2016
DOI: 10.1063/1.4947799
|View full text |Cite
|
Sign up to set email alerts
|

Experimental and theoretical spectroscopic studies of branchlet-like SrCO3 superarchitecture

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1

Citation Types

0
1
0

Year Published

2017
2017
2017
2017

Publication Types

Select...
1

Relationship

0
1

Authors

Journals

citations
Cited by 1 publication
(1 citation statement)
references
References 5 publications
0
1
0
Order By: Relevance
“…The weak band located at around 608 cm -1 is also accounted for F 2g mode of Co 3 O 4 (Cheng et al 1998). The two highintensity Raman modes at 181 (caused by in-plane bending) and 700 cm -1 [comes from librational motion of the (CO 3 ) 2-] are attributed to the vibration bands of SrCO 3 (Divya 2016). In addition, two significant bands were also observed at 1359 and 1595 cm -1 , which are assigned to the D-and G-bands of carbon nanofibers, respectively.…”
Section: Resultsmentioning
confidence: 94%
“…The weak band located at around 608 cm -1 is also accounted for F 2g mode of Co 3 O 4 (Cheng et al 1998). The two highintensity Raman modes at 181 (caused by in-plane bending) and 700 cm -1 [comes from librational motion of the (CO 3 ) 2-] are attributed to the vibration bands of SrCO 3 (Divya 2016). In addition, two significant bands were also observed at 1359 and 1595 cm -1 , which are assigned to the D-and G-bands of carbon nanofibers, respectively.…”
Section: Resultsmentioning
confidence: 94%