NUCLEAR g FACTOR OF THE FIRST EXCITED STATE IN 106Pd AND THE INTERNAL FIELD ON PALLADIUM IN NICKEL

1967 ◽  
Vol 45 (5) ◽  
pp. 1813-1819 ◽  
Author(s):  
J. Murray ◽  
T. A. McMath ◽  
J. A. Cameron
Keyword(s):  
Excited State ◽  
Room Temperature ◽  
Internal Field ◽  
Cobalt Alloys ◽  
G Factor ◽  
Angular Correlations ◽  
Perturbed Angular Correlations ◽  
First Excited State

The nuclear g factor of the first excited state in 106Pd has been measured by the method of perturbed angular correlations. The perturbing fields used were the internal fields on palladium in dilute iron and cobalt alloys. By comparing the rotation caused by these alloys with the rotation observed when nickel was the host, a measurement of the internal field on palladium in nickel has been obtained.The g factor of the first excited state in 106Pd has been determined to be +0.35 ± 0.03. The internal field on palladium in nickel at room temperature was found to be −174 ± 13 kOe.

Perturbed angular correlations in 177Hf

1968 ◽  
Vol 46 (13) ◽  
pp. 1523-1526 ◽  
Author(s):  
W. H. Brooker ◽  
T. A. McMath ◽  
J. Murray ◽  
J. A. Cameron
Keyword(s):  
Room Temperature ◽  
Gamma Ray ◽  
G Factor ◽  
Angular Correlations ◽  
Perturbed Angular Correlations

Ions of 177Lu have been implanted in iron and nickel hosts at concentrations of about 1018/cm3. Perturbation of angular correlations in the gamma-ray cascade through the 113–keV level gives values for the internal fields on hafnium nuclei in these metals at room temperature and for this concentration of H(Fe) = −140 ± 10 kOe and H(Ni) = −60 ± 10 kOe. The rotation of the 250-keV level was also observed in the iron host. The nuclear g factor of this state is g = +0.26 ± 0.09.

Measurement of the g-factor of the first excited state in Pd106

1965 ◽  
Vol 70 (1) ◽  
pp. 28-32 ◽  
Author(s):  
H.J. Körner ◽  
U. Ortabasi
Keyword(s):  
Excited State ◽  
G Factor ◽  
First Excited State

Lifetime and g-factor of the first excited state in Fe56

1961 ◽  
Vol 27 (4) ◽  
pp. 612-619 ◽  
Author(s):  
F.R. Metzger
Keyword(s):  
Excited State ◽  
G Factor ◽  
First Excited State

scholarly journals First-excited state g factor of Te136 by the recoil in vacuum method

2017 ◽  
Vol 96 (1) ◽  
Author(s):  
A. E. Stuchbery ◽  
J. M. Allmond ◽  
M. Danchev ◽  
C. Baktash ◽  
C. R. Bingham ◽  
...  
Keyword(s):  
Excited State ◽  
G Factor ◽  
First Excited State ◽  
Vacuum Method

Synthesis, Characterization, and Photoluminescence of a Novel Eu-Containing Polymer Precursor: {Tris(acetylacetonate)5-acrylamido-1,10-phenanthroline}Europium(III)

2013 ◽  
Vol 345 ◽  
pp. 189-192
Author(s):  
Cun Jin Xu
Keyword(s):  
Excited State ◽  
Acrylic Acid ◽  
Room Temperature ◽  
Functional Group ◽  
Europium Complex ◽  
Polymer Precursor ◽  
Red Emission ◽  
Pl Spectra ◽  
First Excited State ◽  
Antenna Ligand

A new europium complex, Eu (acac)3Aphen (where Hacac and Aphen stand for acetylacetone and 5-acrylamido-1,10-phenanthroline, respectively), was synthesized and characterized by elemental analysis, IR, UV and photoluminescence (PL) spectra. The ligand Aphen not only serves as an antenna ligand but also offers a functional group for polymer precursor. The room-temperature PL spectra of the europium (III) complex are composed of the typical Eu3+ red emission, assigned to transitions between the first excited state (5D0) and the multiplet (7F04). Compared to Eu (acac)2AA (where HAA is acrylic acid), Eu (acac)3Aphen exhibits greatly enhanced quantum efficiency (i.e., 14.1% vs 28.5%) and longer 5D0 lifetime (260 μs vs 568 μs).

The Er3+ and Yb3+-related emission from Er, Yb co-implanted Al0.70Ga0.30As/GaAs substrates prepared MOCVD method

2004 ◽  
Vol 829 ◽  
Author(s):  
Tomoyuki Arai ◽  
Shin-ichiro Uekusa
Keyword(s):  
Excited State ◽  
Room Temperature ◽  
Main Peak ◽  
Gaas Substrates ◽  
Energy Transfers ◽  
First Excited State ◽  
Pl Intensity

ABSTRACTYtterbium (Yb) ions were co-implanted into Al0.70Ga0.30As:Er substrates at room temperature. The photoluminescence (PL) and PL lifetime were characterized. Co-implanted Yb3+ enhanced PL intensity of Er3+-related emission. Er3+-related main peak (1538.2 nm), in addition to Yb3+ dose, was enhanced approximately twice. The energy transfers from 2F5/2 (the first excited state) → 2F7/2 (the grand excited state) of Yb3+ to 4I11/2 (the second excited state) → 4I15/2 (the grand excited state) and 4I15/2 → (the first excited state) 4I15/2 of Er3+ was observed.

GAMMA-RAY ANGULAR CORRELATION MEASUREMENTS IN Ne22

1964 ◽  
Vol 42 (6) ◽  
pp. 1300-1310 ◽  
Author(s):  
C. Broude ◽  
M. A. Eswaran
Keyword(s):  
Excited State ◽  
Angular Correlation ◽  
Gamma Ray ◽  
Amplitude Ratio ◽  
Spin Assignment ◽  
Primary Radiation ◽  
Angular Correlations ◽  
First Excited State

Coincidence gamma-ray angular correlations of the cascade decays from the 3.34- and 4.47-Mev states in Ne22 through the first excited state have been measured. The levels were excited by the reaction F19 (α, p)Ne22. The correlations give an unambiguous spin assignment of 4 to the 3.34-Mev state; the analysis of the correlations from the 4.47-Mev state is not unique, allowing spin 2 or 3. The quadrupole-to-dipole amplitude ratio for the primary radiation is −0.11 ± 0.03 or −1.07 ± 0.10, respectively, for the spin-2 and spin-3 assignments.

The hyperfine field at Ti nuclei in Fe and Ni and the g factor of the 160-keV 7/2− level of 47Ti

1977 ◽  
Vol 55 (9) ◽  
pp. 779-782 ◽  
Author(s):  
B. Bullimore ◽  
J. A. Cameron
Keyword(s):  
Excited State ◽  
Hyperfine Field ◽  
G Factor ◽  
First Excited State ◽  
Average Hyperfine Field

Integral rotation of the 3/2+ 320-keV level of 45Ti and the 7/2− 160 keV level of 47Ti recoil implanted in iron and nickel were measured following (α,n) reactions in 42Ca and 44Ca on magnetized backings. The average hyperfine field at 45Ti nuclei is Hhf(TiFe) = −45 ± 10 kOe and Hhf(TiNi) = −15 ± 3kOe. The g factor of the 7/2− first excited state of 47Ti is −0.55 ± 0.17.

scholarly journals Measurement of the g-factor and lifetime of the first-excited state of 20O

1980 ◽  
Vol 344 (2) ◽  
pp. 294-306 ◽  
Author(s):  
A.J. Rutten ◽  
A. Holthuizen ◽  
J.A.G. De Raedt ◽  
W.A. Sterrenburg ◽  
G. Van Middelkoop
Keyword(s):  
Excited State ◽  
G Factor ◽  
First Excited State

The Nuclear Quadrupole Interaction of 187W(β–)187Re in W(VI)-EDTA Complexes

2002 ◽  
Vol 57 (6-7) ◽  
pp. 620-622 ◽  
Author(s):  
Guida Sun ◽  
Weiqiao Liu ◽  
Tilman Butz
Keyword(s):  
Quadrupole Interaction ◽  
Room Temperature ◽  
Nuclear Quadrupole Interaction ◽  
Edta Complex ◽  
Angular Correlations ◽  
Perturbed Angular Correlations ◽  
Edta Complexes ◽  
Time Differential ◽  
Nuclear Quadrupole ◽  
Asymmetry Parameters

The nuclear quadrupole interaction of 187W(β-)187Re in W(VI)-EDTA complexes at room temperature was determined by time differential perturbed angular correlations (TDPAC) to be VQ = 1270(8) MHz with an asymmetry parameter η= 0.403(4). While the coordination geometry of the Mo(VI)- EDTA complex is known, there appears to be none for the W-analogue. The rather similar asymmetry parameters for the 187W(β-)187Re in W(VI)-EDTA complex and for the 99Mo(β-)99Tc in Mo(VI)- EDTA complex, determined previously, supports the idea that the coordination geometries in the Moand W-complexes are similar

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