TY - JOUR
T1 - Evidence for charge localization in the ferromagnetic phase of from high real-space-resolution x-ray diffraction
AU - Billinge, S.
AU - Proffen, Th
AU - Petkov, V.
AU - Sarrao, J.
PY - 2000
Y1 - 2000
N2 - High real-space-resolution atomic pair distribution functions of (Formula presented) 0.25, and 0.33) have been measured using high-energy x-ray powder diffraction to study the size and shape of the (Formula presented) octahedron as a function of temperature and doping. In the paramagnetic insulating phase we find evidence for three distinct bond lengths which we ascribe to (Formula presented)-short, and (Formula presented)-long bonds, respectively. In the ferromagnetic metallic (FM) phase, for (Formula presented) and (Formula presented) we find a single Mn-O bond length; however, as the metal-insulator transition is approached either by increasing T or decreasing x, intensity progressively appears around (Formula presented) and in the region (Formula presented) suggesting the appearance of (Formula presented)-long bonds and short (Formula presented) bonds. This is strong evidence that charge localized and delocalized phases coexist close to the metal-insulator transition in the FM phase.
AB - High real-space-resolution atomic pair distribution functions of (Formula presented) 0.25, and 0.33) have been measured using high-energy x-ray powder diffraction to study the size and shape of the (Formula presented) octahedron as a function of temperature and doping. In the paramagnetic insulating phase we find evidence for three distinct bond lengths which we ascribe to (Formula presented)-short, and (Formula presented)-long bonds, respectively. In the ferromagnetic metallic (FM) phase, for (Formula presented) and (Formula presented) we find a single Mn-O bond length; however, as the metal-insulator transition is approached either by increasing T or decreasing x, intensity progressively appears around (Formula presented) and in the region (Formula presented) suggesting the appearance of (Formula presented)-long bonds and short (Formula presented) bonds. This is strong evidence that charge localized and delocalized phases coexist close to the metal-insulator transition in the FM phase.
UR - http://www.scopus.com/inward/record.url?scp=0000838005&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.62.1203
DO - 10.1103/PhysRevB.62.1203
M3 - Article
AN - SCOPUS:0000838005
SN - 1098-0121
VL - 62
SP - 1203
EP - 1211
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 2
ER -