메뉴 건너뛰기




Volumn 10, Issue 1, 2010, Pages 146-157

A Series of cation-templated, polycarboxylate-based Cd(II) or Cd(II)/Li(I) frameworks with second-order nonlinear optical and ferroelectric properties

Author keywords

[No Author keywords available]

Indexed keywords


EID: 74049151972     PISSN: 15287483     EISSN: 15287505     Source Type: Journal    
DOI: 10.1021/cg9007476     Document Type: Article
Times cited : (130)

References (94)
  • 12
    • 33847206105 scopus 로고    scopus 로고
    • (a) Scott, J. F. Science 2007 315, 954.
    • (2007) Science , vol.315 , pp. 954
    • Scott, J.F.1
  • 41
    • 0004283942 scopus 로고    scopus 로고
    • University of Göttingen: Göttingen, Germany
    • Sheldrick, G. M. SADABS; University of Göttingen: Göttingen, Germany, 1996.
    • (1996) SADABS
    • Sheldrick, G.M.1
  • 42
    • 0004150157 scopus 로고
    • version 5.10; Siemens Analytical X-ray Instruments Inc.: Madison, WI
    • SHELXTL (version 5.10); Siemens Analytical X-ray Instruments Inc.: Madison, WI, 1994.
    • (1994) SHELXTL
  • 51
    • 74049126463 scopus 로고    scopus 로고
    • See http://rcsr.anu.edu.au
  • 78
    • 74049092609 scopus 로고    scopus 로고
    • The powder second-harmonic generation test was carried out on the sample by the Kurtz and Perry method. Second-harmonic generation intensity data were obtained by placing a sieved (80-100 mesh) powder sample in an intense fundamental beam from a Q-switched Nd:YAG laser of wavelength 1064 nm. The output (X = 532 nm) was filtered first to remove the multiplier and was then displayed on an oscilloscope. This procedure was then repeated using standard NLO material (microcrystalline KDP), and the ratio of the secondharmonic intensity outputs was calculated.
    • The powder second-harmonic generation test was carried out on the sample by the Kurtz and Perry method. Second-harmonic generation intensity data were obtained by placing a sieved (80-100 mesh) powder sample in an intense fundamental beam from a Q-switched Nd:YAG laser of wavelength 1064 nm. The output (X = 532 nm) was filtered first to remove the multiplier and was then displayed on an oscilloscope. This procedure was then repeated using standard NLO material (microcrystalline KDP), and the ratio of the secondharmonic intensity outputs was calculated.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.