2,003 research outputs found
A New Clustering Method for Landsat Images Using Local Maximums of a Multidimensional Histogram
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
We report a high-pressure transport study of the upper-critical field,
, of the topological superconductor SrBiSe ( K). was measured for magnetic fields directed along two
orthogonal directions, and , in the trigonal basal plane. While
superconductivity is rapidly suppressed at the critical pressure
GPa, the pronounced two-fold basal-plane anisotropy at K, recently reported at ambient pressure (Pan et al., 2016), is
reinforced and attains a value of 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
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 GPa. Near the ferromagnetic critical point
superconductivity is enhanced. Upper-critical field measurements under pressure
show attains remarkably large values, which provides solid evidence
for spin-triplet superconductivity over the whole pressure range. The obtained
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
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 and 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
Π methodolocical function of Novi Pazar area songs in teaching primary music literacy of lower grades of a primary school
ΠΠ»Π΅ΠΌΠ΅Π½ΡΠ°ΡΠ½Π° ΠΌΡΠ·ΠΈΡΠΊΠ° ΠΏΠΈΡΠΌΠ΅Π½ΠΎΡΡ ΡΠ΅ Π²Π΅ΡΡΠΈΠ½Π° ΠΏΠΎΡΠ΅Π΄ΠΈΠ½ΡΠ° Π΄Π° ΠΈΡΠΏΡΠ°Π²Π½ΠΎ ΠΈ ΡΠ°
ΡΠ°Π·ΡΠΌΠ΅Π²Π°ΡΠ΅ΠΌ ΠΏΠ΅Π²Π°/ ΡΠ²ΠΈΡΠ° ΠΈ Π·Π°ΠΏΠΈΡΡΡΠ΅ ΡΠ»ΡΡΠ°Π½Ρ ΠΌΡΠ·ΠΈΠΊΡ Π±Π΅Π· Π·Π°ΡΡΠΎΡΠ° Ρ ΡΡ
Π²Π°ΡΠ°ΡΡ. ΠΠ΅Π½Π°
ΠΏΠΎΡΡΠ°Π²ΠΊΠ° ΠΏΡΠ΅Π΄ΡΡΠ°Π²ΡΠ° Π΄ΡΠ³ ΠΈ ΡΠ»ΠΎΠΆΠ΅Π½ ΠΏΡΠΎΡΠ΅Ρ Ρ ΠΊΠΎΠΌΠ΅ ΡΠ΅ Π½Π°ΡΡΠ΅ΠΆΠ΅ ΠΏΠΎΡΡΠ°Π²ΠΈΡΠΈ Π΄Π²Π΅ ΡΠΎΠ½ΡΠΊΠ΅
ΠΎΡΠΎΠ±ΠΈΠ½Π΅ - Π²ΠΈΡΠΈΠ½Ρ (ΠΌΠ΅Π»ΠΎΠ΄ΠΈΡΠ° ΠΈ Ρ
Π°ΡΠΌΠΎΠ½ΠΈΡΠ°) ΠΈ ΡΡΠ°ΡΠ°ΡΠ΅ (ΡΠΈΡΠ°ΠΌ). ΠΠ±Π΅ ΠΎΠ²Π΅ ΠΎΡΠΎΠ±ΠΈΠ½Π΅
ΡΠ²ΡΡΡΠΎ ΡΡ ΠΏΠΎΠ²Π΅Π·Π°Π½Π΅ ΡΠ° ΠΌΡΠ·ΠΈΡΠΊΠΈΠΌ ΠΈ Π³ΠΎΠ²ΠΎΡΠ½ΠΈΠΌ ΠΊΠ°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°ΠΌΠ° ΡΠ΅Π΄Π½ΠΎΠ³ ΠΏΠΎΠ΄ΡΡΡΡΠ° -
Π²ΠΈΡΠΈΠ½Π΅ ΡΠ° ΠΌΠ΅Π»ΠΎΠ΄ΠΈΡΠΎΠΌ ΠΈ ΡΠΎΠ½Π°Π»Π½ΠΈΠΌ ΠΎΡΠ½ΠΎΠ²Π°ΠΌΠ° ΠΏΠ΅ΡΠ°ΠΌΠ°, Π° ΡΡΠ°ΡΠ°ΡΠ° ΡΠ° ΡΠΈΡΠΌΠΎΠΌ ΠΏΠ΅ΡΠ°ΠΌΠ°,
ΠΈΠ³Π°ΡΠ° ΠΈ Π³ΠΎΠ²ΠΎΡΠ½ΠΈΠΌ ΡΠΈΡΠΌΠΎΠΌ (ΠΠ°ΡΠΈΡΠ΅Π²ΠΈΡ, Π., 1991). ΠΠ°ΡΠΎ ΡΡ Π½Π°ΡΠΎΠ΄Π½Π΅ ΠΏΠ΅ΡΠΌΠ΅ - ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈ
Π½Π°ΠΌΠ΅Π½ΡΠΊΠ΅ ΠΏΠ΅ΡΠΌΠ΅, ΠΊΠ°ΠΎ ΠΈ Π³ΠΎΠ²ΠΎΡΠ½ΠΈ ΠΊΠ»ΠΈΡΠ΅ΠΈ (Π±ΡΠΎΡΠ°Π»ΠΈΡΠ΅/ ΡΠ°Π·Π±ΡΠ°ΡΠ°Π»ΠΈΡΠ΅, ΠΏΠΎΡΠ»ΠΎΠ²ΠΈΡΠ΅,
Π·Π°Π³ΠΎΠ½Π΅ΡΠΊΠ΅...) ΠΊΡΡΡΠ½ΠΈ ΡΠ°Π΄ΡΠΆΠ°ΡΠΈ Ρ ΠΏΠΎΡΡΠ°Π²ΡΠΈ Π·Π²ΡΠΊΠ° ΠΌΠ΅Π»ΠΎΠ΄ΠΈΡΡΠΊΠΎ-ΡΠΈΡΠΌΠΈΡΠΊΠ΅
ΠΏΡΠΎΠ±Π»Π΅ΠΌΠ°ΡΠΈΠΊΠ΅ ΠΏΠΎΡΠ΅ΡΠ½Π΅ Π½Π°ΡΡΠ°Π²Π΅ ΠΌΡΠ·ΠΈΡΠΊΠ΅ ΠΏΠΈΡΠΌΠ΅Π½ΠΎΡΡΠΈ. Π‘ ΠΎΠ±Π·ΠΈΡΠΎΠΌ Π΄Π° ΡΠ°Π·Π½Π°ΡΠ° ΠΈΠ·
ΠΌΠ΅ΡΠΎΠ΄ΠΈΠΊΠ΅ Π½Π°ΡΡΠ°Π²Π΅ ΠΌΡΠ·ΠΈΡΠΊΠ΅ ΠΊΡΠ»ΡΡΡΠ΅ ΠΈ ΠΏΡΠΈΡ
ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ ΠΌΡΠ·ΠΈΠΊΠ΅ ΡΠΏΡΡΡΡΡ Π΄Π° Π΅Π»Π΅ΠΌΠ΅Π½ΡΠ°ΡΠ½Ρ
ΠΌΡΠ·ΠΈΡΠΊΡ ΠΏΠΈΡΠΌΠ΅Π½ΠΎΡΡ ΡΡΠ΅Π±Π° ΠΏΠΎΡΡΠ°Π²ΠΈΡΠΈ Π½Π° Π·Π²ΡΡΠ½ΠΈΠΌ ΠΎΡΠ½ΠΎΠ²Π°ΠΌΠ° ΠΌΡΠ·ΠΈΡΠΊΠΎΠ³ ΠΌΠ°ΡΠ΅ΡΡΠ΅Π³
ΡΠ΅Π·ΠΈΠΊΠ° ΡΡΠ΅Π΄ΠΈΠ½Π΅ Ρ ΠΊΠΎΡΠΎΡ ΡΠ΅ Π½Π°ΡΡΠ°Π²Π° ΠΈΠ·Π²ΠΎΠ΄ΠΈ, ΠΎΠ΄Π»ΡΡΠΈΠ»ΠΈ ΡΠΌΠΎ Π΄Π° ΠΊΡΠ΅Π½Π΅ΠΌΠΎ Ρ ΠΏΡΠΎΠ½Π°Π»Π°ΠΆΠ΅ΡΠ΅
ΠΏΠ΅ΡΠ°ΠΌΠ° ΠΌΡΠ»ΡΠΈΠΊΡΠ»ΡΡΡΠ°Π»Π½ΠΎΠ³ Π½ΠΎΠ²ΠΎΠΏΠ°Π·Π°ΡΡΠΊΠΎΠ³ ΠΊΡΠ°ΡΠ° ΠΊΠΎΡΠ΅ ΠΌΠΎΠ³Ρ ΠΏΡΠ΅ΡΠ·Π΅ΡΠΈ ΡΡΠ½ΠΊΡΠΈΡΡ
ΠΌΠΎΠ΄Π΅Π»Π° ΠΈ Π½Π°ΠΌΠ΅Π½ΡΠΊΠΈΡ
ΠΏΠ΅ΡΠ°ΠΌΠ° Ρ ΡΠ΅ΠΌΡ. Π’ΠΎ ΡΠ΅ Π±ΠΈΠ»ΠΎ ΠΌΠΎΠ³ΡΡΠ΅ ΡΠ°ΠΌΠΎ ΠΏΡΡΠ΅ΠΌ ΠΈΡΡΡΠ°ΠΆΠΈΠ²Π°ΡΠ°
ΠΊΠΎΡΠ΅ ΡΠ΅ ΠΈΠΌΠ°Π»ΠΎ Π·Π° ΡΠΈΡ ΡΡΠ²Π°ΡΠ°ΡΠ΅ ΠΎΡΠ½ΠΎΠ²Π½ΠΎΠ³ ΠΌΡΠ·ΠΈΡΠΊΠΎΠ³ ΠΌΠ°ΡΠ΅ΡΠΈΡΠ°Π»Π° ΠΊΠΎΡΠΈ Π·Π°Π΄ΠΎΠ²ΠΎΡΠ°Π²Π°
ΠΌΠ΅ΡΠΎΠ΄ΠΈΡΠΊΠ΅ ΠΊΡΠΈΡΠ΅ΡΠΈΡΡΠΌΠ΅ Π·Π° ΠΏΠΎΡΡΠ°Π²ΠΊΡ Π΅Π»Π΅ΠΌΠ΅Π½ΡΠ°ΡΠ½Π΅ ΠΌΡΠ·ΠΈΡΠΊΠ΅ ΠΏΠΈΡΠΌΠ΅Π½ΠΎΡΡΠΈ. ΠΠ΅ΡΠΎΠ΄ΠΎΠΌ
ΡΠ΅ΠΎΡΠΈΡΡΠΊΠ΅ Π°Π½Π°Π»ΠΈΠ·Π΅ ΡΠ΅Π»Π΅Π²Π°Π½ΡΠ½Π΅ Π»ΠΈΡΠ΅ΡΠ°ΡΡΡΠ΅ ΠΌΡΠ·ΠΈΡΠΊΠ΅ ΠΏΠΈΡΠΌΠ΅Π½ΠΎΡΡΠΈ ΠΈ ΠΌΡΠ·ΠΈΡΠΊΠ΅ Π³ΡΠ°ΡΠ΅
Π½ΠΎΠ²ΠΎΠΏΠ°Π·Π°ΡΡΠΊΠΎΠ³ ΠΊΡΠ°ΡΠ° (Π΅ΡΠ½ΠΎΠΌΡΠ·ΠΈΠΊΠΎΠ»ΠΎΡΠΊΠΈΡ
Π·Π°ΠΏΠΈΡΠ° ΠΏΠ΅ΡΠ°ΠΌΠ°) ΡΡΠ²ΠΎΡΠΈΠ»ΠΈ ΡΠΌΠΎ
ΠΏΡΠ΅ΡΠΏΠΎΡΡΠ°Π²ΠΊΡ Π·Π° ΠΌΠΎΠ³ΡΡΠ½ΠΎΡΡ ΠΊΡΠ΅ΠΈΡΠ°ΡΠ° ΠΌΡΠ·ΠΈΡΠΊΠ΅ Π³ΡΠ°ΡΠ΅ ΠΊΠΎΡΠ° Π·Π°Π΄ΠΎΠ²ΠΎΡΠ°Π²Π° ΠΌΠ΅ΡΠΎΠ΄ΠΈΡΠΊΠ΅
ΠΊΡΠΈΡΠ΅ΡΠΈΡΡΠΌΠ΅ (ΠΌΠ°ΡΠ΅ΡΠΈΡΠ°Π» Π½Π° ΠΊΠΎΠΌΠ΅ ΠΌΠΎΠ³Ρ Π΄Π° ΡΠ΅ ΡΠ΅ΡΠ°Π²Π°ΡΡ ΠΏΡΠΎΠ±Π»Π΅ΠΌΠΈ Π²Π΅Π·Π°Π½ΠΈ Π·Π° Π½Π°ΡΡΠ°Π²Ρ
Π΅Π»Π΅ΠΌΠ΅Π½ΡΠ°ΡΠ½Π΅ ΠΌΡΠ·ΠΈΡΠΊΠ΅ ΠΏΠΈΡΠΌΠ΅Π½ΠΎΡΡΠΈ). Π‘ ΠΎΠ±Π·ΠΈΡΠΎΠΌ Π΄Π° ΡΠ΅ ΠΌΡΠ·ΠΈΡΠΊΠΈ ΠΌΠ°ΡΠ΅ΡΡΠΈ ΡΠ΅Π·ΠΈΠΊ
Π½ΠΎΠ²ΠΎΠΏΠ°Π·Π°ΡΡΠΊΠΎΠ³ ΠΊΡΠ°ΡΠ° Π²ΡΠ΅ΠΌΠ΅Π½ΠΎΠΌ ΠΌΠ΅ΡΠ°ΠΎ ΠΏΠΎΡΡΠ΅Π±Π½ΠΎ ΡΠ΅ Π±ΠΈΠ»ΠΎ ΡΡΡΠ°Π½ΠΎΠ²ΠΈΡΠΈ ΠΈ ΠΏΡΠΈΡΡΡΠ½ΠΎΡΡ
ΠΌΠ΅ΡΠΎΠ΄ΠΈΡΠΊΠΈ ΠΏΡΠΈΠΌΠ΅ΡΠΈΠ²ΠΈΡ
ΠΏΠ΅ΡΠ°ΠΌΠ° ΠΈ ΠΊΡΠ°ΡΠΊΠΈΡ
Π³ΠΎΠ²ΠΎΡΠ½ΠΈΡ
ΡΠΎΡΠΌΠΈ Ρ ΡΠ²Π΅ΡΡΠΈ Π΄Π΅ΡΠ΅.
Π Π΅Π·ΡΠ»ΡΠ°ΡΠΈ ΠΈΡΡΡΠ°ΠΆΠΈΠ²Π°ΡΠ° ΠΏΠΎΠΊΠ°Π·Π°Π»ΠΈ ΡΡ Π΄Π° ΠΎΠ΄ΡΠ΅ΡΠ΅Π½Π΅ ΠΏΠ΅ΡΠΌΠ΅ Π½ΠΎΠ²ΠΎΠΏΠ°Π·Π°ΡΡΠΊΠΎΠ³ ΠΊΡΠ°ΡΠ° (ΡΠ·
ΠΈΠ·Π²Π΅ΡΠ½Π° ΠΏΡΠΈΠ»Π°Π³ΠΎΡΠ°Π²Π°ΡΠ°) ΠΈ ΠΊΡΠ°ΡΠΊΠ΅ Π³ΠΎΠ²ΠΎΡΠ½Π΅ ΡΠΎΡΠΌΠ΅ ΠΌΠΎΠ³Ρ ΠΏΡΠ΅ΡΠ·Π΅ΡΠΈ ΡΡΠ½ΠΊΡΠΈΡΡ
Π΅Π»Π΅ΠΌΠ΅Π½ΡΠ°ΡΠ½ΠΎΠ³ ΠΌΡΠ·ΠΈΡΠΊΠΎΠ³ ΠΎΠΏΠΈΡΠΌΠ΅ΡΠ°Π²Π°ΡΠ° ΡΡΠ΅Π½ΠΈΠΊΠ° ΠΌΠ»Π°ΡΠΈΡ
ΡΠ°Π·ΡΠ΅Π΄Π° ΠΎΡΠ½ΠΎΠ²Π½Π΅ ΡΠΊΠΎΠ»Π΅, ΡΠ΅
Π΄Π° ΡΠ΅ Π²Π΅ΡΠΈΠ½Π° ΡΠΈΡ
ΡΠΎΡ ΡΠ²Π΅ΠΊ ΠΏΡΠΈΡΡΡΠ½Π° Ρ ΡΠ²Π΅ΡΡΠΈ Π»ΠΎΠΊΠ»Π°Π½ΠΎΠ³ ΡΡΠ°Π½ΠΎΠ²Π½ΠΈΡΡΠ²Π°. Π£ ΡΠΊΠ»Π°Π΄Ρ ΡΠ°
ΡΠ΅Π·ΡΠ»ΡΠ°ΡΠΈΠΌΠ° ΠΈΡΡΡΠ°ΠΆΠΈΠ²Π°ΡΠ° ΠΌΡΠ·ΠΈΡΠΊΠΎΠ³ ΠΌΠ°ΡΠ΅ΡΡΠ΅Π³ ΡΠ΅Π·ΠΈΠΊΠ° Π½ΠΎΠ²ΠΎΠΏΠ°Π·Π°ΡΡΠΊΠΎΠ³ ΠΊΡΠ°ΡΠ° Π½Π°ΡΠΈΡΠ΅Π½
ΡΠ΅ ΠΊΠΎΠ½ΡΠ΅ΠΏΡΡΠ°Π»Π½ΠΈ ΠΎΠΊΠ²ΠΈΡ ΠΌΡΠ·ΠΈΡΠΊΠ΅ Π³ΡΠ°ΡΠ΅ ΠΊΠΎΡΠ° ΡΠ΅ Ρ ΡΡΠ½ΠΊΡΠΈΡΠΈ ΠΏΠΎΡΡΠ°Π²ΠΊΠ΅ Π΅Π»Π΅ΠΌΠ΅Π½ΡΠ°ΡΠ½Π΅
ΠΌΡΠ·ΠΈΡΠΊΠ΅ ΠΏΠΈΡΠΌΠ΅Π½ΠΎΡΡΠΈ Π½Π° Π½Π°ΡΠΎΠ΄Π½ΠΈΠΌ ΠΎΡΠ½ΠΎΠ²Π°ΠΌΠ° ΠΎΠ²ΠΎΠ³ ΠΊΡΠ°ΡΠ° ΡΠ° ΡΠ²ΠΈΠΌ ΠΎΡΠΎΠ±Π΅Π½ΠΎΡΡΠΈΠΌΠ°
ΠΌΡΠ»ΡΠΈΠΊΡΠ»ΡΡΡΠ°Π»Π½Π΅ ΡΡΠ΅Π΄ΠΈΠ½Π΅.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
We report a magnetoresistance study of the superconducting ferromagnet UCoGe.
The data, taken on single-crystalline samples, show a pronounced structure at
~T for a field applied along the ordered moment . Angle
dependent measurements reveal this field-induced phenomenon has an uniaxial
anisotropy. Magnetoresistance measurements under pressure show a rapid increase
of to 12.8~T at 1.0~GPa. We discuss in terms of a field induced
polarization change. Upper critical field measurements corroborate the unusual
S-shaped -curve for a field along the -axis of the orthorhombic
unit cell.Comment: 6 pages, 5 figures; accepted for publication in Phys. Rev.
- β¦