X-ray reflectivity theory for determining the density profile of a liquid under nanometre confinement

被引:12
作者
Perret, Edith [1 ]
Nygard, Kim [1 ]
Satapathy, Dillip K. [3 ]
Balmer, Tobias E. [2 ]
Bunk, Oliver [1 ]
Heuberger, Manfred [4 ]
van der Veen, J. Friso [1 ,2 ]
机构
[1] Paul Scherrer Inst, CH-5232 Villigen, Switzerland
[2] ETH, CH-8093 Zurich, Switzerland
[3] Univ Fribourg, CH-1700 Fribourg, Switzerland
[4] EMPA, CH-9014 St Gallen, Switzerland
基金
瑞士国家科学基金会;
关键词
X-ray reflectivity; confined fluids; SURFACE FORCES APPARATUS; FILMS; THICKNESS;
D O I
10.1107/S0909049510014858
中图分类号
TH7 [仪器、仪表];
学科分类号
0804 ; 080401 ; 081102 ;
摘要
An X-ray reflectivity theory on the determination of the density profile of a molecular liquid under nanometre confinement is presented. The confinement geometry acts like an X-ray interferometer, which consists of two opposing atomically flat single-crystal mica membranes with an intervening thin liquid film of variable thickness. The X-rays reflected from the parallel crystal planes (of known structure) and the layered liquid in between them (of unknown structure) interfere with one another, making X-ray reflectivity highly sensitive to the liquid's density profile along the confinement direction. An expression for the reflected intensity as a function of momentum transfer is given. The total structure factor intensity for the liquid-filled confinement device is derived as a sum of contributions from the inner and outer crystal terminations. The method presented readily distinguishes the confined liquid from the liquid adsorbed on the outer mica surfaces. It is illustrated for the molecular liquid tetrakis(trimethyl) siloxysilane, confined by two mica surfaces at a distance of 8.6 nm.
引用
收藏
页码:465 / 472
页数:8
相关论文
共 26 条
[1]  
Born M., 1980, Principles of Optics, V6th, P1
[3]  
FENTER PA, 2002, REV MINERAL GEOCHEM, V149, P221
[4]   Origins of solvation forces in confined films [J].
Gao, JP ;
Luedtke, WD ;
Landman, U .
JOURNAL OF PHYSICAL CHEMISTRY B, 1997, 101 (20) :4013-4023
[5]   CRYSTAL-STRUCTURES OF 2M1 PHENGITE AND 2M1 MUSCOVITE [J].
GUVEN, N .
ZEITSCHRIFT FUR KRISTALLOGRAPHIE KRISTALLGEOMETRIE KRISTALLPHYSIK KRISTALLCHEMIE, 1971, 134 (3-4) :196-&
[6]   The extended surface forces apparatus.: II.: Precision temperature control [J].
Heuberger, M ;
Vanicek, J ;
Zäch, M .
REVIEW OF SCIENTIFIC INSTRUMENTS, 2001, 72 (09) :3556-3560
[7]   The extended surface forces apparatus. Part I. Fast spectral correlation interferometry [J].
Heuberger, M .
REVIEW OF SCIENTIFIC INSTRUMENTS, 2001, 72 (03) :1700-1707
[8]   Layered structure analysis of GMR multilayers by X-ray reflectometry using the anomalous dispersion effect [J].
Hirano, T ;
Usami, K ;
Ueda, K ;
Hoshiya, H .
JOURNAL OF SYNCHROTRON RADIATION, 1998, 5 :969-971
[9]  
Huisman WJ, 1998, SURF SCI, V402, P866, DOI 10.1016/S0039-6028(97)01058-3
[10]   INTERFEROMETRIC METHOD FOR DETERMINING REFRACTIVE INDEX AND THICKNESS OF THIN FILMS [J].
ISRAELAC.J .
NATURE-PHYSICAL SCIENCE, 1971, 229 (03) :85-&