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Journal Articles

Direct energy conversion using Ni/SiC Schottky junction in $$^{237}$$Np and $$^{241}$$Am gamma ray regions

Fukuda, Tatsuo; Kobata, Masaaki; Shobu, Takahisa; Yoshii, Kenji; Kamiya, Junichiro; Iwamoto, Yosuke; Makino, Takahiro*; Yamazaki, Yuichi*; Oshima, Takeshi*; Shirai, Yasuhiro*; et al.

Journal of Applied Physics, 132(24), p.245102_1 - 245102_8, 2022/12

 Times Cited Count:1 Percentile:4.34(Physics, Applied)

Direct energy conversion has been investigated using Ni/SiC Schottky junctions with the irradiation of monochromatized synchrotron X-rays simulating the gamma rays of $$^{237}$$Np (30 keV) and $$^{241}$$Am (60 keV). From current-voltage measurements, electrical energies were obtained for both kinds of gamma rays. The energy conversion efficiencies were found to reach up to $$sim$$1.6%, which is comparable to those of a few other semiconducting systems reported thus far. This result shows a possibility of energy recovery from nuclear wastes using the present system, judging from the radiation tolerant nature of SiC. Also, we found different conversion efficiencies between the two samples. This could be understandable from hard X-ray photoelectron spectroscopy and secondary ion mass spectroscopy measurements, suggesting the formation of Ni-Si compounds at the interface in the sample with a poor performance. Hence, such combined measurements are useful to provide information that cannot be obtained by electrical measurements alone.

Journal Articles

Bromine-isotope selective ionization using field-free alignment of IBr isotopologues with a switched nanosecond laser pulse

Akagi, Hiroshi*; Kumada, Takayuki; Otobe, Tomohito*; Itakura, Ryuji*; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

Chemistry Letters, 49(4), p.416 - 418, 2020/04

 Times Cited Count:1 Percentile:2.92(Chemistry, Multidisciplinary)

Journal Articles

Isotope-selective ionization utilizing field-free alignment of isotopologues using a switched nanosecond laser pulse

Akagi, Hiroshi*; Kumada, Takayuki; Otobe, Tomohito*; Itakura, Ryuji*; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

Applied Physics B, 124(1), p.14_1 - 14_8, 2018/01

 Times Cited Count:2 Percentile:11.77(Optics)

We propose and numerically simulate a method of laser isotope separation based on field-free alignment of isotopologues, utilizing an intense switched nanosecond (ns) laser field which is slowly turned on and rapidly turned off at the peak with the falling time of 200 fs. The femtosecond (fs) laser induced alignment of molecules including a heavy atom is severely disturbed by ionization because of their small ionization potential. Our simulations for I$$^{79}$$Br and I$$^{81}$$Br isotopologues demonstrate that the switched ns laser field can make isotopologues well-aligned with the reduced ionization probability at the laser intensity which is an order-of-magnitude lower than a typical intensity for field-free alignment induced by a fs laser field.

Journal Articles

Isotope-selective ionization utilizing field-free alignment of isotopologues with a train of femtosecond laser pulses

Akagi, Hiroshi; Kasajima, Tatsuya*; Kumada, Takayuki; Itakura, Ryuji; Yokoyama, Atsushi; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

Physical Review A, 91(6), p.063416_1 - 063416_7, 2015/06

 Times Cited Count:9 Percentile:42.07(Optics)

We propose a strategy of isotope-selective ionization for a binary mixture of isotopologues of homonuclear diatomic molecules, utilizing field-free alignment with a train of femtosecond laser pulses. Field-free alignment can be achieved simultaneously for two isotopologues consisting of two atoms with the same atomic mass number $$alpha$$ or $$beta$$, utilizing a pulse train with their time interval of T$$_{com}$$ = $$beta$$ T($$alpha$$) = $$alpha$$ T($$beta$$), where T($$alpha$$) and T($$beta$$) are the rotational revival times of the isotopologues. We demonstrate experimentally that a train of four alignment pulses with their interval of T$$_{com}$$ ($$alpha$$ = 14, $$beta$$ = 15) creates transiently aligned $$^{14}$$N$$_{2}$$ and anti-aligned $$^{15}$$N$$_{2}$$ just before T$$_{com}$$/2 after the last pulse, and vice versa just after T$$_{com}$$/2. Highly isotope-selective N$$_{2}$$ ionization is achieved at these timings with another femtosecond laser pulse, which induces the non-resonant multiphoton ionization with the cross section remarkably depending on the angle between the molecular axis and the laser electric field direction. The ion yield ratio I($$^{15}$$N$$_{2}$$$$^{+}$$)/I($$^{14}$$N$$_{2}$$$$^{+}$$) ranges from 0.49 to 2.00, which is wider than the range obtained with single alignment pulse.

Journal Articles

Ion effects on the structure of water studied by terahertz time-domain spectroscopy

Kondo, Masato; Oshima, Yasuhiro*; Tsubouchi, Masaaki

Chemical Physics Letters, 591, p.317 - 322, 2014/01

 Times Cited Count:60 Percentile:88.39(Chemistry, Physical)

We have investigated dielectric relaxation in aqueous ionic solutions by terahertz time-domain spectroscopy to elucidate the ionic hydration effect on the water structure. In the low frequency region ($$<$$ 1.0 THz), the dielectric spectra decreased in amplitude with decreasing size of dissolved cations, which indicates the deceleration effect of water within the hydration shell. On the other hand, in the high frequency region (1.0-1.8 THz), the spectra increased in amplitude as compared to that of pure water. This finding indicates dissolved ions weaken the hydrogen bonding of water in ionic solution and induce the structure breaking effect beyond the hydration shell.

Journal Articles

Isotope-selective ionization utilizing molecular alignment and non-resonant multiphoton ionization

Akagi, Hiroshi; Kasajima, Tatsuya; Kumada, Takayuki; Itakura, Ryuji; Yokoyama, Atsushi; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

Applied Physics B, 109(1), p.75 - 80, 2012/10

 Times Cited Count:17 Percentile:60.23(Optics)

We demonstrate a laser nitrogen isotope separation, which is based on field-free alignment and angular dependent ionization of $$^{14}$$N$$_{2}$$ and $$^{15}$$N$$_{2}$$ isotopomers. A linearly-polarized short laser pulse ($$lambda$$$$sim$$795 nm, $$Delta$$$$tau$$$$sim$$60 fs) creates rotational wave packets in the isotopomers, which periodically revive with different revival times as a result of different moments of inertia. Another linearly-polarized short laser pulse ($$lambda$$$$sim$$795 nm, $$Delta$$$$tau$$$$sim$$60 fs) ionizes one of the isotopomers selectively as a result of their different angular distributions. In the present experiments, the ion yield ratio $$R$$ [= $$I$$($$^{15}$$N$$_{2}$$$$^{+}$$)/$$I$$($$^{14}$$N$$_{2}$$$$^{+}$$)] can be changed in the range from 0.85 to 1.22, depending on the time delay between the two laser pulses.

Journal Articles

Terahertz tomography of a photo-induced carrier based on pump-probe spectroscopy using counterpropagation geometry

Tsubouchi, Masaaki; Nagai, Masaya*; Oshima, Yasuhiro*

Optics Letters, 37(17), p.3528 - 3530, 2012/09

 Times Cited Count:20 Percentile:65.20(Optics)

A novel technique for the terahertz (THz) tomography of a photo-induced carrier that is based on optical-pump THz-probe time-resolved reflection spectroscopy using counter-propagation geometry of the pump and probe pulses has been proposed. Transient reflection due to the photo-induced carrier provides information about the physical properties and spatial distribution separately. We have experimentally demonstrated this method using a silicon wafer. The obtained complex reflection can be reproduced by the exact solution of Maxwell's equations, assuming an exponential distribution of the photo-induced carrier density.

Journal Articles

Coherent correlation between nonadiabatic rotational excitation and angle-dependent ionization of NO in intense laser fields

Itakura, Ryuji; Hasegawa, Hirokazu*; Kurosaki, Yuzuru; Yokoyama, Atsushi; Oshima, Yasuhiro*

Journal of Physical Chemistry A, 114(42), p.11202 - 11209, 2010/07

 Times Cited Count:13 Percentile:38.30(Chemistry, Physical)

When neutral NO molecules are partly ionized in intense laser fields ($$I$$$$_{0}$$ $$>$$ 35 TW/cm$$^{2}$$), a hole in the rotational wave packet of the remaining neutral NO is created by the ionization, whose rate depends on the alignment angle of the molecular axis with respect to the laser polarization direction. Rotational state distributions of NO are experimentally observed and then the characteristic feature that the population at higher $$J$$ levels is increased by the ionization can be identified. Numerical calculation for solving time-dependent rotational Schrodinger equations including the effect of the ionization is carried out. The numerical results suggest that NO molecules aligned perpendicular to the laser polarization direction are dominantly ionized at the peak intensity of $$I$$$$_{0}$$ = 42 TW/cm$$^{2}$$, where the multiphoton ionization is preferred rather than the tunneling ionization.

Journal Articles

Phase transformation of Mg-Fe alloys

Yoneda, Yasuhiro; Abe, Hiroshi; Oshima, Takeshi; Uchida, Hirohisa*

Journal of Applied Physics, 107(9), p.093505_1 - 093505_6, 2010/05

 Times Cited Count:9 Percentile:32.50(Physics, Applied)

An Mg-Fe alloy system prepared through mechanical alloying was structurally analyzed. Mechanical alloying can produce single-phase bcc alloys using Mg concentrations up to about 15 mol%. Use of conventional average structure analysis and X-ray pair-distribution function method enabled the long-range and short-range order structures of the Mg-Fe alloys to be bridged. The substituted Mg atoms were randomly arranged in the low-Mg composition but started to have an order structure. The partially ordered Mg-Fe alloy undergoes an austenitic (cubic) to martensitic (orthorhombic) phase change, as increasing Mg composition.

Journal Articles

Ion-irradiation effects of hydrogen absorption in palladium metal

Yoneda, Yasuhiro; Tamura, Kazuhisa; Abe, Hiroshi; Oshima, Takeshi; Morimoto, Ryo*; Uchida, Hirohisa*; Mizuki, Junichiro

Transactions of the Materials Research Society of Japan, 33(4), p.1053 - 1056, 2008/12

The effect of ion irradiation on palladium (Pd) metal was investigated by hydrogen-absorption measurements, SEM microscopy and synchrotron X-ray diffraction. N$$^+$$ irradiation was made with an acceleration energy 350 keV. The initial hydrogen absorption rate of the irradiated Pd was three times larger than that of non-irradiated Pd. The microscopic structure was investigated by using the pair-distribution function (PDF) obtained by X-ray diffraction. Although the average structure of the Pd was f.c.c, the Pd atoms displaced and two occupancy sites are revealed. This site occupancy is closely related with the hydrogen-absorption rate.

Journal Articles

Analysis methods of inorganic C-14 in air and river water using an AMS

Amano, Hikaru; Yamamichi, Miwako*; Baba, Masami*; Momoshima, Noriyuki*; Sugihara, Shinji*; Ueda, Yusuke*; Nakamura, Yasuhiro*

JAEA-Conf 2008-003, p.84 - 87, 2008/04

no abstracts in English

Journal Articles

Local modification of hardness in FeCu alloys by using swift heavy ion irradiation

Nakagawa, Sho*; Hori, Fuminobu*; Chimi, Yasuhiro; Ishikawa, Norito; Kitagawa, Michiharu*; Oshima, Ryuichiro*; Tobita, Toru; Taniguchi, Ryoichi*; Suzuki, Masahide; Iwase, Akihiro*

Nuclear Instruments and Methods in Physics Research B, 257(1-2), p.397 - 401, 2007/04

 Times Cited Count:5 Percentile:34.51(Instruments & Instrumentation)

Supersaturated Fe-1.2wt.%Cu alloys were irradiated with 200-MeV Xe and 200-MeV Au ions at elevated temperatures. To make an irradiated region and an unirradiated region in a specimen, a masking plate was put on the specimen during the irradiation. After the irradiation, the hardness was measured by using a conventional microhardness tester or a nano-indenter. We have found that the hardness only in irradiated region increases by the irradiation. The boundary of irradiated and unirradiated regions can be clearly identified by the difference in hardness. The present result implies that swift heavy ion irradiation can be used for the local modification of hardness in supersaturated alloys.

Oral presentation

Isotope selection using intense laser induced molecular alignment and angle-dependent ionization

Akagi, Hiroshi; Kasajima, Tatsuya*; Kumada, Takayuki; Itakura, Ryuji; Yokoyama, Atsushi; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

no journal, , 

We demonstrate the isotope selection with molecular alignment and angle-dependent ionization in intense laser fields. The 14-N2 and 15-N2 mixed gas is irradiated with a linearly polarized femtosecond laser pulse for creation of rotational wavepackets. After a certain delay when one of two isotopologues is aligned along the laser polarization direction, another linearly polarized femtosecond laser pulse is shined for ionization. It is confirmed that the ionization yield ratio between the two isotopologues can be changed as a function of the delay between the two laser pulses.

Oral presentation

Effect of ro-vibrational coupling on rotational wavepacket of N$$_{2}$$

Yokoyama, Atsushi; Akagi, Hiroshi; Kumada, Takayuki; Itakura, Ryuji; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

no journal, , 

Recently, we demonstrated a nitrogen isotope separation based on isotopically different time-evolution of rotational wavepacket by using $$^{14}$$N$$_{2}$$/$$^{15}$$N$$_{2}$$ mixture, in which at first rotational wavepackets of isotopomers were created by the irradiation of a femtosecond laser pulse, then a specific isotopomer molecules were ionized by another femtosecond laser pulse at the time when they align. In the experiment, we found peak shapes of the N$$_{2}$$$$^{+}$$ intensity were distorted as the evolution time passes. The behavior was not predicted by a rigid rotor model. In this work, we examined the effect of ro-vibrational coupling on this behavior by solving a time-dependent Schr$"o$dinger equation including the coupling. As a result, we elucidated that the simulation agreed well with the experimental results and that the effect of ro-vibrational coupling became larger as the rotational temperature increased.

Oral presentation

Laser isotope separation utilizing difference in molecular rotational period

Akagi, Hiroshi; Kasajima, Tatsuya*; Kumada, Takayuki; Itakura, Ryuji; Yokoyama, Atsushi; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

no journal, , 

We propose a laser isotope separation utilizing difference of molecular rotational period, and experimentally demonstrate the principle, showing isotope selective ionization of $$^{14}$$N$$_{2}$$ and $$^{15}$$N$$_{2}$$ isotopologues. A linearly-polarized short laser pulse creates rotational wave packets in the isotopologues, which periodically revive with different revival times as a result of different moments of inertia. Anotherlinearly-polarized short laser pulse ionizes one of the isotopologues preferentially, as a result of their differentangular distributions and angular dependence of ionization probability. In the present experiment, the ion yieldratio R [= I($$^{15}$$N$$_2^{+}$$)/I($$^{14}$$N$$_2^{+}$$)] has been changed in the range from 0.85 to 1.22, depending on the time delaybetween the two laser pulses.

Oral presentation

Isotope-selective rotational excitation with a sequence of femto-second laser pulses

Akagi, Hiroshi; Kasajima, Tatsuya*; Kumada, Takayuki; Itakura, Ryuji; Yokoyama, Atsushi; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

no journal, , 

We propose a laser isotope separation utilizing difference of molecular rotational period, and experimentally demonstrate the principle, showing isotope selective ionization of $$^{14}$$N$$_{2}$$ and $$^{15}$$N$$_{2}$$ isotopologues. A linearly-polarized short laser pulse creates rotational wave packets in the isotopologues, which periodically revive with different revival times as a result of different moments of inertia. Another linearly-polarized short laser pulse ionizes one of the isotopologues preferentially, as a result of their different angular distributions and angular dependence of ionization probability. In the present experiment, the ion yield ratio R [= I($$^{15}$$N$$_2^{+}$$)/I($$^{14}$$N$$_2^{+}$$)] has been changed in the range from 0.85 to 1.22, depending on the time delay between the two laser pulses.

Oral presentation

Improvement in selectivity of isotope-selective ionization utilizing molecular alignment and angular dependent ionization

Akagi, Hiroshi; Kasajima, Tatsuya*; Kumada, Takayuki; Itakura, Ryuji; Yokoyama, Atsushi; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

no journal, , 

We are demostrating isotope-selective ionization of $$^{14}$$N$$_{2}$$ and $$^{15}$$N$$_{2}$$ isotopologues, utilizing molecular alignment and angular dependent ionization. In the present work, we used a train of four identical pulses with 125.7-ps interval to creating rotational wave packets in these isotopologues. We optimized the following experimental conditions to improve the isotope selectivity: mixing ratio of the gas sample, timing of pulse valve to introduce the gas sample into a vacuum chamber, laser beam diameters for the alignment and ionization pulses, and these peak intensities. As the results, we obtained the minimum of the ion yield ratio $$^{15}$$N$$_{2}$$/$$^{14}$$N$$_{2}$$ (= 0.49) and the maximum (= 2.00).

Oral presentation

Isotope-selective ionization utilizing control of molecular rotation with femtosecond laser pulses; High selectivity with multiple pulse irradiation

Akagi, Hiroshi; Kasajima, Tatsuya*; Kumada, Takayuki; Itakura, Ryuji; Yokoyama, Atsushi; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

no journal, , 

We are demostrating isotope-selective ionization of $$^{14}$$N$$_{2}$$ and $$^{15}$$N$$_{2}$$ isotopologues, utilizing molecular alignment and angular dependent ionization. In the present work, we used a train of four identical pulses with 125.7-ps interval to creating rotational wave packets in these isotopologues. The ion yield ratio $$^{15}$$N$$_{2}$$/$$^{14}$$N$$_{2}$$ changed in the range from 0.49 to 2.00, which was two-times wider than that obtained with the single pulse.

Oral presentation

Molecular laser isotope separation without tunable lasers; Isotope-selective ionization of N$$_{2}$$ isotopologues using femtosecond laser-induced molecular alignment

Akagi, Hiroshi; Kasajima, Tatsuya*; Kumada, Takayuki; Itakura, Ryuji; Yokoyama, Atsushi; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

no journal, , 

We propose a laser isotope separation method without tunable lasers, and demonstrate isotope selective ionization of nitrogen isotopologues. This method is based on molecular alignment and angular dependent ionization. A non-resonant femtosecond (fs) laser pulse with a linear polarization creates rotational wave packets in the isotopologues. These wave packets periodically exhibit aligned and antialigned distributions at specific time delays. At a specific time delay when one isotopologue is aligned and the other one is anti-aligned, another non-resonant linearly-polarized fs laser pulse (ionization pulse) ionizes the aligned isotopologue preferentially via the non-resonant multiphoton ionization, because of angular dependence of the N$$_{2}$$ ionization probability. The ion yield ratio R [= I($$^{15}$$N$$_{2}$$) / I($$^{14}$$N$$_{2}$$)] depends on the time delay, ranging from 0.68 to 1.41.

Oral presentation

Isotope-selective ionization utilizing molecular alignment of N$$_{2}$$ isotopologues with a train of femtosecond laser pulses

Akagi, Hiroshi; Kasajima, Tatsuya*; Kumada, Takayuki; Itakura, Ryuji; Yokoyama, Atsushi; Hasegawa, Hirokazu*; Oshima, Yasuhiro*

no journal, , 

We propose a strategy of isotope-selective ionization for a binary mixture of isotopologues of homonuclear diatomic molecules, utilizing field-free alignment with a train of femtosecond laser pulses. Field-free alignment can be achieved simultaneously for two isotopologues consisting of two atoms with the same atomic mass number $$alpha$$ or $$beta$$, utilizing a pulse train with their time interval of T$$_{com}$$ = $$beta$$ T($$alpha$$) = $$alpha$$ T($$beta$$), where T($$alpha$$) and T($$beta$$) are the rotational revival times of the isotopologues. We demonstrate experimentally that a train of four alignment pulses with their interval of T$$_{com}$$ ($$alpha$$ = 14, $$beta$$ = 15) creates transiently aligned $$^{14}$$N$$_{2}$$ and anti-aligned $$^{15}$$N$$_{2}$$ just before T$$_{com}$$/2 after the last pulse, and vice versa just after T$$_{com}$$/2. Highly isotope-selective N$$_{2}$$ ionization is achieved at these timings with another femtosecond laser pulse, which induces the non-resonant multiphoton ionization with the cross section remarkably depending on the angle between the molecular axis and the laser electric field direction. The ion yield ratio I($$^{15}$$N$$_{2}$$$$^{+}$$)/I($$^{14}$$N$$_{2}$$$$^{+}$$) ranges from 0.49 to 2.00, which is wider than the range obtained with single alignment pulse.

46 (Records 1-20 displayed on this page)