Search

Minimal SO(10) models which utilize a 126-plet of Higgs for breaking B - L symmetry are quite predictive for the neutrino oscillation parameters. These models have been known to predict sin2 2θ13 ≃ 0.09, which is consistent with recent measurements. It is shown that the same class of models generates naturally baryon number violating dimension seven operators leading to novel nucleon decay modes such as n → e−K+, e−π+ and p → νπ+ which violate B - L by two units. In two-step breaking schemes of non-supersymmetric SO(10), the partial lifetimes for these modes can be within reach of experiments. The interactions responsible for these decay modes also provide a new way to understand the origin of matter in the universe via the decays of colored scalar bosons with GUT scale masses. Their (B - L)-violating nature guarantees that the GUT scale induced baryon asymmetry is not washed out by the electroweak sphaleron interactions. In minimal SO(10) models this asymmetry is closely tied to the masses of quarks, lep...

The standard model extended by three vector-like families with masses of order 1 TeV – 100 TeV allows for unification of gauge couplings. The values of gauge couplings at the electroweak scale are highly insensitive to fundamental parameters. The grand unification scale is large enough to avoid the problem with fast proton decay. The electroweak minimum of the Higgs potential is stable.

It is shown that the minimal renormalizable supersymmetric SU(5) grand unified theory can be made realistic by the inclusion of a single vectorlike 5 + 5 pair. Such a modification can at the same time correct the usual bad mass relations for the first two generations and safely increase the nucleon lifetime. The model predicts the lifetime of at least some decay rate to be less than approximately 1034 yrs, provided that all the superpartners of the minimal supersymmetric standard model lie below 3 TeV. The two statements will be tested by the next proton decay measurements and LHC, respectively.

The model of supersymmetric SU(5) GUT augmented with anomaly free U(1)F flavor symmetry is presented. The field content and the U(1)F charge assignment is obtained by specific embedding of SU(5) × U(1)F in larger non-Abelian group. We focus on a particular case which gives very economical field content with the U(1)F charges fixed in such a way that for quarks and leptons appealing texture zero Yukawa couplings are generated. The model gives realistic fermion masses and mixings and predict inverted hierarchical neutrino mass scenario with interesting implications.

The Standard Model Higgs boson with the nonminimal coupling to the gravitational curvature can drive cosmological inflation. We study this type of inflationary scenario in the context of supergravity. We first point out that it is naturally implemented in the minimal supersymmetric SU(5) model, and hence virtually in any GUT models. Next we propose another scenario based on the Minimal Supersymmetric Standard Model supplemented by the right-handed neutrinos. These models can be tested by new observational data from the Planck satellite experiments within a few years.

We report on the calculation of the matrix elements of nucleon to pseudoscalar decay through a three quark operator, a part of the low-energy, four-fermion, baryon-number-violating operator originating from grand unified theories. The direct calculation of the form factors using domain-wall fermions on the lattice, incorporating the u, d and s sea-quarks effects yields the results with all the relevant systematic uncertainties controlled for the first time.

Among three typical energy scales, a neutrino mass scale (mν∼0.1eV), a GUT scale (MGUT∼1016GeV), and a TeV-scale (MNP∼1TeV), there is a fascinating relation of MNP≃mν⋅MGUT The TeV-scale, MNP, is a new physics scale beyond the standard model which is regarded as "supersymmetry" (SUSY) in this letter. We investigate phenomenology of SUSY SU(5) GUT with neutrinophilic Higgs, which realizes the above relation dynamically as well as the suitable magnitude of Dirac mass, mν, through a tiny vacuum expectation value of neutrinophilic Higgs. As a remarkable feature of this model, accurate gauge coupling unification can be achieved as keeping with a proton stability. We also evaluate flavor changing processes in quark/lepton sectors.

In the natural GUT, not only realistic quark and lepton mass matrices can be obtained but also the most serious problem in the SUSY GUT, which is called the doublet-triplet splitting problem, can be solved under the natural assumption that all the interactions which are allowed by the symmetry are introduced with O(1) coefficients (including the higher dimensional operators). In this manuscript, we examine several cosmological aspects which are related with the natural GUT, B - L-genesis, non-thermal production of dark matter (DM), vacuum selection by particle production, and the inflation after the trapping. These works are based on several papers[1, 2, 3] collaborated with S. Enomoto, S. Iida, Y. Kurata, and T. Matsuda.

We examined the neutrino sector in E6×SU(2)F SUSY GUT with spontaneous CP violation. At a first glance, the discrete symmetry, which is introduced in order to solve the SUSY CP problem, constrains the allowed operators too strongly for the neutrino sector to be consistent with the experimental data, i.e., the μ neutrino becomes massless as commented in the previous work. We showed that this issue can be solved if some operators are taken into account. The predictions on the neutrino masses and mixings are the same as the E6 models, which are consistent with various experiments on the neutrino oscillations.

In F-term supergravity inflation models, scalar fields other than the inflaton generically receive a Hubble induced mass, which may restore gauge symmetries during inflation and phase transitions may occur during or after inflation as the Hubble parameter decreases. We study topological defect formation associated with such a phase transition in chaotic inflation in supergravity and obtain a severe constraint on the symmetry breaking scale which is related with the tensor-to-scalar ratio. This talk is based on the paper [1].

Diverse mass and mixing patterns between the quarks and leptons makes it challenging to construct a simple grand unified theory of flavor. The SO(10) SUSY GUT with type II seesaw mechanism giving neutrino masses provide a natural framework for addressing this issue. Proton decay suppression is also an important issue to construct SUSY GUT models. We will investigate the flavor structure which are favored to suppress proton decay in SUSY GUT models. The structure in the SO(10) GUT model provides a prediction of the neutrino mixing, and the lepton flavor violating decays will be an important probe of the model.

A central ingredient in many string based Grand Unified Theories (GUTs) is p-branes filling our spacetime and wrapping some number of internal directions. In this talk we discuss the potential role of D3-branes sitting at a point of the internal geometry in an F-theory GUT. These D3-branes can naturally realize additional superconformal sectors which can couple to the states of the Standard Model. We explain how detailed features of these sectors and their impact on the visible sector can be extracted. Additionally, we explain how in scenarios where the scale of conformal symmetry breaking is close to the weak scale, this extra sector can modify the physics of the Higgs.

The problems of renormalizable minimal SUSY SO(10) GUT in 4D are discussed. Its highly predictivity has been charged with many observations, which urges further progresses. We show why and how broad data fittings and conceptual problems drive us to 5D and how it improves the model., 7 pages, 2 figures, talk given at GUT2012

I present a new solution to the doublet-triplet splitting problem which works also in a SUSY SU(5) GUT and is testable at TeV-scale collider experiments. In this model, the SU(5) symmetry is broken through the Hosotani mechanism. Thanks to the phase nature of the Hosotani-breaking, the so-called "missing VEV" can be realized even in an SU(5) model to solve the problem. A general and distinctive prediction of this solution is the existence of light adjoint chiral supermultiplets with masses of the SUSY breaking scale which would be observed at the LHC.

Minimal SO(10) models which utilize a 126–plet of Higgs for breaking B – L symmetry are predictive schemes for neutrino masses and mixings. These models have been known to predict sin22θ13≃0.09, which is consistent with recent measurements. It is shown that the same class of models generates naturally baryon number violating dimension seven operators leading to novel nucleon decay modes such as n→e−K+, e−π+ and p→νπ+ which violate B – L by two units. We find that in two–step breaking schemes of non-supersymmetric SO(10), the partial lifetimes for these modes can be within reach of experiments. The interactions responsible for these decay modes also provide a new way to understand the origin of matter in the universe via the decays of GUT scale colored scalar bosons. Their (B – L)–violating nature guarantees that the GUT scale induced baryon asymmetry is not washed out by the electroweak sphaleron interactions. In minimal SO(10) models this asymmetry is closely tied to the masses of quarks, leptons and the...

Anomalous U(1)A SUSY GUT models are atractive because they can solve many difficulties in SUSY GUT models. In anomalous U(1)A SUSY GUT models, nucleon decay amplitudes of dim 6 effective interactions are larger than that of dim 5 effective interactions. Then, I discuss dim 6 effective interactions in some models, and predict proton lifetimes for many decay modes by calculating interactions. First, I fix unitary matrices that make Yukawa coupling matrices diagonalize, and predict proton lifetimes. Second, I study uncertainties of these unitary matrices, and show these effects on proton lifetimes. From these results, I show that we can distinguish some models from by nucleon decay.

We consider string realization of E6 SUSY GUT with adjoint Higgs fields in heterotic string theory. We require minimum phenomenological requirements for E6 SUSY GUTs (four-dimensional N = 1 supersymmetry, E6 grand unified group, three generations and adjoint representation Higgs fields) for our string model building. In order to realize an adjoint Higgs field, we use diagonal embedding method and utilize lattice engineering technique for the model building. In the framework of Z12 heterotic asymmetric orbifold construction, we obtain two more three-family E6 models with an adjoint Higgs field.

Obtaining a unified description of the quasi‐degenerate neutrino mass spectrum together with the hierarchical charged fermions is a challenging task. In this talk, we discuss two distinct possible scenarios leading to such spectra in the supersymmetric SO(10) grand unified framework. Consistency of both scenarios is demonstrated through detailed fits to fermion masses and mixing angles, all of which can be explained with reasonable accuracy in a model with the most general Yukawa sector of SO(10). The origin of large neutrino mixing angles is linked to neutrino mass degeneracy in both the scenarios.

Neutrino interactions in the few to few tens of MeV range are of importance for several physics topics, including solar, supernova and reactor neutrinos, as well as future proposed oscillation and Standard Model test experiments. Although interaction cross‐sections for some simple targets are well understood, very little experimental data exist for interactions with nuclei. This talk will discuss the motivation for measuring low energy neutrino interactions, the state of knowledge, and possible future strategies.

We examine the effects of the uncertainty of the top quark mass on the standard running analysis such as Higgs physics and the scalar quark sector of the MSSM.

An experiment designed to measure parity violation in the deep inelastic scattering of electrons from deuterium by using a novel solenoidal spectrometer (SoLID) has recently been approved at JLab. The main goal of the experiment is to make a precise measurement of the parity-violating coupling of the electron to the axial current of the quark. By covering a broad range of kinematics, the experiment will also search for charge symmetry violation in the structure functions. In addition the experiment is sensitive to di-quarks.

We briefly review the Standard Model prediction of g−2 and confront it with the formidably accurate measurement from BNL. The focus is on recent improvements of the hadronic vacuum polarisation contributions. We also calculate the running QED coupling at the scale of the Z boson mass, α(MZ2), an important ingredient in electroweak precision fits.

I show that the weak value theory is useful from the viewpoints of the experimentally verifiability, consistency, capacity for explanation as to many quantum paradoxes, and practical advantages. As an example, the initial state in the Hardy paradox can be experimentally verified using the weak value via the weak measurement.

The origins of baryons and dark matter have been considered to be unrelated. We discuss the probability that both of the baryon number and dark matter arise from the same origin in the supersymmetric anomalous U(1) grand unified theory. We derive some conditions to make this scenario successful, and show they can be satisfied with appropriate model parameters.

We present the results of searches for supersymmetry signatures in jets and photons events produced in pp collisions at s = 1.96 TeV. These results are based on up to 2.6 fb−1 of data collected by the CDF detector in the Tevatron Run II. They include a search for squarks and gluinos in events with multiple jets and large missing transverse energy, a search for the supersymmetric partners of the bottom quark, and searches for a long lived neutralino using photons. Observed rates in all these channels are consistent with the standard model predictions and thus limits on masses of various supersymmetric particles are presented.

We discuss status of the minimal supersymmetric SO(10) in both low and split supersymmetry regime. To demonstrate viability of the model we present a good fit of the fermion masses and their mixings. The solution needs a strongly split supersymmetry with gauginos and higgsinos around 102 TeV, sfermions close to 1014 GeV and a GUT scale of around 6×1015 GeV. It predicts fast proton decay rates, hierarchical neutrino masses and large leptonic mixing angle sinθ13≈0.1.

After a decade of design, construction, improvement, data‐taking, simulation, and analysis, the TRIUMF Weak Interaction Symmetry Test (TWIST) muon decay parameter measurements are nearly complete. While the final results are yet to be unblinded, a preliminary estimate of the final precision is available. The goal of an order‐of‐magnitude improvement on pre‐TWIST precisions for the ρ, δ, and Pμξ decay parameters has essentially been achieved, making possible some tighter constraints on parameters of the left‐right symmetric extension to the standard model as well as the fundamental coupling constants of the muon.

Do not replace the word “abstract,” but do replace the rest of this text. Text should remain 10‐pt. If you must insert a hard line break, please use Shift+Enter rather than just tapping your “Enter” key. You may want to print this page and refer to it as a style sample before you begin working on your paper. For an experimentalist in high energy physics, the most interesting experiments that one should pursue is often well known. The very rare CP violating decay of the kaon into a pion and two neutrinos (both the charged and neutral modes) is such an experiment. We have recently proposed the charged kaon experiment to Fermilab as proposal P966. We present her a general overview of that proposal. The goal is to obtain of order 1000 events in order to confront the expected theoretical calculations and to search for physics beyond the standard model.

On November 2009 the Large Hadron Collider produced the first p+p collisions. These, together with the upcoming Pb+Pb data, open up the possibility to answer some of the intriguing questions regarding the Standard Model and likely bring to light new phenomena. In this work I present a short review of the mexican participation in the ALICE experiment, focusing on the detector building and phenemological as well as Monte Carlo simulation work regarding the proton as well as the heavy ion program. I also briefly mention some of the wide spectrum of possible first topics that can be analyzed.

It is still a mystery why the Standard Model as we know it has only three families. At new high energy colliders it is worthwhile to search for a new additional family which obviously would have a heavy neutrino to avoid the LEP bounds. This paper discusses new studies made with the CMS detector for the search of new heavy b‐like quarks in several different decay modes and for different possible mass regions. These studies are based on detailed detector simulation, including all Standard Model backgrounds. Particular emphasis is given to possible early discoveries, i.e. with 100 pb−1 or less. Projected 95% CL exclusion limits as a function of luminosity are presented as well.

Motivated by the recent idea of the “unified explanation” for the Dark Matter (DM) we introduce an explicit model of this kind. The model is built in the context of TeV‐scale supersymmetry (SUSY) and involves high‐scale SUSY‐breaking. In the current talk we briefly describe this model and further elaborate its phenomenological features. In particular we comment on current astrophysical constraints and describe experimental signatures the model predicts.

We discuss the simplest models for the generation of neutrinos masses at tree level and one‐loop level. The realization of the different seesaw mechanisms in the context of renormalizable SU(5) and SO(10) theories is reviewed. A new mechanism for the generation of neutrino masses at one‐loop level is presented. We discuss the first realization of the Type III seesaw mechanism in the context of a renormalizable SU(5) theory, called “Adjoint SU(5).”

We present a Majorana neutrino scenario in a F‐theory SU(5) GUT model, which is recently proposed in [1]. The mass scale of the neutrinos arises from integrating out heavy Kaluza‐Klein modes on the right‐handed neutrinos. The participation of non‐holomorphic Kaluza‐Klein mode wave functions dilutes the mass hierarchy in comparison to the quark and charged lepton sectors, in agreement with experimentally measured mass splittings. The neutrinos are predicted to exhibit a “normal” mass hierarchy, with masses (m3, m2, m1) ∼.05×(1,αGUT1/2,αGUT) eV. The neutrino mixing matrix exhibits a mild hierarchical structure with θ13∼αGUT1/2∼0.2. We also predict mass measurements in single and double beta decay experiments.

The Qweak collaboration is currently preparing a measurement of the proton’s weak charge QWp = (1–4 sin2θW) at the Thomas Jefferson National Accelerator Facility (TJNAF). The experiment has been designed to produce a 4.1% measurement of the weak charge, via a 2.5% measurement of the parity violating asymmetry in the number of elastically scattered 1 GeV electrons from protons, at forward angles. At the proposed precision, the experiment would produce a 0.3% measurement of the weak mixing angle at a momentum transfer of ≈ = 16 GeV, making it the most precise stand alone measurement of the weak mixing angle at low momentum transfer. In combination with other parity measurements, Qweak will also provide a high precision determination of the weak charges of the up and down quarks. Our proposed measurement of QWp will be performed with significantly smaller statistical and systematic errors than existing low Q2 data. Any significant deviation from the Standard Model prediction at low momentum transfer (Q2) wou...

Within the framework of the standard model (SM) of elementary particles and the two Higgs doublet extension to this model (2DHM), we obtained analytical and numerical solutions for the gauge couplings, the vacuum expectation values (VEV) of the Higgs fields, the quark Yukawa couplings and quark masses, the quartic Higgs couplings, and the running Higgs masses, considering the renormalization group equations. The bounds on the SM Higgs running mass have been fixed, and the region of validity of the SM was determined through it, at the one and two loop approximations, using the triviality and stability conditions for the Higgs quartic coupling {lambda}{sub H}.

Advanced analysis techniques together with increasing data samples are bringing the sensitivity of CDF to the Higgs boson very close to the SM predictions. These improvements translate into more stringent exclusions of parameter space in BSM Higgs sectors and of the SM mass range. The CDF Collaboration has a very active program on Higgs searches that comprises most accessible production mechanisms and decay channels in pp collisions at s = 1.96 TeV. This contribution will also review the combination of the different channels, data samples and analysis techinques that currently produces one of the most exciting experimental results in our field.

We discuss the direct detection prospects for neutralino dark matter via elastic scattering in variations of the MSSM with non‐universal supersymmetry‐breaking contributions to the Higgs masses. Taking as our starting point the CMSSM, in which supersymmetry‐breaking contributions to all scalar masses are universal, we examine scenarios in which both Higgs scalar masses are non‐universal by the same amount (NUHM1) and scenarios in which the Higgs scalar masses are independently non‐universal (NUHM2).

A prospective analysis is presented on the observability of the Standard Model Higgs boson produced in the Vector Boson fusion and decaying into τ pairs with the ττ→lvv+vτ−jet final state. The estimates of the upper limit on the cross section times branching ratio for 1 fb−1 for the Higgs boson mass interval 115–145 GeV/c2 are given.

We review unification ideas and explain the spin‐extended model in this context. Its consideration is also motivated by the standard‐model puzzles. With the aim of constructing a common description of discrete degrees of freedom, as spin and gauge quantum numbers, the model departs from q‐bits and generalized Hilbert spaces. Physical requirements reduce the space to one that is represented by matrices. The classification of the representations is performed through Clifford algebras, with its generators associated with Lorentz and scalar symmetries. We study a reduced space with up to two spinor elements within a matrix direct product. At given dimension, the demand that Lorentz symmetry be maintained, determines the scalar symmetries, which connect to vector‐and‐chiral gauge‐interacting fields; we review the standard‐model information in each dimension. We obtain fermions and bosons, with matter fields in the fundamental representation, radiation fields in the adjoint, and scalar particles with the Higgs quantum numbers. We relate the fields’ representation in such spaces to the quantum‐field‐theory one, and the Lagrangian. The model provides a coupling‐constant definition.

In this work, the electroweak phase transition (EWPT) strength has been investigated within the U(1) extended Minimal Supersymmetric Standard Model (UMSSM) without introducing any exotic fields. We found that the EWPT could be strongly first order for reasonable values of the lightest Higgs and neutralino masses.

Modern theories of everything, or theories of the grand unification of all physical interactions, try to describe the whole world starting from the first principles of quantum theory. However, the first principles operate with undetermined notions, such as the wave ψ‐function, particle, lepton and quark, de Broglie and Compton wavelengths, mass, electric charge, spin, electromagnetic field, photon, gravitation, physical vacuum, space, etc. From a logical point of view this means that such modern approach to the theory of everything is condemned to failure… Thus, what should we suggest to improve the situation? It seems quite reasonable to develop initially a theory of something, which will be able to clarify the major fundamental notions (listed above) that physics operates with every day. What would be a starting point in such approach? Of course a theory of space as such, because particles and all physical fields emerge just from space. After that, when a particle and fields (and hence the fields’ carriers) are well defined and introduced in the well defined physical space, different kinds of interactions can be proposed and investigated. Moreover, we must also allow for a possible interaction of a created particle with the space that generated the appearance of the particle. The mathematical studies of Michel Bounias and the author have shown what the real physical space is, how the space is constituted, how it is arranged and what its elements are. Having constructed the real physical space we can then derive whatever we wish, in particular, such basic notions as mass, particle and charge. How are mechanics of such objects (a massive particle, a charged massive particle) organised? The appropriate theory of motion has been called a sub microscopic mechanics of particles, which is developed in the real physical space, not an abstract phase space, as conventional quantum mechanics does. A series of questions arise: can these two mechanics (submicroscopic and conventional quantum mechanics) be unified?, what can such unification bring new for us?, can such submicroscopic mechanics be a starting point for the derivation of the phenomenon of gravity?, can this new theory be a unified physical theory?, does the theory allow experimental verification? These major points have been clarified in detail. And, perhaps, the most intriguing aspect of the theory is the derivation of a new physical field associated with the notion of mass (or rather inertia of a particle, which has been called the inerton field and which represents a real sense of the particle’s wave ψ‐function). This field emerges by analogy with the electromagnetic field associated with the notion of the electric charge. Yes, the postulated inerton field has being tested in a series of different experiments! Even more, the inerton field might have a number of practical applications…

In this talk, we present our calculations for the next‐to‐leading order(NLO) QCD corrections to the cross sections (CS) of the associate production processes pp→gq→qiχj±+X with q = (u,d) in the constrained minimal supersymmetric standard model in the CERN LHC experiments. The NLO QCD corrections can in general provide a 30–40% enhancement to the corresponding cross sections, and significantly reduce the dependence of the total cross section on the renormalization and factorization scales.

In anticipation of data from the Large Hadron Collider (LHC) and the potential discovery of supersymmetry, we calculate the odds of the next‐to‐minimal version of the popular supergravity motivated model (NmSuGra) being discovered at the LHC to be 4:3 (57%). We also demonstrate that viable regions of the NmSuGra parameter space outside the LHC reach can be covered by upgraded versions of dark matter direct detection experiments, such as super‐CDMS, at 95% confidence level. Due to the similarities of the models, we expect very similar results for the constrained minimal supersymmetric standard model (CMSSM).

A pure NCG leptonic asymmetry is obtained for particles propagating in a curved non commutative FRW universe. It is shown that because of the space‐time deformation, an axial like symmetry is generated.

The existence of additional vector bosons are theoretically well motivated, arising naturally in many extensions of the Standard Model. Experimentally, such particles typically have clean signatures and therefore should be observed in hadron colliders if they are produced. We review recent searches for heavy vector bosons with CDF at the Tevatron and provide limits on their production.

We study the effects of a fourth generation t-prime quark in various extensions of the standard model. In the Randall-Sundrum model, the decay t-prime -> t Z has a large branching ratio that could be detected at the Large Hadron Collider (LHC). We also look at the two-Higgs doublet models I, II and III, and note that, in the latter, the branching ratio of t-prime -> t H, where H is a Higgs scalar or pseudoscalar, is huge and we discuss detection at the LHC., 4 pages, 2 figures, to be published in the proceedings of DPF-2009, Detroit, MI, July 2009, eConf C090726

A search for the standard model Higgs boson in pp collisions with s = 1.96 TeV at the Fermilab Tevatron collider is discussed. Recent preliminary results on the Higgs boson production cross section limit obtained by the DO/ collaboration using integrated luminosities up to 4.2 fb1 is presented.

A brief outlook, in two senses, is presented for hadronic physics. The likely near term future for experiment and lattice effort is sketched and I speculate on future directions in theory. I also look out at other fields, presenting a short review of QCD ideas in “Beyond the Standard Model” physics.

We present a curvaton model from type IIB string theory compactified on a warped throat with approximate isometries. Considering an (anti‐)D3‐brane sitting at the throat tip as a prototype standard model brane, we show that the brane’s position in the isometry directions can play the role of curvatons. The basic picture is that the fluctuations of the (anti‐)D3‐brane in the angular isometry directions during inflation eventually turns into the primordial curvature perturbations, and subsequently the brane’s oscillation excites other open string modes on the brane and reheat the universe. We find in the explicit case of the KS throat that a wide range of parameters allows a consistent curvaton scenario. It is also shown that the oscillations of branes at throat tips are capable of producing large non‐Gaussianity, either through curvature or isocurvature perturbations. Since such setups naturally arise in warped (multi‐)throat compactifications and are constrained by observational data, the model can provide tests for compactification scenarios. This work gives an explicit example of string theory providing light fields for generating curvature perturbations. Such mechanisms free the inflaton from being responsible for the perturbations, thus open up new possibilities for inflation models. The discussions in this paper are based on [1].

We present the discovery potential for a heavy new resonance decaying into lepton pairs, or into a high pT lepton and missing ET, using the ATLAS detector at the LHC. The dilepton and lepton+ETmiss final states are robust signatures to look for new physics due to their simplicity. The unprecedented center‐of‐mass energy (c.m.e.) available allows exploring mass regions that are inaccessible to present colliders. The aim of this work is to study prospects for discovering BSM physics with an integrated luminosity in the range between 100 pb−1 and 10 fb−1 at 14 TeV c.m.e.