465 research outputs found
A novel long non-coding natural antisense RNA is a negative regulator of Nos1 gene expression
Long non-coding natural antisense transcripts (NATs) are widespread in eukaryotic species. Although recent studies indicate that long NATs are engaged in the regulation of gene expression, the precise functional roles of the vast majority of them are unknown. Here we report that a long NAT (Mm-antiNos1 RNA) complementary to mRNA encoding the neuronal isoform of nitric oxide synthase (Nos1) is expressed in the mouse brain and is transcribed from the non-template strand of the Nos1 locus. Nos1 produces nitric oxide (NO), a major signaling molecule in the CNS implicated in many important functions including neuronal differentiation and memory formation. We show that the newly discovered NAT negatively regulates Nos1 gene expression. Moreover, our quantitative studies of the temporal expression profiles of Mm-antiNos1 RNA in the mouse brain during embryonic development and postnatal life indicate that it may be involved in the regulation of NO-dependent neurogenesis
The temporal expression profile of a Nos3-related natural antisense RNA in the brain suggests a possible role in neurogenesis
Experimental work over the past several years has revealed an unexpected abundance of long natural antisense transcripts (NATs) in eukaryotic species. In light of the proposed role of such RNA molecules in the regulation of gene expression in the brain, attention is now focused on specific examples of neuronal NATs. Of particular interest are NATs that are complementary to mRNAs encoding nitric oxide synthase (NOS), the enzyme responsible for production of the important gaseous neurotransmitter nitric oxide (NO). Here we study the temporal expression profile of murine Nos3as NAT in the brain. Notably, Nos3as NAT is known to act as a negative regulator of Nos3 gene expression. The results of our quantitative analysis reveal differential expression of Nos3as NAT during embryonic and post-embryonic stages of development of the brain. Also, they show that the low levels of Nos3as NAT coincides with active neurogenesis. In addition we report on an inverse correlation between the relative expression level of Nos3as NAT and the level of Nos3 protein. Thus our data raise the hypothesis that the Nos3as NAT regulates neurogenesis through suppression of Nos3 gene activity. This idea is further supported by experiments conducted on the olfactory bulbs and cultured neuroblastoma cells
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Controllable direction of liquid jets generated by thermocavitation within a droplet.
A high-velocity fluid stream ejected from an orifice or nozzle is a common mechanism to produce liquid jets in inkjet printers or to produce sprays among other applications. In the present research, we show the generation of liquid jets of controllable direction produced within a sessile water droplet by thermocavitation. The jets are driven by an acoustic shock wave emitted by the collapse of a hemispherical vapor bubble at the liquid-solid/substrate interface. The generated shock wave is reflected at the liquid-air interface due to acoustic impedance mismatch generating multiple reflections inside the droplet. During each reflection, a force is exerted on the interface driving the jets. Depending on the position of the generation of the bubble within the droplet, the mechanical energy of the shock wave is focused on different regions at the liquid-air interface, ejecting cylindrical liquid jets at different angles. The ejected jet angle dependence is explained by a simple ray tracing model of the propagation of the acoustic shock wave inside the droplet
ΠΠΠ ΠΠΠΠ’ΠΠ ΠΠΠΠΠΠ’ΠΠ§ΠΠ‘ΠΠ ΠΠΠΠ―Π ΠΠΠΠΠΠΠΠΠΠ Π‘ΠΠΠΠΠΠ Π Π ΠΠΠΠΠΠΠΠΠ¦ΠΠΠΠΠ«Π₯ Π‘Π’ΠΠΠ¦ΠΠ―Π₯ Π‘ Π¦ΠΠ€Π ΠΠΠ«Π Π‘ΠΠΠ’ΠΠΠΠ ΠΠΠΠΠΠΠ ΠΠΠΠ Π’Π£Π Π« ΠΠΠ’ΠΠΠΠ«
The processing of the elliptically polarized reflected signal in the Earth remote sensing systems makes it possible to obtain additional advantages when solving problems of recognition of the observable objects on the ground and under the ground. Full polarization reception implemented in radar stations with digital synthesis of the antenna aperture when remote sensing of the Earth increases the information content of such radars (the radar image of the investigated surface is detailed, the contrast of objects in the field of view is improved, and various negative effects of the image are minimized). The paper considers the quadrature processing of the reflected elliptically polarized signal in radar stations with digital synthesis of the antenna aperture in the mode of lateral survey of the terrestrial (water) surface. The processing of the reflected signal using the methods of radio polarimetry opens new possibilities for such radars while solving problems of remote sensing of the surface and recognition of radar targets. In addition, radar stations with digital synthesis of the antenna aperture with processing of an elliptically polarized signal have a higher interference immunity compared to radars, where a linearly polarized signal is processed. In the article, mathematical modeling is performed in the part of demodulation of the in-phase and quadrature components of the trajectory signal when the geometric parameters of the polarization ellipse change. The obtained analytical expressions allow estimating the influence of the geometric parameters of the polarization ellipse on the trajectory signal being processed. It is analytically confirmed that the angle of ellipticity affects the energy characteristics, and the orientation angle of the polarization ellipse introduces an additional phase shift in the characteristics of the trajectory signal being processed. Not taking into account these nuances while designing digital units and systems of such radars can lead to the loss of all the benefits of processing an elliptically polarized signal. The paper presents a structural scheme of the polarization radar station with digital synthesis of the antenna aperture.ΠΠ±ΡΠ°Π±ΠΎΡΠΊΠ° ΡΠ»Π»ΠΈΠΏΡΠΈΡΠ΅ΡΠΊΠΈ ΠΏΠΎΠ»ΡΡΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΠΎΡΡΠ°ΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π° Π² ΡΠΈΡΡΠ΅ΠΌΠ°Ρ
Π΄ΠΈΡΡΠ°Π½ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π·ΠΎΠ½Π΄ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΠ΅ΠΌΠ»ΠΈ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΠ΅Ρ ΠΏΠΎΠ»ΡΡΠ°ΡΡ Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²Π° ΠΏΡΠΈ ΡΠ΅ΡΠ΅Π½ΠΈΠΈ Π·Π°Π΄Π°Ρ ΡΠ°ΡΠΏΠΎΠ·Π½Π°Π²Π°Π½ΠΈΡ Π½Π°Π±Π»ΡΠ΄Π°Π΅ΠΌΡΡ
ΠΎΠ±ΡΠ΅ΠΊΡΠΎΠ² Π½Π° Π·Π΅ΠΌΠ»Π΅ ΠΈ ΠΏΠΎΠ΄ Π·Π΅ΠΌΠ»Π΅ΠΉ. ΠΠΎΠ»Π½ΡΠΉ ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΎΠ½Π½ΡΠΉ ΠΏΡΠΈΠ΅ΠΌ, ΡΠ΅Π°Π»ΠΈΠ·ΠΎΠ²Π°Π½Π½ΡΠΉ Π² ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΡΡΠ°Π½ΡΠΈΡΡ
Ρ ΡΠΈΡΡΠΎΠ²ΡΠΌ ΡΠΈΠ½ΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π°ΠΏΠ΅ΡΡΡΡΡ Π°Π½ΡΠ΅Π½Π½Ρ, ΠΏΡΠΈ Π΄ΠΈΡΡΠ°Π½ΡΠΈΠΎΠ½Π½ΠΎΠΌ Π·ΠΎΠ½Π΄ΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΠΠ΅ΠΌΠ»ΠΈ ΠΏΠΎΠ²ΡΡΠ°Π΅Ρ ΠΈΠ½ΡΠΎΡΠΌΠ°ΡΠΈΠ²Π½ΠΎΡΡΡ ΡΠ°ΠΊΠΈΡ
ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΎΡΠΎΠ² (Π΄Π΅ΡΠ°Π»ΠΈΠ·ΠΈΡΡΠ΅ΡΡΡ ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΠΎΠ΅ ΠΈΠ·ΠΎΠ±ΡΠ°ΠΆΠ΅Π½ΠΈΠ΅ ΠΈΡΡΠ»Π΅Π΄ΡΠ΅ΠΌΠΎΠΉ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ, ΠΏΠΎΠ΄ΡΠ΅ΡΠΊΠΈΠ²Π°Π΅ΡΡΡ ΠΊΠΎΠ½ΡΡΠ°ΡΡΠ½ΠΎΡΡΡ ΠΎΠ±ΡΠ΅ΠΊΡΠΎΠ², Π½Π°Ρ
ΠΎΠ΄ΡΡΠΈΡ
ΡΡ Π² Π·ΠΎΠ½Π΅ ΠΎΠ±Π·ΠΎΡΠ°, ΠΌΠΈΠ½ΠΈΠΌΠΈΠ·ΠΈΡΡΡΡΡΡ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠ΅ Π½Π΅Π³Π°ΡΠΈΠ²Π½ΡΠ΅ ΡΡΡΠ΅ΠΊΡΡ ΠΈΠ·ΠΎΠ±ΡΠ°ΠΆΠ΅Π½ΠΈΡ). Π ΡΡΠ°ΡΡΠ΅ ΡΠ°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅ΡΡΡ ΠΊΠ²Π°Π΄ΡΠ°ΡΡΡΠ½Π°Ρ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠ° ΠΎΡΡΠ°ΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΠ»Π»ΠΈΠΏΡΠΈΡΠ΅ΡΠΊΠΈ ΠΏΠΎΠ»ΡΡΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π° Π² ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΡΡΠ°Π½ΡΠΈΡΡ
Ρ ΡΠΈΡΡΠΎΠ²ΡΠΌ ΡΠΈΠ½ΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π°ΠΏΠ΅ΡΡΡΡΡ Π°Π½ΡΠ΅Π½Π½Ρ Π² ΡΠ΅ΠΆΠΈΠΌΠ΅ Π±ΠΎΠΊΠΎΠ²ΠΎΠ³ΠΎ ΠΎΠ±Π·ΠΎΡΠ° Π·Π΅ΠΌΠ½ΠΎΠΉ (Π²ΠΎΠ΄Π½ΠΎΠΉ) ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ. ΠΠ±ΡΠ°Π±ΠΎΡΠΊΠ° ΠΎΡΡΠ°ΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π° Ρ ΠΈΡΠΏΠΎΠ»ΡΠ·ΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΌΠ΅ΡΠΎΠ΄ΠΎΠ² ΡΠ°Π΄ΠΈΠΎΠΏΠΎΠ»ΡΡΠΈΠΌΠ΅ΡΡΠΈΠΈ ΠΎΡΠΊΡΡΠ²Π°Π΅Ρ Π½ΠΎΠ²ΡΠ΅ Π²ΠΎΠ·ΠΌΠΎΠΆΠ½ΠΎΡΡΠΈ ΠΏΠ΅ΡΠ΅Π΄ ΡΠ°ΠΊΠΈΠΌΠΈ ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΎΡΠ°ΠΌΠΈ ΠΏΡΠΈ ΡΠ΅ΡΠ΅Π½ΠΈΠΈ Π·Π°Π΄Π°Ρ Π΄ΠΈΡΡΠ°Π½ΡΠΈΠΎΠ½Π½ΠΎΠ³ΠΎ Π·ΠΎΠ½Π΄ΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΠ²Π΅ΡΡ
Π½ΠΎΡΡΠΈ ΠΈ ΡΠ°ΡΠΏΠΎΠ·Π½Π°Π²Π°Π½ΠΈΡ ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΡΡ
ΡΠ΅Π»Π΅ΠΉ. ΠΡΠΎΠΌΠ΅ ΡΠΎΠ³ΠΎ, ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΡΠ΅ ΡΡΠ°Π½ΡΠΈΠΈ Ρ ΡΠΈΡΡΠΎΠ²ΡΠΌ ΡΠΈΠ½ΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π°ΠΏΠ΅ΡΡΡΡΡ Π°Π½ΡΠ΅Π½Π½Ρ Ρ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΎΠΉ ΡΠ»Π»ΠΈΠΏΡΠΈΡΠ΅ΡΠΊΠΈ ΠΏΠΎΠ»ΡΡΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π° ΠΈΠΌΠ΅ΡΡ Π±ΠΎΠ»Π΅Π΅ Π²ΡΡΠΎΠΊΡΡ ΠΏΠΎΠΌΠ΅Ρ
ΠΎΡΡΡΠΎΠΉΡΠΈΠ²ΠΎΡΡΡ ΠΏΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΡ Ρ ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΎΡΠ°ΠΌΠΈ, Π³Π΄Π΅ ΠΎΠ±ΡΠ°Π±Π°ΡΡΠ²Π°Π΅ΡΡΡ Π»ΠΈΠ½Π΅ΠΉΠ½ΠΎΠΏΠΎΠ»ΡΡΠΈΠ·ΠΎΠ²Π°Π½Π½ΡΠΉ ΡΠΈΠ³Π½Π°Π». Π ΡΡΠ°ΡΡΠ΅ ΠΏΡΠΎΠΈΠ·Π²ΠΎΠ΄ΠΈΡΡΡ ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ Π² ΡΠ°ΡΡΠΈ Π΄Π΅ΠΌΠΎΠ΄ΡΠ»ΡΡΠΈΠΈ ΡΠΈΠ½ΡΠ°Π·Π½ΠΎΠΉ ΠΈ ΠΊΠ²Π°Π΄ΡΠ°ΡΡΡΠ½ΠΎΠΉ ΡΠΎΡΡΠ°Π²Π»ΡΡΡΠΈΡ
ΡΡΠ°Π΅ΠΊΡΠΎΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π° ΠΏΡΠΈ ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΠΈ Π³Π΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΡΠ»Π»ΠΈΠΏΡΠ° ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ Π°Π½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Π²ΡΡΠ°ΠΆΠ΅Π½ΠΈΡ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡΡ ΠΎΡΠ΅Π½ΠΈΡΡ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π³Π΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΡΠ»Π»ΠΈΠΏΡΠ° ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ Π½Π° ΠΎΠ±ΡΠ°Π±Π°ΡΡΠ²Π°Π΅ΠΌΡΠΉ ΡΡΠ°Π΅ΠΊΡΠΎΡΠ½ΡΠΉ ΡΠΈΠ³Π½Π°Π». ΠΠ½Π°Π»ΠΈΡΠΈΡΠ΅ΡΠΊΠΈ ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π°Π΅ΡΡΡ, ΡΡΠΎ ΡΠ³ΠΎΠ» ΡΠ»Π»ΠΈΠΏΡΠΈΡΠ½ΠΎΡΡΠΈ ΠΎΠΊΠ°Π·ΡΠ²Π°Π΅Ρ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π° ΡΠ½Π΅ΡΠ³Π΅ΡΠΈΡΠ΅ΡΠΊΠΈΠ΅ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ, Π° ΡΠ³ΠΎΠ» ΠΎΡΠΈΠ΅Π½ΡΠ°ΡΠΈΠΈ ΡΠ»Π»ΠΈΠΏΡΠ° ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΈ Π²Π½ΠΎΡΠΈΡ Π΄ΠΎΠΏΠΎΠ»Π½ΠΈΡΠ΅Π»ΡΠ½ΡΠΉ ΡΠ°Π·ΠΎΠ²ΡΠΉ ΡΠ΄Π²ΠΈΠ³ Π² Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠΈ ΠΎΠ±ΡΠ°Π±Π°ΡΡΠ²Π°Π΅ΠΌΠΎΠ³ΠΎ ΡΡΠ°Π΅ΠΊΡΠΎΡΠ½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π°. ΠΠ΅ΡΡΠ΅Ρ ΡΡΠΈΡ
Π½ΡΠ°Π½ΡΠΎΠ² ΠΏΡΠΈ ΠΏΡΠΎΠ΅ΠΊΡΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΡΠΈΡΡΠΎΠ²ΡΡ
Π±Π»ΠΎΠΊΠΎΠ² ΠΈ ΡΠΈΡΡΠ΅ΠΌ ΡΠ°ΠΊΠΈΡ
ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΎΡΠΎΠ² ΠΌΠΎΠΆΠ΅Ρ ΠΏΡΠΈΠ²Π΅ΡΡΠΈ ΠΊ ΠΏΠΎΡΠ΅ΡΠ΅ Π²ΡΠ΅Ρ
ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ² ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠΈ ΡΠ»Π»ΠΈΠΏΡΠΈΡΠ΅ΡΠΊΠΈ ΠΏΠΎΠ»ΡΡΠΈΠ·ΠΎΠ²Π°Π½Π½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π°. Π ΡΡΠ°ΡΡΠ΅ ΠΏΡΠΈΠ²ΠΎΠ΄ΠΈΡΡΡ ΡΡΡΡΠΊΡΡΡΠ½Π°Ρ ΡΡ
Π΅ΠΌΠ° ΠΏΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΠ°Π΄ΠΈΠΎΠ»ΠΎΠΊΠ°ΡΠΈΠΎΠ½Π½ΠΎΠΉ ΡΡΠ°Π½ΡΠΈΠΈ Ρ ΡΠΈΡΡΠΎΠ²ΡΠΌ ΡΠΈΠ½ΡΠ΅Π·ΠΈΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ Π°ΠΏΠ΅ΡΡΡΡΡ Π°Π½ΡΠ΅Π½Π½Ρ
Electron-phonon scattering at the intersection of two Landau levels
We predict a double-resonant feature in the magnetic field dependence of the
phonon-mediated longitudinal conductivity of a two-subband
quasi-two-dimensional electron system in a quantizing magnetic field. The two
sharp peaks in appear when the energy separation between two
Landau levels belonging to different size-quantization subbands is favorable
for acoustic-phonon transitions. One-phonon and two-phonon mechanisms of
electron conductivity are calculated and mutually compared. The phonon-mediated
interaction between the intersecting Landau levels is considered and no avoided
crossing is found at thermal equilibrium.Comment: 13 pages, 8 figure
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