174 research outputs found

    Global Partial Density of States: Statistics and Localization Length in Quasi-one Dimensional disordered systems

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    We study the distributions functions for global partial density of states (GPDOS) in quasi-one-dimensional (Q1D) disordered wires as a function of disorder parameter from metal to insulator. We consider two different models for disordered Q1D wire: a set of two dimensional Ξ΄\delta potentials with an arbitrary signs and strengths placed randomly, and a tight-binding Hamiltonian with several modes and on-site disorder. The Green functions (GF) for two models were calculated analytically and it was shown that the poles of GF can be presented as determinant of the rank NΓ—NN\times N, where NN is the number of scatters. We show that the variances of partial GPDOS in the metal to insulator crossover regime are crossing. The critical value of disorder wcw_c where we have crossover can be used for calculation a localization length in Q1D systems.Comment: RevTex4 8 .eps figure

    Comparative evaluation of biochemical parameters and mineral composition of Cucurbita ficifolia, C. maxima and C. moschata fruit, grown in the northern hemisphere

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    Fruit peel/pulp distribution of biologically active compounds is an important characteristic of plant physiology and the basis of zero waste production in agriculture. Among C. ficifolia, C. maxima and C. moschata the former showed the lowest dry matter content, especially in peel, similar peel and pulp values of antioxidant activity (AOA) and polyphenol content (TP), with the highest levels in fruit placenta. Peel carbohydrate profile of C. ficifolia fruit was characterized by lower levels of disaccharides compared to C. maxima and C. moschata peel and an opposite pattern of monosaccharides accumulation. The analysis of 25 elements content in Cucurbita peel and pulp, using ICP-MS, indicated that C. ficifolia fruit are characterized by significantly high concentrations of Sr, Si and I in pulp compared to the values of C. maxima and C. moschata. On the contrary, C. maxima and C. moschata were characterized by low concentration of pulp Mn. Highly significant positive correlations were recorded between Cr-Sr, Cr-Ca and CaSr (r=0.906; 0.939 and 0.974 respectively) and P-Cu (r=0.968). Despite C. ficifolia, does not contain carotenoids, it is highly valuable due to the high levels of Si, I, Cr and Ca in peel and pulp, which reveals new areas of its application

    Π‘Ρ€Π°Π²Π½ΠΈΡ‚Π΅Π»ΡŒΠ½Π°Ρ ΠΎΡ†Π΅Π½ΠΊΠ° биохимичСских ΠΏΠΎΠΊΠ°Π·Π°Ρ‚Π΅Π»Π΅ΠΉ ΠΈ ΠΌΠΈΠ½Π΅Ρ€Π°Π»ΡŒΠ½ΠΎΠ³ΠΎ состава ΠΏΠ»ΠΎΠ΄ΠΎΠ² Cucurbita ficifolia, C. maxima ΠΈ C. moschata

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    Fruit peel/pulp distribution of biologically active compounds is an important characteristic of plant physiology and the basis of zero waste production in agriculture. Among C. ficifolia, C. maxima and C. moschata the former showed the lowest dry matter content, especially in peel, similar peel and pulp values of antioxidant activity (AOA) and polyphenol content (TP), with the highest levels in fruit placenta. Peel carbohydrate profile of C. ficifolia fruit was characterized by lower levels of disaccharides compared to C. maxima and C. moschata peel and an opposite pattern of monosaccharides accumulation. The analysis of 25 elements content in Cucurbita peel and pulp, using ICP-MS, indicated that C. ficifolia fruit are characterized by significantly high concentrations of Sr, Si and I in pulp compared to the values of C. maxima and C. moschata. On the contrary, C. maxima and C. moschata were characterized by low concentration of pulp Mn. Highly significant positive correlations were recorded between Cr-Sr, Cr-Ca and CaSr (r=0.906; 0.939 and 0.974 respectively) and P-Cu (r=0.968). Despite C. ficifolia, does not contain carotenoids, it is highly valuable due to the high levels of Si, I, Cr and Ca in peel and pulp, which reveals new areas of its application. РаспрСдСлСниС биологичСски Π°ΠΊΡ‚ΠΈΠ²Π½Ρ‹Ρ… соСдинСний ΠΌΠ΅ΠΆΠ΄Ρƒ ΠΊΠΎΠΆΡƒΡ€ΠΎΠΉ ΠΈ ΠΌΡΠΊΠΎΡ‚ΡŒΡŽ ΠΏΠ»ΠΎΠ΄ΠΎΠ² являСтся Π²Π°ΠΆΠ½ΠΎΠΉ характСристикой особСнности Ρ„ΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈ растСния ΠΈ ΠΌΠΎΠΆΠ΅Ρ‚ ΡΠ»ΡƒΠΆΠΈΡ‚ΡŒ основой для Π±Π΅Π·ΠΎΡ‚Ρ…ΠΎΠ΄Π½ΠΎΠ³ΠΎ производства Π² сСльском хозяйствС.Π Π΅Π·ΡƒΠ»ΡŒΡ‚Π°Ρ‚Ρ‹. УстановлСно, Ρ‡Ρ‚ΠΎ срСди Ρ‚Ρ€Π΅Ρ… Π²ΠΈΠ΄ΠΎΠ² Ρ‚Ρ‹ΠΊΠ²Ρ‹: фиголистной (C. ficifolia), ΠΊΡ€ΡƒΠΏΠ½ΠΎΠΏΠ»ΠΎΠ΄Π½ΠΎΠΉ (C. maxima) ΠΈ мускатной (C. moschata), – фиголистная Ρ‚Ρ‹ΠΊΠ²Π° содСрТит наимСньшСС количСство сухого вСщСства, особСнно Π² ΠΊΠΎΠΆΡƒΡ€Π΅ ΠΏΠ»ΠΎΠ΄ΠΎΠ², сходныС ΡƒΡ€ΠΎΠ²Π½ΠΈ ΠΎΠ±Ρ‰Π΅ΠΉ антиоксидантной активности (АОА) ΠΈ содСрТания ΠΏΠΎΠ»ΠΈΡ„Π΅Π½ΠΎΠ»ΠΎΠ² (Π’Π ) Π² ΠΊΠΎΠΆΡƒΡ€Π΅ ΠΈ мякоти ΠΏΡ€ΠΈ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡŒΠ½Ρ‹Ρ… показатСлях антиоксидантного статуса Π² ΠΏΠ»Π°Ρ†Π΅Π½Ρ‚Π΅. Π£Π³Π»Π΅Π²ΠΎΠ΄Π½Ρ‹ΠΉ ΠΏΡ€ΠΎΡ„ΠΈΠ»ΡŒ ΠΊΠΎΠΆΡƒΡ€Ρ‹ фиголистной Ρ‚Ρ‹ΠΊΠ²Ρ‹ C. ficifolia характСризовался наимСньшими уровнями дисахаридов ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с ΠΊΠΎΠΆΡƒΡ€ΠΎΠΉ ΠΊΡ€ΡƒΠΏΠ½ΠΎΠΏΠ»ΠΎΠ΄Π½ΠΎΠΉ C. maxima ΠΈ мускатной Ρ‚Ρ‹ΠΊΠ²Ρ‹ C. moschata ΠΈ наибольшими уровнями моносахаров. ИБП-МБ Π°Π½Π°Π»ΠΈΠ· содСрТания 25 элСмСнтов Π² ΠΊΠΎΠΆΡƒΡ€Π΅ ΠΈ мякоти исслСдованных Π²ΠΈΠ΄ΠΎΠ² Ρ‚Ρ‹ΠΊΠ²Ρ‹ ΠΏΠΎΠΊΠ°Π·Π°Π», Ρ‡Ρ‚ΠΎ фиголистная Ρ‚Ρ‹ΠΊΠ²Π° отличаСтся Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎ Π±ΠΎΠ»Π΅Π΅ высокими уровнями накоплСния Π² мякоти Sr, Si, I ΠΏΠΎ ΡΡ€Π°Π²Π½Π΅Π½ΠΈΡŽ с Π°Π½Π°Π»ΠΎΠ³ΠΈΡ‡Π½Ρ‹ΠΌΠΈ Π΄Π°Π½Π½Ρ‹ΠΌΠΈ для Ρ‚Ρ‹ΠΊΠ²Ρ‹ ΠΊΡ€ΡƒΠΏΠ½ΠΎΠΏΠ»ΠΎΠ΄Π½ΠΎΠΉ C. maxima ΠΈ мускатной C. moschata. Напротив, ΠΏΠ»ΠΎΠ΄Ρ‹ ΠΊΡ€ΡƒΠΏΠ½ΠΎΠΏΠ»ΠΎΠ΄Π½ΠΎΠΉ ΠΈ мускатной Ρ‚Ρ‹ΠΊΠ²Ρ‹ Ρ…Π°Ρ€Π°ΠΊΡ‚Π΅Ρ€ΠΈΠ·ΠΎΠ²Π°Π»ΠΈΡΡŒ Π½ΠΈΠ·ΠΊΠΈΠΌΠΈ концСнтрациями Mn Π² мякоти. УстановлСны статистичСски достовСрныС ΠΏΠΎΠ»ΠΎΠΆΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Π΅ коррСляции ΠΌΠ΅ΠΆΠ΄Ρƒ Cr-Sr, Cr-Ca ΠΈ Ca-Sr (r=0.906; 0.939 ΠΈ 0.974 соотвСтствСнно), Π° Ρ‚Π°ΠΊΠΆΠ΅ P-Cu (r=0.968). НСсмотря Π½Π° Ρ‚ΠΎ, Ρ‡Ρ‚ΠΎ ΠΏΠ»ΠΎΠ΄Ρ‹ фиголистной Ρ‚Ρ‹ΠΊΠ²Ρ‹ C. ficifolia Π½Π΅ содСрТат ΠΊΠ°Ρ€ΠΎΡ‚ΠΈΠ½ΠΎΠΈΠ΄Ρ‹, ΠΈΡ… пищСвая Ρ†Π΅Π½Π½ΠΎΡΡ‚ΡŒ Π² Π·Π½Π°Ρ‡ΠΈΡ‚Π΅Π»ΡŒΠ½ΠΎΠΉ стСпСни связана с высокими уровнями Si, I, Cr ΠΈ Ca Π² ΠΊΠΎΠΆΡƒΡ€Π΅ ΠΏΠ»ΠΎΠ΄ΠΎΠ² ΠΈ мякоти, Ρ‡Ρ‚ΠΎ ΠΎΡ‚ΠΊΡ€Ρ‹Π²Π°Π΅Ρ‚ Π½ΠΎΠ²Ρ‹Π΅ Π³ΠΎΡ€ΠΈΠ·ΠΎΠ½Ρ‚Ρ‹ использования этого Π²ΠΈΠ΄Π°.

    First Results from The GlueX Experiment

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    The GlueX experiment at Jefferson Lab ran with its first commissioning beam in late 2014 and the spring of 2015. Data were collected on both plastic and liquid hydrogen targets, and much of the detector has been commissioned. All of the detector systems are now performing at or near design specifications and events are being fully reconstructed, including exclusive production of Ο€0\pi^{0}, Ξ·\eta and Ο‰\omega mesons. Linearly-polarized photons were successfully produced through coherent bremsstrahlung and polarization transfer to the ρ\rho has been observed.Comment: 8 pages, 6 figures, Invited contribution to the Hadron 2015 Conference, Newport News VA, September 201

    Search for a new gauge boson in the Aβ€²A' Experiment (APEX)

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    We present a search at Jefferson Laboratory for new forces mediated by sub-GeV vector bosons with weak coupling Ξ±β€²\alpha' to electrons. Such a particle Aβ€²A' can be produced in electron-nucleus fixed-target scattering and then decay to an e+eβˆ’e^+e^- pair, producing a narrow resonance in the QED trident spectrum. Using APEX test run data, we searched in the mass range 175--250 MeV, found no evidence for an Aβ€²β†’e+eβˆ’A'\to e^+e^- reaction, and set an upper limit of Ξ±β€²/α≃10βˆ’6\alpha'/\alpha \simeq 10^{-6}. Our findings demonstrate that fixed-target searches can explore a new, wide, and important range of masses and couplings for sub-GeV forces.Comment: 5 pages, 5 figures, references adde

    Nanoscopic Tunneling Contacts on Mesoscopic Multiprobe Conductors

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    We derive Bardeen-like expressions for the transmission probabilities between two multi-probe mesoscopic conductors coupled by a weak tunneling contact. We emphasize especially the dual role of a weak coupling contact as a current source and sink and analyze the magnetic field symmetry. In the limit of a point-like tunneling contact the transmission probability becomes a product of local, partial density of states of the two mesoscopic conductors. We present expressions for the partial density of states in terms of functional derivatives of the scattering matrix with respect to the local potential and in terms of wave functions. We discuss voltage measurements and resistance measurements in the transport state of conductors. We illustrate the theory for the simple case of a scatterer in an otherwise perfect wire. In particular, we investigate the development of the Hall-resistance as measured with weak coupling probes.Comment: 10 pages, 5 figures, revte

    Measurement of the Electric Form Factor of the Neutron at Q^2=0.5 and 1.0 (GeV/c)^2

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    The electric form factor of the neutron was determined from measurements of the \vec{d}(\vec{e},e' n)p reaction for quasielastic kinematics. Polarized electrons were scattered off a polarized deuterated ammonia target in which the deuteron polarization was perpendicular to the momentum transfer. The scattered electrons were detected in a magnetic spectrometer in coincidence with neutrons in a large solid angle detector. We find G_E^n = 0.0526 +/- 0.0033 (stat) +/- 0.0026 (sys) and 0.0454 +/- 0.0054 +/- 0.0037 at Q^2 = 0.5 and 1.0 (GeV/c)^2, respectively.Comment: 5 pages, 2 figures, as publishe
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