83 research outputs found
Fitting Neutrino Physics with a U(1)_R Lepton Number
We study neutrino physics in the context of a supersymmetric model where a
continuous R-symmetry is identified with the total Lepton Number and one
sneutrino can thus play the role of the down type Higgs. We show that
R-breaking effects communicated to the visible sector by Anomaly Mediation can
reproduce neutrino masses and mixing solely via radiative contributions,
without requiring any additional degree of freedom. In particular, a relatively
large reactor angle (as recently observed by the Daya Bay collaboration) can be
accommodated in ample regions of the parameter space. On the contrary, if the
R-breaking is communicated to the visible sector by gravitational effects at
the Planck scale, additional particles are necessary to accommodate neutrino
data.Comment: 19 pages, 3 figures; v2: references added, constraints updated,
overall conclusions unchange
Dirac gauginos, R symmetry and the 125 GeV Higgs
We study a supersymmetric scenario with a quasi exact R-symmetry in light of the discovery of a Higgs resonance with a mass of 125 GeV. In such a framework, the additional adjoint superfields, needed to give Dirac masses to the gauginos, contribute both to the Higgs mass and to electroweak precision observables. We analyze the interplay between the two aspects, finding regions in parameter space in which the contributions to the precision observables are under control and a 125 GeV Higgs boson can be accommodated. We estimate the fine-tuning of the model finding regions of the parameter space still unexplored by the LHC with a fine-tuning considerably improved with respect to the minimal supersymmetric scenario. In particular, sizable non-holomorphic (non-supersoft) adjoints masses are required to reduce the fine-tuning
"L = R" - U(1) R as the origin of leptonic 'RPV'
A classification of phenomenologically interesting supersymmetric extensions of the Standard-Model with a U(1) R symmetry is presented. Some of these are consistent with subsets of leptonic or baryonic "R-parity violating" (RPV) operators, thereby providing a natural motivation for them. We then focus on a particular class of models in which the U(1) R symmetry coincides with lepton number when restricted to the SM sector. In this case, the extension of lepton number to the superpartners is "non-standard", implying, in particular, the existence of the leptonic RPV operators LLE c and LQD c, and a vacuum structure where one of the left-handed sneutrinos acquires a significant vacuum-expectation-value, while not being constrained by neutrino mass bounds. The model can be naturally consistent with bounds from electroweak precision measurements and flavor-changing processes. It can also easily accommodate the recently measured Higgs mass due to the existence of a scalar triplet that couples to the Higgs with an order one coupling, with only moderate fine-tuning. The phenomenology is rather rich and distinctive, with features such as heavy-but-natural Dirac gauginos, relaxed bounds on squarks, resonant slepton/sneutrino production, lepto-quark signals, as well as an interesting connection to neutrino physics arising from R-breaking. The broad qualitative features are discussed in this paper, with a more detailed phenomenological study carried out in a companion paper [1]
UV friendly T-parity in the SU(6)/Sp(6) little Higgs model
Electroweak precision tests put stringent constraints on the parameter space
of little Higgs models. Tree-level exchange of TeV scale particles in a generic
little Higgs model produce higher dimensional operators that make contributions
to electroweak observables that are typically too large. To avoid this problem
a discrete symmetry dubbed T-parity can be introduced to forbid the dangerous
couplings. However, it was realized that in simple group models such as the
littlest Higgs model, the implementation of T-parity in a UV completion could
present some challenges. The situation is analogous to the one in QCD where the
pion can easily be defined as being odd under a new symmetry in the
chiral Lagrangian, but this is not a symmetry of the quark Lagrangian. In
this paper we examine the possibility of implementing a T-parity in the low
energy model that might be easier to realize in the UV. In our
model, the T-parity acts on the low energy non-linear sigma model field in way
which is different to what was originally proposed for the Littlest Higgs, and
lead to a different low energy theory. In particular, the Higgs sector of this
model is a inert two Higgs doublets model with an approximate custodial
symmetry. We examine the contributions of the various sectors of the model to
electroweak precision data, and to the dark matter abundance.Comment: 21 pages,4 figures. Clarifications added, typos corrected and
references added. Published in JHE
R-parity violation in SU(5)
We show that judiciously chosen R-parity violating terms in the minimal
renormalizable supersymmetric SU(5) are able to correct all the
phenomenologically wrong mass relations between down quarks and charged
leptons. The model can accommodate neutrino masses as well. One of the most
striking consequences is a large mixing between the electron and the Higgsino.
We show that this can still be in accord with data in some regions of the
parameter space and possibly falsified in future experiments.Comment: 30 pages, 1 figure. Revised version. To appear in JHE
US Cosmic Visions: New Ideas in Dark Matter 2017: Community Report
This white paper summarizes the workshop "U.S. Cosmic Visions: New Ideas in
Dark Matter" held at University of Maryland on March 23-25, 2017.Comment: 102 pages + reference
How Many Supersymmetries?
Supersymmetry in the gauge sector could be realized as N=1 or N=2
Supersymmetry, but the current LHC searches assume an N=1 realization. In this
paper we show that squarks could be as light as few hundreds of GeV for N=2. We
also describe an experimental procedure to count the number of supersymmetries,
i.e. to distinguish between N=1 and N=2 supersymmetry, based on counting bins
with different jet multiplicities and number of leptons.Comment: 7 pages, 3 figure
Dirac gauginos and unification in F-theory
Supersymmetric models in which the gauginos acquire Dirac masses, rather than
Majorana masses, offer an appealing alternative to the minimal supersymmetric
standard model, especially in the light of the bounds set on superpartner
masses by the 2011 LHC data. Dirac gauginos require the presence of chiral
multiplets in the adjoint representation of the gauge group, and the
realisation of such scenarios in F-theory is the subject of this paper. The
chiral adjoints drastically alter the usual picture of gauge coupling
unification, but this is disturbed anyway in F-theory models with non-trivial
hypercharge flux. The interplay between these two factors is explored, and it
is found for example that viable F-theory unification can be achieved at around
the reduced Planck scale, if there is an extra vector-like pair of singlet
leptons with TeV-scale mass. I then discuss the conditions which must be
satisfied by the geometry and hypercharge flux of an F-theory model with Dirac
gauginos. One nice possibility is for the visible sector to be localised on a
K3 surface, and this is discussed in some detail. Finally, I describe how to
achieve an unbroken discrete R-symmetry in such compactifications, which is an
important ingredient in many models with Dirac gauginos, and write down a
simple example which has adjoint chiral multiplets, an appropriate R-symmetry,
and allows for viable breaking of SU(5) by hypercharge flux.Comment: 25 pages, 4 figures. v2: Minor changes; references added. v3: Section
4 modified and expanded; other minor change
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