981 research outputs found
Near-capacity FEC codes for non-regenerative MIMO-aided relays
In this contribution, we derive the Discrete-inputContinuous-output Memoryless Channel (DCMC) capacity of the non-regenerative Multiple-Input Multiple-Output (MIMO) relay channel, when the source-to-destination link is inferior and hence considered absent. We design near-capacity Forward Error Correction (FEC) codes for approaching this capacity limit. It is shown that our design is capable of approaching the DCMC capacity within 0.4 dB, when communicating over uncorrelated Raleigh fading channels, where the source node, relay node and destination node are equipped with two antennas each
Flux Jumping and a Bulk-to-Granular Transition in the Magnetization of a Compacted and Sintered MgB2 Superconductor
The recent discovery of intermediate-temperature superconductivity (ITC) in
MgB2 by Akimitsu et al. and its almost simultaneous explanation in terms of a
hole-carrier-based pairing mechanism by Hirsch, has triggered an avalanche of
studies of its structural, magnetic and transport properties. As a further
contribution to the field we report the results of field (H) and temperature
(T) dependent magnetization (M) measurements of a pellet of uniform,
large-grain sintered MgB2. We show that at low temperatures the size of the
pellet and its critical current density, Jc(H) - i.e. its M(H) - ensure low
field flux jumping, which of course ceases when M(H) drops below a critical
value. With further increase of H and T the individual grains decouple and the
M(H) loops drop to lower lying branches, unresolved in the usual full M(H)
representation. After taking into account the sample size and grain size,
respectively, the bulk sample and the grains were deduced to exhibit the same
magnetically determined Jc s (e.g. 105 A/cm2, 20 K, 0T) and hence that for each
temperature of measurement Jc(H) decreased monotonically with H over the entire
field range, except for a gap within the grain-decoupling zone.Comment: 7 pages, 6 figures, Changes: Fig 6 Vertical scale an order of
magnitude out (changed figure and associated text). Also corrected typo in
last sectio
Numerical simulation research on ecological protection device for marine water intake engineering based on cfd
1941-1948The ecological protection originated from marine engineering is the key factor for the healthy and sustainable development of marine ecological system. Combined with the tidal dynamic characteristics, a new optimistic ecological protection device concept model is designed for marine water intake engineering to avoid the ecological loss, which following the principles of safe, stable, easy installation and maintenance, unaffected water intake. Based on computational fluid dynamics (CFD), the three dimensional mathematical model of ecological protection device for marine water intake engineering is constructed to simulate and evaluate the feasibility of the proposed device. The flow field and pressure distribution are simulated and analyzed before and after the device installation. The numerical results of flow velocity in the intake, intake box and intake channel show that the ecological protection device has a weak effect on the flow field and the device can provide ecological safeguard for marine intake engineering. The pressure distribution from the ecological protection device would also reflect the underlying reason of the flow velocity change
Diffuse interstitial and multiple cavitary lung lesions due to Talaromyces marneffei infection in a non-HIV patient
AbstractA 57-year-old man presented with unproductive cough and dyspnea for 6 months in Fujian Province, China. His misuse of a large amount of steroids (accumulated dose equivalent to 3530Β mg prednisolone) resulted in Talaromyces marneffei infection. Chest computed tomographic scan revealed diffuse interstitial and multiple cavitary lung lesions. Treatment with amphotericin B combined with itraconazole resulted in total recovery, with marked regression of lung lesions
Compressive Properties of SiC Particle-Reinforced Aluminum Matrix Composites under Repeated Impact Loading
Under repeated impact loading, SiC particle-reinforced aluminum matrix composites (SiCp/Al) experience severe plastic strains, which can lead to local changes in their microstructure. Microstructure variations have a significant effect on the dynamic behavior of SiCp/Al composites under subsequent impact loading. Their microstructure was analyzed by scanning electron microscopy (SEM). Then the dynamic compressive properties of SiCp/Al composites were studied using the split Hopkinson pressure bar (SHPB), and the dynamic compression stressβstrain curve for each impact was plotted.Π ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΠΏΠΎΠ²ΡΠΎΡΠ½ΠΎΠ³ΠΎ ΡΠ΄Π°ΡΠ½ΠΎΠ³ΠΎ Π½Π°Π³ΡΡΠΆΠ΅Π½ΠΈΡ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΠ΅ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Ρ Ρ Π°Π»ΡΠΌΠΈΠ½ΠΈΠ΅Π²ΠΎΠΉ ΠΌΠ°ΡΡΠΈΡΠ΅ΠΉ, ΡΠΏΡΠΎΡΠ½Π΅Π½Π½ΡΠ΅ ΡΠ°ΡΡΠΈΡΠ°ΠΌΠΈ SiC (SiCp/Al), ΠΈΡΠΏΡΡΡΠ²Π°ΡΡ Π΄Π΅ΠΉΡΡΠ²ΠΈΠ΅ Π²ΡΡΠΎΠΊΠΈΡ
ΠΏΠ»Π°ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΉ, ΡΡΠΎ ΠΌΠΎΠΆΠ΅Ρ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡΡ ΠΊ Π»ΠΎΠΊΠ°Π»ΡΠ½ΡΠΌ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡΠΌ ΠΈΡ
ΠΌΠΈΠΊΡΠΎΡΡΡΡΠΊΡΡΡΡ. ΠΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΠΌΠΈΠΊΡΠΎΡΡΡΡΠΊΡΡΡΡ ΠΎΠΊΠ°Π·ΡΠ²Π°ΡΡ ΡΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎΠ΅ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΏΠΎΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² SiCp/Al ΠΏΡΠΈ ΠΏΠΎΡΠ»Π΅Π΄ΡΡΡΠ΅ΠΌ ΡΠ΄Π°ΡΠ½ΠΎΠΌ Π½Π°Π³ΡΡΠΆΠ΅Π½ΠΈΠΈ. ΠΡ
ΠΌΠΈΠΊΡΠΎΡΡΡΡΠΊΡΡΡΠ° ΠΏΡΠΎΠ°Π½Π°Π»ΠΈΠ·ΠΈΡΠΎΠ²Π°Π½Π° Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΠΊΠ°Π½ΠΈΡΡΡΡΠ΅ΠΉ ΡΠ»Π΅ΠΊΡΡΠΎΠ½Π½ΠΎΠΉ ΠΌΠΈΠΊΡΠΎΡΠΊΠΎΠΏΠΈΠΈ. ΠΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΡΡ ΡΠΆΠΈΠΌΠ°Π΅ΠΌΠΎΡΡΡ ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΎΠ½Π½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ² ΠΈΠ·ΡΡΠ°Π»ΠΈ Ρ ΠΏΠΎΠΌΠΎΡΡΡ ΡΠ°Π·ΡΠ΅Π·Π½ΠΎΠ³ΠΎ ΡΡΠ΅ΡΠΆΠ½Ρ ΠΠΎΠΏΠΊΠΈΠ½ΡΠΎΠ½Π°, Π±ΡΠ»Π° ΠΏΠΎΡΡΡΠΎΠ΅Π½Π° Π·Π°Π²ΠΈΡΠΈΠΌΠΎΡΡΡ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΠΎΡ Π΄ΠΈΠ½Π°ΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΆΠΈΠΌΠ°ΡΡΠ΅Π³ΠΎ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΡ Π΄Π»Ρ ΠΊΠ°ΠΆΠ΄ΠΎΠ³ΠΎ ΡΠ΄Π°ΡΠ½ΠΎΠ³ΠΎ Π²ΠΎΠ·Π΄Π΅ΠΉΡΡΠ²ΠΈΡ
Molecular cytogenetic aberrations in patients with multiple myeloma studied by interphase fluorescence in situ hybridization
Background: Multiple myeloma (MM) is an incurable hematological disorder characterized by the accumulation of malignant plasma cells within the bone marrow (BM). The clinical heterogeneity of MM is dictated by the cytogenetic aberrations present in the clonal plasma cells (PCs). Cytogenetic studies in MM are hampered by the hypoproliferative nature of plasma cells in MM. Therefore, fluorescence in situ hybridization (FISH) analysis combined with magnetic-activated cell sorting (MACS) is an attractive alternative for evaluation of numerical and structural chromosomal changes in MM. Methods: Interphase FISH studies with three different specific probes for the regions containing 13q14.3 (D13S319), 14q32 (IGHC/IGHV) and 1q12(CEP1 ) were performed in 48 MM patients. Interphase FISH studies with LSI IGH/CCND1, LSI IGH/FGFR3, and LSI IGH/MAF probes were used to detect t(11;14)(q13;q32), t(4;14)(p16;q32), and t(14;16)(q32;q23) in patients with 14q32 rearrangement. Results: Molecular cytogenetic aberrations were found in 40 (83.3%) of the 48 MM patients. 13 patients (27.1%) simultaneously had 13q deletion/monosomy 13 [del(13q14)], illegitimate IGH rearrangement and chromosome 1 abnormality. Del(13q14) was detected in 21 cases (43.7%), and illegitimate IGH rearrangements in 29 (60.4%) including 6 with t(11;14) and 5 with t(4;14). None of 9 patients with illegitimate IGH rearrangements and without t(11;14) or t(4;14) we detected had t(14;16) (q32;q23). 24 of the 48 MM patients (50%) had chromosome 1 abnormalities. Among 21 patients with del(13q14), 15 patients had Amp1q12;16 had IgH rearrangements. Whereas, among 27 cases without del(13q14), 8 had Amp1q12; 13 had IgH rearrangements. There was a strong association between del(13q14) and Amp1q12(c2 = 8.26, Ρ < 0.01), and between del(13q14) and IgH rearrangement(c2 = 3.88, p < 0.05). Conclusion: 13q deletion/monosomy 13, IGH rearrangement and chromosome 1 abnormality are frequent in MM. They are not randomly distributed, but strongly interconnected. Interphase FISH technique combined with MACS using CD138-specific antibody is a highly sensitive technique at detecting molecular cytogenetic aberrations in MM.ΠΠ±ΠΎΡΠ½ΠΎΠ²Π°Π½ΠΈΠ΅: ΠΌΠ½ΠΎΠΆΠ΅ΡΡΠ²Π΅Π½Π½Π°Ρ ΠΌΠΈΠ΅Π»ΠΎΠΌΠ° (MM) β Π½Π΅ΠΈΠ·Π»Π΅ΡΠΈΠΌΠΎΠ΅ Π³Π΅ΠΌΠ°ΡΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ΅ Π·Π°Π±ΠΎΠ»Π΅Π²Π°Π½ΠΈΠ΅, Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΠ·ΠΈΡΡΡΡΠ΅Π΅ΡΡ
Π½Π°ΠΊΠΎΠΏΠ»Π΅Π½ΠΈΠ΅ΠΌ Π·Π»ΠΎΠΊΠ°ΡΠ΅ΡΡΠ²Π΅Π½Π½ΡΡ
ΠΏΠ»Π°Π·ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΊΠ»Π΅ΡΠΎΠΊ Π² ΠΊΠΎΡΡΠ½ΠΎΠΌ ΠΌΠΎΠ·Π³Π΅ (ΠM). ΠΠ»ΠΈΠ½ΠΈΡΠ΅ΡΠΊΠ°Ρ Π³Π΅ΡΠ΅ΡΠΎΠ³Π΅Π½Π½ΠΎΡΡΡ MM ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅ΡΡΡ
ΡΠΈΡΠΎΠ³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ Π°Π±Π΅ΡΡΠ°ΡΠΈΡΠΌΠΈ, ΠΏΡΠΈΡΡΡΡΡΠ²ΡΡΡΠΈΠΌΠΈ Π² ΠΊΠ»ΠΎΠ½Π΅ ΠΏΠ»Π°Π·ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΊΠ»Π΅ΡΠΎΠΊ (ΠΠ). Π¦ΠΈΡΠΎΠ³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ
MM ΠΎΡΠ»ΠΎΠΆΠ½Π΅Π½Ρ Π³ΠΈΠΏΠΎΠΏΡΠΎΠ»ΠΈΡΠ΅ΡΠ°ΡΠΈΠ²Π½ΡΠΌΠΈ ΠΎΡΠΎΠ±Π΅Π½Π½ΠΎΡΡΡΠΌΠΈ ΠΠ. Π ΡΠ²ΡΠ·ΠΈ Ρ ΡΡΠΈΠΌ ΡΠ»ΡΠΎΡΠ΅ΡΡΠ΅Π½ΡΠ½Π°Ρ Π³ΠΈΠ±ΡΠΈΠ΄ΠΈΠ·Π°ΡΠΈΡ in situ (FISH)
Π² ΠΊΠΎΠΌΠ±ΠΈΠ½Π°ΡΠΈΠΈ Ρ ΡΠΎΡΡΠΈΡΠΎΠ²ΠΊΠΎΠΉ ΠΊΠ»Π΅ΡΠΎΠΊ, Π°ΠΊΡΠΈΠ²ΠΈΡΠΎΠ²Π°Π½Π½ΡΡ
ΠΌΠ°Π³Π½ΠΈΡΠ½ΡΠΌΠΈ ΠΏΠΎΠ»ΡΠΌΠΈ (MACS) ΠΏΡΠ΅Π΄ΡΡΠ°Π²Π»ΡΠ΅ΡΡΡ Π΄ΠΎΡΡΠΎΠΉΠ½ΠΎΠΉ Π°Π»ΡΡΠ΅ΡΠ½Π°ΡΠΈΠ²ΠΎΠΉ
ΠΌΠ΅ΡΠΎΠ΄Π°ΠΌ ΠΎΡΠ΅Π½ΠΊΠΈ ΡΠΎΡΠ΅ΡΠ½ΡΡ
ΠΈ ΡΡΡΡΠΊΡΡΡΠ½ΡΡ
ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΉ Ρ
ΡΠΎΠΌΠΎΡΠΎΠΌ ΠΏΡΠΈ MM. ΠΠ΅ΡΠΎΠ΄Ρ: ΠΈΠ½ΡΠ΅ΡΡΠ°Π·Π½ΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ
FISH Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΡΡΠ΅Ρ
ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΠΏΠ΅ΡΠΈΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π·ΠΎΠ½Π΄ΠΎΠ² Π΄Π»Ρ ΡΡΠ°ΡΡΠΊΠΎΠ², ΡΠΎΠ΄Π΅ΡΠΆΠ°ΡΠΈΡ
13q14.3 (D13S319), 14q32
(IGHC/IGHV) ΠΈ 1q12(CEP1), ΠΏΡΠΎΠ²ΠΎΠ΄ΠΈΠ»ΠΈ Ρ 48 Π±ΠΎΠ»ΡΠ½ΡΡ
Ρ MM. ΠΠ½ΡΠ΅ΡΡΠ°Π·Π½ΡΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ FISH Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ
Π·ΠΎΠ½Π΄ΠΎΠ² LSI IGH/CCND1, LSI IGH/FGFR3 ΠΈ LSI IGH/MAF ΠΏΡΠΈΠΌΠ΅Π½ΡΠ»ΠΈ Π΄Π»Ρ Π΄Π΅ΡΠ΅ΠΊΡΠΈΠΈ t(11;14)(q13;q32), t(4;14)(p16;q32), ΠΈ
t(14;16)(q32;q23) Ρ ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΠΎΠΉ 14q32. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ: ΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΡΠ΅ ΡΠΈΡΠΎΠ³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π°Π±Π΅ΡΡΠ°ΡΠΈΠΈ Π²ΡΡΠ²Π»ΡΠ»ΠΈ Ρ
40 (83,3%) ΠΈΠ· 48 Π±ΠΎΠ»ΡΠ½ΡΡ
Ρ MM. Π£ 13 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² (27,1%) ΠΎΠ΄Π½ΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Ρ 13q Π΄Π΅Π»Π΅ΡΠΈΡ/ΠΌΠΎΠ½ΠΎΡΠΎΠΌΠΈΡ 13 [del(13q14)],
Π°Π½ΠΎΠΌΠ°Π»ΡΠ½Π°Ρ ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΠ° IGH ΠΈ Π°Π½ΠΎΠΌΠ°Π»ΠΈΡ Ρ
ΡΠΎΠΌΠΎΡΠΎΠΌΡ 1. Del(13q14) Π΄Π΅ΡΠ΅ΠΊΡΠΈΡΠΎΠ²Π°Π»ΠΈ Π² 21 ΡΠ»ΡΡΠ°Π΅ (43,7%), Π° Π°Π½ΠΎΠΌΠ°Π»ΡΠ½ΡΠ΅
ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΠΈ IGH β Π² 29 (60,4%), Π² ΡΠΎΠΌ ΡΠΈΡΠ»Π΅ Ρ 6 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ t(11;14) ΠΈ 5 Ρ t(4;14). ΠΠΈ Ρ ΠΎΠ΄Π½ΠΎΠ³ΠΎ ΠΈΠ· 9 Π±ΠΎΠ»ΡΠ½ΡΡ
Ρ Π°Π½ΠΎΠΌΠ°Π»ΡΠ½ΡΠΌΠΈ
ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΠ°ΠΌΠΈ IGH ΠΈ Π±Π΅Π· t(11;14) ΠΈΠ»ΠΈ t(4;14) Π½Π΅ Π²ΡΡΠ²Π»ΡΠ»ΠΈ ΡΡΠ°Π½ΡΠ»ΠΎΠΊΠ°ΡΠΈΡ t(14;16) (q32;q23). Π£ 24 ΠΈΠ· 48 ΠΏΠ°ΡΠΈΠ΅Π½ΡΠΎΠ² Ρ MM
(50%) ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ»ΠΈ Π°Π½ΠΎΠΌΠ°Π»ΠΈΠΈ Ρ
ΡΠΎΠΌΠΎΡΠΎΠΌΡ 1. Π Π³ΡΡΠΏΠΏΠ΅ ΠΈΠ· 21 Π±ΠΎΠ»ΡΠ½ΡΡ
Ρ del(13q14) Π² 15 ΡΠ»ΡΡΠ°ΡΡ
ΠΈΠΌΠ΅Π»ΠΈΡΡ ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΠΈ IgH
Amp1q12;16. Π ΡΠΎ ΠΆΠ΅ Π²ΡΠ΅ΠΌΡ ΠΈΠ· 27 ΡΠ»ΡΡΠ°Π΅Π² Π±Π΅Π· del(13q14) Ρ 8 ΡΠΎΠ΄Π΅ΡΠΆΠ°Π»ΠΈΡΡ Amp1q12; Π² 13 ΡΠ»ΡΡΠ°ΡΡ
ΠΎΡΠΌΠ΅ΡΠ°Π»ΠΈ ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΠΈ
IgH. ΠΡΡΠ²Π»Π΅Π½Π° Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·Ρ ΠΌΠ΅ΠΆΠ΄Ρ del(13q14) ΠΈ Amp1q12(Ο2
= 8,26, p < 0,01) ΠΈ ΠΌΠ΅ΠΆΠ΄Ρ del(13q14) ΠΈ ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΠ°ΠΌΠΈ IgH
(Ο2 = 3,88, p < 0,05). ΠΡΠ²ΠΎΠ΄Ρ: 13q Π΄Π΅Π»Π΅ΡΠΈΡ/ΠΌΠΎΠ½ΠΎΡΠΎΠΌΠΈΡ 13, ΠΏΠ΅ΡΠ΅ΡΡΡΠΎΠΉΠΊΡ IGH ΠΈ Π°Π½ΠΎΠΌΠ°Π»ΠΈΡ Ρ
ΡΠΎΠΌΠΎΡΠΎΠΌΡ 1 ΡΠ°ΡΡΠΎ ΠΎΡΠΌΠ΅ΡΠ°ΡΡ
ΠΏΡΠΈ MM, ΠΏΡΠΈΡΠ΅ΠΌ ΠΈΡ
ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠ΅ Π½Π΅ ΡΠ»ΡΡΠ°ΠΉΠ½ΠΎ ΠΈ ΡΠ΅ΡΠ½ΠΎ Π²Π·Π°ΠΈΠΌΠΎΡΠ²ΡΠ·Π°Π½ΠΎ. ΠΠ½ΡΠ΅ΡΡΠ°Π·Π½ΡΠΉ Π°Π½Π°Π»ΠΈΠ· FISH Π² ΠΊΠΎΠΌΠ±ΠΈΠ½Π°ΡΠΈΠΈ Ρ
MACS Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ CD138-ΡΠΏΠ΅ΡΠΈΡΠΈΡΠ½ΡΡ
Π°Π½ΡΠΈΡΠ΅Π» ΡΠ²Π»ΡΠ΅ΡΡΡ Π²ΡΡΠΎΠΊΠΎΡΡΠ²ΡΡΠ²ΠΈΡΠ΅Π»ΡΠ½ΡΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠΌ Π΄Π΅ΡΠ΅ΠΊΡΠΈΠΈ ΠΌΠΎΠ»Π΅ΠΊΡΠ»ΡΡΠ½ΡΡ
ΡΠΈΡΠΎΠ³Π΅Π½Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΡ
Π°Π±Π΅ΡΡΠ°ΡΠΈΠΉ ΠΏΡΠΈ MM
First Measurements of Rayleigh-Taylor-Induced Magnetic Fields in Laser-produced Plasmas
The first experimental demonstration of Rayleigh-Taylor-induced magnetic fields due to the Biermann battery effect has been made. Experiments with laser-irradiated plastic foils were performed to investigate these illusive fields using a monoenergetic proton radiography system. Path-integrated B field strength measurements were inferred from radiographs and found to increase from 10 to 100ββTβΞΌm during the linear growth phase for 120ββΞΌm perturbations. Proton fluence modulations were corrected for Coulomb scattering using measured areal density profiles from x-ray radiographs.United States. Dept. of Energy (grant DE-FG52-09NA29553)University of Rochester. Fusion Science Center (grant 415023-G)University of Rochester. Laboratory for Laser Energetics (grant 414090-G)Lawrence Livermore National Laboratory (grant B580243)National Laser Userβs Facility (grant DE-NA0000877
Anomalous Crossing Frequency in Odd Proton Nuclei
A generic explanation for the recently observed anomalous crossing
frequencies in odd proton rare earth nuclei is given. As an example, the proton
band in Ta is discussed in detail by using the
angular momentum projection theory. It is shown that the quadrupole pairing
interaction is decisive in delaying the crossing point and the changes in
crossing frequency along the isotope chain are due to the different neutron
shell fillings
Metamaterial Polarization Converter Analysis: Limits of Performance
In this paper we analyze the theoretical limits of a metamaterial converter
that allows for linear-to- elliptical polarization transformation with any
desired ellipticity and ellipse orientation. We employ the transmission line
approach providing a needed level of the design generalization. Our analysis
reveals that the maximal conversion efficiency for transmission through a
single metamaterial layer is 50%, while the realistic re ection configuration
can give the conversion efficiency up to 90%. We show that a double layer
transmission converter and a single layer with a ground plane can have 100%
polarization conversion efficiency. We tested our conclusions numerically
reaching the designated limits of efficiency using a simple metamaterial
design. Our general analysis provides useful guidelines for the metamaterial
polarization converter design for virtually any frequency range of the
electromagnetic waves.Comment: 10 pages, 11 figures, 2 table
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