Soft Terms Research Articles

Next-to-minimal SOFTSUSY

We describe an extension to the SOFTSUSY program that provides for the calculation of the sparticle spectrum in the Next-to-Minimal Supersymmetric Standard Model (NMSSM), where a chiral superfield that is a singlet of the Standard Model gauge group is added to the Minimal Supersymmetric Standard Model (MSSM) fields. Often, a Z3 symmetry is imposed upon the model. SOFTSUSY can calculate the spectrum in this case as well as the case where general Z3 violating (denoted as ▪) terms are added to the soft supersymmetry breaking terms and the superpotential. The user provides a theoretical boundary condition for the couplings and mass terms of the singlet. Radiative electroweak symmetry breaking data along with electroweak and CKM matrix data are used as weak-scale boundary conditions. The renormalisation group equations are solved numerically between the weak scale and a high energy scale using a nested iterative algorithm. This paper serves as a manual to the NMSSM mode of the program, detailing the approximations and conventions used. Program SummaryProgram title: SOFTSUSYCatalogue identifier: ADPM_v4_0Program summary URL:http://cpc.cs.qub.ac.uk/summaries/ADPM_v4_0.htmlProgram obtainable from: CPC Program Library, Queen’s University, Belfast, N. IrelandLicensing provisions: Standard CPC licence, http://cpc.cs.qub.ac.uk/licence/licence.htmlNo. of lines in distributed program, including test data, etc.: 154886No. of bytes in distributed program, including test data, etc.: 1870890Distribution format: tar.gzProgramming language: C++, fortran.Computer: Personal computer.Operating system: Tested on Linux 3.x.Word size: 64 bitsClassification: 11.1, 11.6.Does the new version supersede the previous version?: YesCatalogue identifier of previous version: ADPM_v3_0Journal reference of previous version: Comput. Phys. Comm. 183 (2012) 785Nature of problem: Calculating supersymmetric particle spectrum and mixing parameters in the next-to-minimal supersymmetric standard model. The solution to the renormalisation group equations must be consistent with boundary conditions on supersymmetry breaking parameters, as well as on the weak-scale boundary condition on gauge couplings, Yukawa couplings and the Higgs potential parameters.Solution method: Nested iterative algorithm and numerical minimisation of the Higgs potential.Reasons for new version: Major extension to include the next-to-minimal supersymmetric standard model.Summary of revisions: Added additional supersymmetric and supersymmetry breaking parameters associated with the additional gauge singlet. Electroweak symmetry breaking conditions are significantly changed in the next-to-minimal mode, and some sparticle mixing changes. An interface to NMSSMTools has also been included. Some of the object structure has also changed, and the command line interface has been made more user friendly.Restrictions: SOFTSUSY will provide a solution only in the perturbative regime and it assumes that all couplings of the model are real (i.e. CP-conserving). If the parameter point under investigation is non-physical for some reason (for example because the electroweak potential does not have an acceptable minimum), SOFTSUSY returns an error message.Running time: A few seconds per parameter point.

Inert Higgs doublet extension of the NMSSM

We introduce one pair of inert Higgs doublets {H_d, H_u} and singlets {N^c, N}, and consider their couplings with the Higgs doublets of the minimal supersymmetric standard model (MSSM), W \supset y_N N^c h_u H_d + y_N' N h_d H_u. We assign extra U(1)_{Z'} gauge charges only to the extra vector-like superfields, and so all the MSSM superfields remain neutral under the new U(1)_{Z'}. They can be an extension of the "\lambda term," W \supset \lambda S h_u h_d in the next-to-MSSM (NMSSM). Due to the U(1)_{Z'}, the maximally allowed low energy value of y_N can be lifted up to 0.85, avoiding a Landau-pole (LP) below the grand unification scale. Such colorless vector-like superfields remarkably enhance the radiative MSSM Higgs mass particularly for large tan\beta through the y_N term and the corresponding holomorphic soft term. As a result, the lower bound of \lambda and the upper bound of tan\beta can be relaxed to disappear from the restricted parameter space of the original NMSSM, 0.6 < \lambda < 0.7 and 1< tan\beta < 3. Thus, the valid parameter space significantly expands up to 0 < \lambda < 0.7, 0 < y_N < 0.85, and 2 < tan\beta < 50, evading the LP problem and also explaining the 126 GeV Higgs mass naturally.

“Nanosized latexes for textile printing applications obtained by miniemulsion polymerization”

We report the synthesis and design of aqueous monodisperse copolymer latexes by miniemulsion polymerization and their application as binders in pigment printing and ink-jet printing of cotton fabrics. For that purpose, miniemulsion radical polymerization was carried out with a high content of the soft butyl acrylate (BA) and a low content of the hard methyl methacrylate (MMA) in the presence of hexadecane as osmotic costabilizer. The addition of small amounts of functional monomers such as methacrylic acid MAA and N-methylol acrylamide NMA to some miniemulsion recipes allowed to impart cross-linking sites and functionality to the copolymer chains. Dynamic light scattering (DLS), small angle neutron scattering (SANS), and transmission electron microscopy (TEM) showed that the particle size diameter and size distributions could be controlled in the range of 50 to 400 nm by the amount of SDS surfactant, while the presence of a costabilizer such as hexadecane determines the particle size and, to a lesser extent, the polydispersity of the obtained miniemulsion latex dispersions. The glass transition temperature of the different miniemulsion latexes ranged between −14 and −33 °C, depending on the monomer composition. Selected samples of these nanolatexes were then employed in textile printing. The miniemulsion binders with their uniform shape and smaller size have technological advantages over conventional processes for the pigment and ink-jet printing and yielded better printing properties in terms of softness, fastness, and color strength of the printed fabric. Accordingly, by optimized use of the miniemulsion method, one is not only able to control the particle size but also to improve the properties of these latexes for textile applications.

Light third-generation squarks from flavour gauge messengers

We study models of gauge-mediated supersymmetry breaking with a gauged horizontal SU(3)_F symmetry acting on the quark superfields. If SU(3)_F is broken non-supersymmetrically by F-term vacuum expectation values, the massive gauge bosons and gauginos become messengers for SUSY breaking mediation. These gauge messenger fields induce a flavour-dependent, negative contribution to the soft masses of the squarks at one loop. In combination with the soft terms from standard gauge mediation, one obtains large and degenerate first- and second-generation squark masses, while the stops and sbottoms are light. We discuss the implications of this mechanism for the superparticle spectrum and for flavour precision observables. We also provide an explicit realization in a model with simultaneous SUSY and SU(3)_F breaking.

Neutrino masses in RPV models with two pairs of Higgs doublets

We study the generation of neutrino masses and mixing in supersymmetric R-parity violating models containing two pairs of Higgs doublets. In these models, new RPV terms $\hat H_{D_1} \hat H_{D_2} \hat E$ arise in the superpotential, as well as new soft terms. Such terms give new contributions to neutrino masses. We identify the different parameters and suppression/enhancement factors that control each of these contributions. At tree level, just like in the MSSM, only one neutrino acquires a mass due to neutrino-neutralino mixing. There are no new one loop effects. We study the two loop contributions and find the conditions under which they can be important.

Higgs mass in the MSSM with flavor mixing soft terms

The Minimal Supersymmetric Standard Model assumes scalar masses universality as a simplification to avoid undesired flavor changing neutral currents (FCNC). In this work, we consider that the trilinear SUSY soft–terms have a hierarchical structure of flavor mixing within generations, leading to a non–degeneration on sfermion masses preserving FCNC under control. We consider this kind of mixing for the u–type squark mass matrix and analyze the consequences on the radiative corrections to the Higgs mass. We work under the consideration of mmaxh benchmark scenario, in which the parameter space is set to maximize the radiative contributions to the Higgs mass. Based on recent experimental results on possible Higgs signals, we calculate the mass of the neutral light CP–even Higgs taking into account flavor mixing contributions.

Niğde Altunhisar Yöresi Bademlerinin Seleksiyonu

This study was to carried out to determine of promosing almond genotypes in Altunhisar county of Niğde province in 2013. 280 genotypes in terms of nut size, suture opening of the shell, shell thickness, softness of the shell, kernel color intensity, shriveling of kernel, kernel pubescence, kernel taste, percentage of double kernel, percentage of sound kernel, nut weight, shell thickness, nut length, nut width, nut thickness, nut shape, marking of outer shell, shell color, kernel weight, kernel length, kernel width, kernel thickness, kernel ratio, kernel size, percentages of twin kernels, width indice and thickness indice were examined. The genotyips had more than 0.70 g kernel weight and %25 kernel rate were taken for evaluation, Total Weight-Ranked Points were calculated with considering genotype quality situations. Nut size, suture opening of the shell, softness of the shell, kernel color, shriveling of kernel, kernel pubescence, kernel taste, percentage of double kernel, percentage of sound kernel etc. characters were used. 15 genotypes (98, 160, 196, 187, 162, 191, 282, 168, 176, 261, 213, 6, 112, 147, 241 ) taken highest points were selected as promosing genotypes. Selected genotypes had 2.37 (no 187) – 3.80 (no 241) g nut weight; 0.71 (no 187) – 1.0 (no 241) g kernel weight; %25.17 (no 162) - 29.97 (no 6) kernel ratio; 1.96 (no 282) – 3.29 (no 162) mm shell thickness; %0.00 – 19.00 percentage of double kernel; %0.00 – 5.00 percentage of twin kernel. It was found that in terms of softness of the shell,15 genotype was very hard; in terms of kernel weight, 14 genotypes were small and 1 genotype was medium; in terms of kernel taste, 12 genotypes were sweet and 3 genotypes were intermediate; in terms of kernel pubescence, 6 genotypes were intermediate, 9 genotypes were low; in terms of color intensity, 8 genotypes were intermediate light and 1 genotype was light and 6 genotypes were dark. In the begining of vegetation in 2014, in promosing genotypes, phenological observations will be taken and in the end of the second year of the research, superior genotypes will be determined.

Synthesis and properties of silicone polyetheramine block copolymer surfactant

In the presence of Pt catalyst, α,ω-hydrogenpolysiloxane reacted with allyl glycidyl ether, and an intermediate α,ω-diepoxysiloxane was formed. The epoxy cyclic-opening reaction was conducted between the intermediate and polyetheramine in isopropanol solution, the silicone polyetheramine block copolymer (BPEAS) was thus made. The chemical structures of BPEAS were characterized using IR and 1H-NMR separately. Then cotton fabric was treated with BPEAS for application purpose. The finishing effects were tested in terms of film morphology, hydrophilic ability, softness and mechanical properties. The recorded results showed that BPEAS can be used directly to treat cotton fabrics without adding any emulsifier at the viscosity of 6700 mPa·s and amino value of 0.6009 mmol/g. Bending rigidity and hysteresis of the treated fabric decreased by 53.53 % and 67.39 %, the drape coefficient dropped by 15 %, whereas the wrinkle recovery angle increased by 57.14 %. The treated cotton fabric is hydrophilic, and has a bulky soft hand, better anti-wrinkle property compared to the untreated one.

On axionic dark matter in Type IIA string theory

AbstractWe investigate viable scenarios with various axions in the context of supersymmetric field theory and in globally consistent D‐brane models. The Peccei‐Quinn symmetry is associated with an anomalous U(1) symmetry, which acquires mass at the string scale but remains as a perturbative global symmetry at low energies. The origin of the scalar Higgs‐axion potential from F‐, D‐ and soft breaking terms is derived, and two Standard Model examples of global intersecting D6‐brane models in Type II orientifolds are presented, which differ in the realisation of the Higgs sector and in the hidden sector, the latter of which is of particluar importance for the soft supersymmetry breaking terms.

Research of Innovative Risk Management in L/C Settlement - Based on Quality Control of Import Goods

Quality of import goods is possibly not up to standard in letter of credit settlement. In order to control the quality of import goods and to prevent exporter from fraudulent credit, importer takes some of the most effective terms that will be considered as soft term fraud by exporter. This paper analyzed the reason for the existence of such risks, and proposed innovative ideas on how to effectively control the quality of import goods in letter of credit settlement. Letter of credit (hereinafter referred as L/C) settlement serves as a more effective, timely and safe transaction way for both sellers and buyer in international trade, but there is still the risk of fraud [. Fraud risk is the greatest one in letter of credit settlement. Buyers will attach great importance to the quality of import goods, but exporter fraud will lead import goods not up to standard. In order to prevent such a quality risk, the importer will set some terms in the L/C, but these terms may be considered as soft term fraud by exporter. Research of risk management in L/C settlement will help importer effectively control the quality of import goods, and promote the L/C settlement.

A novel approach for development and characterization of effective mosquito repellent cream formulation containing citronella oil.

Citronella essential oil (CEO) has been reported as an excellent mosquito repellent; however, mild irritancy and rapid volatility limit its topical application. It was aimed to develop a nonirritant, stable, and consistent cream of CEO with improved residence time on skin using an industrial approach. Phase inversion temperature technique was employed to prepare the cream. It was optimized and characterized based on sensorial evaluation, emulsification, and consistency in terms of softness, greasiness, stickiness, and pH. The optimum batch (B5) was evaluated for viscosity (90249.67 ± 139.95 cP), texture profile with respect to firmness (38.67 ± 0.88 g), spreadability (70.33 ± 0.88 mJ), and extrudability (639.67 ± 8.09 ± 0.1 mJ) using texture analyzer along with two most popular marketed products selected as reference standard. Subsequently, B5 was found to be stable for more than 90 days and showed enhanced duration of mosquito repellency as compared to CEO. HS-GC ensured the intactness of CEO in B5. Investigated primary irritation index (PII 0.45) positioned B5 into the category of irritation barely perceptible. The pronounced texture profile and stability of B5 with extended residence time and less PII revealed its potential application in industry and offered a promising alternative to the marketed products of synthetic origin.

The ASY-EOS experiment at GSI: investigating symmetry energy at supra-saturation densities

The elliptic-flow ratio of neutrons with respect to protons or light complex particles in reactions of heavy-ions at pre-relativistic energies has been proposed as an observable sensitive to the strength of the symmetry term of the nuclear equation of state at supra-saturation densities. The results obtained from the existing FOPI/LAND data for 197Au+197Au collisions at 400 MeV/nucleon in comparison with the UrQMD model simulations favoured a moderately soft symmetry term, but suffer from a considerable statistical uncertainty. These results have been confirmed by an independent analysis based on the Tübingen QMD simulations. In order to obtain an improved data set for Au+Au collisions and to extend the study to other systems, a new experiment was carried out at the GSI laboratory by the ASY-EOS collaboration. The present status of the data analysis is reported

LANDAU CONFINING REPLICA MODEL FROM AN EXPLICITLY BREAKING OF A SU(3) GROUP WITHOUT AUXILIARY FIELDS

We propose a mechanism displaying gluon confinement, as defined by the behavior of the propagators, in a model of SU(2) gauge fields. The model originates from an explicitly broken SU(3) gauge theory giving rise to a replica model composed of three mixed SU(2) groups. The mechanism consists in the usual SU(3) Yang–Mills theory in the Landau gauge, with a soft breaking term in such a way as to change the field propagation and group content at low energies. The relation of this soft mass term with the Gribov problem is presented and the link between soft terms and the scaling and decoupling solutions is discussed.

Sparticle spectroscopy from SO(10) GUT with a unified Higgs sector

We study the low energy implications, especially the particle spectroscopy, of SO(10) grand unification in which the SO(10) symmetry is broken to the Standard Model gauge group with a single pair of ($144+\overline{144}$)-dimensional Higgs multiplet (unified Higgs sector). In this class of models, the asymptotic relation ${Y}_{b}\ensuremath{\approx}{Y}_{\ensuremath{\tau}}\ensuremath{\approx}{Y}_{t}/6$ among the third generation quark and lepton Yukawa couplings can be derived. This relation leads to the prediction $\mathrm{tan}\ensuremath{\beta}\ensuremath{\approx}14$, where $\mathrm{tan}\ensuremath{\beta}$ is the well known Minimal Supersymmetric Standard Model parameter. We find that this type of Yukawa coupling unification (YU) is realized only by employing nonuniversal soft supersymmetry breaking terms, dictated by SO(10) symmetry, for the gauginos. A 125 GeV Higgs boson mass is also found to be consistent with YU at the $\ensuremath{\sim}5%$ level. Without imposing a constraint on the relic abundance of dark matter in these models, the squark and slepton masses, with the exception of the top squark, exceed 2 TeV and the gluino is heavier than 1 TeV. We show that the neutralino in this model is an acceptable dark matter candidate through the neutralino--top squark coannihilation scenario, with the top squark being relatively light ($\ensuremath{\gtrsim}500\text{ }\text{ }\mathrm{GeV}$).

How conventional measures overestimate electroweak fine-tuning in supersymmetric theory

The lack of evidence for superparticles at the CERN LHC, along with the rather high value of the Higgs mass, has sharpened the perception that supersymmetric model parameter space is highly electroweak fine-tuned (EWFT). We compare three measures of fine-tuning in SUSY models. 1. \Del_HS measures a terms containing large log contributions to m_Z that are inevitable in models defined at scales much higher than the electroweak scale. 2. \Del_BG measures variation in m_Z against variation of model parameters and allows for correlations among high scale parameters which are not included in \Del_HS. 3. The model-independent \Del_EW measures how naturally a model can generate the measured value of m_Z=91.2 GeV in terms of weak scale parameters alone. We hypothesize an overarching Ultimate Theory (UTH) wherein the high scale soft terms are all correlated. The UTH might be contained within the more general effective SUSY theories popular in the literature. For \Del_HS, EWFT can be overestimated by neglecting additional non-independent terms which lead to large cancellations. For \Del_BG, EWFT can be overestimated by applying the measure to the effective theories instead of to the UTH. The measure \Del_EW allows for the possibility of parameter correlations which should be present in the UTH and, since it is model-independent, provides the same value of EWFT for the effective theories as should occur for the UTH. We find that the well-known mSUGRA/CMSSM model is fine-tuned under all three measures so that it is unlikely to contain the UTH. The non-universal Higgs model NUHM2 appears fine-tuned with \Del_HS,BG > 10^3. But since \Del_EW can be as small as 7 (corresponding to 14% fine-tuning), it may contain the UTH for parameter ranges which allow for low true EWFT.

R-symmetry breaking in supersymmetric hybrid inflation

We consider a supersymmetric hybrid inflation scenario in which the U(1) $R$-symmetry is explicitly broken by Planck scale suppressed operators in the superpotential. We provide an example with minimal K\"ahler potential, with the $R$-symmetry breaking term relevant during inflation being $\alpha S^4$, where $S$ denotes the well-known gauge singlet inflaton superfield. The inflationary potential takes into account the radiative and supergravity corrections, as well as the soft supersymmetry breaking terms. For successful inflation, with the scalar spectral index in the currently preferred range, $n_s \approx 0.97 \pm 0.010$, $| \alpha |$ $\lesssim 10^{-7}$. The tensor to scalar ratio $r \lesssim 10^{-4}$, while $| \text{d} n_s / \text{d} \ln k | \sim \mathcal{O}(10^{-3})-\mathcal{O}(10^{-4})$

Higgs sector of the supersymmetric reduced 331 model

A supersymmetric version of the recently proposed reduced minimal 3-3-1 model is considered and its Higgs sector is investigated. We focus on the mass spectrum of the lightest scalars of the model. We show that Higgs mass of 125 GeV requires substantial radiative corrections. However, stops may develop small mixing and must have mass around TeV. Moreover, some soft SUSY breaking terms may lie at the electroweak scale, which alleviates some tension concerning fine tuning of the related parameters. The lightest doubly charged scalar may have mass around few hundreds of GeV, which can be probed at the LHC, while the remaining scalars of the model have masses at TeV scale.

Auxiliary gauge mediation: a new route to mini-split supersymmetry

The discovery of a standard-model-like Higgs at 126 GeV and the absence of squark signals thus far at the LHC both point towards a mini-split spectrum for supersymmetry. Within standard paradigms, it is non-trivial to realize a mini-split spectrum with heavier sfermions but lighter gauginos while simultaneously generating Higgs sector soft terms of the correct magnitude, suggesting the need for new models of supersymmetry breaking and mediation. In this paper, we present a new approach to mini-split model building based on gauge mediation by ``auxiliary groups'', which are the anomaly-free continuous symmetries of the standard model in the limit of vanishing Yukawa couplings. In addition to the well-known flavor SU(3)_F and baryon-minus-lepton U(1)_{B-L} groups, we find that an additional U(1)_H acting on the Higgs doublets alone can be used to generate Higgs soft masses and B-terms necessary for a complete model of mini-split. Auxiliary gauge mediation is a special case of Higgsed gauge mediation, and we review the resulting two-loop scalar soft terms as well as three-loop gaugino masses. Along the way, we present a complete two-loop calculation of A-terms and B-terms in gauge mediation, which---contrary to a common misconception---includes a non-zero contribution at the messenger threshold which can be sizable in models with light gauginos. We present several phenomenologically acceptable mini-split spectra arising from auxiliary gauge mediation and highlight a complete minimal model which realizes the required spectrum and Higgs sector soft terms with a single U(1)_X auxiliary gauge symmetry. We discuss possible experimental consequences.

Universal soft terms in the MSSM on D-branes

In Type II string vacua constructed from intersecting/magnetized D-branes, the supersymmetry-breaking soft terms are genericaly non-universal. It is shown that universal supersymmetry-breaking soft terms may arise in a realistic MSSM constructed from intersecting/magnetized D-branes in Type II string theory. For the case of dilaton-dominated supersymmetry breaking, it is shown that the universal scalar mass and trilinear coupling are fixed such that m0=(1/2)m3/2 and A0=−m1/2. In addition, soft terms where the universal scalar mass m0 is much larger than the universal gaugino mass m1/2 may be easily obtained within the model. Finally, it is shown that the special dilaton and no-scale strict moduli boundary conditions, which are well known in heterotic string constructions, may also be obtained.

The string origin of SUSY flavor violation

We argue that in large classes of string compactifications with a MSSM-like structure substantial flavor violating SUSY-breaking soft terms are generically induced. We specify to the case of flavor dependent soft-terms in type IIB/F-theory SU(5) unified models, although our results can be easily extended to other settings. The Standard Model (SM) degrees of freedom reside in a local system of 7-branes wrapping a 4-fold S in the extra dimensions. It is known that in the presence of closed string 3-form fluxes SUSY-breaking terms are typically generated. We explore the generation dependence of these soft terms and find that non-universalities arise whenever the flux varies over the 4-fold S. These non-universalities are parametrically suppressed by (M GUT /M Pl)1/3. They also arise in the case of varying open string fluxes, in this case parametrically suppressed by $ \alpha_{\mathrm{GUT}}^{{{1 \left/ {2} \right.}}} $ . For a standard unification scheme with M GUT ≃ 1016 GeV and α GUT ≃ 1/24 these suppressions are very mild. Although limits from the kaon mass difference Δm K are easily obeyed for squark masses above the present LHC limits, constraints from the CP-violation parameter ϵ K imply squark masses in the multi-TeV region. The constraints from BR(μ → eγ) turn out to be the strongest ones, with slepton masses of order ~ 10 TeV or heavier required to obey the experimental limits. These sfermion masses are consistent with the observed large value m H ≃ 126 GeV of the Higgs mass. We discuss under what conditions such strong limits may be relaxed allowing for SUSY particle production at LHC.