NMR Imaging and the Electric Quadrupole Interaction in Solid Materials

1990 ◽  
Vol 217 ◽  
Author(s):  
B. H. Suits

ABSTRACTNuclei with a spin, 1 > 1/2, possess a nuclear quadrupole moment which can couple to the electric field gradients in a material. They can be static, leading to NMR frequency shifts, or dynamic, which can influence relaxation times. In either case, an NMR image can be made which is sensitized to changes in the electric quadrupole interaction to provide a sensitive measure of the macroscopic spatial dependence of the microscopic changes in the material. Several examples are presented. Special considerations need to be given in the case when the strength of the Zeeman interaction between the nucleus and the magnetic field and/or the rf field is small compared to the electric quadrupole interaction.

1998 ◽  
Vol 53 (6-7) ◽  
pp. 355-357
Author(s):  
P. Wodniecki ◽  
B. Wodniecka ◽  
A. Kulińska ◽  
A. Z. Hrynkiewicz

Abstract The quadrupole interaction of 181Ta probes in isostructural Cu8Hf3 and Cu8Zr3 intermetallic compounds was studied in the temperature range 24 K -1100 K with the time-differential perturbed angular correlation technique. Two nonaxial electric field gradients corresponding to two nonequiv-alent hafnium or zirconium sites in the investigated structure were found. A linear decrease in the quadrupole interaction frequency with increase of temperature for the 8(d) sites was evidenced, while the vQ(T) dependence for the 4(c) sites is weaker and has a T3/2 character.


Time-differential angular correlation studies of the electric quadrupole interaction of 181 Ta in various Hf compounds are presented. Methods for the analysis of the time spectra are discussed. The experiments yield information on the strength of the quadrupole interaction, and on the axial asymmetry and distribution of the field gradient. Electric field gradients V zz are derived for 181 Ta in Hf metal, HfO 2 , and (NH 4 ) 2 HfF 6 .


Spin-echo amplitudes for spins I = 1, 3/2 and 5/2 have been worked out in the presence of weak electric quadrupole interaction in crystals with non-axial electric field gradients. The effects of first- and second-order perturbation due to the quadrupole interaction in causing a modulation of the spin-echo signals have been analyzed in detail in comparison with the splitting and shift effects they cause in the steady experiment.


1994 ◽  
Vol 49 (1-2) ◽  
pp. 407-417 ◽  
Author(s):  
H. Haas

Abstract The measurement of the electric quadrupole interaction with nuclear techniques allows the study of monolayer coverages or even isolated atoms at surfaces and interfaces due to the inherent sensitivity of these methods. Recently electric field gradients at surface atoms have been investigated with Mößbauer Spectroscopy, Polarized Beam NMR , and Perturbed Angular Correlation (PAC). The highly sensitive PAC technique with 111In and 111mCd sources, in particular, has been applied to several metal and semiconductor surfaces. The use of flat as well as stepped surfaces has allowed the assignment of the measured quadrupole interaction frequencies to specific surface sites. For the Pd(111) surface a particularly complete description is possible, since for five different sites (terrace adatoms, ledge adatoms, kink adatoms, ledge and terrace atoms) the field gradients and their orientation could be determined. They represent a challenging problem for understanding the electronic structure of metallic surfaces. Through the study of the temperature dependence of the different components the diffusion of the radioactive probe atoms can be followed. The data from 57Fe Mößbauer spectroscopy on iron surfaces with monolayer coverage and NMR surface studies of 7Li and 23Na at high temperatures are reviewed. An outlook for further developments of the nuclear techniques is presented, particularly in view of the variety of radioactive isotope beams available from on-line isotope separators like the ISOLDE facility at CERN.


1992 ◽  
Vol 46 (14) ◽  
pp. 8818-8827 ◽  
Author(s):  
B. Kastelein ◽  
M. W. J. Prins ◽  
J. Andriessen ◽  
H. Postma ◽  
L. Klostermann ◽  
...  

1985 ◽  
Vol 23 (1) ◽  
pp. 89-102 ◽  
Author(s):  
M. B. Kurup ◽  
K. G. Prasad ◽  
K. Raghunathan ◽  
R. P. Sharma

1981 ◽  
Vol 10 (1-4) ◽  
pp. 963-966 ◽  
Author(s):  
H. Barfu� ◽  
G. B�hnlein ◽  
H. Hohenstein ◽  
W. Kreische ◽  
H. Niedrig ◽  
...  

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