1982
DOI: 10.1016/0370-2693(82)91167-4
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Isotope shifts and hyperfine structure of 38–47K by laser spectroscopy

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Cited by 82 publications
(71 citation statements)
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“…In the odd-A K (Z 20 1 = -) and Cu (Z 28 1 = + ) isotopes it had been observed that the first-excited-state energy decreases dramatically with an increasing number of neutrons between N=20 and 28 in potassium and beyond N=40 in copper. In the K isotopes the energy of the 1/2 + level (due to a hole in the πs 1 2 orbital) decreases gradually as the νf 7 2 level is being filled and this level becomes the ground state in 47 K [73]. In the Cu isotopes the 5/2 − level energy (due to a proton in the πf 5 2 level) was seen to decrease between 69 Cu and 73 Cu [74], as the νg 9 2 is being filled.…”
Section: New Methods and Highlights Since 2000mentioning
confidence: 99%
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“…In the odd-A K (Z 20 1 = -) and Cu (Z 28 1 = + ) isotopes it had been observed that the first-excited-state energy decreases dramatically with an increasing number of neutrons between N=20 and 28 in potassium and beyond N=40 in copper. In the K isotopes the energy of the 1/2 + level (due to a hole in the πs 1 2 orbital) decreases gradually as the νf 7 2 level is being filled and this level becomes the ground state in 47 K [73]. In the Cu isotopes the 5/2 − level energy (due to a proton in the πf 5 2 level) was seen to decrease between 69 Cu and 73 Cu [74], as the νg 9 2 is being filled.…”
Section: New Methods and Highlights Since 2000mentioning
confidence: 99%
“…In the K isotopes the energy of the 1/2 + level (due to a hole in the πs 1 2 orbital) decreases gradually as the νf 7 2 level is being filled and this level becomes the ground state in 47 K [73]. In the Cu isotopes the 5/2 − level energy (due to a proton in the πf 5 2 level) was seen to decrease between 69 Cu and 73 Cu [74], as the νg 9 2 is being filled. In 2005 Otsuka et al explained this monopole migration of single-particle levels as due to the tensor part of the nucleon-nucleon monopole interaction, and they provided an intuitive explanation as to where and how this monopole migration would occur in the nuclear chart [75].…”
Section: New Methods and Highlights Since 2000mentioning
confidence: 99%
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“…This symmetry is not reproduced by the radii behaviour of the neighbouring elements. The shape asymmetry of the δ r 2 curves for the elements with Z > 20 and Z < 20 occurs in opposite directions: for the Ti chain (Z = 22) there is a steady increase of the charge radii towards N = 20 [5], whereas for the chains with Z = 18, 19 the radii increase towards N = 28 [2,4]. The oddeven staggering (OES) effect decreases away from calcium, to argon or titanium, but is smallest for the odd-Z element potassium.…”
Section: Introductionmentioning
confidence: 97%
“…In the vicinity of this region the information about radii is rather scarce. Isotope shift measurements on 38 47 K [11] just include one nucleus of the sd-shell (Z;N < 20). The corresponding 39 Ca has been investigated recently [12], and a similar collinear laser spectroscopy experiment on 50 Ca has extended the calcium data into the 2p 3=2 -subshell beyond N = 28 [13].…”
Section: Introductionmentioning
confidence: 99%