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Abstract

In [4], Császár has introduced the notions of weak structures and the structures α(w), π(w), σ(w), β(w). The main aim of this paper is to introduce and study properties of the structures r(w), α(w), π(w), σ(w) and β(w).

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Abstract

We define weak structures and show that these structures can replace in many situations generalized topologies or minimal structures.

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[Cu2(μ-(3,4,5-meo-ba)2bn)(μ-I)2] n , a new 1D polymeric copper(I) chain

Synthesis, crystal structure, spectral and thermal studies

Journal of Thermal Analysis and Calorimetry
Authors: Aliakbar Dehno Khalaji, Smail Triki, and Debasis Das

c wR 2 = {Σ[ w ( F o 2 – F c 2 ) 2 ]/Σ[ w(F o 2 ) 2 ]} 1/2 d GooF = {Σ[ w ( F o 2 – F c 2 ) 2 ]/( N obs

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) ( f c + f c t ) 2 , (9.b) τ ( σ ) W A L T H E R = 1 2   f c   σ − σ 2   if   σ > f c / 4 ,   or τ ( σ ) W A L T H E R = f c 8 1 + 8 σ f c   if   σ < f c / 4 ,   and   f c t = f c / 8 , where f ct is the tensile strength and f c is the compressive

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K −1 50 Boltzmann's constant σ /W m −2 K −4 5.67 × 10 −8 Surface radiation

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Crystal structures and thermal properties of some rare earth alkoxides with tertiary alcohols

Possible precursors for atomic layer deposition of rare earth oxides

Journal of Thermal Analysis and Calorimetry
Authors: Timo Hatanpää, Kaupo Kukli, Mikko Ritala, and Markku Leskelä

= Σ|| F o | − | F c ||/| F o |; b wR 2 = [Σ w ( F o 2 − F c 2 ) 2 /Σ w ( F o 2 ) 2 ] 1/2 ALD studies Thin films were grown by ALD using alkoxides 1, 2, 3, and 10 and water in a

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Journal of Thermal Analysis and Calorimetry
Authors: K. Sreekanth, M. Kondaiah, D. Sravana Kumar, and D. Krishna Rao

) G 12 σ H 12 σ

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first stage using a Probit model, and then w i t ′ γ ˜ were obtained used in the second step, to obtain β and the consistent estimator of β λ through least square regression. If ρ ≠ 0 , then there is a bias equalling ρ σ ( − w i t   ′ γ ) . 5

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