Multilayered polycrystallization in single-crystal YSZ by laser-shock compression
Creators
- Nishimura, Yasuhiko1
- Kitagawa, Yoneyoshi1
- Mori, Yoshitaka1
- Ishii, Katsuhiro1
- Hanayama, Ryohei1
- Hioki, Tatsumi2
- Azuma, Hirozumi2
- Motohiro, Tomoyoshi2
- Kajino, Tsutomu2
- Nishi, Teppei2
- Komeda, Osamu3
- Kondo, Takuya3
- Fujine, Manabu3
- Sekine, Takashi4
- Sato, Nakahiro4
- Kurita, Takashi4
- Kawashima, Toshiyuki4
- Kan, Hirofumi4
- Sunahara, Atsushi5
- Miura, Eisuke6
- and others
- 1. The Graduate School for the Creation of New Photonics Industries, 1955-1 Kurematsu-cho, Nishi-ku, Hamamatsu, Shizuoka 431-1202 (Japan)
- 2. Toyota Central Research and Development Laboratories, Inc., 41-1 Yokomichi, Nagakute, Aichi 480-1192 (Japan)
- 3. Toyota Motor Corporation, 1200 Mishuku, Susono, Shizuoka 410-1193 (Japan)
- 4. Hamamatsu Photonics K.K., 1820 Kurematsu-cho, Nishi-ku, Hamamatsu, Shizuoka 431-1202 (Japan)
- 5. Institute for Laser Technology, 1-8-4 Utsubo-honmachi, Nishi-ku, Osaka 550-0004 (Japan)
- 6. The National Institute of Advanced Industrial Science and Technology, 1-1-1 Umezono, Tsukuba, Ibaraki 305-8568 (Japan)
Description
A single shot of an ultra-intense laser with 0.8 J of energy and a pulse width of 110 fs (peak intensity of W cm−2) is divided into two beams and the two beams counter-irradiated onto a 0.5 mm-thick single crystal yttria-stabilized zirconia (YSZ), changing the YSZ into a multilayered polycrystalline state. The laser-driven shock wave of the intensity 7.6 Pa penetrated the crystal as deep as 96 m, causing formation of a four-layered structure (the first layer from the surface to 12 m, the second from 12 to 28 m, the third from 28 to 96 m, and the fourth from 96 to 130 m, respectively). The grain size of the first layer was 1 m, while that of the second layer was broken into a few tens nanometers. The grain size of the third layer was a few hundred nanometers to a few ten micrometers. The area deeper than 96 m remained as a single crystal. The plasma heat wave might remelt the first layer, resulting in the grain size becoming larger than that of the second layer. The surface polycrystallization seems to maintain the residual stresses frozen in the film thickness direction. Our experimentally observed spatial profile of the grain size can be explained by this shock and heat waves model. (paper)
Availability note (English)
Available from http://dx.doi.org/10.1088/0022-3727/48/32/325305Additional details
Identifiers
Publishing Information
- Journal Title
- Journal of Physics. D, Applied Physics
- Journal Volume
- 48
- Journal Issue
- 32
- Journal Page Range
- [6 p.]
- ISSN
- 0022-3727
- CODEN
- JPAPBE
INIS
- Country of Publication
- United Kingdom
- Country of Input or Organization
- International Atomic Energy Agency (IAEA)
- INIS RN
- 51046604
- Subject category
- S75: CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY;
- Descriptors DEI
- COMPRESSION; GRAIN SIZE; IRRADIATION; LASERS; LAYERS; MONOCRYSTALS; PLASMA; POLYCRYSTALS; RESIDUAL STRESSES; SHOCK WAVES; SURFACES; THICKNESS; THIN FILMS; YTTRIUM OXIDES; ZIRCONIUM OXIDES
- Descriptors DEC
- CHALCOGENIDES; CRYSTALS; DIMENSIONS; FILMS; MICROSTRUCTURE; OXIDES; OXYGEN COMPOUNDS; SIZE; STRESSES; TRANSITION ELEMENT COMPOUNDS; YTTRIUM COMPOUNDS; ZIRCONIUM COMPOUNDS