Bifurcation of axons from cranial sensory neurons is disabled in the absence of Npr2-induced cGMP signaling

Axonal branching is a prerequisite for the establishment of complex neuronal circuits and their capacity for parallel information processing. Previously, we have identified a cGMP signaling pathway composed of the ligand C-type natriuretic peptide (CNP), its receptor, the guanylyl cyclase natriuretic peptide receptor 2 (Npr2), and the cGMP-dependent kinase I{alpha} (cGKI{alpha}) that regulates axon bifurcation of dorsal root ganglion (DRG) neurons in the spinal cord. Now we asked whether this cascade also controls axon bifurcation elsewhere in the nervous system. An Npr2-lacZ reporter mouse line was generated to clarify the pattern of the CNP receptor expression. It was found that during the period of axonal outgrowth, Npr2 and cGKI{alpha} were strongly labeled in neurons of all cranial sensory ganglia (gV, gVII, gVIII, gIX, and gX). In addition, strong complementary expression of CNP was detected in the hindbrain at the entry zones of sensory afferents. To analyze axon branching in individual Npr2-positive neurons, we generated a mouse mutant expressing a tamoxifen-inducible variant of Cre recombinase expressed under control of the Npr2-promoter (Npr2-CreER(T2)). After crossing this strain with conditional reporter mouse lines, we revealed that the complete absence of Npr2 activity indeed prohibited the bifurcation of cranial sensory axons in their entrance region. Consequently, axons only turned in either an ascending or descending direction, while collateral formation and growth of the peripheral arm was not affected. These findings indicate that in neurons of the cranial sensory ganglia, as in DRG neurons, cGMP signals are necessary for the execution of an axonal bifurcation program

Molecular analysis of sensory axon branching unraveled a cGMP-dependent signaling cascade

Axonal branching is a key process in the establishment of circuit connectivity within the nervous system. Molecular-genetic studies have shown that a specific form of axonal branching - the bifurcation of sensory neurons at the transition zone between the peripheral and the central nervous System - is regulated by a cyclic guanosine monophosphate (cGMP)-dependent signaling cascade which is composed of C-type natriuretic peptide (CNP), the receptor guanylyl cyclase Npr2, and cGMP-dependent protein kinase Iα (cGKIα). In the absence of any one of these components, neurons in dorsal root ganglia (DRG) and cranial sensory ganglia no longer bifurcate, and instead turn in either an ascending or a descending direction. In contrast, collateral axonal branch formation which represents a second type of axonal branch formation is not affected by inactivation of CNP, Npr2, or cGKI. Whereas axon bifurcation was lost in mouse mutants deficient for components of CNP-induced cGMP formation; the absence of the cGMP-degrading enzyme phosphodiesterase 2A had no effect on axon bifurcation. Adult mice that lack sensory axon bifurcation due to the conditional inactivation of Npr2-mediated cGMP signaling in DRG neurons demonstrated an altered shape of sensory axon terminal fields in the spinal cord, indicating that elaborate compensatory mechanisms reorganize neuronal circuits in the absence of bifurcation. On a functional level, these mice showed impaired heat sensation and nociception induced by chemical irritants, whereas responses to cold sensation, mechanical stimulation, and motor coordination are normal. These data point to a critical role of axon bifurcation for the processing of acute pain perception

Statistics of low-energy levels of a one-dimensional weakly localized Frenkel exciton: A numerical study

Numerical study of the one-dimensional Frenkel Hamiltonian with on-site randomness is carried out. We focus on the statistics of the energy levels near the lower exciton band edge, i. e. those determining optical response. We found that the distribution of the energy spacing between the states that are well localized at the same segment is characterized by non-zero mean, i.e. these states undergo repulsion. This repulsion results in a local discrete energy structure of a localized Frenkel exciton. On the contrary, the energy spacing distribution for weakly overlapping local ground states (the states with no nodes within their localization segments) that are localized at different segments has zero mean and shows almost no repulsion. The typical width of the latter distribution is of the same order as the typical spacing in the local discrete energy structure, so that this local structure is hidden; it does not reveal itself neither in the density of states nor in the linear absorption spectra. However, this structure affects the two-exciton transitions involving the states of the same segment and can be observed by the pump-probe spectroscopy. We analyze also the disorder degree scaling of the first and second momenta of the distributions.Comment: 10 pages, 6 figure

Investigation of pulse shape neutron-gamma discrimination

The role of neutron beam investigation is significant not only for fundamental science but also for various fields of applied science. This work is dedicated to the formation of neutron beams using the external 18-MeV proton beam of IBA cyclotron C18/18 with a beam current of up to 100 µA. The facility is located at the A. Alikhanyan National Science Laboratory (Yerevan Physics Institute). The possibility to obtain thermal or epithermal neutron beams using the external proton beam of the cyclotron is studied using Geant4 simulations. In this case, a quasimonoenergetic neutron source 9Be (p, n)9B reaction is chosen. As a result of the simulations, the optimal thickness of the 9Be beryllium isotope target is determined. The induced neutron beam is accompanied by a gamma ray background. To decrease the number of accompanying gamma rays, the lead absorber is considered. As a method of separating neutrons from gamma rays, the pulse shape discrimination (PSD) technique is developed. This study shows the possibility of neutron-gamma PSD and its applicability using the EJ-299-33A plastic scintillator

Land of Kaghrdik According to Armenian Sources

Поступила в редакцию: 11.05.2023. Принята к печати: 12.10.2023.Submitted: 11.05.2023. Accepted: 12.10.2023.Отдельные детали восточных походов императора Иоанна II Комнина (1118–1143) до сих пор вызывают в среде историков споры, а неясные сведения источников о месте гибели императора в Киликии 1143 г. породили множество гипотез. Обстоятельства его кончины нам известны в основном из византийских, латинских и сирийских источников. Армянские же источники содержат уникальные сведения о тех событиях, которые ускользнули от внимания исследователей. В частности, в армянских летописях XIII в. Смбата Спарапета, Ваграма Рабуни и Гетума Патмича, повествующих о походе императора Иоанна II Комнина 1142–1143 гг., упоминается, что внутренности императора были захоронены в местности Кагрдик. Латинский хронист Вильгельм Тирский местом гибели Иоанна II называет Pratum palliorum. На основе лингвистического анализа, а также сопоставления сведений из разных источников в статье доказывается, что Кагрдик не может совпадать с Pratum palliorum. Кагрдик, очевидно, находился вблизи Анаварзы. Локализация места гибели Иоанна II Комнина позволяет также уточнить местонахождение в XII–XIII вв. православных храмов в районе Анаварзы. Сравнительный анализ показывает, что наиболее вероятным местонахождением Кагрдика были окрестности руин замка Тумлу и монастыря св. Симанкла.Historians continue debating the details of Emperor John II Komnenos’ (1118–1143) campaigns in the east. The exact place of his death in Cilicia in 1143 is unclear due to vague account of the sources in possession. The Byzantine, Latin, and Syrian writers provide the most information about the emperor’s death. However, the Armenian sources, specifically the thirteenth-century chronicles of Smbat Sparapet, Vahram Rabuni, and Getum Patmich, provide unique information on the events in John Komnenos’ campaign of 1142–1143. These sources mention that the emperor’s entrails were buried in the land of Kagrdik. William of Tyre, a Latin chronicler, said that John II died at the place called Pratum palliorum. However, the linguistic analysis and comparison of various sources undertaken in this article has proved that the Kaghrdik was not the same as Pratum palliorum. The Kaghrdik was probably located near Anavarza. The discovery of the John II Komnenos burial place may shed light on the location of the twelfth- and thirteenth-century Orthodox churches in the Anavarza region. The comparative analysis has suggested that the Kaghrdik was most likely located in the vicinity of the ruins of Tumlu castle and St. Simankla monastery

Measurement of Scintillation and Ionization Yield and Scintillation Pulse Shape from Nuclear Recoils in Liquid Argon

We have measured the scintillation and ionization yield of recoiling nuclei in liquid argon as a function of applied electric field by exposing a dual-phase liquid argon time projection chamber (LAr-TPC) to a low energy pulsed narrow band neutron beam produced at the Notre Dame Institute for Structure and Nuclear Astrophysics. Liquid scintillation counters were arranged to detect and identify neutrons scattered in the TPC and to select the energy of the recoiling nuclei. We report measurements of the scintillation yields for nuclear recoils with energies from 10.3 to 57.3 keV and for median applied electric fields from 0 to 970 V/cm. For the ionization yields, we report measurements from 16.9 to 57.3 keV and for electric fields from 96.4 to 486 V/cm. We also report the observation of an anticorrelation between scintillation and ionization from nuclear recoils, which is similar to the anticorrelation between scintillation and ionization from electron recoils. Assuming that the energy loss partitions into excitons and ion pairs from $^{83m}$Kr internal conversion electrons is comparable to that from $^{207}$Bi conversion electrons, we obtained the numbers of excitons ($N_{ex}$) and ion pairs ($N_i$) and their ratio ($N_{ex}/N_i$) produced by nuclear recoils from 16.9 to 57.3 keV. Motivated by arguments suggesting direction sensitivity in LAr-TPC signals due to columnar recombination, a comparison of the light and charge yield of recoils parallel and perpendicular to the applied electric field is presented for the first time.Comment: v2 to reflect published versio

Measurement of the Spin-Dependence of the pbar-p Interaction at the AD-Ring

We propose to use an internal polarized hydrogen storage cell gas target in the AD ring to determine for the first time the two total spin-dependent pbar-p cross sections sigma_1 and sigma_2 at antiproton beam energies in the range from 50 to 450 MeV. The data obtained are of interest by themselves for the general theory of pbar-p interactions since they will provide a first experimental constraint of the spin-spin dependence of the nucleon-antinucleon potential in the energy range of interest. In addition, measurements of the polarization buildup of stored antiprotons are required to define the optimum parameters of a future, dedicated Antiproton Polarizer Ring (APR), intended to feed a double-polarized asymmetric pbar-p collider with polarized antiprotons. Such a machine has recently been proposed by the PAX collaboration for the new Facility for Antiproton and Ion Research (FAIR) at GSI in Darmstadt, Germany. The availability of an intense stored beam of polarized antiprotons will provide access to a wealth of single- and double-spin observables, thereby opening a new window on QCD spin physics.Comment: 51 pages, 23 figures, proposal submitted to the SPS committee of CER

Effect of Layer-Stacking on the Electronic Structure of Graphene Nanoribbons

The evolution of electronic structure of graphene nanoribbons (GNRs) as a function of the number of layers stacked together is investigated using \textit{ab initio} density functional theory (DFT) including interlayer van der Waals interactions. Multilayer armchair GNRs (AGNRs), similar to single-layer AGNRs, exhibit three classes of band gaps depending on their width. In zigzag GNRs (ZGNRs), the geometry relaxation resulting from interlayer interactions plays a crucial role in determining the magnetic polarization and the band structure. The antiferromagnetic (AF) interlayer coupling is more stable compared to the ferromagnetic (FM) interlayer coupling. ZGNRs with the AF in-layer and AF interlayer coupling have a finite band gap while ZGNRs with the FM in-layer and AF interlayer coupling do not have a band gap. The ground state of the bi-layer ZGNR is non-magnetic with a small but finite band gap. The magnetic ordering is less stable in multilayer ZGNRs compared to single-layer ZGNRs. The quasipartcle GW corrections are smaller for bilayer GNRs compared to single-layer GNRs because of the reduced Coulomb effects in bilayer GNRs compared to single-layer GNRs.Comment: 10 pages, 5 figure

Superradiance from an ultrathin film of three-level V-type atoms: Interplay between splitting, quantum coherence and local-field effects

We carry out a theoretical study of the collective spontaneous emission (superradiance) from an ultrathin film comprised of three-level atoms with $V$-configuration of the operating transitions. As the thickness of the system is small compared to the emission wavelength inside the film, the local-field correction to the averaged Maxwell field is relevant. We show that the interplay between the low-frequency quantum coherence within the subspace of the upper doublet states and the local-field correction may drastically affect the branching ratio of the operating transitions. This effect may be used for controlling the emission process by varying the doublet splitting and the amount of low-frequency coherence.Comment: 15 pages, 5 figure

Hard Two-Photon Contribution to Elastic Lepton-Proton Scattering: Determined by the OLYMPUS Experiment

The OLYMPUS collaboration reports on a precision measurement of the positron-proton to electron-proton elastic cross section ratio, $R_{2\gamma}$, a direct measure of the contribution of hard two-photon exchange to the elastic cross section. In the OLYMPUS measurement, 2.01~GeV electron and positron beams were directed through a hydrogen gas target internal to the DORIS storage ring at DESY. A toroidal magnetic spectrometer instrumented with drift chambers and time-of-flight scintillators detected elastically scattered leptons in coincidence with recoiling protons over a scattering angle range of $\approx 20\degree$ to $80\degree$. The relative luminosity between the two beam species was monitored using tracking telescopes of interleaved GEM and MWPC detectors at $12\degree$, as well as symmetric M{\o}ller/Bhabha calorimeters at $1.29\degree$. A total integrated luminosity of 4.5~fb$^{-1}$ was collected. In the extraction of $R_{2\gamma}$, radiative effects were taken into account using a Monte Carlo generator to simulate the convolutions of internal bremsstrahlung with experiment-specific conditions such as detector acceptance and reconstruction efficiency. The resulting values of $R_{2\gamma}$, presented here for a wide range of virtual photon polarization $0.456<\epsilon<0.978$, are smaller than some hadronic two-photon exchange calculations predict, but are in reasonable agreement with a subtracted dispersion model and a phenomenological fit to the form factor data.Comment: 5 pages, 3 figures, 2 table