174 research outputs found
Global Partial Density of States: Statistics and Localization Length in Quasi-one Dimensional disordered systems
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 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 , where 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 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
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‘ΡΠ°Π²Π½ΠΈΡΠ΅Π»ΡΠ½Π°Ρ ΠΎΡΠ΅Π½ΠΊΠ° Π±ΠΈΠΎΡ ΠΈΠΌΠΈΡΠ΅ΡΠΊΠΈΡ ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»Π΅ΠΉ ΠΈ ΠΌΠΈΠ½Π΅ΡΠ°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠΎΡΡΠ°Π²Π° ΠΏΠ»ΠΎΠ΄ΠΎΠ² Cucurbita ficifolia, C. maxima ΠΈ C. moschata
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.Β Π Π°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈ Π°ΠΊΡΠΈΠ²Π½ΡΡ
ΡΠΎΠ΅Π΄ΠΈΠ½Π΅Π½ΠΈΠΉ ΠΌΠ΅ΠΆΠ΄Ρ ΠΊΠΎΠΆΡΡΠΎΠΉ ΠΈ ΠΌΡΠΊΠΎΡΡΡ ΠΏΠ»ΠΎΠ΄ΠΎΠ² ΡΠ²Π»ΡΠ΅ΡΡΡ Π²Π°ΠΆΠ½ΠΎΠΉ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΎΠΉ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΠΈ ΡΠΈΠ·ΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈ ΡΠ°ΡΡΠ΅Π½ΠΈΡ ΠΈ ΠΌΠΎΠΆΠ΅Ρ ΡΠ»ΡΠΆΠΈΡΡ ΠΎΡΠ½ΠΎΠ²ΠΎΠΉ Π΄Π»Ρ Π±Π΅Π·ΠΎΡΡ
ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΡΡΠ²Π° Π² ΡΠ΅Π»ΡΡΠΊΠΎΠΌ Ρ
ΠΎΠ·ΡΠΉΡΡΠ²Π΅.Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½ΠΎ, ΡΡΠΎ ΡΡΠ΅Π΄ΠΈ ΡΡΠ΅Ρ
Π²ΠΈΠ΄ΠΎΠ² ΡΡΠΊΠ²Ρ: ΡΠΈΠ³ΠΎΠ»ΠΈΡΡΠ½ΠΎΠΉ (C. ficifolia), ΠΊΡΡΠΏΠ½ΠΎΠΏΠ»ΠΎΠ΄Π½ΠΎΠΉ (C. maxima) ΠΈ ΠΌΡΡΠΊΠ°ΡΠ½ΠΎΠΉ (C. moschata), β ΡΠΈΠ³ΠΎΠ»ΠΈΡΡΠ½Π°Ρ ΡΡΠΊΠ²Π° ΡΠΎΠ΄Π΅ΡΠΆΠΈΡ Π½Π°ΠΈΠΌΠ΅Π½ΡΡΠ΅Π΅ ΠΊΠΎΠ»ΠΈΡΠ΅ΡΡΠ²ΠΎ ΡΡΡ
ΠΎΠ³ΠΎ Π²Π΅ΡΠ΅ΡΡΠ²Π°, ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎ Π² ΠΊΠΎΠΆΡΡΠ΅ ΠΏΠ»ΠΎΠ΄ΠΎΠ², ΡΡ
ΠΎΠ΄Π½ΡΠ΅ ΡΡΠΎΠ²Π½ΠΈ ΠΎΠ±ΡΠ΅ΠΉ Π°Π½ΡΠΈΠΎΠΊΡΠΈΠ΄Π°Π½ΡΠ½ΠΎΠΉ Π°ΠΊΡΠΈΠ²Π½ΠΎΡΡΠΈ (ΠΠΠ) ΠΈ ΡΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΡ ΠΏΠΎΠ»ΠΈΡΠ΅Π½ΠΎΠ»ΠΎΠ² (Π’Π ) Π² ΠΊΠΎΠΆΡΡΠ΅ ΠΈ ΠΌΡΠΊΠΎΡΠΈ ΠΏΡΠΈ ΠΌΠ°ΠΊΡΠΈΠΌΠ°Π»ΡΠ½ΡΡ
ΠΏΠΎΠΊΠ°Π·Π°ΡΠ΅Π»ΡΡ
Π°Π½ΡΠΈΠΎΠΊΡΠΈΠ΄Π°Π½ΡΠ½ΠΎΠ³ΠΎ ΡΡΠ°ΡΡΡΠ° Π² ΠΏΠ»Π°ΡΠ΅Π½ΡΠ΅. Π£Π³Π»Π΅Π²ΠΎΠ΄Π½ΡΠΉ ΠΏΡΠΎΡΠΈΠ»Ρ ΠΊΠΎΠΆΡΡΡ ΡΠΈΠ³ΠΎΠ»ΠΈΡΡΠ½ΠΎΠΉ ΡΡΠΊΠ²Ρ C. ficifolia Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΠΎΠ²Π°Π»ΡΡ Π½Π°ΠΈΠΌΠ΅Π½ΡΡΠΈΠΌΠΈ ΡΡΠΎΠ²Π½ΡΠΌΠΈ Π΄ΠΈΡΠ°Ρ
Π°ΡΠΈΠ΄ΠΎΠ² ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΠΊΠΎΠΆΡΡΠΎΠΉ ΠΊΡΡΠΏΠ½ΠΎΠΏΠ»ΠΎΠ΄Π½ΠΎΠΉ C. maxima ΠΈ ΠΌΡΡΠΊΠ°ΡΠ½ΠΎΠΉ ΡΡΠΊΠ²Ρ C. moschata ΠΈ Π½Π°ΠΈΠ±ΠΎΠ»ΡΡΠΈΠΌΠΈ ΡΡΠΎΠ²Π½ΡΠΌΠΈ ΠΌΠΎΠ½ΠΎΡΠ°Ρ
Π°ΡΠΎΠ². ΠΠ‘Π-ΠΠ‘ Π°Π½Π°Π»ΠΈΠ· ΡΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΡ 25 ΡΠ»Π΅ΠΌΠ΅Π½ΡΠΎΠ² Π² ΠΊΠΎΠΆΡΡΠ΅ ΠΈ ΠΌΡΠΊΠΎΡΠΈ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½Π½ΡΡ
Π²ΠΈΠ΄ΠΎΠ² ΡΡΠΊΠ²Ρ ΠΏΠΎΠΊΠ°Π·Π°Π», ΡΡΠΎ ΡΠΈΠ³ΠΎΠ»ΠΈΡΡΠ½Π°Ρ ΡΡΠΊΠ²Π° ΠΎΡΠ»ΠΈΡΠ°Π΅ΡΡΡ Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π±ΠΎΠ»Π΅Π΅ Π²ΡΡΠΎΠΊΠΈΠΌΠΈ ΡΡΠΎΠ²Π½ΡΠΌΠΈ Π½Π°ΠΊΠΎΠΏΠ»Π΅Π½ΠΈΡ Π² ΠΌΡΠΊΠΎΡΠΈ Sr, Si, I ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ Π°Π½Π°Π»ΠΎΠ³ΠΈΡΠ½ΡΠΌΠΈ Π΄Π°Π½Π½ΡΠΌΠΈ Π΄Π»Ρ ΡΡΠΊΠ²Ρ ΠΊΡΡΠΏΠ½ΠΎΠΏΠ»ΠΎΠ΄Π½ΠΎΠΉ C. maxima ΠΈ ΠΌΡΡΠΊΠ°ΡΠ½ΠΎΠΉ C. moschata. ΠΠ°ΠΏΡΠΎΡΠΈΠ², ΠΏΠ»ΠΎΠ΄Ρ ΠΊΡΡΠΏΠ½ΠΎΠΏΠ»ΠΎΠ΄Π½ΠΎΠΉ ΠΈ ΠΌΡΡΠΊΠ°ΡΠ½ΠΎΠΉ ΡΡΠΊΠ²Ρ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΠΎΠ²Π°Π»ΠΈΡΡ Π½ΠΈΠ·ΠΊΠΈΠΌΠΈ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΡΠΌΠΈ Mn Π² ΠΌΡΠΊΠΎΡΠΈ. Π£ΡΡΠ°Π½ΠΎΠ²Π»Π΅Π½Ρ ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΈ Π΄ΠΎΡΡΠΎΠ²Π΅ΡΠ½ΡΠ΅ ΠΏΠΎΠ»ΠΎΠΆΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ ΠΊΠΎΡΡΠ΅Π»ΡΡΠΈΠΈ ΠΌΠ΅ΠΆΠ΄Ρ Cr-Sr, Cr-Ca ΠΈ Ca-Sr (r=0.906; 0.939 ΠΈ 0.974 ΡΠΎΠΎΡΠ²Π΅ΡΡΡΠ²Π΅Π½Π½ΠΎ), Π° ΡΠ°ΠΊΠΆΠ΅ P-Cu (r=0.968). ΠΠ΅ΡΠΌΠΎΡΡΡ Π½Π° ΡΠΎ, ΡΡΠΎ ΠΏΠ»ΠΎΠ΄Ρ ΡΠΈΠ³ΠΎΠ»ΠΈΡΡΠ½ΠΎΠΉ ΡΡΠΊΠ²Ρ C. ficifolia Π½Π΅ ΡΠΎΠ΄Π΅ΡΠΆΠ°Ρ ΠΊΠ°ΡΠΎΡΠΈΠ½ΠΎΠΈΠ΄Ρ, ΠΈΡ
ΠΏΠΈΡΠ΅Π²Π°Ρ ΡΠ΅Π½Π½ΠΎΡΡΡ Π² Π·Π½Π°ΡΠΈΡΠ΅Π»ΡΠ½ΠΎΠΉ ΡΡΠ΅ΠΏΠ΅Π½ΠΈ ΡΠ²ΡΠ·Π°Π½Π° Ρ Π²ΡΡΠΎΠΊΠΈΠΌΠΈ ΡΡΠΎΠ²Π½ΡΠΌΠΈ Si, I, Cr ΠΈ Ca Π² ΠΊΠΎΠΆΡΡΠ΅ ΠΏΠ»ΠΎΠ΄ΠΎΠ² ΠΈ ΠΌΡΠΊΠΎΡΠΈ, ΡΡΠΎ ΠΎΡΠΊΡΡΠ²Π°Π΅Ρ Π½ΠΎΠ²ΡΠ΅ Π³ΠΎΡΠΈΠ·ΠΎΠ½ΡΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΡ ΡΡΠΎΠ³ΠΎ Π²ΠΈΠ΄Π°.
First Results from The GlueX Experiment
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
, and mesons. Linearly-polarized photons were
successfully produced through coherent bremsstrahlung and polarization transfer
to the 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 Experiment (APEX)
We present a search at Jefferson Laboratory for new forces mediated by
sub-GeV vector bosons with weak coupling to electrons. Such a
particle can be produced in electron-nucleus fixed-target scattering and
then decay to an 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 reaction, and set an upper limit of
. 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
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
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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