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Researchers

phase12006.10`2010.3@2007.10`2011.3@
Masaaki
Ashida
Kenichi
L. Ishikawa
Tetsuya
Ido
Hideki
Ohmura
Takashige
Omatu
Masayuki
Katuragawa
Atsushi
Kubo
Mitsutaka
Kumakura
Muneaki
Hase
Akiyoshi
Hishikawa
 
  URLF iJap) http://bukko.bk.tsukuba.ac.jp/~mhase/indexJ.html
iEng) http://www.bk.tsukuba.ac.jp/~mhase/index.htm
@Curriculum Vitae

y Education z

BS in Applied Physics, Osaka University, Osaka, Japan 1993,
PhD in Applied Physics, Osaka University, Osaka, Japan 1998.

y Academic Experience z

Postdoctoral Fellow, Japan Society for the Promotion of Science (JSPS) 1998,
Research Scientist, National Research Institute for Metals (NRIM) 1999,
Research Scientist, National Institute for Materials Science (NIMS) 2001,
Senior Research Scientist, National Institute for Materials Science 2004, Associate Professor, Institute of Applied Physics at the University of Tukuba 2006.
Visiting Research Scholar, Dept. of Physics and Astronomy,
University of Pittsburgh, USA, 2003 ~ 2004.

|Research Interest|
Ultrafast Spectroscopy and Condensed Matter Physics.
|Research Achievement|
Study of coherent phonons and photoexcited electrons in semiconductors and semimetals.
|Hobby|
Riding bicycles and playing golf
@Introduction of the project

@Under the irradiation of the femtosecond laser pulses, coherent oscillations of Raman active phonons can be excited through electronic excitation via real or virtual intermediate states, which are characterized by displacive and impulsive excitations of coherent phonons, respectively. There have been extensive studies on the generation of coherent phonons and on the dephasing dynamics of coherent phonons, in semimetals, semiconductors, and superconductors in the past decade. Recently, it has been revealed that coherent phonons in solids can be optically controlled by the irradiation of terahertz-rate pulse trains whose time periods match to the oscillation period of the coherent phonons. Thus the coherent phonon has been the focus of much attention because of its wide applications as well as its fundamental interest from the viewpoint of lattice dynamics.

@As the characteristic of the coherent phonon, the reflectance change of 10-2 to 10-‚S is induced by coherent oscillations at a sample surface. Therefore, by use of this reflectance changes, amplitude modulation of the light can be possible. In addition, phonons in solids are closely related to structural phase transition. In particular, in displacement-type ferroelectrics there is so-called soft mode whose frequency becomes extremely low near the critical point, and it has been accepted that phase transitions are caused by displacement of this soft mode. Therefore, operation of structure phase transition is expected if light pulses can control the amplitude of the coherent soft mode.

@In the present study, I will try to manipulate the phase transitions in solids, the mobility of electrons, and the properties of photons, which are interacting with coherent phonons, by precisely controlling the amplitude, the frequency, and the phase of coherent phonons. Furthermore, in the near future, I would propose completely new phonon devises by using controllability of the coherent phonons.

Hase Fig.

References:
•  M. Hase , K. Ishioka, J. Demsar, K. Ushida, M. Kitajima,h Ultrafast dynamics of coherent optical phonons and nonequilibrium electrons in transition metalsh, Phys. Rev. B. Vol. 71 , 184301 (2005).
•  M. Hase , M. Kitajima, A. M. Constantinescu and H. Petek,hThe birth of quasiparticles in Si observed in time-frequency spaceh, Nature , Vol. 426 , pp.51-54 (2003).
•  M. Hase , M. Kitajima, S. Nakashima and K. Mizoguchi,hForcibly driven coherent soft phonons in GeTe with intense THz-rate pump fieldsh, Appl. Phys. Lett., Vol. 83 , No. 24, pp.4921 (2003).
•  M. Hase , M. Kitajima, S. Nakashima, and K. Mizoguchi,hDynamics of coherent anharmonic phonons in bismuth using high density photoexcitationh, Phys. Rev. Lett., Vol. 88, No. 6, pp. 067401 (2002).

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