5,754 research outputs found

    New Formulas and Predictions for Running Fermion Masses at Higher Scales in SM, 2HDM, and MSSM

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    Including contributions of scale-dependent vacuum expectation values, we derive new analytic formulas and obtain substantially different numerical predictions for the running masses of quarks and charged-leptons at higher scales in the SM, 2HDM and MSSM. These formulas exhibit significantly different behaviours with respect to their dependence on gauge and Yukawa couplings than those derived earlier. At one-loop level the masses of the first two generations are found to be independent of Yukawa couplings of the third generation in all the three effective theories in the small mixing limit. Analytic formulas are also obtained for running tanβ(μ)\tan\beta(\mu) in 2HDM and MSSM. Other numerical analyses include study of the third generation masses at high scales as functions of low-energy values of tanβ\tan\beta and SUSY scale MS=MZ104M_S=M_Z-10^4 GeV.Comment: 42 pages RevTeX, including 16 figures. Typos corrected and one reference adde

    Vanishing corrections on the intermediate scale and implications for unification of forces

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    In two-step breaking of a class of grand unified theories including SO(10),we prove a theorem showing that the scale MIM_I where the Pati-Salam gauge symmetry with parity breaks down to the standard gauge group,has vanishing corrections due to all sources emerging from higher scales μ>MI \mu >M_I such as the one-loop and all higher loop effects,the GUT-threshold,gravitational smearing,and string threshold effects. Implications of such a scale for the unification of gauge couplings with small Majorana neutrino masses are discussed.In string inspired SO(10) we show that MI5×1012M_I \simeq 5\times 10^{12},needed for neutrino masses,with the GUT scale MUMstrM_U \simeq M_{str} can be realized provided certain particle states in the predicted spectum are light.Comment: 21 pages, Late

    Precision and uncertainties in mass scale predictions in SUSY SO(10) with SU(2)_L x SU(2)_R x U(1)_{B-L} x SU(3)_C intermediate breaking

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    In a class of SUSY SO(10) with SU(2)LxSU(2)RxU(1)BLxSU(3)CSU(2)_L x SU(2)_R x U(1)_{B-L} x SU(3)_C (g2Lg2R)(g_{2L}\neq g_{2R}) intermediate gauge symmetry, we observe that the prediction on the unification mass (MU)(M_U) is unaffected by Planck-scale-induced gravitational and intermediate-scale-threshold effects, although the intermediate scale (MI)(M_I) itself is subject to such corrections. In particular, without invoking the presence of additional lighter scalar degrees of freedom but including plausible and reasonable threshold effects, we find that interesting solutions for neutrino physics corresponding to MI10101013M_I\simeq 10^{10}-10^{13} GeV and MU(56)x1017M_U\simeq (5-6) x 10^{17} GeV are permitted in the minimal models. Possibilities of low-mass right-handed gauge bosons corresponding to MI110M_I\simeq 1-10 TeV consistent with the CERN-LEP data are pointed out in a number of models when threshold effects are included using effective mass parameters.Comment: 12 pages including 7 tables (Typos corrected as per the published version

    Offline e-cash system

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    The e-cash scheme and the digital content transactions are the need of the hour. In the coming years, all these digital transactions will grow tremendously. So, a secure e-cash scheme is of utmost requirement. e-cash scheme, which is untraceable and maintains the security features, make it possible for the customers and the merchants to exchange the e-cash and the merchandise with privacy. So, there is a need to design an e-cash scheme with strong cryptosystem and algorithms in order to facilitate efficient digital transactions. There are two types of e-cash systems: Offine e-cash systems and online e-cash systems. Offine e-cash systems make it possible for the customer to pay the e-coin to the merchant without any involvement of bank. In online schemes, we require the involvement of the bank. The two most fundamental security features associated with offine scheme is the anonymity and the double spending detection. The proposed scheme maintains both the above features along with unforgeability. Besides, the E-coins have their expiration date so that the bank faces no hassles and can manage its database efficiently. This feature also ensures portability as the coins can be transferred to storage devices through the networks

    Threshold Effects on Quasi-degenerate Neutrinos with High-scale Mixing Unification

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    We consider threshold effects on neutrino masses and mixings in a recently proposed model for understanding large solar and atmospheric mixing angles using radiative magnification for the case of quasi-degenerate neutrinos. We show that the magnitude of the threshold effects is sufficient to bring concordance between the predictions of this model and latest data from KamLAND{\rm KamLAND} and SNO{\rm SNO} on observations of neutrino oscillations.Comment: Four pages, no figure

    Intermediate left-right gauge symmetry, unification of couplings and fermion masses in SUSY SO(10)×S4SO(10)\times S_4

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    If left-right gauge theory occurs as an intermediate symmetry in a GUT then, apart from other advantages, it is possible to obtain the see-saw scale necessary to understand small neutrino masses with Majorana coupling of order unity. Barring threshold or non-renormalizable gravitational effects, or assumed presence of additional light scalar particles of unprescribed origin, all other attempts to achieve manifest one-loop gauge coupling unification in SUSY SO(10) with left-right intermediate symmetry have not been successful so far. Attributing this failure to lack of flavor symmetry in the GUT, we show how the spontaneous symmetry breaking of SO(10)×S4SO(10)\times S_4 leads to such intermediate scale extending over a wide range, MR5×109M_R \simeq 5\times 10^{9} GeV to 101510^{15} GeV. All the charged fermion masses are fitted at the see-saw scale, MNMR4×1013M_N\simeq M_R \simeq 4 \times 10^{13} GeV which is obtained with Majorana coupling f01f_0 \simeq 1. Using a constrained parametrization in which CP-violation originates only from quark sector, besides other predictions made in the neutrino sector, the reactor mixing angle is found to be θ1335\theta_{13} \simeq 3^{\circ} - 5^{\circ} which is in the range accessible to ongoing and planned experiments. The leptonic Dirac phase turns out to be δ2.93.1\delta \sim 2.9- 3.1 radians with Jarlskog invariant J2.95×105103J \sim 2.95 \times 10^{-5} - 10^{-3}.Comment: Minor clarification and few references added to match the published versio

    Radiative stability of neutrino-mass textures

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    Neutrino-mass textures proposed at high-scales are known to be unstable against radiative corrections especially for nearly degenerate eigen values. Within the renormalization group constraints we find a mechanism in a class of gauge theories which guarantees reproduction of any high-scale texture at low energies with radiative stability. We also show how the mechanism explains solar and atmospheric neutrino anomalies through the bimaximal texture at high scale.Comment: 4 pages REVTEX, 1 Postscript fi

    Type II Seesaw Dominance in Non-supersymmetric and Split Susy SO(10) and Proton Life Time

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    Recently type II seesaw dominance in a supersymmetric SO(10) framework has been found useful in explaining large solar and atmospheric mixing angles as well as larger values of theta13theta_{13} while unifying quark and lepton masses. An important question in these models is whether there exists consistency between coupling unification and type II seesaw dominance. Scenarios where this consistency can be demonstrated have been given in a SUSY framework. In this paper we give examples where type II dominance occurs in SO(10) models without supersymmetry but with additional TeV scale particles and also in models with split-supersummetry. Grand unification is realized in a two-step process via breaking of SO(10) to SU(5) and then to a TeV scale standard model supplemented by extra fields and an SU(5) Higgs multiplet 15H{15}_H at a scale about 101210^{12} GeV to give type-II seesaw. The predictions for proton lifetime in these models are in the range τp0=2×1035\tau_p^0 = 2\times 10^{35} yrs. to τp0=6×1035\tau_p^0 = 6\times 10^{35} yrs.. A number of recent numerical fits to GUT-scale fermion masses can be accommodated within this model.Comment: 7 pages LaTeX, 3 figures, related areas: hep-ex, hep-th, astro-ph; Reference added, typo corrected, version to appear in Physical Review

    Rapid Detection of Ricin by Sensitising Carboxylated Latex Particles by Ricin Antibodies

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    Ricin is a highly toxic glycoprotein of Ricinus communis seeds. The toxin was purified and antisera was raised against ricin in rabbit. Polyclonal antibodies were covalently coupled througha water soluble carbodiimide to carboxylated latex particles in various concentrations (800 pg to 3200 pg proteid0.5 ml). Maximum antibodies binding was obtained at 2400 pg to 3200 pgproteid0.5 ml of 2 per cent (wtlvol) latex particles with a sensitivity of 200 pg toxin per test (9 pglml). The sensitivity of latex agglutination test increased as amount of protein bound tothe latex particles increased. The optimum sensitivity of test was recorded when latex particles were sensitised with 2800 pg proteid0.5 ml of latex particles. The reagents were stable for one year without loss of its sensitivity. Developed latex agglutination test is rapid, sensitive, and also does not require trained personnel and costly equipment
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