1962
DOI: 10.1002/bscb.19620710907
|View full text |Cite
|
Sign up to set email alerts
|

Structure des Cyanostilbènes VI. Détermination radiocristallographique de la structure du dibromo‐2,6, α‐cyanostilbène

Abstract: Le dibromo-2-6, a-cyanostilbhe est triclinique, PI. a = 9,63, b = 9,69, c = 7,21A; a = 90°, p = 99,S0, y = !No. Z = 2. La structure a 6tk rkolue en appliquant la mtthode de l'atome lourd aux rbflexions hkO, hkl, hhl. Elle a kt6 affinde par moindres carrk. La molhle est cis et les deux cycles sont presque perpendiculaires l'un B l'autre.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1

Citation Types

0
2
0

Year Published

1975
1975
1983
1983

Publication Types

Select...
3

Relationship

0
3

Authors

Journals

citations
Cited by 3 publications
(2 citation statements)
references
References 9 publications
0
2
0
Order By: Relevance
“…Electric discharge.--For microelectronics purposes diluted silane is injected in a rf discharge. However for our study this kind of discharge must be discarded for several reasons: (i) The power transmitted to the gas by the rf generator cannot be estimated with sufficient accuracy (4). (it) Numerous problems, depending on the high frequency, are related to the measurement of parameters, such as electric field and electronic temperature.…”
Section: Choice Of the Experimental Conditionsmentioning
confidence: 99%
See 1 more Smart Citation
“…Electric discharge.--For microelectronics purposes diluted silane is injected in a rf discharge. However for our study this kind of discharge must be discarded for several reasons: (i) The power transmitted to the gas by the rf generator cannot be estimated with sufficient accuracy (4). (it) Numerous problems, depending on the high frequency, are related to the measurement of parameters, such as electric field and electronic temperature.…”
Section: Choice Of the Experimental Conditionsmentioning
confidence: 99%
“…A more practical form is obtained when using the molar fraction of silane, XSiH4 --dXsiH4/dt ----aeVene*ZsiH4 [4] If the Maxwell-Boltzmann function is used, one obtains dXsis4/dt --_ creVeneXsiH 4 exp (--eV,/RTe) [5] where V, is the excitation potential of the silane molecule on its first electronic level. The current density is J = neevd and the electron drift velocity, Vd, is proportional to the electron thermal velocity, ve ( 18)…”
Section: Measured; --- Calculated (]3)mentioning
confidence: 99%