Hang Liu Fei Wu
Keiji GOTO Toru KAWANO Ryohei NAKAMURA
Takahiro SASAKI Yukihiro KAMIYA
Xiang XIONG Wen LI Xiaohua TAN Yusheng HU
Anton WIDARTA
Hiroshi OKADA Mao FUKINAKA Yoshiki AKIRA
Shun-ichiro Ohmi
Tohgo HOSODA Kazuyuki SAITO
Shohei Matsuhara Kazuyuki Saito Tomoyuki Tajima Aditya Rakhmadi Yoshiki Watanabe Nobuyoshi Takeshita
Koji Abe Mikiya Kuzutani Satoki Furuya Jose A. Piedra-Lorenzana Takeshi Hizawa Yasuhiko Ishikawa
Yihan ZHU Takashi OHSAWA
Shengbao YU Fanze MENG Yihan SHEN Yuzhu HAO Haigen ZHOU
Ryo KUMAGAI Ryosuke SUGA Tomoki UWANO
Jun SONODA Kazusa NAKAMICHI
Kaiji Owaki Yusuke Kanda Hideaki Kimura
Takuya FUJIMOTO
Yuji Wada
Fuyuki Kihara Chihiro Matsui Ken Takeuchi
Keito YUASA Michihiro IDE Sena KATO Kenichi OKADA Atsushi SHIRANE
Tomoo Ushio Yuuki Wada Syo Yoshida
Futoshi KUROKI
Jun FURUTA Shotaro SUGITANI Ryuichi NAKAJIMA Takafumi ITO Kazutoshi KOBAYASHI
Yuya Ichikawa Ayumu Yamada Naoko Misawa Chihiro Matsui Ken Takeuchi
Ayumu Yamada Zhiyuan Huang Naoko Misawa Chihiro Matsui Ken Takeuchi
Yoshinori ITOTAGAWA Koma ATSUMI Hikaru SEBE Daisuke KANEMOTO Tetsuya HIROSE
Hikaru SEBE Daisuke KANEMOTO Tetsuya HIROSE
Zhibo CAO Pengfei HAN Hongming LYU
Takuya SAKAMOTO Itsuki IWATA Toshiki MINAMI Takuya MATSUMOTO
Koji YAMANAKA Kazuhiro IYOMASA Takumi SUGITANI Eigo KUWATA Shintaro SHINJO
Minoru MIZUTANI Takashi OHIRA
Katsumi KAWAI Naoki SHINOHARA Tomohiko MITANI
Baku TAKAHARA Tomohiko MITANI Naoki SHINOHARA
Akihiko ISHIWATA Yasumasa NAKA Masaya TAMURA
Atsushi Fukuda Hiroto Yamamoto Junya Matsudaira Sumire Aoki Yasunori Suzuki
Ting DING Jiandong ZHU Jing YANG Xingmeng JIANG Chengcheng LIU
Fan Liu Zhewang Ma Masataka Ohira Dongchun Qiao Guosheng Pu Masaru Ichikawa
Ludovico MINATI
Minoru Fujishima
Hyunuk AHN Akito IGUCHI Keita MORIMOTO Yasuhide TSUJI
Kensei ITAYA Ryosuke OZAKI Tsuneki YAMASAKI
Akira KAWAHARA Jun SHIBAYAMA Kazuhiro FUJITA Junji YAMAUCHI Hisamatsu NAKANO
Seiya Kishimoto Ryoya Ogino Kenta Arase Shinichiro Ohnuki
Yasuo OHTERA
Tomohiro Kumaki Akihiko Hirata Tubasa Saijo Yuma Kawamoto Tadao Nagatsuma Osamu Kagaya
Haonan CHEN Akito IGUCHI Yasuhide TSUJI
Keiji GOTO Toru KAWANO Munetoshi IWAKIRI Tsubasa KAWAKAMI Kazuki NAKAZAWA
Shinichiro KOBA Moriaki UCHIYA Akio NAKAO Satoru HIGO Iwazo KAWANO Tetsuya OGUSHI
The barrier-layer was successfully fabricated for a preparation of tunneling junction using high Tc oxidesuperconductor such as Bi-Sr-Ca-Cu-O system. Bi2Sr2Ca2Cu3Ox films were used for both superconducting electrodes and the barrier was mainly Bi2Sr2CaCu2O and the rest that was formed by effects of de-calcium from the first sputtered (2223) film. The reaction of de-calcium occurred immersing it in carbonated water. The change of (2223) phase of BSCCO was confirmed with a comparison of the intensity of X-ray diffraction. The superconductive transition temperature of the junction is different from that of the single film (2223) which had no treatment with carbonated water. Zero-bias-currents through fabricated barrier are observed and the critical currents depend on temperature so far as measured temperature region of 79 K-72 K.
Akio KAWABATA Tadayuki KOBAYASHI Kouichi USAMI Toshinari GOTO
A sputtering system using dc hollow cathode discharge was developed for the propose of high Tc superconducting devices. Using this system, as-grown superconducting thin films of YBCO have been formed on MgO and SrTiO3 substrates. Influence of the sputtering conditions such as the substrate temperature and discharge gas pressure on the Tc and lattice parameter was investigated. It was found that superconducting films on MgO with Tc・zero higher than 87 K ere routinely obtained at the pressure of 820 mTorr (5%O2) and substrate temperature of 700
Katsuro OKUYAMA Shigetoshi OHSHIMA Hiroaki UENISHI Shiro KAMBE
Amorphous films of YBCO and BSCCO (2212) sputtered on MgO substrate were crystallized using zonemelt technique. For YBCO films, thin Ag intermediate layer was found to be effective in enhancing crystal growth and preferred orientation. Zone-melted BSCCO films included both (2201) phase and Cu(Sr, Ca)O2 in a form of dendritic crystallites. Tc's obtained for YBCO and BSCCO films were 70 and 75 K, respectively.
Kazuo SAKAI Shinji MIGITA Hiroyuki OTA Hiroshi OTERA Ryozo AOKI
Bi2Sr2CuOx (Bi(2201)) thin films have been fabricated by atomic layer-by-layer deposition using ion beam sputtering (IBS) method. During the deposition, 14 wt%-ozone/oxygen mixture gas of typical pressure of 5.0
Mitsuhiko OGIHARA Fumihiko TODA Takehiko MAKITA Hitoshi ABE
The (100) oriented BaxRb1-xBiO3 (BRBO) thin films were prepared on MgO (100) and SrTiO3(100) (STO(100)) substrate by molecular beam epitaxy using distilled ozone. The (100)-oriented BRBO thin film deposited on STO(100) substrate, showed onset superconducting transition temperature (Tc(onset)) value of 28 K and zero-resistance superconducting transition temperature (Tc(0)) value of 26 K. The respective values for Tc(onset) and Tc(0) of BRBO thin film on MgO(100) substrate were 21 K and 19 K. The growth process of the BRBO thin films grown on MgO(100) and STO(100) substrates were studied by the atomic force microscope (AFM) and the X-ray photoelectron spectroscopy (XPS). Difference in XPS-intensity of Ba as a function of the average thickness for the BRBO thin films deposited on STO(100) substrate and on MgO(100) substrate were observed. The electrical properties of junction using the BRBO thin film and the Nb-doped STO substrate (BRBO/STO(Nb)) was also investigated. The results of the current-voltage measurement and the capacitance-voltage measurement revealed that it is not necessary to take into account the unknown dielectric layer at the interface of BRBO/STO (Nb). It was not possible to interpret well the resistance-temperature behavior of Rb-doped-BaBiO3 thin film (semiconducting BBO(Rb) thin film) with the help of hopping model.
Isao SHIME Shiro KAMBE Shigetoshi OHSHIMA Katsuro OKUYAMA
Structure and resistivity of BaBiOy were compared with those of Ba1-xLaxBiO3. Decrease in an average Bi valence from 3.91 to 3.03 for BaBiOy leads to an increase in the lattice parameter c from 4.37
Kazuya KINOSHITA Syuuji ARISAKA Takeshi KOBAYASHI
We have fabricated bi-epitaxial grain boundary junctions in YBa2Cu3O7
A YBCO/CeO2/Au MIS structure (YBCO:YBa2Cu3O7
Tadashi IMAI Takaaki SAKAKIBARA Yoshio KOBAYASHI
In order to explain the temperature and frequency characteristics of high-Tc superconductors, a new model is proposed, which will be called the improved three-fluid model, where the momentum relaxation time τ is assumed to depend on temperature in the superconducting and normal states, respectively, although τ has been assumed to be independent of temperature for the conventional three-fluid model. According to this model, the complex conductivity
Kumiko IMAI Hironori MATSUBA Peter SPEAR Alistair FIFE
Bi2Sr2Ca1Cu2Ox thick film superconducting shields have been fabricated for use with HTc SQUIDs. Shielding factors and internal noise levels of the shields were measured using a DC SQUID magnetometer. A sample in which BSCCO was coated on the outside of a cylindrical Ag substrate exhibited larger noise levels than that with a sample in which BSCCO was coated on the inside of the Ag cylinder. The difference is explained by the thermally driven (Johnson) noise from the Ag substrate. A sample with the Ag cylinder outside the superconductor and samples with MgO substrates inside the superconductor showed good performance with a shielding factors of 10-8 and internal noise levels which did not exceed the DC SQUID magnetometer resolution (
Keiji YOSHIDA Noriaki HORIGUCHI Yutaka KANDA
Microwave characteristics of a LiNbO3 optical modulator employing superconductor electrodes (Pb-In-Au) as a transmission line of a traveling signal has been studied experimentally in the temperature range from 300 K to 4.2 K. At frequencies between 8 GHz and 12 GHz it is shown that the obtained modulation efficiency increases as expected from theory when the superconductor undergoes the transition from a normal state to a superconducting state. The present results dumonstrate the possible applications of superconducting electrodes to high performance LiNbO3 optical modulators.
Yoshinao MIZUGAKI Koji NAKAJIMA Tsutomu YAMASHITA
The threshold characteristics of mutually coupled SQUIDs (Superconducting Quantum Interference Devices) have been analytically and numerically investigated. The mutually coupled SQUIDs investigated is composed of an rf-SQUID and a dc-SQUID. Here, the rf-SQUID is a flux quantum generator and the dc-SQUID is a flux detector. The linearization method substituting sin-1x by (π/2)x (
Nojima and Fujita have found a universal relation, irrespective of temperatures T, between the reduced field h
In order to investigate the characteristics of the superconducting gap structures of BSCCO oxide superconductor, tunneling spectrum measurements were carried out with several junctions on the bulk single crystal surfaces. Point contact tunneling studies by means of the M/I/S and S/(I)/S junctions have shown the reproducible gap values, 2Δ (//c-axis) of 40
Ryozo AOKI Hironaru MURAKAMI Tetsuro NAKAMURA
The Cooper pairing interaction in high Tc oxide superconductor is discussed in terms of an empirical expression; Tc
Shigeru YOSHIMORI Wataru NAKAHAMA Mitsuo KAWAMURA
Experimental results of an N-S junction and analysis of the results using the Arnold theory were reported. Au and Pb were employed as a normal metal and a superconducting material, respectively. The excess current effect due to the Andreev reflection was observed in the current-voltage characteristics of an N-S junction whose normal resistance was 1.603 Ω. The excess current at 4.62 K was about 0.7 mA when the applied voltage was 2 mV. The barrier height and width were estimated to be 1.0169 eV and 0.7
Takakuni DOUSEKI Kazuo AOYAMA Yasuhisa OMURA
This paper describes the dependence of the delay time of a CMOS/SIMOX inverter on the gate-overlap capacitance. An analytical delay-time equation for the CMOS/SIMOX inverter, which includes the gate-overlap capacitance, is derived. This equation shows that the feed-forward effect dominates the characteristics of inverters with a small fanout. The validity of the delay-time equation is confirmed by the comparison to experimental measurements of 0.4-µm CMOS/SIMOX devices. Moreover, a sensitivity analysis shows that it is very important to reduce the gate-drain overlap capacitance for fabricating high-speed scaled-down CMOS/SIMOX devices.
Masashi HOTTA Masahiro GESHIRO Shinnosuke SAWA
The beam propagation method (BPM) is a powerful and manageable method for the analysis of wave propagation along weakly guiding optical waveguides. However, the effects of reflected waves are not considered in the original BPM. In this paper, we propose two simple modifications of the BPM to make it relevant in characterizing waveguide discontinuities at which a significant amount of reflection is expected to be observed. Validity of the present modifications is confirmed by the numerical results for the slab waveguide discontinuities and the butt-joints between different slab waveguides which either support the dominant mode or higher order modes.
Xue Jun MENG Naomichi OKAMOTO Okihiro SUGIHARA
Properties of a strongly-coupled nonlinear directional coupler (NLDC) with a lossy MQW coupling layer is analyzed using the Galerkin finite element method accompanied by a predictor-corrector algorithm. It is shown that the propagation attenuation along the NLDC is considerably smaller than that in the bulk MQW and tends to reduce with the input power. By the presence of losses, the powers guided in two waveguides do not become a maximum and a minimum at the same propagation length, unlike the lossless coupler. The losses make the nonlinear effect weak due to the decrease in guided power, and hence the coupling length decreases and the switching power increases. The extinction ratio of the switching becomes the largest value not in the cases of nonloss and high losses but in the case of moderately high losses, although the switching power is somewhat larger than that of the lossless case.
Masashi HOTTA Masahiro GESHIRO Katsuaki KANOH Haruo KANETAKE
Power transmission properties are investigated for a butt-joint which contains an air gap between an isotropic planar waveguide and an anisotropic one whose optical axis is lying in the plane defined by the propagation axis and the normal of the waveguide surface. New transmission coefficients are introduced for estimating the optical-power which is launched out into the gap from the incoming waveguide. Wave propagation through the gap is analyzed on the basis of the BPM concept. And the power transmitted across the interface between the gap and the outgoing waveguide is evaluated by means of the overlap integral of the field profiles. The effects of the air gap and the refractive index of filling liquid as well as axial displacement and angular misalignment are discussed on the basis of numerical results.