Mitsue Takahashi

Dr. Mitsue Takahashi

orcid

Research Focus & Metrics

Academic Career Length

30Years (1997-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 March 2006 in Journal of Applied Physics
Verified
Journal Article
Closed access
CWCan Wang
Can Wang
MTMitsue Takahashi
Mitsue Takahashi
HFHidetoshi Fujino
Hidetoshi Fujino
XZXia Zhao
Xia Zhao
EKEiji Kume
Eiji Kume
SSShigeki Sakai
Shigeki Sakai
Thin films of multiferroic (Bi0.6Tb0.3La0.1)FeO3 were grown on Pt∕Ti∕SiO2∕Si substrate under various oxygen pressures by pulsed laser deposition technique. X-ray diffraction patterns show that the crystallinity of the thin film is improved with decreasing depositing oxygen pressure and the thin film grown at a lower oxygen pressure of 0.01torr exhibits a single perovskite phase with preferred (001) orientation. Leakage current of the as-deposited thin films decreases with decreasing grown oxygen pressure. Significantly, the leakage current of the thin films can be reduced largely by an annealing process at 800°C with flowing oxygen. The annealed thin films show a relatively high resistivity and stable polarization loops with double remnant polarization of about 3μC∕cm2. The conduction properties of the thin films have been well analyzed, and it is indicated that the dominant conduction mechanism is the space-charge-limited conduction for the thin film grown at higher oxygen pressure and the Poole-Frenkel conduction for the thin films grown at lower oxygen pressure.

1 June 2005 in Japanese Journal of Applied Physics
Verified
Journal Article
Closed access
MTMitsue Takahashi
Mitsue Takahashi
SSShigeki Sakai
Shigeki Sakai
Self-aligned-gate Pt/SrBi2Ta2O9/HfAlO/Si metal/ferroelectric/insulator/semiconductor (MFIS) field-effect transistors (FETs) were fabricated. Drain current (I d) versus gate voltage curves of the MFIS FETs showed almost the same steepness as that of a non-self-aligned-gate Pt/HfAlO/Si metal/insulator/semiconductor FET. Long retention times with large on- and off-state I d ratios were obtained for the MFIS FETs. The retention times more than 33 days with an on- and off-state I d ratio over 105 were demonstrated for the self-aligned-gate MFIS FET with a 2-µm-long and 80-µm-wide gate. This device showed the longest memory retention among all of the ferroelectric-gate FETs reported ever before.

18 November 2010 in Materials
Verified
Journal Article
Open access
PDF file
SSShigeki Sakai
Shigeki Sakai
MTMitsue Takahashi
Mitsue Takahashi
We have investigated ferroelectric-gate field-effect transistors (FeFETs) with Pt/SrBi2Ta2O9/(HfO2)x(Al2O3)1−x (Hf-Al-O) and Pt/SrBi2Ta2O9/HfO2 gate stacks. The fabricated FeFETs have excellent data retention characteristics: The drain current ratio between the on- and off-states of a FeFET was more than 2 × 106 after 12 days, and the decreasing rate of this ratio was so small that the extrapolated drain current ratio after 10 years is larger than 1 × 105. A fabricated self-aligned gate Pt/SrBi2Ta2O9/Hf-Al-O/Si FET revealed a sufficiently large drain current ratio of 2.4 × 105 after 33.5 day, which is 6.5 × 104 after 10 years by extrapolation. The developed FeFETs also revealed stable retention characteristics at an elevated temperature up to 120 °C and had small transistor threshold voltage (Vth) distribution. The Vth can be adjusted by controlling channel impurity densities for both n-channel and p-channel FeFETs. These performances are now suitable to integrated circuit application with nonvolatile functions. Fundamental properties for the applications to ferroelectric-CMOS nonvolatile logic-circuits and to ferroelectric-NAND flash memories are demonstrated.

1 November 1999 in Physical Review B
Verified
Journal Article
Closed access
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YHYuko Hosokoshi
Yuko Hosokoshi
YNYasuhiro Nakazawa
Yasuhiro Nakazawa
KIKatsuya Inoue
Katsuya Inoue
KTKohichi Takizawa
Kohichi Takizawa
HNHiroki Nakano
Hiroki Nakano
TGTsuneaki Goto
Tsuneaki Goto
Stable organic biradical crystals PNNNO, F2PNNNO, and PIMNO of the PNNNO family were synthesized. {PNNNO=2−[4′− (N−tert−butyl−N−oxyamino)phenyl]−4,4,5,5−tetramethyl−4,5−dihydro−1H−imidazol−1−oxyl 3−oxide, F2PNNNO=2−[2′,6′,−difluoro−4′−(N−tert−butyl−N−oxyamino)phenyl]−4,4,5,5−tetramethyl−4, 5−dihydro−1H−imidazol−1−oxyl 3−oxide, PIMNO=2−[4′−(N−tert−butyl−N−oxyamino)−phenyl]−4,4,5,5−tetramethyl−4,5−dihydro−1H−imidazol−1−oxyl.} PNNNO and PIMNO crystallize to form quasi-one-dimensional lattices, but F2PNNNO to form a quasi-two-dimensional lattice. The temperature dependences of the susceptibility and the high-field magnetization process up to 34 T were measured down to 0.5 K. The results are analyzed by comparing with the theoretical calculations based on the crystal structures. PNNNO and PIMNO are considered to be antiferromagnetic Heisenberg spin chains consisting of S=1/2 spin pairs (dimers) in which the two spins are coupled ferromagnetically. At low temperatures, an antiferromagnetic ordering occurs in these crystals, which is confirmed by the thermodynamic discussion through specific heat measurements. On the other hand, F2PNNNO is thought to be a two-dimensional Heisenberg system, in which the spin pairs are connected by two types of antiferromagnetic interactions. The ground state is singlet. The high-field magnetization process shows a two-step saturation with a plateau of the half value of the saturation magnetization.

15 November 2004 in Japanese Journal of Applied Physics
Verified
Journal Article
Closed access
SSShigeki Sakai
Shigeki Sakai
RIRajangam Ilangovan
Rajangam Ilangovan
MTMitsue Takahashi
Mitsue Takahashi

1 April 2001 in Japanese Journal of Applied Physics
Verified
Journal Article
Closed access
MTMitsue Takahashi
Mitsue Takahashi
HSHideki Sugiyama
Hideki Sugiyama
TNToshiyuki Nakaiso
Toshiyuki Nakaiso
KKKazushi Kodama
Kazushi Kodama
MNMinoru Noda
Minoru Noda
MOMasanori Okuyama
Masanori Okuyama
Retention characteristics of metal-ferroelectric-insulator-semiconductor (MFIS) structures have been studied theoretically by considering effects of charge injections derived from the difference between leakage current densities in the ferroelectric and insulator layers. The calculated curves for time-dependent capacitance have shown good agreements with experimental results. The numerical results for the MFIS structure have indicated that excess current over a certain value through the ferroelectric and the insulator layers causes the retention time to rapidly degrade. An idea of inserting an insulator film between the metal and the ferroelectric layers in an MFIS has also been examined in order to cut down the currents through the ferroelectric layer. The calculations based on our model have found this metal-insulator-ferroelectric-insulator-semiconductor (M-I-FIS) structure to exhibit much longer retention time than the conventional MFIS.