TY - JOUR
T1 - Aggregate frequency width, nuclear hyperfine coupling and Jahn-Teller effect of Cu2+ impurity ion ESR in SrLaAlO4 dielectric resonator at 20 millikelvin
AU - Hosain, M. A.
AU - Le Floch, J. M.
AU - Krupka, J.
AU - Tobar, M. E.
PY - 2018/1/10
Y1 - 2018/1/10
N2 - The impurity paramagnetic ion, Cu2+ substitutes Al in the SrLaAlO4 single crystal lattice, this results in a CuO6 elongated octahedron, and the resulting measured g-factors satisfy four-fold axes variation condition. The aggregate frequency width of the electron spin resonance with the required minimum level of impurity concentration has been evaluated in this single crystal SrLaAlO4at 20 millikelvin. Measured parallel hyperfine constants, A∥Cu, were determined to be -155.7 × 10-4 cm-1, - 163.0 × 10-4 cm-1, - 178.3 × 10-4 cm-1 and -211.1 × 10-4 cm-1 at 9.072 GHz (WGH4,1,1) for the nuclear magnetic quantum number MI = +3/2 ,+1/2 ,-1/2 , and-3/2 respectively. The anisotropy of the hyperfine structure reveals the characteristics of the static JahnTeller effect. The second-order-anisotropy term, ≈ ( spin-orbit coupling/10Dq )2, is significant and cannot be disregarded, with the local strain dominating over the observed Zeeman-anisotropy-energy difference. The Bohr electron magneton, - = 9.23 × 10-24JT-1, (within -0.43% so-called experimental error) has been found using the measured spin-Hamiltonian parameters. Measured nuclear dipolar hyperfine structure parameter P- = 12.3 × 10-4 cm-1 shows that the mean inverse third power of the electron distance from the nucleus is 〈rq -3〉 ≲ 5.23 a.u. for Cu2+ ion in the substituted Al3+ion site assuming nuclear electric quadruple moment Q = -0.211 barn.
AB - The impurity paramagnetic ion, Cu2+ substitutes Al in the SrLaAlO4 single crystal lattice, this results in a CuO6 elongated octahedron, and the resulting measured g-factors satisfy four-fold axes variation condition. The aggregate frequency width of the electron spin resonance with the required minimum level of impurity concentration has been evaluated in this single crystal SrLaAlO4at 20 millikelvin. Measured parallel hyperfine constants, A∥Cu, were determined to be -155.7 × 10-4 cm-1, - 163.0 × 10-4 cm-1, - 178.3 × 10-4 cm-1 and -211.1 × 10-4 cm-1 at 9.072 GHz (WGH4,1,1) for the nuclear magnetic quantum number MI = +3/2 ,+1/2 ,-1/2 , and-3/2 respectively. The anisotropy of the hyperfine structure reveals the characteristics of the static JahnTeller effect. The second-order-anisotropy term, ≈ ( spin-orbit coupling/10Dq )2, is significant and cannot be disregarded, with the local strain dominating over the observed Zeeman-anisotropy-energy difference. The Bohr electron magneton, - = 9.23 × 10-24JT-1, (within -0.43% so-called experimental error) has been found using the measured spin-Hamiltonian parameters. Measured nuclear dipolar hyperfine structure parameter P- = 12.3 × 10-4 cm-1 shows that the mean inverse third power of the electron distance from the nucleus is 〈rq -3〉 ≲ 5.23 a.u. for Cu2+ ion in the substituted Al3+ion site assuming nuclear electric quadruple moment Q = -0.211 barn.
KW - crystal field
KW - effective spin
KW - g-factor
KW - hyperfine structure
KW - multiplet
KW - spin-Hamiltonian
KW - whispering gallery mode
UR - https://www.scopus.com/pages/publications/85038595279
U2 - 10.1088/1361-648X/aa9a1e
DO - 10.1088/1361-648X/aa9a1e
M3 - Article
C2 - 29130900
AN - SCOPUS:85038595279
SN - 0953-8984
VL - 30
JO - Journal of Physics Condensed Matter
JF - Journal of Physics Condensed Matter
IS - 1
M1 - 015802
ER -