SCOPUS 정보 검색 플랫폼

7
- 84927264837
- For CoSi/2 Si (111), there are no kinematically allowed CoSi2 bands near the Si conduction-band minimum, so ballistic transmission cannot occur.
- (1988) Phys. Rev. B , vol.37 , pp. 623
- Mattheiss, L.F.¹ Hamann, D.R.²

8
- 84927374662
- A. F. J. Levi, R. T. Tung, J. L. Batstone, and M. Anzlowar, in Silicon on Insulators and Buried Metals in Semiconductors, edited by J. C. Sturm, C. K. Chen, L. Pfeiffer, and P. L. F. Hemment, Materials Research Society Symposia Proceedings, Vol. 107 (Materials Research Society, Pittsburgh, 1988), p. 259.

9
- 0000392344
- (1988) Phys. Rev. Lett. , vol.60 , pp. 1406
- Kaiser, W.J.¹ Bell, L.D.²

10
- 17244365811
- (1988) Phys. Rev. Lett. , vol.61 , pp. 2368
- Bell, L.D.¹ Kaiser, W.J.²

11
- 0001162544
- (1988) Phys. Rev. B , vol.38 , pp. 2021
- Stiles, M.D.¹ Hamann, D.R.²

13
- 0001722643
- (1986) Phys. Rev. B , vol.33 , pp. 823
- Mattheiss, L.F.¹ Hamann, D.R.²

15
- 84927374661
- For the LAPW's, we used lmax= 8, 6, and 10 in the Ni, Si, and cut Si muffin tins, | k vec + g vec |2< 15 a.u. [ k vec , g vec = ( K vec , kz) , G vec , gz) ], and | K vec + G vec |2< 10.5 a.u. For the potential and cut muffin-tin projector, we used lmax= 6, 6, and 12, in the Ni, Si, and cut Si muffin tins, | g vec |2< 70 a.u. for the bulk interstitial regions, and | G vec |2< 70, gz2 < 5600 a.u. for the cut supercell interstitial region. For the basis sets, we used 150 (300) eigenfunctions per kz and 2 (1) kz's for the bulk (interface) layers. For the generalized Bloch states and layer matching, we used | K vec + G vec |2< 6.5 a.u.

19
- 25544479230
- (1986) Phys. Rev. B , vol.34 , pp. 5390
- Hybertsen, M.S.¹ Louie, S.G.²

* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.