Add to ORKGFine structure is observed in the photoemission of Gd and Tb 5p levels as a result of multiplet splitting. These splittings are the consequence of different J final states that occur as a result of interactions with partly filled 4f and/or 5d levels
The 5p3/2 to 5p1/2 shallow core level branching ratios in different - photoemission geometries provi...
By comparing femtosecond laser-pulse-induced spin dynamics in the surface state of the rare earth me...
Resonant photoemission in the Pu 5f and Pu 6p states is compared to that in the Gd 4f and Gd 5p stat...
Fine structure is observed in the photoemission of Gd and Tb 5p levels as a result of multiplet spli...
Fine structure is observed in the photoemission of the gadolinium and terbium 5p levels. The 5p leve...
Fine structure is observed in the photoemission of the gadolinium and terbium 5p levels. The 5p leve...
By growing gadolinium films on W(110), it has been possible to observe the development of the Gd(000...
Ultrathin Gd films have been studied with constant initial-state spectroscopy (CIS) of photoemission...
Ultrathin Gd films have been studied with constant initial-state spectroscopy (CIS) of photoemission...
Photoelectron spectroscopy, low energy electron diffraction (LEED), Auger electron spectroscopy (AES...
The constructive summing of direct and indirect channels above the absorption threshold of a core le...
There is interplay between intra-atomic orbital hybridization and extra-atomic hybridization in vari...
The temperature dependence of the rare-earth valence bands has been regarded as a realization of the...
Broad peaks observed in the photoabsorption spectra of rare earths ∼10-20 eV above the 4d edge are a...
The magnetic phase transitions for Gd(0 0 0 1) grown on W(1 1 0) - a bulk transition at 293 K and a ...
The 5p3/2 to 5p1/2 shallow core level branching ratios in different - photoemission geometries provi...
By comparing femtosecond laser-pulse-induced spin dynamics in the surface state of the rare earth me...
Resonant photoemission in the Pu 5f and Pu 6p states is compared to that in the Gd 4f and Gd 5p stat...
Fine structure is observed in the photoemission of Gd and Tb 5p levels as a result of multiplet spli...
Fine structure is observed in the photoemission of the gadolinium and terbium 5p levels. The 5p leve...
Fine structure is observed in the photoemission of the gadolinium and terbium 5p levels. The 5p leve...
By growing gadolinium films on W(110), it has been possible to observe the development of the Gd(000...
Ultrathin Gd films have been studied with constant initial-state spectroscopy (CIS) of photoemission...
Ultrathin Gd films have been studied with constant initial-state spectroscopy (CIS) of photoemission...
Photoelectron spectroscopy, low energy electron diffraction (LEED), Auger electron spectroscopy (AES...
The constructive summing of direct and indirect channels above the absorption threshold of a core le...
There is interplay between intra-atomic orbital hybridization and extra-atomic hybridization in vari...
The temperature dependence of the rare-earth valence bands has been regarded as a realization of the...
Broad peaks observed in the photoabsorption spectra of rare earths ∼10-20 eV above the 4d edge are a...
The magnetic phase transitions for Gd(0 0 0 1) grown on W(1 1 0) - a bulk transition at 293 K and a ...
The 5p3/2 to 5p1/2 shallow core level branching ratios in different - photoemission geometries provi...
By comparing femtosecond laser-pulse-induced spin dynamics in the surface state of the rare earth me...
Resonant photoemission in the Pu 5f and Pu 6p states is compared to that in the Gd 4f and Gd 5p stat...