早稲田大学 武岡真司研究室の博士論文の疑惑まとめ

早稲田大学 先進理工学研究科 生命医科学専攻 の武岡 真司氏（小保方晴子氏の博士論文の審査委員）の研究室の藤枝俊宣氏の論文の文章は、Stephan Forster氏らの論文からのコピペです（引用はあり）。Fig.1.4もコピペです。

著者：藤枝俊宣　（Toshinori FUJIE）
　　　　（早稲田大学大学院先進理工学研究科 生命医科学専攻 生体分子集合科学研究）

論 文 題 目　（February 2009）
Construction of Biomacromolecular Nanosheets and Their Biomedical Application as a Wound Dressing Material
生体高分子からなるナノシートの構築と 創傷被覆材としての医用応用
https://dspace.wul.waseda.ac.jp/dspace/bitstream/2065/34612/3/Honbun-5032.pdf


藤枝俊宣氏の博士論文のIntroにおける文章
The ordered state is distinguished by the fact that individual molecules are located
at restricted three-dimensional regions, for example, a lattice site in a crystal or the
position in the three-dimensional structure of a protein. A localization is always
accompanied by a decrease of the number of realizable states and hence a loss of
entropy. Temperature plays always an important role in the case of phase transitions
between different order states because of the contribution T'S to the free energy.
Besides temperature, further external fields E may influence the degree of order and the
phase transitions. The field strength and temperature at which the phase transitions take
place can be depicted schematically in phase diagrams (Fig. 1-4). The critical
temperature Tc above which the system is disordered is indicated on the temperature
axis. Phase transitions from the disordered phase (U) to different ordered phases (L, H)
may take place below the critical temperature. These phase transitions are accompanied
by a self-organization of the system. The stability range of the different phases can be
taken from the phase diagram. Different ordered structures for one and the same
material can be produced by varying the temperature and field strength. This variability
has a favorable effect on the production and optimization of materials.



文章コピペ元の論文
From Self-Organizing Polymers to Nanohybrid and Biomaterials
Stephan Forster and Thomas Plantenberg
http://www.eng.buffalo.edu/Courses/ce435/Forster02.pdf

Stephan Forster氏らの論文の文章
The ordered state is distinguished by the fact that individual molecules are located at restricted three-dimensional regions, for example, a lattice site in a crystal or the position in the three-dimensional structure of a protein. A localization is always accompanied by a decrease of the number of realizable states and hence a loss of entropy. Temperature plays always an important role in the case of phase transitions between different order states because of the contribution T S to the free energy. Besides temperature, further external fields E may influence the degree of order and the phase transitions. The field strength and temperature at which the phase transitions take place can be depicted schematically in phase diagrams (Figure 1). The critical temperature Tc above which
Figure 1. Transition from a disordered phase (U) to ordered phases (H, L) by variation of the temperature Tand the external field E. Tc is the critical temperature above which ordered phases are not accessible. The transition UH,L corresponds to a self-organization. the system is disordered is indicated on the temperature axis. Phase transitions from the disordered phase (U) to different ordered phases (L, H) may take place below the critical temperature. These phase transitions are accompanied by a self-organization of the system. The stability range of the different phases can be taken from the phase diagram. Different ordered structures for one and the same material
can be produced by varying the temperature and field strength. This variability has a favorable effect on the production and optimization of materials.