By Stuart A. Rice
The Advances in Chemical Physics sequence provides the leading edge in each sector of the self-discipline and offers the sector with a discussion board for severe, authoritative reviews of advances. It offers a piece of writing framework that makes each one quantity a great complement to complex graduate periods, with contributions from specialists around the globe and a convenient thesaurus for simple reference on new terminology. This sequence is a superb consultant for college students and execs in chemical physics and actual chemistry, from academia, govt, and industries together with chemical compounds, prescription drugs, and polymers.
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Additional info for Advances in Chemical Physics (Volume 143)
H. Weiner Macromolecules, 27, 1201 (1994). 19. J. H. Weiner and J. J. , Prentice Hall, New York, 1991, pp. 255–261. 20. A. F. Bower and J. H. Weiner, J. Chem. Phys. 125, 096101 (2006). 21. J. Gao and J. H. Weiner, Macromolecules 22, 979 (1989). 22. W. A. Curtin and R. E. Miller, Modelling Simul. Mater. Sci. Eng. 11, R33-R68. MULTIPLE AMORPHOUS–AMORPHOUS TRANSITIONS THOMAS LOERTING Institute of Physical Chemistry, University of Innsbruck, Innrain 52a, A-6020 Innsbruck, Austria VADIM V. BRAZHKIN Institute for High Pressure Physics, Troitsk, Moscow Region, 142190 Russia TETSUYA MORISHITA Research Institute for Computational Sciences (RICS), National Institute of Advanced Industrial Science and Technology (AIST), Central 2, 1-1-1 Umezono, Tsukuba, Ibaraki, 305-8568 Japan CONTENTS I.
Sci. Eng. 11, R33-R68. MULTIPLE AMORPHOUS–AMORPHOUS TRANSITIONS THOMAS LOERTING Institute of Physical Chemistry, University of Innsbruck, Innrain 52a, A-6020 Innsbruck, Austria VADIM V. BRAZHKIN Institute for High Pressure Physics, Troitsk, Moscow Region, 142190 Russia TETSUYA MORISHITA Research Institute for Computational Sciences (RICS), National Institute of Advanced Industrial Science and Technology (AIST), Central 2, 1-1-1 Umezono, Tsukuba, Ibaraki, 305-8568 Japan CONTENTS I. Introduction II.
Ice III or its protonordered counterpart ice IX are amorphized by particle bombardment at electron doses above 2400 electrons nmÀ2 . Ice I amorphizes by keV ionbombardment at 10–80 K . Similarly, after a dose of few eV per mol of UV photons amorphization of ice I is observed [166, 167]. The conversion rates increase as the temperature decreases . Using 700 keV proton irradiation at 13 K, even oscillations between crystalline and amorphous ice can be achieved, whereas above 27 K, the amorphous ice remains .
Advances in Chemical Physics (Volume 143) by Stuart A. Rice