|
|
|
|
LEADER |
01000caa a22002652 4500 |
001 |
NLM112737811 |
003 |
DE-627 |
005 |
20250202155507.0 |
007 |
tu |
008 |
231222s2001 xx ||||| 00| ||eng c |
028 |
5 |
2 |
|a pubmed25n0376.xml
|
035 |
|
|
|a (DE-627)NLM112737811
|
035 |
|
|
|a (NLM)11367792
|
040 |
|
|
|a DE-627
|b ger
|c DE-627
|e rakwb
|
041 |
|
|
|a eng
|
100 |
1 |
|
|a Kitabayashi, H
|e verfasserin
|4 aut
|
245 |
1 |
0 |
|a Analysis of SAW propagation in gratings on ZnO/diamond substrates
|
264 |
|
1 |
|c 2001
|
336 |
|
|
|a Text
|b txt
|2 rdacontent
|
337 |
|
|
|a ohne Hilfsmittel zu benutzen
|b n
|2 rdamedia
|
338 |
|
|
|a Band
|b nc
|2 rdacarrier
|
500 |
|
|
|a Date Completed 07.06.2001
|
500 |
|
|
|a Date Revised 15.09.2019
|
500 |
|
|
|a published: Print
|
500 |
|
|
|a Citation Status PubMed-not-MEDLINE
|
520 |
|
|
|a The space harmonic method is used to analyze surface acoustic wave (SAW) propagation under an infinite periodic metal grating on ZnO/diamond composite layered substrates. Dispersion properties for shorted and open gratings are derived as a function of the thickness of the grating electrodes. From these dispersion relations, the coupling of modes (COM) parameters are derived. Energy profiles inside ZnO/diamond show that the energies contained in each of the ZnO and diamond layers are of the same order when the thickness of the ZnO layer is P/pi (P = grating period) and that the energy is contained within two wavelengths below the ZnO/diamond interface
|
650 |
|
4 |
|a Journal Article
|
700 |
1 |
|
|a Smith, P M
|e verfasserin
|4 aut
|
773 |
0 |
8 |
|i Enthalten in
|t IEEE transactions on ultrasonics, ferroelectrics, and frequency control
|d 1999
|g 48(2001), 1 vom: 29. Jan., Seite 249-61
|w (DE-627)NLM098181017
|x 0885-3010
|7 nnns
|
773 |
1 |
8 |
|g volume:48
|g year:2001
|g number:1
|g day:29
|g month:01
|g pages:249-61
|
912 |
|
|
|a GBV_USEFLAG_A
|
912 |
|
|
|a SYSFLAG_A
|
912 |
|
|
|a GBV_NLM
|
912 |
|
|
|a GBV_ILN_22
|
912 |
|
|
|a GBV_ILN_24
|
912 |
|
|
|a GBV_ILN_350
|
951 |
|
|
|a AR
|
952 |
|
|
|d 48
|j 2001
|e 1
|b 29
|c 01
|h 249-61
|