Tuberculosis in Lemurs and a Fossa at National Zoo, Madagascar, 2022.

We diagnosed Mycobacterium tuberculosis in captive lemurs and a fossa in Antananarivo, Madagascar. We noted clinical signs in the animals and found characteristic lesions during necropsy. The source of infection remains unknown. Our results illustrate the potential for reverse zoonotic infections and intraspecies transmission of tuberculosis in captive wildlife.

Design of JT-60SA core Thomson scattering diagnostic system.

An incoherent Thomson scattering diagnostic will be installed in the JT-60SA tokamak to measure electron temperature and electron density profiles. The target radial spatial resolution is 25 mm with 46 spatial channels. The accuracy in electron temperature and density is a few percent at ne = 7.5 × 1019 m-3, which is the expected value in the plasma core. This paper presents the designs of collection optics, fibers with their alignment system, and polychromators. The collection optics overcomes unique issues for superconducting fusion devices, i.e., limited design space, high-temperature measurements, and harsh radiation condition. When in several years the more performing plasma will generate intense nuclear radiation, the lens materials of the optics can be replaced by radiation resistant glasses without major changes in the lens holder. It will prevent transmission degradation and keep stable measurement accuracy.

Validations of calibration-free measurements of electron temperature using double-pass Thomson scattering diagnostics from theoretical and experimental aspects.

This paper evaluates the accuracy of electron temperature measurements and relative transmissivities of double-pass Thomson scattering diagnostics. The electron temperature (Te) is obtained from the ratio of signals from a double-pass scattering system, then relative transmissivities are calculated from the measured Te and intensity of the signals. How accurate the values are depends on the electron temperature (Te) and scattering angle (θ), and therefore the accuracy of the values was evaluated experimentally using the Large Helical Device (LHD) and the Tokyo spherical tokamak-2 (TST-2). Analyzing the data from the TST-2 indicates that a high Te and a large scattering angle (θ) yield accurate values. Indeed, the errors for scattering angle θ = 135° are approximately half of those for θ = 115°. The method of determining the Te in a wide Te range spanning over two orders of magnitude (0.01-1.5 keV) was validated using the experimental results of the LHD and TST-2. A simple method to provide relative transmissivities, which include inputs from collection optics, vacuum window, optical fibers, and polychromators, is also presented. The relative errors were less than approximately 10%. Numerical simulations also indicate that the Te measurements are valid under harsh radiation conditions. This method to obtain Te can be considered for the design of Thomson scattering systems where there is high-performance plasma that generates harsh radiation environments.

Demonstration of improvement in the signal-to-noise ratio of Thomson scattering signal obtained by using a multi-pass optical cavity on the Tokyo Spherical Tokamak-2.

The multi-pass Thomson scattering (TS) scheme enables obtaining many photons by accumulating multiple TS signals. The signal-to-noise ratio (SNR) depends on the accumulation number. In this study, we performed multi-pass TS measurements for ohmically heated plasmas, and the relationship between SNR and the accumulation number was investigated. As a result, improvement of SNR in this experiment indicated similar tendency to that calculated for the background noise dominant situation.

Signal evaluations using singular value decomposition for Thomson scattering diagnostics.

This paper provides a novel method for evaluating signal intensities in incoherent Thomson scattering diagnostics. A double-pass Thomson scattering system, where a laser passes through the plasma twice, generates two scattering pulses from the plasma. Evaluations of the signal intensities in the spectrometer are sometimes difficult due to noise and stray light. We apply the singular value decomposition method to Thomson scattering data with strong noise components. Results show that the average accuracy of the measured electron temperature (Te) is superior to that of temperature obtained using a low-pass filter (<20 MHz) or without any filters.

Note: Multi-pass Thomson scattering measurement on the TST-2 spherical tokamak.

In multi-pass Thomson scattering (TS) scheme, a laser pulse makes multiple round trips through the plasma, and the effective laser energy is enhanced, and we can increase the signal-to-noise ratio as a result. We have developed a coaxial optical cavity in which a laser pulse is confined, and we performed TS measurements using the coaxial cavity in tokamak plasmas for the first time. In the optical cavity, the laser energy attenuation was approximately 30% in each round trip, and we achieved a photon number gain of about 3 compared with that obtained in the first round trip. In addition, the temperature measurement accuracy was improved by accumulating the first three round trip waveforms.

Optical designs of reflection and refraction collection optics for a JT-60SA core Thomson scattering system.

Collection optics for core measurements in a JT-60SA Thomson scattering system were designed. The collection optics will be installed in a limited space and have a wide field of view and wide wavelength range. Two types of the optics are therefore suggested: refraction and reflection types. The reflection system, with a large primary mirror, avoids large chromatic aberrations. Because the size limit of the primary mirror and vignetting due to the secondary mirror affect the total collection throughput, conditions that provide the high throughput are found through an optimization. A refraction system with four lenses forming an Ernostar system is also employed. The use of high-refractive-index glass materials enhances the freedom of the lens curvatures, resulting in suppression of the spherical and coma aberration. Moreover, sufficient throughput can be achieved, even with smaller lenses than that of a previous design given in [H. Tojo, T. Hatae, T. Sakuma, T. Hamano, K. Itami, Y. Aida, S. Suitoh, and D. Fujie, Rev. Sci. Instrum. 81, 10D539 (2010)]. The optical resolutions of the reflection and refraction systems are both sufficient for understanding the spatial structures in plasma. In particular, the spot sizes at the image of the optics are evaluated as ~0.3 mm and ~0.4 mm, respectively. The throughput for the two systems, including the pupil size and transmissivity, are also compared. The results show that good measurement accuracy (<10%) even at high electron temperatures (<30 keV) can be expected in the refraction system.

Anisotropic electron temperature measurements without knowing the spectral transmissivity for a JT-60SA Thomson scattering diagnostic.

This paper focuses on a method for measuring the electron temperature (T(e)) without knowing the transmissivity using Thomson scattering diagnostic with a double-pass scattering system. Application of this method for measuring the anisotropic T(e), i.e., the T(e) in the directions parallel (T(eparallel)) and perpendicular (T(eperpendicular)) to the magnetic field, is proposed. Simulations based on the designed parameters for a JT-60SA indicate the feasibility of the measurements except in certain T(e) ranges, e.g., T(eparallel) ~ 3.5T(eperpendicular) at 120° of the scattering angle.

First measurement of electron temperature from signal ratios in a double-pass Thomson scattering system.

This paper presents an experimental demonstration to determine electron temperature (T(e)) with unknown spectral sensitivity (transmissivity) in a Thomson scattering system. In this method, a double-pass scattering configuration is used and the scattered lights from each pass (with different scattering angles) are measured separately. T(e) can be determined from the ratio of the signal intensities without knowing a real chromatic dependence in the sensitivity. Note that the wavelength range for each spectral channel must be known. This method was applied to the TST-2 Thomson scattering system. As a result, T(e) measured from the ratio (T(e,r)) and T(e) measured from a standard method (T(e,s)) showed a good agreement with <∣T(e,r) - T(e,s)∣∕T(e,s)> = 7.3%.

Design of collection optics and polychromators for a JT-60SA Thomson scattering system.

This paper presents designs of collection optics for a JT-60SA Thomson scattering system. By using tangential (to the toroidal direction) YAG laser injection, three collection optics without strong chromatic aberration generated by the wide viewing angle and small design volume were found to measure almost all the radial space. For edge plasma measurements, the authors optimized the channel number and wavelength ranges of band-pass filters in a polychromator to reduce the relative error in T(e) by considering all spatial channels and a double-pass laser system with different geometric parameters.

Poloidal mode analysis of magnetic probe data in a spherical tokamak configuration.

A method to determine the poloidal mode number m in a spherical tokamak based on magnetic probe data was developed. Perturbed magnetic fields at Mirnov coils are calculated for distributed helical filamentary currents on rational surfaces assuming the maximum current amplitude, m and n (toroidal mode number), and the toroidal location of the filaments. These free parameters were determined from the best fit to the measured signals. The residual error was reduced by a factor of 2 by introducing helical filaments instead of toroidal filaments. Using this method, m/n=2/1 and 3/2 modes were identified in Mega-Ampere Spherical Tokamak discharges, and the time evolution of the tearing modes was derived.

Detection of a new parametric decay instability branch in TST-2 during high harmonic fast wave heating.

Parametric decay instability (PDI) is often observed in the TST-2 spherical tokamak during high harmonic fast wave heating by rf pickup probes. The frequency spectrum exhibits lower and upper sideband peaks in addition to the pump wave at f(0)=21 MHz. Two types of PDI are observed. One is the well-known decay into the ion-cyclotron quasimode (nf(ci)) and the ion Bernstein wave (f(0)-nf(ci)). The other is a newly found decay with the sideband frequency between f(0) and f(0)-f(ci). The frequency difference between this sideband and the pump increases in proportion to B(t). Moreover, high-speed visible light measuring systems with photomultiplier tubes or hybrid photodetectors viewing the plasma core detected oscillation of light emission at around f(0).

Expression and localization of matrix metalloproteinases (MT1-MMP, MMP-2) and tissue inhibitor of metalloproteinase-2 (TIMP-2) during synepitheliochorial placentation of goats (Capra hircus).

Matrix metalloproteinases (MMPs) and tissue inhibitor of metalloproteinases (TIMPs) play key roles during the placentation of highly invasive haemochorial type. Our knowledge is yet scanty, however, regarding the roles played by MMPs and TIMPs in the placentation of non-invasive synepitheliochorial type. In the present study, expression patterns of MT1-MMP, MMP-2 and TIMP-2 mRNAs as well as the encoded proteins in the endometrium and the placenta were examined on Days 35, 75, and 100 of pregnancy, representing roughly the 1st, 2nd and 3rd trimesters of caprine gestation, by means of quantitative RT-PCR analysis, in situ hybridization, immunoblotting, gelatin zymography and immunohistochemistry. In the endometrium and the intercotyledonal trophoblast, the expression levels of the 3 genes remained relatively uniform throughout the period of gestation examined. Curiously, however, in the placentomes, the relative expression levels of MT1-MMP mRNA increased linearly from Day 35 to Day 100, while those of MMP-2 and TIMP-2 were clearly down-regulated in Day 100 placentae. The expression levels of MT1-MMP and TIMP-2 proteins in placentomes were well correlated with those of the respective mRNAs. In the case of MMP-2, the total amount of MMP-2 protein (the combined values of the latent, the intermediate and the active forms) decreased slightly, while the levels of the active form increased markedly from Day 35 to Day 100. Immunohistochemical analysis of the placentome revealed that MT1-MMP and TIMP-2 proteins were co-localized in the binucleate trophoblast cells; expression of these 2 proteins was not detected in the uninuclear principal trophoblast cells. MMP-2 expression was detected both in the binucleate and in the uninuclear principal cells of the trophoblast and in the endometrial stromal cells of the uterine septum, regardless of the stages of gestation examined. The co-localization of MT1-MMP, MMP-2 and TIMP-2 in binucleate trophoblast cells, the cotyledonal trophoblast cells and the subsyncytial stromal cells is likely to reflect the functional coordination of the 3 proteins in these cells during trophoblastic invasion and the placental tissue remodeling in the placentome.

Activation of ribosomal S6 kinase (RSK) during porcine oocyte maturation.

The normal kinetics of ribosomal S6 kinase (RSK) during the meiotic maturation of porcine oocytes were examined. The phosphorylation states of RSK and extracellular signal-regulated kinase (ERK), major mitogen-activated protein (MAP) kinases in maturating porcine oocytes, were detected by Western blotting analysis. The S6 protein kinase activity was assayed using a specific substrate peptide which contained the major phosphorylation sites of S6 kinase. Full phosphorylation of RSK was correlated with ERK phosphorylation and was observed before germinal vesicle breakdown. S6 kinase activity was low in both freshly isolated and 20 h cultured oocytes. S6 kinase activity was significantly elevated in matured oocytes to a level about 6 times higher than that in freshly isolated oocytes. Furthermore, full phosphorylation of RSK was inhibited when oocytes were treated with U0126, a specific MAP kinase kinase inhibitor, in dose-dependent manner, indicating that RSK is one of the substrates of MAP kinase. These results suggest that the activation of RSK is involved in the regulation of meiotic maturation of porcine oocytes.

[Anesthesia for a patient with alcoholic heart disease and transient complete heart block].

A 70-year-old man who had been drinking a bottle of whisky each day was scheduled for laser resection of a tongue tumor. His electrocardiogram showed sinus bradycardia (heart rate was 35-40 bpm), and transient complete heart block was observed. Echocardiography showed hypertrophic cardiomyopathy. After a temporary transvenous pacemaker had been inserted, anesthesia was induced with thiopental and vecuronium bromide, and maintained with sevoflurane and fentanyl. Heart rate was 45.min-1 before the induction of anesthesia, and after the induction increased to 70-80.min-1. Analysis of heart rate variability suggested that the increase in heart rate was due to augmentation of sympathetic nervous activity after intubation and operation stress. After the operation his bradycardia improved gradually, and after 3 months heart rate settled at about 55.min-1. Cadiomyopathy is known to be one of the complications of alcoholism. It was reported that alcoholic heart disease was improved promptly by abstinence from alcohol. During his long hospitalization, abstinence might have improved his severe bradycardia. Thiopental is useful for induction of anesthesia in a patient with severe bradycardia from alcoholic cadiomyopathy.

Immunocytochemical demonstration of the secretory dynamics of zymogenic contents in rat gastric gland processed by high-pressure freezing/freeze substitution, with special references to phospholipase A(2) and phospholipase Cgamma1.

High-pressure freezing/freeze substitution followed by Lowicryl K4M embedding provided an excellent morphology and antigenicity of the gastric glands, as well as the intraluminal fluid contents. Taking advantage of this, we histochemically investigated the secretory dynamics of the zymogenic contents in rat gastric gland, with special references to phospholipase A(2) (PLA(2)) and phospholipase Cgamma1 (PLCgamma1). The combination of immunogold labeling and KMnO4-uranyl acetate-lead citrate staining for zymogenic contents clearly demonstrated the rapid diffusion of PLA(2) molecules from the exocytosed zymogenic contents into the mucinous contents in gastric glandular lumens. In contrast, the exocytosed PLCgamma1 molecules remained within the zymogenic contents in the glandular lumens. These findings indicated the distinction between the exocytosed PLA(2) and PLCgamma1 in their diffusion rate. In addition, the mucinous contents surrounding the exocytosed zymogenic contents were intensely labeled with Griffonia simplicifolia II lectin which specifically recognizes the mucin of mucous neck cells. Interestingly, some of the PLA(2) immunolabeling on the mucinous contents was associated with the apical membranes of gastric epithelial cells, especially that of parietal cells. The secretory dynamics of the zymogenic contents in rat gastric glands, including their interaction with the mucinous contents are discussed.

The trophinin gene encodes a novel group of MAGE proteins, magphinins, and regulates cell proliferation during gametogenesis in the mouse.

Trophinin is a membrane protein that mediates apical cell adhesion between trophoblastic cells and luminal epithelial cells of the endometrium and is implicated in the initial attachment during the process of human embryo implantation. The present study identified novel trophinin gene transcripts, which encode proteins structurally distinct from trophinin protein in the mouse. We designated these proteins "magphinins," because they share consensus amino acid sequences with MAGE (melanoma-associated antigen) superfamily proteins. Among many MAGE proteins, magphinins are closely related to NRAGE, which mediates p75 neurotrophin receptor-dependent apoptosis, and necdin, which is a strong suppressor of cell proliferation in post-mitotic neurons. There are three major forms of magphinins, i.e. magphinin-alpha, -beta, and -gamma, in the mouse, which are formed due to alternative usage of different exons. Northern blot analysis revealed that magphinins are expressed in brain, ovary, testis, and epididymis. In addition, Western blot analysis and in vitro translation experiments showed that magphinins expressed in the mouse ovary and testis are translation products utilizing the second initiation AUG codon and contain an active nuclear localization signal. Ectopic expression of magphinins in mammalian cells resulted in nuclear localization of magphinin and suppressed cell proliferation. Immunohistochemistry of the mouse ovary and testis showed that magphinin proteins are distributed in the cytoplasm of the male and female germ cells, whereas these proteins are translocated to the nucleus at a specific stage of gametogenesis. These results strongly suggest that magphinins regulate cell proliferation during gametogenesis in the mouse.

Characterization of mesonephric cells that migrate into the XY gonad during testis differentiation.

In mouse fetal gonads, sex differentiation begins at 10.5-11.5 days postcoitum (dpc). With XY gonads of 12.5 dpc, cord-like structures are visible and stromal cells migrate from adjacent mesonephros, unlike in XX gonads. However, the migrated mesonephric cells, except for the endothelial cells, have not been specifically identified because they have not expressed differentiation markers over the course of organ coculture in previous experiments. In this study, we have for the first time succeeded in isolating only the mesonephric cells that migrate into the XY gonad from the mesonephros with alive and then cultured these cells in vitro through the use of an organ coculture system using EGFP-transgenic mice and a FACS Vantage. The migrated and isolated cells were used for morphological and molecular characterization. The migrated mesonephric cells contained three cell forms; a sharp cell form, a round cell form, and a cluster-forming cell. The sharp cells have the characters of peritubular myoid cells. The round cells and cluster-forming cells have the potential to differentiate into Leydig cells, as some of them are 3beta-HSD-positive. In in vitro culture of migrated mesonephric cells, the cluster-forming cells proliferated well and then differentiated into round cells, suggesting that the cluster-forming cells may be stem or precursor cells for the round cells. Thus, our findings provide important information related to the migration and differentiation of migrated mesonephric cells in the XY gonad.

A device for stereotactic transection of fiber bundles in rats.

We have designed a device for stereotactic transection of fiber bundles in experiments using rats. Here, we present our assessment of its features relative to those of conventional methods. The instrument consists of a stainless steel cannula and a thin inner wire with a hook at one end and a hilt at the other. The hook can be extended or withdrawn freely by pushing or pulling the hilt. Lesions were evaluated in 12 male Wistar rats, after two targets, the anterior commissure (n=6) and the caudate-putamen (n=6), were transected. After the cannula was introduced into the target, the inner hook was extended in an anterior direction orthogonally to the transverse plane. Next, the entire device was pulled back along the insertion path to transect the neuronal fibers. Then the inner hook was withdrawn into the cannula and the entire device was removed. Seven days later, brains were removed for histologic processing. Microscopic examination demonstrated a slit like gap produced by transection at the target; the lesions were infiltrated by microglia and surrounded by gliosis. Adjacent regions were minimally damaged. The path of the cannula demonstrated only minimal gliosis. Unlike conventional methods, this device permits precise transection of deep fiber bundles with minimal damage to surrounding brain tissue.

Germinal vesicle materials are not required for the activation of MAP kinase in porcine oocyte maturation.

The requirement of the germinal vesicle (GV) for the normal kinetics of mitogen-activated protein (MAP) kinase activity during porcine oocyte maturation was investigated. Porcine follicular oocytes were enucleated, and the locations of their extracellular signal-regulated kinases 1 and 2 (ERK1/2), major MAP kinases in maturating porcine oocytes, were detected by indirect immunofluorescent microscopy. The MAP kinase activity was assayed as myelin basic protein (MBP) kinase activity, and the phosphorylation states of ERK1/2 were detected by immunoblotting analyses. Translocation of MAP kinase into the GV and association with the spindle were observed in intact oocytes, while MAP kinase in enucleated oocytes was distributed almost uniformly in cytoplasm throughout the culturing period. The phosphorylation and the activation of MAP kinase were induced, and the activity was comparable with that of control denuded oocytes. The high level of activity was maintained through maturation, even in the absence of spindle formation. These results indicate that the presence of nuclear material and translocation into the GV are dispensable for the activation of MAP kinase and that associating with the spindle is not required for maintenance of its activity though porcine oocyte maturation.