Abstract
M.Sc.
This dissertation presents experimental data on the near Fermi-level electronic structure of Sr₄Ru₃O₁₀.
This summary gives a review of the facts that have been observed in the analysis of the data taken, and
directions for future work are suggested.
The first part of this dissertation (from chapter 1 to chapter 3) is dedicated to a review on the studied
system and the experimental technique exploited in this study. In fact, chapter 1 gives a review of
the general physical properties of different members of the Ruddlesden Popper strontium ruthenate
family Srn+1RunO3n+1, focusing on the trilayered Sr4Ru3O10 in particular. Furthermore, chapters 2
and 3 discuss some essential features of the theoretical and experimental aspects of angle resolved
photoemission spectroscopy (ARPES), respectively. In the second part of the dissertation (chapter 4),
the fi rst experimental ARPES data on band dispersions and Fermi surface maps of Sr4Ru3O10, are
presented and discussed.
The experiment was performed at the beamline Cassiopee of the Soleil synchrotron radiation facility in
Paris (France). The study has provided the first information on the near Fermi-level band dispersions
and Fermi surface of Sr4Ru3O10, the effect of changing different matrix elements on electronic band
dispersions and Fermi surface maps of Sr4Ru3O10, and electronic correlations effects present in this
compound.
Remarkably, low temperature ( 5 K) ARPES data presented in this study suggest that there is only a
45 rotation of the square unit cell of Sr4Ru3O10, due to correlated rotations about the c-axis of the
RuO6 octahedra, but no elongation of the sides of this unit cell; and consequently in reciprocal space
the square BZ, determined by considering the symmetry of the Fermi surface sheets, is only rotated by
45 but its size is unchanged with respect to the non-distorted situation. However, this is not what
is expected. Using room temperature lattice parameters from ref. [17], the BZ of this compound
would be 45 rotated and reconstructed into a square twice smaller, a situation that was also previously
observed in band structure calculations and ARPES data of Sr3Ru2O7 from ref. [4]. This behaviour
was ascribed to the fact that the structure of this system is possibly not the same at room temperature
as at low temperatures (down to 5 K), where the ARPES data of this work were acquired. Therefore
low temperature (<100 K) X-ray diffraction data of Sr4Ru3O10 are needed in order to determine low
temperature lattice parameters and compare them with room temperature ones so as to verify whether
the structure of Sr4Ru3O10 is not the same at room and low temperatures.