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Regulatory impact of the C-terminal tail on charge transfer pathways in drosophila cryptochrome
Interconnected transcriptional and translational feedback loops are at the core of the molecular mechanism of the circadian clock. Such feedback loops are synchronized to external light entrainment by the blue light photoreceptor cryptochrome (CRY) that undergoes conformational changes upon light absorption by an unknown photoexcitation mechanism. Light-induced charge transfer (CT) reactions in Drosophila CRY (dCRY) are investigated by state-of-the-art simulations that reveal a complex, multi-redox site nature of CT dynamics on the microscopic level. The simulations consider redox-active chromophores of the tryptophan triad (Trp triad) and further account for pathways mediated by W314 and W422 residues proximate to the C-terminal tail (CTT), thus avoiding a pre-bias to specific W-mediated CT pathways. The conducted dissipative quantum dynamics simulations employ microscopically derived model Hamiltonians and display complex and ultrafast CT dynamics on the picosecond timescale, subtly balanced by the electrostatic environment of dCRY. In silicio point mutations provide a microscopic basis for rationalizing particular CT directionality and demonstrate the degree of electrostatic control realized by a discrete set of charged amino acid residues. The predicted participation of CT states in proximity to the CTT relates the directionality of CT reactions to the spatial vicinity of a linear interaction motif. The results stress the importance of CTT directional charge transfer in addition to charge transfer via the Trp triad and call for the use of full-length CRY models including the interactions of photolyase homology region (PHR) and CTT domains. Β© 2020 by the authors. Licensee MDPI, Basel, Switzerland
COS-Weak: Probing the CGM using analogs of weak Mg II absorbers at z < 0.3
We present a sample of 34 weak metal line absorbers at complied via
the simultaneous detections () of the SiII and
CII absorption lines, with (SiII) \AA\ and
(CII) \AA, in archival HST/COS spectra. Our sample increases the
number of known low- "weak absorbers" by a factor of . The column
densities of HI and low-ionization metal lines obtained from Voigt profile
fitting are used to build simple photoionization models using CLOUDY. The
inferred densities and total hydrogen column densities are in the ranges of
and , respectively. The line of sight thicknesses of the absorbers
have a wide range of 1 pc50 kpc with a median value of 500 pc.
The high-ionization OVI absorption, detected in 12/18 cases, always stems from
a different gas-phase. Most importantly, 85% (50%) of these absorbers show a
metallicity of (0.0). The fraction of systems showing high
metallicity (i.e., ) in our sample is significantly higher
than the HI-selected sample (Wotta et al. 2016) and the galaxy-selected sample
(Prochaska et al. 2017) of absorbers probing the circum-galactic medium (CGM)
at similar redshift. A search for galaxies has revealed a significant
galaxy-overdensity around these weak absorbers compared to random places with a
median impact parameter of 166 kpc to the nearest galaxy. Moreover, we find the
presence of multiple galaxies in % of the cases, suggesting group
environments. The observed of indicates that such
metal-enriched, compact, dense structures are ubiquitous in the halos of
low- galaxies that are in groups. We suggest that these are transient
structures that are related to outflows and/or stripping of metal-rich gas from
galaxies.Comment: Published (2018MNRAS.476.4965M) after minor revision. Appendix A is
newly added
Π ΠΎΡΡΠΈΡ Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΠΎΠΉ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ Π³Π»ΠΎΠ±Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ
Π ΡΡΠ°ΡΡΠ΅ Π°Π²ΡΠΎΡ ΠΏΡΡΠ°Π΅ΡΡΡ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΠΈΡΡ ΡΠΎΠ΄Π΅ΡΠΆΠ°Π½ΠΈΠ΅ Π³Π»ΠΎΠ±Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΊΠ°ΠΊ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΊΠ°ΡΠ΅Π³ΠΎΡΠΈΠΈ. Π Π°ΡΡΠΌΠ°ΡΡΠΈΠ²Π°Π΅Ρ ΡΠ°Π·Π»ΠΈΡΠ½ΡΠ΅ ΠΏΠΎΠ΄Ρ
ΠΎΠ΄Ρ ΠΊ ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΡ Π³Π»ΠΎΠ±Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ. ΠΡΠ΄Π΅Π»ΡΠ΅Ρ Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠ½ΡΠ΅ ΠΏΡΠΈΠ·Π½Π°ΠΊΠΈ Π³Π»ΠΎΠ±Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ, ΠΏΠΎΠ»ΠΎΠΆΠΈΡΠ΅Π»ΡΠ½ΡΠ΅ ΠΈ ΠΎΡΡΠΈΡΠ°ΡΠ΅Π»ΡΠ½ΡΠ΅ ΡΡΠΎΡΠΎΠ½Ρ ΡΡΠΎΠ³ΠΎ ΡΠ²Π»Π΅Π½ΠΈΡ. ΠΠ° Π±Π°Π·Π΅ Π°Π½Π°Π»ΠΈΠ·Π° Π³Π»ΠΎΠ±Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ ΠΊΠ°ΠΊ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ²Π»Π΅Π½ΠΈΡ ΠΎΠ½ ΠΏΡΡΠ°Π΅ΡΡΡ ΡΠ΄Π΅Π»Π°ΡΡ Π²ΡΠ²ΠΎΠ΄Ρ Π΄Π»Ρ ΡΠΎΡΡΠΈΠΉΡΠΊΠΎΠΉ ΡΠΊΠΎΠ½ΠΎΠΌΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΏΠΎΠ»ΠΈΡΠΈΠΊΠΈ. ΠΠΊΡΠ΅Π½ΡΠΈΡΡΠ΅Ρ Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ Π½Π° Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΡΡΠΈ Π°Π΄Π΅ΠΊΠ²Π°ΡΠ½ΠΎ ΡΠ΅Π°Π³ΠΈΡΠΎΠ²Π°ΡΡ Π½Π° Π²ΡΠ·ΠΎΠ²Ρ ΠΌΠΈΡΠΎΠ²ΠΎΠΉ ΠΊΠ°ΠΏΠΈΡΠ°Π»ΠΈΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠ΅Π°Π»ΡΠ½ΠΎΡΡΠΈ, ΠΎΠ±ΡΠ°ΡΠ°Π΅Ρ Π²Π½ΠΈΠΌΠ°Π½ΠΈΠ΅ Π½Π° ΡΠΎ, ΡΡΠΎ Π°Π±ΡΠΎΠ»ΡΡΠΈΠ·Π°ΡΠΈΡ ΡΡΠ½ΠΎΡΠ½ΡΡ
Π½Π°ΡΠ°Π» Π΄ΠΈΡΠΊΡΠ΅Π΄ΠΈΡΠΈΡΡΠ΅Ρ ΠΈΠ΄Π΅Ρ Π³Π»ΠΎΠ±Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ. ΠΠ΅Π»Π°Π΅Ρ Π²ΡΠ²ΠΎΠ΄ ΠΎ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΡΡΠΈ ΡΡΠΈΠ»Π΅Π½ΠΈΡ Π²Π½ΠΈΠΌΠ°Π½ΠΈΡ ΠΊ ΡΠΎΡΠΈΠ°Π»ΡΠ½ΡΠΌ Π°ΡΠΏΠ΅ΠΊΡΠ°ΠΌ ΠΈ ΠΏΡΠΎΡΠΈΠ²ΠΎΡΠ΅ΡΠΈΡΠΌ Π³Π»ΠΎΠ±Π°Π»ΠΈΠ·Π°ΡΠΈΠΈ Ρ ΡΠ΅Π»ΡΡ ΠΌΠΈΠ½ΠΈΠΌΠΈΠ·Π°ΡΠΈΠΈ Π½Π΅Π³Π°ΡΠΈΠ²Π½ΡΡ
ΠΏΠΎΡΠ»Π΅Π΄ΡΡΠ²ΠΈΠΉ ΡΡΠΎΠ³ΠΎ ΡΠ²Π»Π΅Π½ΠΈΡ
Selektive Biofunktionalisierung dreidimensionaler Mikrostrukturen
Zellen werden in ihrer natΓΌrlichen Umgebung von einer Vielzahl von Faktoren beeinflusst. FΓΌr zukΓΌnftige Zellexperimente wΓ€re es optimal alle Faktoren (Geometrie, Nanotopographie, Steifigkeit, rΓ€umliche und quantitative Ligandenverteilung) kontrollieren zu kΓΆnnen um Aufschluss ΓΌber eine optimale Wachstumsumgebung fΓΌr Zellen zu erhalten. Deshalb werden in dieser Arbeit verschiedene Methoden zur selektiven Biofunktionalisierung dreidimensionaler Mikrostrukturen vorgestellt
Classical and Quantum Signatures of Quantum Phase Transitions in a (Pseudo) Relativistic Many-Body System
We identify a (pseudo) relativistic spin-dependent analogue of the celebrated quantum phase transition driven by the formation of a bright soliton in attractive one-dimensional bosonic gases. In this new scenario, due to the simultaneous existence of the linear dispersion and the bosonic nature of the system, special care must be taken with the choice of energy region where the transition takes place. Still, due to a crucial adiabatic separation of scales, and identified through extensive numerical diagonalization, a suitable effective model describing the transition is found. The corresponding mean-field analysis based on this effective model provides accurate predictions for the location of the quantum phase transition when compared against extensive numerical simulations. Furthermore, we numerically investigate the dynamical exponents characterizing the approach from its finite-size precursors to the sharp quantum phase transition in the thermodynamic limit
Blazed oblique plane microscopy reveals scale-invariant inference of brain-wide population activity
Due to the size and opacity of vertebrate brains, it has until now been impossible to simultaneously record neuronal activity at cellular resolution across the entire adult brain. As a result, scientists are forced to choose between cellular-resolution microscopy over limited fields-of-view or whole-brain imaging at coarse-grained resolution. Bridging the gap between these spatial scales of understanding remains a major challenge in neuroscience. Here, we introduce blazed oblique plane microscopy to perform brain-wide recording of neuronal activity at cellular resolution in an adult vertebrate. Contrary to common belief, we find that inferences of neuronal population activity are near-independent of spatial scale: a set of randomly sampled neurons has a comparable predictive power as the same number of coarse-grained macrovoxels. Our work thus links cellular resolution with brain-wide scope, challenges the prevailing view that macroscale methods are generally inferior to microscale techniques and underscores the value of multiscale approaches to studying brain-wide activity
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