results the simulation results showed that the penetration depth and temperature rise of 980 nm wavelengths were different from those of 1064 nm wavelength. it appeared that 1064 nm wavelength penetrated to deeper layers of tissue compared with 980 nm. moreover, temperature rise during 1064 nm irradiation led to temperature increase in allowable ranges. the findings proved the reason why 1064 n...

Department of Advanced Preventive Medicine for Infectious Disease, Tohoku University Graduate School of Medicine, Sendai, 980-8575 Japan; Institute of Tropical Medicine, Nagasaki University, Nagasaki, 852-8523 Japan; Department of Thoracic Surgery, Department of Anesthesiology, Tohoku University School of Medicine, Sendai, 980-8575 Japan; Department of Infection Control and Laboratory Diagnosti...

1 Research Institute of Electrical Communication, Tohoku University, 2-1-1 Katahira, Aoba-ku, 980-8577 Sendai, Japan 2 Institute of Fluid Science, Tohoku University, 2-1-1 Katahira, Aoba-ku, 980-8577 Sendai, Japan Advanced Institute of Materials Research, Tohoku University, 2-1-1 Katahira, Aoba-ku, 980-8577 Sendai, Japan Microsystems Technology Laboratories, Massachusetts Institute of Technolog...

..................................................................................................................................................... 367 INTRODUCTION .............................................................................................................................................. 367 PAX GENES, PAIRED DOMAINS AND PAX HOMEODOMAINS .......................................

1 Department of Applied Chemistry, Graduate School of Engineering, Tohoku University, 6-6-11-1302 Aoba, Aramaki, Aoba-ku, Sendai, 980-8579. Japan 2 PRESTO, Japan Science and Technology Agency. 4-1-8 Honcho, Kawaguchi, Saitama 332-0012. Japan 3 Biomedical Engineering Research Organization, Tohoku University, Aoba-ku, Sendai, 980-8579, Japan 4 New Industry Creation Hatchery Center (NICHe), Tohoku...

From the amplitude analysis of $D^+_s \to \pi^+ \pi^0 \eta$ decay, BESIII Collaboration firstly observed a_0(980)^+\pi^0$ and a_0(980)^0\pi^+$ decay modes, which are expected to occur through pure $W$-annihilation processes. The measured branching fraction $\mathcal{B}[D_{s}^{+}\to a_{0}(980)^{+(0)}\pi^{0(+)},a_{0}(980)^{+(0)}\to \pi^{+(0)}\eta]$ is, however, found be larger than those known de...

From the amplitude analysis of $D^+_s \to \pi^+ \pi^0 \eta$ decay, BESIII Collaboration firstly observed a_0(980)^+\pi^0$ and a_0(980)^0\pi^+$ decay modes, which are expected to occur through pure $W$-annihilation processes. The measured branching fraction $\mathcal{B}[D_{s}^{+}\to a_{0}(980)^{+(0)}\pi^{0(+)},a_{0}(980)^{+(0)}\to \pi^{+(0)}\eta]$ is, however, found be larger than those known de...

Motivated by the measurements of branching fractions quasi-two-body decays ${B}^{0}\ensuremath{\rightarrow}{K}^{*0}({f}_{0}(980)\ensuremath{\rightarrow}){\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$ and ${B}^{0}\ensuremath{\rightarrow}{\ensuremath{\rho}}^{0}({f}_{0}(980)\ensuremath{\rightarrow}){\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$, we study charmless $B\ensure...