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Norio KATO
1988 Volume 57 Issue 2 Pages
173
Published: February 10, 1988
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Takayoshi KOBA-YASHL
1988 Volume 57 Issue 2 Pages
174-189
Published: February 10, 1988
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Shunsuke OHTANI
1988 Volume 57 Issue 2 Pages
190-203
Published: February 10, 1988
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Hisao NAKASHIMA, Toshiaki FUKUNAGA
1988 Volume 57 Issue 2 Pages
204-208
Published: February 10, 1988
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Ken-ichi TANAKA, Taro YAMADA
1988 Volume 57 Issue 2 Pages
209-215
Published: February 10, 1988
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Norihiko KAMATA, Hisashi KATAHAMA, Kikuo KOBAYASHI, Takeo SUZUKI
1988 Volume 57 Issue 2 Pages
216-220
Published: February 10, 1988
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Takashi HIRAO, Kentaro SETSUNE, Kiyotaka WASA
1988 Volume 57 Issue 2 Pages
221-226
Published: February 10, 1988
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Toshiaki MURAKAMI, Youichi ENOMOTO, Minoru SUZUKI
1988 Volume 57 Issue 2 Pages
227-231
Published: February 10, 1988
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Koichiro SAM, Koji ANDO, Yasuhiro SATO, Atsushi KOMA, Tanemasa ASANO
1988 Volume 57 Issue 2 Pages
232-234
Published: February 10, 1988
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Tadaki MIYOSHI, Yasunori MATSUDA
1988 Volume 57 Issue 2 Pages
235-240
Published: February 10, 1988
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Young L. KUK, Toshio SAKURAI
1988 Volume 57 Issue 2 Pages
247-248
Published: February 10, 1988
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Katsumichi YAGI
1988 Volume 57 Issue 2 Pages
249-250
Published: February 10, 1988
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Itaru KAMIYA
1988 Volume 57 Issue 2 Pages
251-252
Published: February 10, 1988
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Takashi TSUNO, Takashi AIZAWA, Hiroshi DAIMON, Shozo INO
1988 Volume 57 Issue 2 Pages
253-254
Published: February 10, 1988
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Tomihiro HASHIZUME, Toshio SAKURAI
1988 Volume 57 Issue 2 Pages
255-256
Published: February 10, 1988
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Tornihiro HASHIZUME
1988 Volume 57 Issue 2 Pages
257-258
Published: February 10, 1988
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Toshio TAKAHASHI
1988 Volume 57 Issue 2 Pages
259-260
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Akira SAKAI
1988 Volume 57 Issue 2 Pages
261-262
Published: February 10, 1988
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Takanori UCHIYAMA, Makoto SAKATA
1988 Volume 57 Issue 2 Pages
263-269
Published: February 10, 1988
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The maximum entropy method (MEM) was applied to the free induction decay (FID) signal data by a Fourier transform NMR spectrometer to estimate super-resolved spectra. For
31P NMR spectra of the phosphate solution, the chemical shifts by the MEM agreed with those by FFT. For higher plant cells (mung bean root tips), the resolution of
31P NMR spectra by the MEM was more highly resolved than that by FFT. Moreover, the MEM estimation gave consistent cytoplasmic pH from Pi and G-6-P chemical shifts, but FFT did not. From the FID for one fifth of the usual accumulation time, we could also obtain intracellular pH accurately. Therefore, it is believed that the MEM will develop to be an important means in the
31P NMR study.
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Mitsuyoshi ONODA, Hiroshi NAKAYAMA, Kiyoshi AMAKAWA, Hal Bon GU, Katsu ...
1988 Volume 57 Issue 2 Pages
270-276
Published: February 10, 1988
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Thermally-stimulated currnt (TSC) in poly (p-phenylene vinylene) (PPV) and its doping effect were studied. TSC peak in undoped PPV is observed at around 60°C. The activation energy was evaluated as 0.5eV. In I
2-doped PPV, two TSC peaks (P
1, P
2) were observed. The P
1 peak moves to the low-temperature side upon increasing the I
2 concentration. The P
2 peak was observed in the same temperature range as the peak in undoped PPV. The activation energies were evaluated as 0.2 and 0.4eV for P
1 and P
2 peak, respectively, regardless of the amount of dopant. It is assumed that the P
1 peak originates from electron traps formed by the effect of doped I
2 molecules. Moreover, it is considered that the localized center of the peak for undoped PPV and the P
2 peak for I
2-doped PPV is due to defects originally existing in PPV.
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Toshiyuki NAKAJIMA, Toshiko OTSUKI
1988 Volume 57 Issue 2 Pages
277-280
Published: February 10, 1988
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A radiation dosimeter has been developed by observing the free radicals created in sucrose. The free radicals were observed by using the electron spin resonance (ESR) equipment of JES-PE-1X type. ESR absorption due to the free radical in sucrose appeared at the magnetic field between the third and fourth ESR ones of the standard Mn
+2 sample. Hardly any fading of free radicals in sucrose was observable even two months after irradiation. Sucrose as a radiation dosimeter can linearly measure the dose from 4×10
-2Gy to 10
5Gy. If the new model of the ESR equipment is used and ESR observation is carried out at lower temperatures such as liquid nitrogen or liquid helium temperature, the sucrose ESR dosimeter will be able to detect about 1mGy or less of the dose.
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