Search for sub-eV scalar and pseudoscalar resonances via four-wave mixing with a laser collider

The quasi-parallel photon-photon scattering by combining two-color laser fields is an approach to produce resonant states of low-mass fields in laboratory. In this system resonances can be probed via the four-wave mixing process in the vacuum. A search for scalar and pseudoscalar fields was performed by combining 9.3 $\mu$J/0.9 ps Ti-Sapphire laser and 100 $\mu$J/9 ns Nd:YAG laser. No significant signal of four-wave mixing was observed. We provide the upper limits on the coupling-mass relation for scalar and pseudoscalar fields, respectively, at a 95\% confidence level in the mass region below 0.15~eV.Comment: Accepted by Prog. Theor. Exp. Phy

Computing longest common square subsequences

A square is a non-empty string of form YY. The longest common square subsequence (LCSqS) problem is to compute a longest square occurring as a subsequence in two given strings A and B. We show that the problem can easily be solved in O(n^6) time or O(|M|n^4) time with O(n^4) space, where n is the length of the strings and M is the set of matching points between A and B. Then, we show that the problem can also be solved in O(sigma |M|^3 + n) time and O(|M|^2 + n) space, or in O(|M|^3 log^2 n log log n + n) time with O(|M|^3 + n) space, where sigma is the number of distinct characters occurring in A and B. We also study lower bounds for the LCSqS problem for two or more strings

Jitter-free 40-fs 375-keV electron pulses directly accelerated by an intense laser beam and their application to direct observation of laser pulse propagation in a vacuum

ジッターフリーな超短パルスな電子ビームを実証 --超短パルス電子による超高速な電磁場観察--. 京都大学プレスリリース. 2020-12-04.We report the generation of ultrashort bright electron pulses directly driven by irradiating a solid target with intense femtosecond laser pulses. The duration of electron pulses after compression by a phase rotator composed of permanent magnets was measured as 89 fs via the ponderomotive scattering of electron and laser pulses, which were almost at the compression limit due to the dispersion of the electron optics. The electron pulse compression system consisting of permanent magnets enabled extremely high timing stability between the laser pulse and electron pulse. The long-term RMS arrival time drift was below 14 fs in 4 h, which was limited by the resolution of the current setup. Because there was no time-varying field to generate jitter, the timing jitter was essentially reduced to zero. To demonstrate the capability of the ultrafast electron pulses, we used them to directly visualize laser pulse propagation in a vacuum and perform 2D mapping of the electric fields generated by low-density plasma in real time

Effects of peripheral administration of rat urotensinII on circulation, and on distribution of c-Fos immunoreactive neurons in the brain

The purpose of this study was to examine the effects of intravenous injection of urotensinII on the systemic blood pressure and heart rate, and to examine whether the intraperitoneal administration of urotensinII evoked the stimulation of central neurons. Urotensin, originally isolated fish neuro-endocrine systems, is a peptide which consists of 12 amino acids. Lately human urotensinII was identified to be consisted from 11 amino acids. Receptors of urotensin have been found to highly distribute in the mammalian cadrdiovascular systems. It has been reported that urotensin evoked contraction of thoracic artery, while the dilatation of blood vessels was alternatively induced. In this study, we examined the effects of peripheral injection of rat urotensinII consisted of 14 amino acids on the circulation and on the activity of neurons in the brain. It was found that intravenous injection of rat urotensinII elicited dose-dependently decrease in blood pressure, and increase or decrease in heart rate. To examine whether an intraperitoneal injection of rat urotensinII induced an excitation of central neurons, we used immunohistochemical method to study the expression of c-Fos protein in neurons of the rat brain after intraperitoneal injection of rat urotensinII (test experiment). In the control experiment rat was intraperitoneally injected saline solution without rat urotensinII. It was found that intraperitoneal injection of rat urotensinII induced expression of c-Fos protein in several nuclei in the brain. These results suggested that rat urotensinII might exhibit physiological functions via central neuronal pathway as well as peripheral direct pathways

Early patency rate and fate of reattached intercostal arteries after repair of thoracoabdominal aortic aneurysms

ObjectivesThe present study analyzes the early patency of intercostal artery reconstruction, using graft interposition and aortic patch anastomosis, and determines the fate of reattached intercostal arteries after repair of thoracoabdominal aortic aneurysms.MethodsWe selected 115 patients (mean age, 63 ± 15 years; range, 19-83 years; male, n = 83) treated by thoracoabdominal aortic aneurysm repair with 1 or more reconstructed intercostal arteries at the Kobe University Graduate School of Medicine between October 1999 and December 2012. The intercostal arteries were reconstructed using graft interposition (n = 66), aortic patch anastomosis (n = 42), or both (n = 7).ResultsThe hospital mortality rate was 7.8% (n = 9). Eleven patients (9.6%) developed spinal cord ischemic injury (permanent, n = 6, transient, n = 5). The average number of reconstructed intercostal arteries per patient was 3.0 ± 1.5 (1-7), and 345 intercostal arteries were reattached. The overall patency rate was 74.2% (256/345) and that of aortic patch anastomosis was significantly better than that of graft interposition (90.8% [109/120] vs 65.3% [147/225], P < .01), but significantly worse for patients with than without spinal cord ischemic injury (51.9% [14/27] vs 76.1% [242/318], P = .01). There was no patch aneurysm in graft interposition during a mean of 49 ± 38 (range, 2-147) postoperative months, but aortic patch anastomosis including 4 intercostal arteries became dilated in 2 patients.ConclusionsAortic patch anastomosis might offer better patency rates and prevent spinal cord ischemic injury compared with graft interposition. Although aneurysmal changes in intercostal artery reconstructions are rare, large blocks of aortic wall reconstruction should be closely monitored

Creation of NV centers over a millimeter-sized region by intense single-shot ultrashort laser irradiation

一つの超短レーザーパルスでダイヤモンド量子センサ源を広領域で作製 --超短時間でダイヤモンドを超高感度量子センサに--. 京都大学プレスリリース. 2023-03-15.Recently, ultrashort laser processing has attracted attention for creating nitrogen-vacancy (NV) centers because this method can create single NV centers in spatially-controlled positions, which is an advantage for quantum information devices. On the other hand, creating high-density NV centers in a wide region is also important for quantum sensing because the sensitivity is directly enhanced by increasing the number of NV centers. A recent study demonstrated the creation of high-density NV centers by irradiating femtosecond laser pulses, but the created region was limited to micrometer size, and this technique required many laser pulses to avoid graphitization of diamond. Here, we demonstrate the creation of NV centers in a wide region using only an intense single femtosecond laser pulse irradiation. We irradiated a diamond sample with a femtosecond laser with a focal spot size of 41 µm and a laser fluence of up to 54 J/cm², which is much higher than the typical graphitization threshold in multi-pulse processing. We found that single-pulse irradiation created NV centers without post-annealing for a laser fluence higher than 1.8 J/cm², and the region containing NV centers expanded with increasing laser fluence. The diameter of the area was larger than the focal spot size and reached over 100 µm at a fluence of 54 J/cm². Furthermore, we demonstrated the NV centers' creation in a millimeter-sized region by a single-shot defocused laser pulse over 1100 µm with a fluence of 33 J/cm². The demonstrated technique will bring interest in the fundamentals and applications of fabricating ultrahigh-sensitivity quantum sensors

Molecular mechanisms of fragile X syndrome

Fragile X syndrome is the most common form of inherited mental retardation. Mutations which abolish expression of an X-linked gene, FMR1, result in pathogenesis of the disease. FMR1 encodes a cytoplasmic RNA-binding protein which interacts with two autosomal homologs, FXR1 and FXR2. These proteins are highly expressed in neurons. In addition, the FMR1/FXR proteins are associated with ribosomes. Given their RNA-binding activity and association with ribosomes, these proteins are hypothesized to bind to specific RNAs and regulate their expression at translational levels in a manner critical for correct development of neurons. Much progress has been made in FMR1 research over the past several years, but little light has yet to be shed on the physiological function of these proteins. It will be critical to define the biochemical properties of these proteins, and identify potential downstream targets to clarify the molecular mechanisms underlying the potential roles of these proteins in translation. A basic understanding of the function of this new family of RNA-binding proteins should then allow us to begin to address the question of how the lack of FMR1 expression leads to symptoms in fragile X syndrome

Effect of Impeller Agitation on Preparation of Tetra- n

The slurries-containing tetra-n-butyl ammonium bromide (TBAB) solution and its semiclathrate hydrate have attracted a lot of interest as latent heat transport media. These hydrate slurries contain some microparticles of crystal, and the size and shape of these hydrate particles could affect the mobility of slurries. Hence, it is essential to investigate the efficient hydrate-slurry preparation methods and the effect of hydrate particles on the fluid property of slurries for the application to latent heat transport media. In the present study, the effect of agitation on particle size distribution and aggregation of particles was studied to prepare easily flowing TBAB hydrate slurries that were suitable for fluid transport. First of all, the effects of impeller rotational speed and impeller type on the particle size and frequency of aggregation were investigated. The results suggested that the particle size distribution and the frequency of particle aggregation are strongly affected by the intensity of shear rate and its uniformity, which was controllable with impeller type and its rotation speed

Plausible phosphoenolpyruvate binding site revealed by 2.6 Å structure of Mn2+-bound phosphoenolpyruvate carboxylase from Escherichia coli11The coordinates and structure factors have been deposited in the Protein Data Bank (accession number 1QB4).

AbstractWe have determined the crystal structure of Mn2+-bound Escherichia coli phosphoenolpyruvate carboxylase (PEPC) using X-ray diffraction at 2.6 Å resolution, and specified the location of enzyme-bound Mn2+, which is essential for catalytic activity. The electron density map reveals that Mn2+ is bound to the side chain oxygens of Glu-506 and Asp-543, and located at the top of the α/β barrel in PEPC. The coordination sphere of Mn2+ observed in E. coli PEPC is similar to that of Mn2+ found in the pyruvate kinase structure. The model study of Mn2+-bound PEPC complexed with phosphoenolpyruvate (PEP) reveals that the side chains of Arg-396, Arg-581 and Arg-713 could interact with PEP

Directional linearly polarized terahertz emission from argon clusters irradiated by noncollinear double-pulse beams

It has been demonstrated that the interaction between argon clusters and intense femtosecond double laser pulses with appropriate intervals in time and space provides important properties for terahertz electromagnetic wave generation, namely, high forward directivity, power enhancement, and linear polarization with a variable direction. Irradiating argon clusters with double pulses (1 and 3 mJ, 40 fs, 810 nm) in 133-ps and 40-μm intervals results in terahertz wave emission in the forward direction that is 10 times greater than that for a single pulse. The polarization direction of terahertz electromagnetic waves can be varied by changing the relative focal positions of the first and second pulses