Add to ORKGElectron-energy-loss spectra of stage-1 K-intercalated graphite single crystals were obtained with a scanning transmission electron microscope. The complex dielectric function with electric polarization perpendicular to the c axis was derived by Kramers-Kronig analysis. The energy-loss peak at 2.5 eV is consistent with previous optical measurements, while the splitting of the one at 27 eV can be interpreted by folding the Brillouin zone of pristine graphite. Splittings and shifts of the interband transitions were observed and compared with calculations
We used hard X-ray photoelectron spectroscopy (HAXPES) with 8 keV X-rays to investigate the 1s emiss...
The Shubnikov-deHaas (SdH) effect has been used to study the electronic properties of graphite inter...
We used hard X-ray photoelectron spectroscopy (HAXPES) with 8 keV X-rays to investigate the Is emiss...
Electron-energy-loss spectra of stage-1 K-intercalated graphite single crystals were obtained with a...
The dielectric function ϵ(q,ω) of potassium intercalated graphite (KC8) with q| c-axis was deduced f...
The dielectric function ϵ(q,ω) of potassium intercalated graphite (KC8) with q| c-axis was deduced f...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
Optical spectroscopy (Raman, FTIR and Reflection ) was used to study a variety of acceptor- and dono...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
The Shubnikov-deHaas (SdH) effect has been used to study the electronic properties of graphite inter...
Electrons in isolated graphene layers are a two-dimensional gas of massless Dirac Fermions. In reali...
We used hard X-ray photoelectron spectroscopy (HAXPES) with 8 keV X-rays to investigate the 1s emiss...
The Shubnikov-deHaas (SdH) effect has been used to study the electronic properties of graphite inter...
We used hard X-ray photoelectron spectroscopy (HAXPES) with 8 keV X-rays to investigate the Is emiss...
Electron-energy-loss spectra of stage-1 K-intercalated graphite single crystals were obtained with a...
The dielectric function ϵ(q,ω) of potassium intercalated graphite (KC8) with q| c-axis was deduced f...
The dielectric function ϵ(q,ω) of potassium intercalated graphite (KC8) with q| c-axis was deduced f...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
Optical spectroscopy (Raman, FTIR and Reflection ) was used to study a variety of acceptor- and dono...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
The physical and electronic structure of the dispersed and (2×2) phases of K/graphite have been char...
The Shubnikov-deHaas (SdH) effect has been used to study the electronic properties of graphite inter...
Electrons in isolated graphene layers are a two-dimensional gas of massless Dirac Fermions. In reali...
We used hard X-ray photoelectron spectroscopy (HAXPES) with 8 keV X-rays to investigate the 1s emiss...
The Shubnikov-deHaas (SdH) effect has been used to study the electronic properties of graphite inter...
We used hard X-ray photoelectron spectroscopy (HAXPES) with 8 keV X-rays to investigate the Is emiss...