Density, sp3 fraction, and cross-sectional structure of amorphous carbon films determined by x-ray reflectivity and electron energy-loss spectroscopy

被引:502
作者
Ferrari, AC [1 ]
Li Bassi, A
Tanner, BK
Stolojan, V
Yuan, J
Brown, LM
Rodil, SE
Kleinsorge, B
Robertson, J
机构
[1] Univ Cambridge, Dept Engn, Cambridge CB2 1PZ, England
[2] Univ Durham, Dept Phys, Durham DH1 3LE, England
[3] Univ Cambridge, Cavendish Lab, Cambridge CB3 0HE, England
关键词
D O I
10.1103/PhysRevB.62.11089
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Grazing-angle x-ray reflectivity (XRR) is described as an efficient, nondestructive, parameter-free means to measure the mass density of various types of amorphous carbon films down to the nanometer thickness range. It is shown how XRR can also detect layering if it is present-in the films, in which case the reflectivity profile must be modeled to derive the density. The mass density can also be derived from the valence electron density via the plasmon energy, which is measured by electron energy-loss spectroscopy (EELS). We formally define an interband effective electron mass m*, which accounts for the finite band gap. Comparison of XRR and EELS densities allows us to fit an average m* = 0.87m for carbon systems, m being the free-electron mass. We show that, within the Drude-Lorentz model of the optical spectrum, m* = [1-n(0)(-2)]m, where n(0) is the refractive index at zero optical frequency. The fraction of sp(2) bonding is derived from the carbon K-edge EELS spectrum, and it is shown how a choice of "magic" incidence and collection angles in the scanning transmission electron microscope can give sp(2) fraction values that are independent of sample orientation or anisotropy. We thus give a general relationship between mass density and sp(3) content for carbon films.
引用
收藏
页码:11089 / 11103
页数:15
相关论文
共 84 条
[1]   Carbon films with an sp2 network structure [J].
Alexandrou, I ;
Scheibe, HJ ;
Kiely, CJ ;
Papworth, AJ ;
Amaratunga, GAJ ;
Schultrich, B .
PHYSICAL REVIEW B, 1999, 60 (15) :10903-10907
[2]   Synthesis of carbon films with controlled nanostructure by separation of neutral clusters in supersonic beams [J].
Barborini, E ;
Piseri, P ;
Li Bassi, A ;
Ferrari, AC ;
Bottani, CE ;
Milani, P .
CHEMICAL PHYSICS LETTERS, 1999, 300 (5-6) :633-638
[3]   EXPERIMENTAL ENERGY-LOSS FUNCTION, IM[-1/EPSILON(Q,OMEGA)], FOR ALUMINUM [J].
BATSON, PE ;
SILCOX, J .
PHYSICAL REVIEW B, 1983, 27 (09) :5224-5239
[4]   EELS ANALYSIS OF VACUUM ARC-DEPOSITED DIAMOND-LIKE FILMS [J].
BERGER, SD ;
MCKENZIE, DR ;
MARTIN, PJ .
PHILOSOPHICAL MAGAZINE LETTERS, 1988, 57 (06) :285-290
[5]   Structural and mechanical properties of diamond-like carbon films prepared by pulsed laser deposition with varying laser intensity [J].
Bonelli, M ;
Ferrari, AC ;
Fioravanti, AP ;
Miotello, A ;
Ossi, PM .
AMORPHOUS AND NANOSTRUCTURED CARBON, 2000, 593 :359-364
[6]   Cathodic arc deposition of films [J].
Brown, IG .
ANNUAL REVIEW OF MATERIALS SCIENCE, 1998, 28 :243-269
[7]   REAL-SPACE DETERMINATION OF ANISOTROPIC ELECTRONIC-STRUCTURE BY ELECTRON-ENERGY LOSS SPECTROSCOPY [J].
BROWNING, ND ;
YUAN, J ;
BROWN, LM .
ULTRAMICROSCOPY, 1991, 38 (3-4) :291-298
[8]   Optical constants of tetrahedral amorphous carbon films in the infrared region and at a wavelength of 633 nm [J].
Chen, ZY ;
Zhao, JP .
JOURNAL OF APPLIED PHYSICS, 2000, 87 (09) :4268-4273
[9]  
CHHOWALLA M, 1998, THESIS CAMBRIDGE U
[10]  
CRAVEN AJ, 1981, QUANTITATIVE MICROAN, P141