• 検索結果がありません。

Absolutely Contradictory Self-Identity of Form and Emptiness, and the self-awareness of Absolute Nothingness (Nishida): 沖縄地域学リポジトリ

N/A
N/A
Protected

Academic year: 2021

シェア "Absolutely Contradictory Self-Identity of Form and Emptiness, and the self-awareness of Absolute Nothingness (Nishida): 沖縄地域学リポジトリ"

Copied!
6
0
0

読み込み中.... (全文を見る)

全文

(1)

Title Absolutely Contradictory Self-Identity of Form and Emptiness,and the self-awareness of Absolute Nothingness (Nishida)

Author(s) Aoki, Kumi

Citation 沖縄工業高等専門学校紀要 = Bulletin of Okinawa NationalCollege of Technology(5): 55-59

Issue Date 2011-03

URL http://hdl.handle.net/20.500.12001/18686

(2)

55 沖縄工業高等専門学校紀要 第 5 号:p.55-59, 2011

(3)
(4)

57 沖縄高専紀要 第 5 号(2011)

(5)
(6)

59 沖縄高専紀要 第 5 号(2011)

参照

関連したドキュメント

Keywords: Convex order ; Fréchet distribution ; Median ; Mittag-Leffler distribution ; Mittag- Leffler function ; Stable distribution ; Stochastic order.. AMS MSC 2010: Primary 60E05

In this section we look at spectral sequences for calculating the homology of the bar and cobar constructions on operads and cooperads in based spaces or spectra.. It turns out that

In Section 3, we show that the clique- width is unbounded in any superfactorial class of graphs, and in Section 4, we prove that the clique-width is bounded in any hereditary

Inside this class, we identify a new subclass of Liouvillian integrable systems, under suitable conditions such Liouvillian integrable systems can have at most one limit cycle, and

We present combinatorial proofs of several non-commutative extensions, and find a β-extension that is both a generalization of Sylvester’s identity and the β-extension of the

Includes some proper curves, contrary to the quasi-Belyi type result.. Sketch of

We shall refer to Y (respectively, D; D; D) as the compactification (respec- tively, divisor at infinity; divisor of cusps; divisor of marked points) of X. Proposition 1.1 below)

The first group contains the so-called phase times, firstly mentioned in 82, 83 and applied to tunnelling in 84, 85, the times of the motion of wave packet spatial centroids,