Low-energy spin-polarized radioactive beams as a nano-scale probe of matter

被引:26
作者
Kiefl, RF
MacFarlane, WA
Morris, GD
Amaudruz, P
Arseneau, D
Azumi, H
Baartman, R
Beals, TR
Behr, J
Bommas, C
Brewer, JH
Chow, KH
Dumont, E
Dunsiger, SR
Daviel, S
Greene, L
Hatakeyama, A
Heffner, RH
Hirayama, Y
Hitti, B
Kreitzman, SR
Levy, CDP
Miller, RI
Olivo, M
Poutissou, R
机构
[1] TRIUMF, Vancouver, BC V6T 2A3, Canada
[2] Univ British Columbia, Dept Phys & Astron, Vancouver, BC V6T 1Z1, Canada
[3] Univ British Columbia, Canadian Inst Adv Res, Vancouver, BC V6T 1Z1, Canada
[4] Univ British Columbia, Dept Chem, Vancouver, BC V6T 1Z1, Canada
[5] Los Alamos Natl Lab, Los Alamos, NM 87545 USA
[6] Osaka Univ, Grad Sch Sci, Dept Phys, Osaka 5600043, Japan
[7] Univ Bonn, Dept Phys, D-5300 Bonn, Germany
[8] Univ Alberta, Dept Phys, Edmonton, AB T6G 2J1, Canada
[9] Univ Illinois, Dept Phys, Urbana, IL 61801 USA
基金
加拿大自然科学与工程研究理事会;
关键词
beta-NMR; nuclear magnetic resonance; radioactive ion beams; nuclear probes;
D O I
10.1016/S0921-4526(02)01600-9
中图分类号
O469 [凝聚态物理学];
学科分类号
070205 ;
摘要
We have commissioned a polarized low-energy Li-8 ion beam line, which together with a high-field beta-NMR spectrometer, can act as sensitive new probe of thin films and interfaces. The implantation energy can be continuously adjusted from 1 to 90 keV and the maximum polarization achieved thus far is 80%. This instrument opens up new applications for beta-NMR which parallel and complement efforts with low-energy muons. For example, it is possible to probe the magnetic field distribution near the surface of a material by stopping a polarized Li-8 beam in a thin overlayer of Ag. Since the Li-8 adopts a site with cubic symmetry in Ag there is no quadrupolar splitting of the resonance, and the Li-8 acts as a purely magnetic sensor. (C) 2002 Elsevier Science B.V. All rights reserved.
引用
收藏
页码:189 / 195
页数:7
相关论文
共 9 条
[1]  
Ackermann H., 1983, TOPICS CURRENT PHYS, V31, P291, DOI DOI 10.1007/978-3-642-81969-8_6
[2]   Defect properties of implanted boron in ZnSe [J].
Ittermann, B ;
Welker, G ;
Kroll, F ;
Mai, F ;
Marbach, K ;
Peters, D .
PHYSICAL REVIEW B, 1999, 59 (04) :2700-2712
[3]  
KEIM M, 1995, HYPERFINE INTERACT, V97, P543
[4]  
LEE SL, 1999, MUON SCI
[5]  
LEVY CDP, 2002, P EMIS 14 C VICT BC
[6]  
MORENZONI E, 1999, MUON SCI
[7]   Direct observation of a flux line lattice field distribution across an YBa2Cu3O7-δ surface by low energy muons [J].
Niedermayer, C ;
Forgan, EM ;
Glückler, H ;
Hofer, A ;
Morenzoni, E ;
Pleines, M ;
Prokscha, T ;
Riseman, TM ;
Birke, M ;
Jackson, TJ ;
Litterst, J ;
Long, MW ;
Luetkens, H ;
Schatz, A ;
Schatz, G .
PHYSICAL REVIEW LETTERS, 1999, 83 (19) :3932-3935
[8]   Lattice locations of 8Li in Cu [J].
Ohsumi, F ;
Matsuta, K ;
Mihara, M ;
Onishi, T ;
Miyake, T ;
Sasaki, M ;
Sato, K ;
Ha, C ;
Morishita, A ;
Fujio, T ;
Kobayashi, Y ;
Fukuda, M ;
Minamisono, T .
HYPERFINE INTERACTIONS, 1999, 120 (1-8) :419-422
[9]  
Slichter C. P., 1989, PRINCIPLES MAGNETIC