [ref] .
Supersymmetry after the Higgs · Fine tuning · 0.89
Cites it as support 3 papers
-
This is due to the fact that the stop masses are driven to be large by the gluino, giving a large $Q=√(m_m_)$, and it was shown in [ref] that $Q≳1$ corresponds to a hyperbolic geometry of soft parameters that give radiative EWSB (a large SUSY scale in the tens of TeV also arises in a certain class of string motivated models [ref] ).
Gluino-driven Radiative Breaking, Higgs Boson Mass, Muon $\mathbf{g-2}$, and the Higgs Diphoton Decay in SUGRA Unification · Results · 0.97
-
Again scalar masses in the 50-100 TeV range resolve this problem in a natural way [ref] .
Supergravity Models with 50-100 TeV Scalars, SUSY Discovery at the LHC and Gravitino Decay Constraints · Conclusions · 0.99
-
For a low scale of weak scale supersymmetry, a suppression of this again requires a fine tuning but for scale of weak scale supersymmetry lying in the several TeV region this suppression is more easily accomplished [ref] .
Supersymmetry at a 28 TeV hadron collider: HE-LHC · Introduction · 0.97
Cites it as background 3 papers
-
For more detail related GUTs and $M_GUT$ related bosons see [ref] .
Probing the Supersymmetric Grand Unified Theories with Gravity Mediation at the Future Proton-Proton Colliders and Hyper-Kamiokande Experiment · Probing the Supersymmetric Grand Unified Theories at the Hyper-Kamiokande Experiment · 0.95
-
It has long been claimed that electroweak naturalness requires that the superpartners of the SM fields exist with masses of order the weak scale [ref] $m(sparticles)∼m_weak∼m_Z$.
SUSY models under siege: LHC constraints and electroweak fine-tuning · Introduction · 0.89
-
Instead of considering the global picture after the $125$ GeV Higgs discovery, which has been the aim of many studies in the past few years (see for example [ref] ), we focus in this work on one specific aspect of theories with additional Higgs doublets, namely, the presence of a charged Higgs boson, $H^±$.
Status of the Charged Higgs Boson in Two Higgs Doublet Models · Introduction · 0.95
What it cites · 26 sentences without a confident label
Uses data or values from 8 papers
-
Thus the ATLAS Collaboration finds a signal at $126.0 ±0.4 (stat)±0.4(sys) GeV$ which is at the $5.0σ$ level [ref] while the CMS Collaboration finds a signal at $125.3±0.4 (stat)±0.5(sys) GeV$ at the $5.0σ$ level [ref] .
Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC · Introduction · 0.99
-
Thus the ATLAS Collaboration finds a signal at $126.0 ±0.4 (stat)±0.4(sys) GeV$ which is at the $5.0σ$ level [ref] while the CMS Collaboration finds a signal at $125.3±0.4 (stat)±0.5(sys) GeV$ at the $5.0σ$ level [ref] .
Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC · Introduction · 0.99
-
This is done under the constraints of the most recent LHC searches [ref] and other experimental constraints including the most recent results from the Planck experiment [ref] .
Search for supersymmetry using final states with one lepton, jets, and missing transverse momentum with the ATLAS detector in sqrt{s} = 7 TeV pp · Higgs mass and branches of radiative breaking of the electroweak symmetry · 0.83
Cites as background 17 papers
-
In supersymmetric GUTs proton decay from dimension five operators depends very sensitively on the sparticle spectrum since the sparticle spectrum enters in the dressing loop diagrams which involve the exchange of squarks and sleptons, gluinos, charginos, and neutralinos [ref] (for recent reviews see [ref] ).
Fundamental Physics at the Intensity Frontier · Proton stability · 0.93
-
In supersymmetric GUTs proton decay from dimension five operators depends very sensitively on the sparticle spectrum since the sparticle spectrum enters in the dressing loop diagrams which involve the exchange of squarks and sleptons, gluinos, charginos, and neutralinos [ref] (for recent reviews see [ref] ).
DUSEL Theory White Paper · Proton stability · 0.93
-
We will also consider NuSUGRA models (for recent works on NuSUGRA see [ref] and for a review see [ref] .
Gluino NLSP, Dark Matter via Gluino Coannihilation, and LHC Signatures · Higgs mass and branches of radiative breaking of the electroweak symmetry · 0.92
Discussion
Disagree with the review, or know something it missed? Leave a comment, highlight any passage above to comment on it, or challenge this review formally.