205 research outputs found

    Π‘Ρ‚Ρ€ΡƒΠΊΡ‚ΡƒΡ€Π° износостойких ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ ΠΊΠ°Π±ΠΎΠ½ΠΈΡ‚Ρ€ΠΈΠ΄Π° циркония

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    A structure of zirconium carbonitride coatings obtained by an arc cathodic deposition in the medium of reactant mixture of nitrogen and acetylene was investigated. Using X-ray diffraction and X-ray photoelectron spectroscopy it was shown that the coatings consist of both ultra dispersive Ξ΄ phase zirconium carbonitride and amorphous carbon containing considerable amount of sp3 bonds. The coatings were textured greatly with texture axis (111). The texture degree influenced a substrate material like tool steel X12M and cemented carbide BK6.ИсслСдована кристалличСская структура ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΈΡ‚Ρ€ΠΈΠ΄Π° циркония, ΠΏΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹Ρ… ΠΊΠ°Ρ‚ΠΎΠ΄Π½ΠΎ-Π΄ΡƒΠ³ΠΎΠ²Ρ‹ΠΌ осаТдСниСм Π² Ρ€Π΅Π°ΠΊΡ†ΠΈΠΎΠ½Π½ΠΎΠΉ срСдС смСси Π³Π°Π·ΠΎΠ² Π°Π·ΠΎΡ‚Π° ΠΈ Π°Ρ†Π΅Ρ‚ΠΈΠ»Π΅Π½Π°. ΠœΠ΅Ρ‚ΠΎΠ΄Π°ΠΌΠΈ Ρ€Π΅Π½Ρ‚Π³Π΅Π½ΠΎΠ³Ρ€Π°Ρ„ΠΈΠΈ ΠΈ рСнтгСновской фотоэлСктронной спСктроскопии ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ, Ρ‡Ρ‚ΠΎ структура покрытия ΠΎΠ±Ρ€Π°Π·ΠΎΠ²Π°Π½Π° ΡƒΠ»ΡŒΡ‚Ρ€Π°Π΄ΠΈΡΠΏΠ΅Ρ€ΡΠ½ΠΎΠΉ Ξ΄-Ρ„Π°Π·ΠΎΠΉ ΠΊΠ°Ρ€Π±ΠΎΠ½ΠΈΡ‚Ρ€ΠΈΠ΄Π° циркония ΠΈ Π°ΠΌΠΎΡ€Ρ„Π½ΠΎΠ³ΠΎ Π°Π»ΠΌΠ°Π·ΠΎΠΏΠΎΠ΄ΠΎΠ±Π½ΠΎΠ³ΠΎ ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π° с большим содСрТаниСм sΡ€3-связанных Π°Ρ‚ΠΎΠΌΠΎΠ². ΠŸΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΡ сильно тСкстурированы с осью тСкстуры (111). Показано, Ρ‡Ρ‚ΠΎ Π½Π° ΡΡ‚Π΅ΠΏΠ΅Π½ΡŒ тСкстурирования Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ влияСт ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π» основы, Π² качСствС ΠΊΠΎΡ‚ΠΎΡ€ΠΎΠΉ использовалась ΠΈΠ½ΡΡ‚Ρ€ΡƒΠΌΠ΅Π½Ρ‚Π°Π»ΡŒΠ½Π°Ρ ΡΡ‚Π°Π»ΡŒ Π₯12М ΠΈ Ρ‚Π²Π΅Ρ€Π΄Ρ‹ΠΉ сплав Π’Πš6

    Tuning supersymmetric models at the LHC: A comparative analysis at two-loop level

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    We provide a comparative study of the fine tuning amount (Delta) at the two-loop leading log level in supersymmetric models commonly used in SUSY searches at the LHC. These are the constrained MSSM (CMSSM), non-universal Higgs masses models (NUHM1, NUHM2), non-universal gaugino masses model (NUGM) and GUT related gaugino masses models (NUGMd). Two definitions of the fine tuning are used, the first (Delta_{max}) measures maximal fine-tuning wrt individual parameters while the second (Delta_q) adds their contribution in "quadrature". As a direct result of two theoretical constraints (the EW minimum conditions), fine tuning (Delta_q) emerges as a suppressing factor (effective prior) of the averaged likelihood (under the priors), under the integral of the global probability of measuring the data (Bayesian evidence p(D)). For each model, there is little difference between Delta_q, Delta_{max} in the region allowed by the data, with similar behaviour as functions of the Higgs, gluino, stop mass or SUSY scale (m_{susy}=(m_{\tilde t_1} m_{\tilde t_2})^{1/2}) or dark matter and g-2 constraints. The analysis has the advantage that by replacing any of these mass scales or constraints by their latest bounds one easily infers for each model the value of Delta_q, Delta_{max} or vice versa. For all models, minimal fine tuning is achieved for M_{higgs} near 115 GeV with a Delta_q\approx Delta_{max}\approx 10 to 100 depending on the model, and in the CMSSM this is actually a global minimum. Due to a strong (β‰ˆ\approx exponential) dependence of Delta on M_{higgs}, for a Higgs mass near 125 GeV, the above values of Delta_q\approx Delta_{max} increase to between 500 and 1000. Possible corrections to these values are briefly discussed.Comment: 23 pages, 46 figures; references added; some clarifications (section 2

    Interpreting a 1 fb^-1 ATLAS Search in the Minimal Anomaly Mediated Supersymmetry Breaking Model

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    Recent LHC data significantly extend the exclusion limits for supersymmetric particles, particularly in the jets plus missing transverse momentum channels. The most recent such data have so far been interpreted by the experiment in only two different supersymmetry breaking models: the constrained minimal supersymmetric standard model (CMSSM) and a simplified model with only squarks and gluinos and massless neutralinos. We compare kinematical distributions of supersymmetric signal events predicted by the CMSSM and anomaly mediated supersymmetry breaking (mAMSB) before calculating exclusion limits in mAMSB. We obtain a lower limit of 900 GeV on squark and gluino masses at the 95% confidence level for the equal mass limit, tan(beta)=10 and mu>0.Comment: 18 pages, 11 figure

    R-parity Conservation via the Stueckelberg Mechanism: LHC and Dark Matter Signals

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    We investigate the connection between the conservation of R-parity in supersymmetry and the Stueckelberg mechanism for the mass generation of the B-L vector gauge boson. It is shown that with universal boundary conditions for soft terms of sfermions in each family at the high scale and with the Stueckelberg mechanism for generating mass for the B-L gauge boson present in the theory, electric charge conservation guarantees the conservation of R-parity in the minimal B-L extended supersymmetric standard model. We also discuss non-minimal extensions. This includes extensions where the gauge symmetries arise with an additional U(1)_{B-L} x U(1)_X, where U(1)_X is a hidden sector gauge group. In this case the presence of the additional U(1)_X allows for a Z' gauge boson mass with B-L interactions to lie in the sub-TeV region overcoming the multi-TeV LEP constraints. The possible tests of the models at colliders and in dark matter experiments are analyzed including signals of a low mass Z' resonance and the production of spin zero bosons and their decays into two photons. In this model two types of dark matter candidates emerge which are Majorana and Dirac particles. Predictions are made for a possible simultaneous observation of new physics events in dark matter experiments and at the LHC.Comment: 38 pages, 7 fig

    Constraints on supersymmetry with light third family from LHC data

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    We present a re-interpretation of the recent ATLAS limits on supersymmetry in channels with jets (with and without b-tags) and missing energy, in the context of light third family squarks, while the first two squark families are inaccessible at the 7 TeV run of the Large Hadron Collider (LHC). In contrast to interpretations in terms of the high-scale based constrained minimal supersymmetric standard model (CMSSM), we primarily use the low-scale parametrisation of the phenomenological MSSM (pMSSM), and translate the limits in terms of physical masses of the third family squarks. Side by side, we also investigate the limits in terms of high-scale scalar non-universality, both with and without low-mass sleptons. Our conclusion is that the limits based on 0-lepton channels are not altered by the mass-scale of sleptons, and can be considered more or less model-independent.Comment: 20 pages, 8 figures, 2 tables. Version published in JHE

    Π‘Ρ‚Ρ€ΡƒΠΊΡ‚ΡƒΡ€Π° ΠΈ оптичСскиС свойства ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ Π°Π»ΠΌΠ°Π·ΠΎΠΏΠΎΠ΄ΠΎΠ±Π½ΠΎΠ³ΠΎ ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π°

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    Using a hybrid method of cathodic arc (PVD) and chemical (CVD) deposition from the gas phase, a new type of coatings containing high amount of sp3 bonds of carbon, capable of absorbing effectively light has been developed.This thin film material is a promised one for optical devices operating in open space environment as antireflective coating Β for photoreceiver bodies. The hybrid method permits to obtain effective light absorbing coatings having excellent mechanical and tribological properties and is able to sustain temperature cycling in a range from plus 150 to minus 100 oC. Β The optical characteristics of DLC coatings were studied depending on the content of sp2bound content. The combined physical and chemical deposition of DLC coatings allows to achieve a sufficiently high light absorption (a~10 5 cm–1) and low reflection with a relatively small coating thickness about 1 mm. It has been established that the antireflective properties of such coatings depend on the conditions for their preparation, first of all on hydrocarbon gas pressureΒ Π‘ использованиСм Π³ΠΈΠ±Ρ€ΠΈΠ΄Π½ΠΎΠ³ΠΎ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° ΠΊΠ°Ρ‚ΠΎΠ΄Π½ΠΎΒ­Π΄ΡƒΠ³ΠΎΠ²ΠΎΠ³ΠΎ (PVD) ΠΈ химичСского (CVD) осаТдСния ΠΈΠ· Π³Π°Π·ΠΎΠ²ΠΎΠΉ Ρ„Π°Π·Ρ‹ Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½ Π½ΠΎΠ²Ρ‹ΠΉ Ρ‚ΠΈΠΏ ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ с большим содСрТаниСм sp2­химичСски связанных Π°Ρ‚ΠΎΠΌΠΎΠ² ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π°, способных эффСктивно ΠΏΠΎΠ³Π»ΠΎΡ‰Π°Ρ‚ΡŒ Π²ΠΈΠ΄ΠΈΠΌΠΎΠ΅ оптичСскоС ΠΈΠ·Π»ΡƒΡ‡Π΅Π½ΠΈΠ΅.Аморфный Ρ‚ΠΎΠ½ΠΊΠΎΠΏΠ»Π΅Π½ΠΎΡ‡Π½Ρ‹ΠΉ ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π½Ρ‹ΠΉ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΠ°Π» являСтся пСрспСктивным для нанСсСния ΠΏΠΎΠ³Π»ΠΎΡ‰Π°ΡŽΡ‰ΠΈΡ… Π°Π½Ρ‚ΠΈΠ±Π»ΠΈΠΊΠΎΠ²Ρ‹Ρ… ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ Π½Π° корпусныС Π΄Π΅Ρ‚Π°Π»ΠΈ Ρ„ΠΎΡ‚ΠΎΠΏΡ€ΠΈΠ΅ΠΌΠ½ΠΈΠΊΠΎΠ² оптичСского излучСния, Ρ€Π°Π±ΠΎΡ‚Π°ΡŽΡ‰ΠΈΡ… Π² ΠΎΡ‚ΠΊΡ€Ρ‹Ρ‚ΠΎΠΌ космосС. Π“ΠΈΠ±Ρ€ΠΈΠ΄Π½Ρ‹ΠΉ ΠΌΠ΅Ρ‚ΠΎΠ΄ позволяСт ΠΏΠΎΠ»ΡƒΡ‡Π°Ρ‚ΡŒ ΡΠΈΠ»ΡŒΠ½ΠΎΠΏΠΎΠ³Π»ΠΎΡ‰Π°ΡŽΡ‰ΠΈΠ΅ покрытия, ΠΎΠ±Π»Π°Π΄Π°ΡŽΡ‰ΠΈΠ΅ Ρ‚Π°ΠΊΠΆΠ΅ высокими мСханичСскими ΠΈ трибологичСскими свойствами ΠΈ способныС Π²Ρ‹Π΄Π΅Ρ€ΠΆΠΈΠ²Π°Ρ‚ΡŒ Ρ‚Π΅Ρ€ΠΌΠΎΡ†ΠΈΠΊΠ»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΎΡ‚ + 150 Π΄ΠΎ – 100 Β°Π‘.ΠŸΡ€ΠΎΠ²Π΅Π΄Π΅Π½ΠΎ исслСдованиС оптичСских характСристик АПУ ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ Π² зависимости ΠΎΡ‚ содСрТания sp2­связанных Π°Ρ‚ΠΎΠΌΠΎΠ² ΡƒΠ³Π»Π΅Ρ€ΠΎΠ΄Π°. ΠŸΠΎΠ»ΡƒΡ‡Π΅Π½Π½Ρ‹ΠΉ ΠΊΠΎΠΌΠ±ΠΈΠ½ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹ΠΌ способом физичСского ΠΈ химичСского осаТдСния АПУ Π² Π²ΠΈΠ΄Π΅ Ρ‚ΠΎΠ½ΠΊΠΈΡ… слоСв позволяСт Π΄ΠΎΡΡ‚ΠΈΡ‡ΡŒ достаточно высокого поглощСния ΠΈ Π½ΠΈΠ·ΠΊΠΎΠ³ΠΎ отраТСния ΠΏΡ€ΠΈ ΡΡ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ ΠΌΠ°Π»ΠΎΠΉ Ρ‚ΠΎΠ»Ρ‰ΠΈΠ½Π΅ покрытия (a ~ 105 см–1). УстановлСно, Ρ‡Ρ‚ΠΎ Π°Π½Ρ‚ΠΈΠ±Π»ΠΈΠΊΠΎΠ²Ρ‹Π΅ свойства Ρ‚Π°ΠΊΠΈΡ… ΠΏΠΎΠΊΡ€Ρ‹Ρ‚ΠΈΠΉ зависят ΠΎΡ‚ условий Π΅Π³ΠΎ получСния, ΠΈ ΠΏΡ€Π΅ΠΆΠ΄Π΅ всСго – ΠΎΡ‚ давлСния Π³Π°Π·Π° ΡƒΠ³Π»Π΅Π²ΠΎΠ΄ΠΎΡ€ΠΎΠ΄ΠΎΠ²

    New perturbation theory representation of the conformal symmetry breaking effects in gauge quantum field theory models

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    We propose a hypothesis on the detailed structure for the representation of the conformal symmetry breaking term in the basic Crewther relation generalized in the perturbation theory framework in QCD renormalized in the MSˉ{\rm \bar{MS}} scheme. We establish the validity of this representation in the O(αs4)O(\alpha_s^4) approximation. Using the variant of the generalized Crewther relation formulated here allows finding relations between specific contributions to the QCD perturbation series coefficients for the flavor nonsinglet part of the Adler function DAnsD^{ns}_A for the electron-positron annihilation in hadrons and to the perturbation series coefficients for the Bjorken sum rule SBjpS_\text{Bjp} for the polarized deep-inelastic lepton-nucleon scattering. We find new relations between the αs4\alpha_s^4 coefficients of DAnsD^{ns}_A and SBjpS_\text{Bjp}. Satisfaction of one of them serves as an additional theoretical verification of the recent computer analytic calculations of the terms of order αs4\alpha_s^4 in the expressions for these two quantities.Comment: 12 pages, Title modified, abstract modified, improved and extended variant of the talks, presented at Int. Seminar "Quarks-2010" (6-12 June, 2010, Kolomna) and Int. Workshop Hadron Structure and QCD: From Low to High Energies (5-9 July 2010, Gatchina

    Exploring the Higgs Portal with 10/fb at the LHC

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    We consider the impact of new exotic colored and/or charged matter interacting through the Higgs portal on Standard Model Higgs boson searches at the LHC. Such Higgs portal couplings can induce shifts in the effective Higgs-gluon-gluon and Higgs-photon-photon couplings, thus modifying the Higgs production and decay patterns. We consider two possible interpretations of the current LHC Higgs searches based on ~ 5/fb of data at each detector: 1) a Higgs boson in the mass range (124-126) GeV and 2) a `hidden' heavy Higgs boson which is underproduced due to the suppression of its gluon fusion production cross section. We first perform a model independent analysis of the allowed sizes of such shifts in light of the current LHC data. As a class of possible candidates for new physics which gives rise to such shifts, we investigate the effects of new scalar multiplets charged under the Standard Model gauge symmetries. We determine the scalar parameter space that is allowed by current LHC Higgs searches, and compare with complementary LHC searches that are sensitive to the direct production of colored scalar states.Comment: 27 pages, 11 figures; v2: references added, correction to scalar form factor, numerical results updated with Moriond 2012 data, conclusions unchange

    The Intermediate Scale MSSM, the Higgs Mass and F-theory Unification

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    Even if SUSY is not present at the Electro-Weak scale, string theory suggests its presence at some scale M_{SS} below the string scale M_s to guarantee the absence of tachyons. We explore the possible value of M_{SS} consistent with gauge coupling unification and known sources of SUSY breaking in string theory. Within F-theory SU(5) unification these two requirements fix M_{SS} ~ 5 x 10^{10} GeV at an intermediate scale and a unification scale M_c ~ 3 x 10^{14} GeV. As a direct consequence one also predicts the vanishing of the quartic Higgs SM self-coupling at M_{SS} ~10^{11} GeV. This is tantalizingly consistent with recent LHC hints of a Higgs mass in the region 124-126 GeV. With such a low unification scale M_c ~ 3 x 10^{14} GeV one may worry about too fast proton decay via dimension 6 operators. However in the F-theory GUT context SU(5) is broken to the SM via hypercharge flux. We show that this hypercharge flux deforms the SM fermion wave functions leading to a suppression, avoiding in this way the strong experimental proton decay constraints. In these constructions there is generically an axion with a scale of size f_a ~ M_c/(4\pi)^2 ~ 10^{12} GeV which could solve the strong CP problem and provide for the observed dark matter. The prize to pay for these attractive features is to assume that the hierarchy problem is solved due to anthropic selection in a string landscape.Comment: 48 pages, 8 figures. v3: further minor correction

    Probing the charged Higgs boson at the LHC in the CP-violating type-II 2HDM

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    We present a phenomenological study of a CP-violating two-Higgs-doublet Model with type-II Yukawa couplings at the Large Hadron Collider (LHC). In the light of recent LHC data, we focus on the parameter space that survives the current and past experimental constraints as well as theoretical bounds on the model. Once the phenomenological scenario is set, we analyse the scope of the LHC in exploring this model through the discovery of a charged Higgs boson produced in association with a W boson, with the former decaying into the lightest neutral Higgs and a second W state, altogether yielding a b\bar b W^+W^- signature, of which we exploit the W^+W^- semileptonic decays.Comment: 37 pages, 16 figures; v2 updated treatment of LHC constraint
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