2,003 research outputs found

    A New Clustering Method for Landsat Images Using Local Maximums of a Multidimensional Histogram

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    This paper describes a new clustering method for a huge satellite image. This method is composed of two major schemes, a multi-layered hashing scheme for multi-dimensional histogram (MDH) and a histogram clustering scheme using MDH. The MDH construction scheme works in 3 stages. In the 1st stage it constructs a few histogram layers for each part of an image, and in the 2nd and 3rd stages histogram layers are combined into one histogram. The clustering scheme searches for local maximums of MDH, and decides clusters around local maximums as sets of hyperrectangles. The major parameters of the clustering scheme are briefly discussed, and some results are also shown

    High-pressure study of the basal-plane anisotropy of the upper critical field of the topological superconductor SrxBi2Se3

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    We report a high-pressure transport study of the upper-critical field, Bc2(T)B_{c2}(T), of the topological superconductor Sr0.15_{0.15}Bi2_2Se3_3 (Tc=3.0T_c = 3.0 K). Bc2(T)B_{c2}(T) was measured for magnetic fields directed along two orthogonal directions, aa and aβˆ—a^*, in the trigonal basal plane. While superconductivity is rapidly suppressed at the critical pressure pc∼3.5p_c \sim 3.5 GPa, the pronounced two-fold basal-plane anisotropy Bc2a/Bc2aβˆ—=3.2B_{c2}^a/B_{c2}^{a^*} = 3.2 at T=0.3T=0.3 K, recently reported at ambient pressure (Pan et al., 2016), is reinforced and attains a value of ∼5\sim 5 at the highest pressure (2.2 GPa). The data reveal that the unconventional superconducting state with broken rotational symmetry is robust under pressure

    Enhancement of superconductivity near the ferromagnetic quantum critical point in UCoGe

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    We report a high-pressure single crystal study of the superconducting ferromagnet UCoGe. Ac-susceptibility and resistivity measurements under pressures up to 2.2 GPa show ferromagnetism is smoothly depressed and vanishes at a critical pressure pc=1.4p_c = 1.4 GPa. Near the ferromagnetic critical point superconductivity is enhanced. Upper-critical field measurements under pressure show Bc2(0)B_{c2}(0) attains remarkably large values, which provides solid evidence for spin-triplet superconductivity over the whole pressure range. The obtained pβˆ’Tp-T phase diagram reveals superconductivity is closely connected to a ferromagnetic quantum critical point hidden under the superconducting `dome'.Comment: 4 pages, 3 figures; accepted for publication in PR

    Reconstruction of the spontaneously broken gauge theory in non-commutative geometry

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    The scheme previously proposed by the present authors is modified to incorporate the strong interaction by affording the direct product internal symmetry. We do not need to prepare the extra discrete space for the color gauge group responsible for the strong interaction to reconstruct the standard model and the left-right symmetric gauge model(LRSM). The approach based on non-commutative geometry leads us to presents many attractive points such as the unified picture of the gauge and Higgs field as the generalized connection on the discrete space; Minkowski space multipied by N-points discrete space. This approach leads us to unified picture of gauge and Higgs fields as the generalized connection. The standard model needs N=2 discrete space for reconstruction in this formalism. \lr is still alive as a model with the intermediate symmetry of the spontaneously broken SO(10) grand unified theory(GUT). N=3 discrete space is needed for the reconstruction of LRSM to include two Higgs bosons Ο•\phi and ΞΎ\xi which are as usual transformed as (2,2*,0)$ and (1,3,-2) under left-handed SU(2)x right-handed SU(2)x U(1), respectively. xi is responsible to make the right handed-neutrino Majorana fermion and so well explains the seesaw mechanism. Up and down quarks have the different masses through the vacuum expectation value of phi.Comment: 21 page

    А methodolocical function of Novi Pazar area songs in teaching primary music literacy of lower grades of a primary school

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    Π•Π»Π΅ΠΌΠ΅Π½Ρ‚Π°Ρ€Π½Π° ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠ° писмСност јС Π²Π΅ΡˆΡ‚ΠΈΠ½Π° ΠΏΠΎΡ˜Π΅Π΄ΠΈΠ½Ρ†Π° Π΄Π° исправно ΠΈ са Ρ€Π°Π·ΡƒΠΌΠ΅Π²Π°ΡšΠ΅ΠΌ ΠΏΠ΅Π²Π°/ свира ΠΈ Π·Π°ΠΏΠΈΡΡƒΡ˜Π΅ ΡΠ»ΡƒΡˆΠ°Π½Ρƒ ΠΌΡƒΠ·ΠΈΠΊΡƒ Π±Π΅Π· Π·Π°ΡΡ‚ΠΎΡ˜Π° Ρƒ ΡΡ…Π²Π°Ρ‚Π°ΡšΡƒ. ЊСна поставка прСдставља Π΄ΡƒΠ³ ΠΈ слоТСн процСс Ρƒ ΠΊΠΎΠΌΠ΅ јС Π½Π°Ρ˜Ρ‚Π΅ΠΆΠ΅ поставити Π΄Π²Π΅ тонскС особинС - висину (мСлодија ΠΈ Ρ…Π°Ρ€ΠΌΠΎΠ½ΠΈΡ˜Π°) ΠΈ Ρ‚Ρ€Π°Ρ˜Π°ΡšΠ΅ (Ρ€ΠΈΡ‚Π°ΠΌ). ОбС ΠΎΠ²Π΅ особинС чврсто су ΠΏΠΎΠ²Π΅Π·Π°Π½Π΅ са ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠΈΠΌ ΠΈ Π³ΠΎΠ²ΠΎΡ€Π½ΠΈΠΌ карактСристикама јСдног ΠΏΠΎΠ΄Ρ€ΡƒΡ‡Ρ˜Π° - висинС са мСлодијом ΠΈ Ρ‚ΠΎΠ½Π°Π»Π½ΠΈΠΌ основама пСсама, Π° Ρ‚Ρ€Π°Ρ˜Π°ΡšΠ° са Ρ€ΠΈΡ‚ΠΌΠΎΠΌ пСсама, ΠΈΠ³Π°Ρ€Π° ΠΈ Π³ΠΎΠ²ΠΎΡ€Π½ΠΈΠΌ Ρ€ΠΈΡ‚ΠΌΠΎΠΌ (ВасиљСвић, Π—., 1991). Π—Π°Ρ‚ΠΎ су Π½Π°Ρ€ΠΎΠ΄Π½Π΅ пСсмС - ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈ намСнскС пСсмС, ΠΊΠ°ΠΎ ΠΈ Π³ΠΎΠ²ΠΎΡ€Π½ΠΈ клишСи (Π±Ρ€ΠΎΡ˜Π°Π»ΠΈΡ†Π΅/ Ρ€Π°Π·Π±Ρ€Π°Ρ˜Π°Π»ΠΈΡ†Π΅, пословицС, Π·Π°Π³ΠΎΠ½Π΅Ρ‚ΠΊΠ΅...) ΠΊΡ™ΡƒΡ‡Π½ΠΈ ΡΠ°Π΄Ρ€ΠΆΠ°Ρ˜ΠΈ Ρƒ поставци Π·Π²ΡƒΠΊΠ° мСлодијско-Ρ€ΠΈΡ‚ΠΌΠΈΡ‡ΠΊΠ΅ ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌΠ°Ρ‚ΠΈΠΊΠ΅ ΠΏΠΎΡ‡Π΅Ρ‚Π½Π΅ наставС ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠ΅ писмСности. Π‘ ΠΎΠ±Π·ΠΈΡ€ΠΎΠΌ Π΄Π° сазнања ΠΈΠ· ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΠΊΠ΅ наставС ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠ΅ ΠΊΡƒΠ»Ρ‚ΡƒΡ€Π΅ ΠΈ ΠΏΡΠΈΡ…ΠΎΠ»ΠΎΠ³ΠΈΡ˜Π΅ ΠΌΡƒΠ·ΠΈΠΊΠ΅ ΡƒΠΏΡƒΡ›ΡƒΡ˜Ρƒ Π΄Π° Π΅Π»Π΅ΠΌΠ΅Π½Ρ‚Π°Ρ€Π½Ρƒ ΠΌΡƒΠ·ΠΈΡ‡ΠΊΡƒ писмСност Ρ‚Ρ€Π΅Π±Π° поставити Π½Π° Π·Π²ΡƒΡ‡Π½ΠΈΠΌ основама ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠΎΠ³ ΠΌΠ°Ρ‚Π΅Ρ€ΡšΠ΅Π³ јСзика срСдинС Ρƒ којој сС настава ΠΈΠ·Π²ΠΎΠ΄ΠΈ, ΠΎΠ΄Π»ΡƒΡ‡ΠΈΠ»ΠΈ смо Π΄Π° ΠΊΡ€Π΅Π½Π΅ΠΌΠΎ Ρƒ ΠΏΡ€ΠΎΠ½Π°Π»Π°ΠΆΠ΅ΡšΠ΅ пСсама ΠΌΡƒΠ»Ρ‚ΠΈΠΊΡƒΠ»Ρ‚ΡƒΡ€Π°Π»Π½ΠΎΠ³ новопазарског ΠΊΡ€Π°Ρ˜Π° којС ΠΌΠΎΠ³Ρƒ ΠΏΡ€Π΅ΡƒΠ·Π΅Ρ‚ΠΈ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΡ˜Ρƒ ΠΌΠΎΠ΄Π΅Π»Π° ΠΈ намСнских пСсама Ρƒ ΡšΠ΅ΠΌΡƒ. Π’ΠΎ јС Π±ΠΈΠ»ΠΎ ΠΌΠΎΠ³ΡƒΡ›Π΅ само ΠΏΡƒΡ‚Π΅ΠΌ ΠΈΡΡ‚Ρ€Π°ΠΆΠΈΠ²Π°ΡšΠ° којС јС ΠΈΠΌΠ°Π»ΠΎ Π·Π° Ρ†ΠΈΡ™ ΡΡ‚Π²Π°Ρ€Π°ΡšΠ΅ основног ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠΎΠ³ ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΡ˜Π°Π»Π° који Π·Π°Π΄ΠΎΠ²ΠΎΡ™Π°Π²Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΡ‡ΠΊΠ΅ ΠΊΡ€ΠΈΡ‚Π΅Ρ€ΠΈΡ˜ΡƒΠΌΠ΅ Π·Π° поставку Π΅Π»Π΅ΠΌΠ΅Π½Ρ‚Π°Ρ€Π½Π΅ ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠ΅ писмСности. ΠœΠ΅Ρ‚ΠΎΠ΄ΠΎΠΌ Ρ‚Π΅ΠΎΡ€ΠΈΡ˜ΡΠΊΠ΅ Π°Π½Π°Π»ΠΈΠ·Π΅ Ρ€Π΅Π»Π΅Π²Π°Π½Ρ‚Π½Π΅ Π»ΠΈΡ‚Π΅Ρ€Π°Ρ‚ΡƒΡ€Π΅ ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠ΅ писмСности ΠΈ ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠ΅ Π³Ρ€Π°Ρ’Π΅ новопазарског ΠΊΡ€Π°Ρ˜Π° (Π΅Ρ‚Π½ΠΎΠΌΡƒΠ·ΠΈΠΊΠΎΠ»ΠΎΡˆΠΊΠΈΡ… записа пСсама) створили смо прСтпоставку Π·Π° могућност ΠΊΡ€Π΅ΠΈΡ€Π°ΡšΠ° ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠ΅ Π³Ρ€Π°Ρ’Π΅ која Π·Π°Π΄ΠΎΠ²ΠΎΡ™Π°Π²Π° ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΡ‡ΠΊΠ΅ ΠΊΡ€ΠΈΡ‚Π΅Ρ€ΠΈΡ˜ΡƒΠΌΠ΅ (ΠΌΠ°Ρ‚Π΅Ρ€ΠΈΡ˜Π°Π» Π½Π° ΠΊΠΎΠΌΠ΅ ΠΌΠΎΠ³Ρƒ Π΄Π° сС Ρ€Π΅ΡˆΠ°Π²Π°Ρ˜Ρƒ ΠΏΡ€ΠΎΠ±Π»Π΅ΠΌΠΈ Π²Π΅Π·Π°Π½ΠΈ Π·Π° наставу Π΅Π»Π΅ΠΌΠ΅Π½Ρ‚Π°Ρ€Π½Π΅ ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠ΅ писмСности). Π‘ ΠΎΠ±Π·ΠΈΡ€ΠΎΠΌ Π΄Π° сС ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠΈ ΠΌΠ°Ρ‚Π΅Ρ€ΡšΠΈ јСзик новопазарског ΠΊΡ€Π°Ρ˜Π° Π²Ρ€Π΅ΠΌΠ΅Π½ΠΎΠΌ мСњао ΠΏΠΎΡ‚Ρ€Π΅Π±Π½ΠΎ јС Π±ΠΈΠ»ΠΎ установити ΠΈ присутност ΠΌΠ΅Ρ‚ΠΎΠ΄ΠΈΡ‡ΠΊΠΈ ΠΏΡ€ΠΈΠΌΠ΅ΡšΠΈΠ²ΠΈΡ… пСсама ΠΈ ΠΊΡ€Π°Ρ‚ΠΊΠΈΡ… Π³ΠΎΠ²ΠΎΡ€Π½ΠΈΡ… Ρ„ΠΎΡ€ΠΌΠΈ Ρƒ свСсти Π΄Π΅Ρ†Π΅. Π Π΅Π·ΡƒΠ»Ρ‚Π°Ρ‚ΠΈ ΠΈΡΡ‚Ρ€Π°ΠΆΠΈΠ²Π°ΡšΠ° ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ су Π΄Π° ΠΎΠ΄Ρ€Π΅Ρ’Π΅Π½Π΅ пСсмС новопазарског ΠΊΡ€Π°Ρ˜Π° (ΡƒΠ· извСсна ΠΏΡ€ΠΈΠ»Π°Π³ΠΎΡ’Π°Π²Π°ΡšΠ°) ΠΈ ΠΊΡ€Π°Ρ‚ΠΊΠ΅ Π³ΠΎΠ²ΠΎΡ€Π½Π΅ Ρ„ΠΎΡ€ΠΌΠ΅ ΠΌΠΎΠ³Ρƒ ΠΏΡ€Π΅ΡƒΠ·Π΅Ρ‚ΠΈ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΡ˜Ρƒ Π΅Π»Π΅ΠΌΠ΅Π½Ρ‚Π°Ρ€Π½ΠΎΠ³ ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠΎΠ³ описмСњавања ΡƒΡ‡Π΅Π½ΠΈΠΊΠ° ΠΌΠ»Π°Ρ’ΠΈΡ… Ρ€Π°Π·Ρ€Π΅Π΄Π° основнС школС, Ρ‚Π΅ Π΄Π° јС Π²Π΅Ρ›ΠΈΠ½Π° ΡšΠΈΡ… још ΡƒΠ²Π΅ΠΊ присутна Ρƒ свСсти Π»ΠΎΠΊΠ»Π°Π½ΠΎΠ³ ΡΡ‚Π°Π½ΠΎΠ²Π½ΠΈΡˆΡ‚Π²Π°. Π£ складу са Ρ€Π΅Π·ΡƒΠ»Ρ‚Π°Ρ‚ΠΈΠΌΠ° ΠΈΡΡ‚Ρ€Π°ΠΆΠΈΠ²Π°ΡšΠ° ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠΎΠ³ ΠΌΠ°Ρ‚Π΅Ρ€ΡšΠ΅Π³ јСзика новопазарског ΠΊΡ€Π°Ρ˜Π° Π½Π°Ρ‡ΠΈΡšΠ΅Π½ јС ΠΊΠΎΠ½Ρ†Π΅ΠΏΡ‚ΡƒΠ°Π»Π½ΠΈ ΠΎΠΊΠ²ΠΈΡ€ ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠ΅ Π³Ρ€Π°Ρ’Π΅ која јС Ρƒ Ρ„ΡƒΠ½ΠΊΡ†ΠΈΡ˜ΠΈ поставкС Π΅Π»Π΅ΠΌΠ΅Π½Ρ‚Π°Ρ€Π½Π΅ ΠΌΡƒΠ·ΠΈΡ‡ΠΊΠ΅ писмСности Π½Π° Π½Π°Ρ€ΠΎΠ΄Π½ΠΈΠΌ основама ΠΎΠ²ΠΎΠ³ ΠΊΡ€Π°Ρ˜Π° са свим особСностима ΠΌΡƒΠ»Ρ‚ΠΈΠΊΡƒΠ»Ρ‚ΡƒΡ€Π°Π»Π½Π΅ срСдинС.The primary music literacy is a skill of an individual to sing/play correctly and write down music that is heard, with no pauses in its understanding. Its establishment represents a long and complex process, where it is the most difficult to set two tones characteristics- its altitude (melody and harmony), and its duration (rhythm). These two characteristics are tightly connected with music and speech characteristics of an areaaltitude with melody and tonal bases/ scales of songs, and duration with the songs rhythm, dancing and speech rhythm (Vasiljevic, Z., 1991). Therefore, folk songsmodels and dedicated songs, and also speech clichΓ©s (chants/nursery rhythms, proverbs, riddles), are key contents in a sound establishment with a melodic-rhythmical issue of the starting setting of music literacy. Since the knowledge from methodology of Music Culture teaching and Psychology should be established on sound bases of a music mother tongue of the area where teaching is being performed, we have decided to start in finding songs of the multicultural Novi Pazar area that can overtake a function of a model and dedicated songs in it. It has been possible only through a research that has had for its aim a creation of the primary music material that satisfies methodological criteria for establishment of the primary music literacy. With the method of a theoretical analyze of a relevant literature music literacy and music material of Novi Pazar area (ethno-music recordings of songs), we have created an assumption for a possible creation of the music material (the material where issues can be solved related to the primary teaching of music literacy). Since music mother tongue of Novi Pazar area has been changed by the time, it has also been necessary to establish the presence of methodologically applied songs and short speech forms to the awareness of the local population. The research results have shown that certain songs of Novi Pazar area (with certain modifications) and short speech forms can overtake the function of the primary music literacy of lower grades pupils of a Primary School, and thus, most of them are still present in the awareness of the children. Pursuant to the research results of the music mother tongue of Novi Pazar area, it has been made a conceptual framework of music material that is in the function of the primary music literacy in the folk bases of this area, with all its specifics of the multicultural area

    Angular variation of the magnetoresistance of the superconducting ferromagnet UCoGe

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    We report a magnetoresistance study of the superconducting ferromagnet UCoGe. The data, taken on single-crystalline samples, show a pronounced structure at Bβˆ—=8.5B^* = 8.5~T for a field applied along the ordered moment m0m_0. Angle dependent measurements reveal this field-induced phenomenon has an uniaxial anisotropy. Magnetoresistance measurements under pressure show a rapid increase of Bβˆ—B^* to 12.8~T at 1.0~GPa. We discuss Bβˆ—B^* in terms of a field induced polarization change. Upper critical field measurements corroborate the unusual S-shaped Bc2(T)B_{c2}(T)-curve for a field along the bb-axis of the orthorhombic unit cell.Comment: 6 pages, 5 figures; accepted for publication in Phys. Rev.
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