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2019, Journal of Physics: Condensed Matter
Previous luminescence and absorption experiments in Co-doped ZnO revealed two ionization and one intrashell transition of d(Co 2+ ) electrons. Those optical properties are analyzed within the generalized gradient approximation to the density functional theory. The two ionization channels involve electron excitations from the two Co 2+ gap states, the t 2↑ triplet and the e 2↓ doublet, to the conduction band. The third possible ionization channel, in which an electron is excited from the valence band to the Co 2+ level, requires energy in excess of 4 eV, and cannot lead to absorption below the ZnO band gap, contrary to earlier suggestions. We also consider two recombination channels, the direct recombination and a two-step process, in which a photoelectron is captured by Co 3+ and then recombines via the internal transition. Finally, the observed increase the band gap with the Co concentration is well reproduced by theory. The accurate description of ZnO:Co is achieved after including +U corrections to the relevant orbitals of Zn, O, and Co. The +U (Co) value was calculated by the linear response approach, and independently was obtained by fitting the calculated transition energies to the optical data. The respective values, 3.4 and 3.0 eV, agree well. Ionization of Co induces large energy shifts of the gap levels, driven by the varying Coulomb coupling between the d(Co) electrons, and by large lattice relaxations around Co ions. In turn, over ∼ 1 eV changes of Co 2+ levels induced by the internal transition are mainly caused by the occupation-dependent U (Co) corrections.
Physical Review B, 2004
A systematic local spin density approximation ͑LSDA͒ + U study of doping effects on the electronic and structural properties of single layer CoO 2 is presented. Undoped CoO 2 is a charge transfer insulator within LSDA+ U and a metal with a high density of states (DOS) at the Fermi level within LSDA. ͑CoO 2 ͒ 1.0− , on the other hand, is a band insulator with a gap of 2.2 eV. Systems with fractional doping are metals if no charge orderings are present. Due to the strong interaction between the doped electron and other correlated Co d electrons, the calculated electronic structure of ͑CoO 2 ͒ x− depends sensitively on the doping level x. Zone center optical phonon energies are calculated under the frozen phonon approximation and are in good agreement with measured values. Softening of the E g phonon at doping x ϳ 0.25 seems to indicate a strong electron-phonon coupling in this system. Possible intermediate spin states of Co ions, Na ordering, as well as magnetic and charge orderings in this system are also discussed.
Journal of Physics B: …, 2004
High level ab initio calculations have been undertaken of potential energy curves of CO 2+ (and for the CO neutral ground state). The accuracy of the potentials was tested by a synthesis of the available vibrationally resolved threshold photoelectrons in coincidence (TPEsCO) and time of flight, photo electron photo electron coincidence (TOF-PEPECO) spectra of CO 2+ . Good agreement was found between experimental and theoretical spectra once relative energies of the calculated double ionization energies were slightly adjusted (by approximately 1%) to match experiment. Vibrational separations within individual electronic states are very well reproduced (the worst error is 0.07%).
Physical Review B, 2006
We present a crystal field theory of transition metal impurities in semiconductors in a trigonally distorted tetrahedral coordination. We develop a perturbative scheme to treat covalency effects within the weak ligand field case (Coulomb interaction dominates over one-particle splitting) and apply it to ZnO:Co 2+ (3d 7). Using the large value of the charge transfer energy ∆ pd compared to the p-d hoppings, we perform a canonical transformation which eliminates the coupling with ligands to first order. As a result, we obtain an effective single-ion Hamiltonian, where the influence of the ligands is reduced to the one-particle 'crystal field' acting on d-like-functions. This derivation allows to elucidate the microscopic origin of various 'crystal field' parameters and covalency reduction factors which are usually used empirically for the interpretation of optical and electron spin resonance experiments. The connection of these parameters with the geometry of the local environment becomes transparent. The experimentally known g-values and the zero-field splitting 2D are very well reproduced by the exact diagonalization of the effective single-ion Hamiltonian with only one adjustable parameter ∆ pd. Alternatively to the numerical diagonalization we use perturbation theory in the weak field scheme (Coulomb interaction ≫ cubic splitting ≫ trigonal splitting and spin-orbit coupling) to derive compact analytical expressions for the spin-Hamiltonian parameters that reproduce the result of exact diagonalization within 20% of accuracy.
Phys. Chem. Chem. Phys., 2015
The state-to-state photodissociation Q3 of CO 2 is investigated in the VUV range of 11.94-12.20 eV by using two independently tunable vacuum ultraviolet (VUV) lasers and the time-sliced velocity-map-imaging-photoion (VMI-PI) method.
Chemical Physics, 1981
An extended CNDO formalism for the treatment of large transition metal cluster systems is presented. After a detailed discussion of parametrization it is applied to a family of compounds, namely to Co(CO)~-, Co2(CO)s, Co~(CO)12, Mn2(CO)lo.
The Journal of Physical Chemistry C, 2017
In the present study, valence band (VB) and core level photoelectron spectroscopy was carried out to investigate the electronic structural changes from polycrystalline Co to spinel Co 3 O 4 , via CoO at near ambient pressures (NAP; ~0.1 mbar). O 2-Co and H 2-CoO x gas-solid oxidative and reductive interactions, respectively, has been explored with UV photons (He-I) or low kinetic energy electrons (≤16 eV) at NAP conditions. Typical VB features of Co metal, CoO, Co 3 O 4 and a mixed phase between any two adjacent features were observed and well corroborated with core level changes. Very significant and characteristic changes were observed with Co 3d features in the VB for each stage from Co oxidation to Co 3 O 4 as well as Co 3 O 4 reduction to CoO. Co 3 O 4 and CoO can be reversibly obtained by alternating the conditions between 0.1 mbar H 2 /650 K and 0.1 mbar O 2 at 400 K, respectively. A meaningful correlation is observed between the changes in work function with cation oxidation state; small changes in the stoichiometry can strongly influence the shift in Fermi level and changes in work function under NAP conditions. Reversible work function changes are observed between oxidation and reduction conditions. While O 2p derived feature for CoO x was observed at a constant BE (~5 eV) throughout the redox conditions, Co 3d band and molecular oxygen or hydrogen vibration feature shifts significantly underscoring the physicochemical changes, such as charge transfer energy and hence changes in satellite intensity. The peak close to E F originated from the 3d 6 L final state of the octahedral Co 3+ 3d band of Co 3 O 4 .
International Journal of Mass Spectrometry, 2003
Reactivity of the dication CO 2 2+ in dependence on its internal energy was studied in collision with CO 2 and CO. The dication was obtained by photoionization of the CO 2 molecule by synchrotron radiation and the guided beam apparatus CERISES was used in these studies. Spontaneous dissociation of CO 2 2+ to CO + and O + was observed without any target gas in the reaction cell. With CO 2 or CO as a target gas, CO + and O + fragment ions were formed as products of dissociative charge transfer, while the contribution of collision-induced dissociation of the reactant CO 2 2+ to their formation was found negligible. The CO + yield showed a considerable dependence on the internal energy of the reactant dication CO 2 2+ : the branching ratio CO + /O + increased gradually with photon energy between 38.7 and 39.4 eV. We interpret this observation as being due to the increase in the instantaneous distances at the extrema of vibrational motion of the dication with increasing internal energy. This modifies the Franck-Condon factors in the charge transfer process and leads to a preferential population of the vibrationally excited states of the product cation CO 2 + (C) known to lead exclusively to the dissociation products CO + + O. An indirect mechanism that requires the coupling of the first excited (a) state of the dication with the higher vibrational states of the CO 2 2+ (X) state is proposed to explain the threshold behaviour observed in our results.
Chemical Physics Letters, 1999
. The zero kinetic energy ZEKE photoelectron spectrum of CO has been obtained from 22.3-23.75 eV with resolution of 2 Ž q . 2 q Ž q . 0.7 meV and shows the structure of the D P Õ s 0-8 and 3 S Õ s 0-4 bands. The intensity with which these are formed at threshold, band origins, rotational constants and spin orbit splittings of the D 2 P state are reported. The decreased lifetimes of the D 2 P, Õ q s 3, 4 levels are also recorded. All states observed are above the lowest dissociation limit of the ion, and these spectra provide information about the intramolecular dynamics in this high energy region. q
Physical Review B
We present a many-body diffusion quantum Monte Carlo (DMC) study on the ground and excited state properties of crystalline CoO polymorphs. To our knowledge, DMC is the only electronic structure method available to provide correct energetic ordering within experimental error bars between the three CoO polymorphs: Rocksalt, Wurtzite, and Zincblende. We compare these results to density functional theory (DFT) using state-of-the-art functionals such as SCAN. For the structural properties, such as the lattice parameters and bulk moduli, our results are comparable to HSE and SCAN. Using DMC, we calculated the indirect and direct optical gaps as 3.8(2) and 5.2(2) eV. Our indirect optical gap compares well with the conductivity measurements of 3.6(5) eV and GW calculations with 3.4 eV. Similarly, we obtained the DMC indirect and direct quasiparticle gaps as 3.9(2) and 5.5(2) eV. DMC direct quasiparticle gaps compare well with the direct band gap of 5.53 eV obtained from ellipsometry studies.
Chemistry of Materials, 2014
This work investigates the electronic structure and photoluminescence properties of Co 2+ -doped ZnO and their pressure and temperature dependences through high-resolution absorption and emission spectroscopy as a function of Co 2+ concentration and their structural conformations as a single crystal, thin film, nanowire, and nanoparticle. Absorption and emission spectra of diluted ZnO:Co 2+ (0.01 mol %) can be related to the 4 T 1 (P) → 4 A 2 (F) transition of CoO 4 (T d ), contrary to MgAl 2 O 4 :Co 2+ and ZnAl 2 O 4 :Co 2+ spinels in which the red emission is ascribed to the 2 E(G) → 4 A 2 (F) transition. We show that the low-temperature emission band consists of a 4 T 1 (P) zero-phonon line and a phonon-sideband, which is described in terms of the phonon density of states within an intermediate coupling scheme (S = 1.35) involving all ZnO lattice phonons. Increasing pressure to the sample shifts the zerophonon line to higher energy as expected for the 4 T 1 (P) state upon compression. The low-temperature emission quenches above 5 GPa as a consequence of the pressure-induced wurtzite to rocksalt structural phase transition, yielding a change of Co 2+ coordination from 4-fold T d to 6-fold O h . We also show that the optical properties of ZnO:Co 2+ (T d ) are similar, independent of the structural conformation of the host and the cobalt concentration. The Co 2+ enters into regular Zn 2+ sites in low concentration systems (less than 5% of Co 2+ ), although some slight shifts and peak broadening appear as the dimensionality of the sample decreases. These structural effects on the optical spectra are also supported by Raman spectroscopy.
The Journal of Physical Chemistry C, 2009
Linear response time-dependent hybrid density functional theory has been applied for the first time to describe optical transitions characteristic of Co 2+-and Mn 2+-doped ZnO quantum dots (QDs) with sizes up to 300 atoms (∼1.8 nm diam) and to investigate QD size effects on the absorption spectra. Particular attention is given to charge-transfer (CT or "photoionization") excited states. For both dopants, CT transitions are calculated to appear at sub-band-gap energies and extend into the ZnO excitonic region. CT transitions involving excitation of dopant d electrons to the ZnO conduction band occur lowest in energy, and additional CT transitions corresponding to promotion of ZnO valence band electrons to the dopant d orbitals are found at higher energies, consistent with experimental results. The CT energies are found to depend on the QD diameter. Analysis of excited-state electron and hole density distributions shows that, for both CT types, the electron and hole are localized to some extent around the impurity ion, which results in "heavier" photogenerated carriers than predicted from simple effective mass considerations. In addition to CT transitions, the Co 2+-doped ZnO QDs also exhibit characteristic d-d excitations whose experimental energies are reproduced well and do not depend on the size of the QD.
Physical Review B - PHYS REV B, 2008
The reflectivity of single-crystalline CoO has been studied by optical spectroscopy for wave numbers ranging from 100 to 28000cm-1 and for temperatures 8<T<325K . A splitting of the cubic IR-active phonon mode on passing the antiferromagnetic phase transition at TN=289K has been observed. At low temperatures the splitting amounts to 15.0cm-1 . In addition, we studied the splitting of the cubic crystal-field ground state of the Co2+ ions due to spin-orbit coupling, a tetragonal crystal field, and exchange interaction. Below TN , magnetic-dipole transitions between the exchange-split levels are identified, and the energy-level scheme can be well described with a spin-orbit coupling lambda=151.1cm-1 , an exchange constant J=17.5cm-1 , and a tetragonal crystal-field parameter D=-47.8cm-1 . Already in the paramagnetic state electric-quadrupole transitions between the spin-orbit split level have been observed. At high frequencies, two electronic levels of the crystal-field-split d m...
Chemical Physics, 2001
The photoionization of CO is studied with ab initio and density functional theory (DFT) methods. The interactive channel and separate channel random phase approximation with polynomial Gaussian type orbitals is employed for ab initio calculations. The DFT method employed consists in the time-dependent version of the theory (TD-DFT) employing a basis set of B-spline functions. The performances of the two theoretical methods are compared to each other and with experimental data. The two methods are both competitive for an accurate description of the phenomenon. Ó
Chemical Physics Letters, 2012
Molecular dissociation following radiative decay of O 1s hole states in CO 2 has been studied by detecting photoions in coincidence with undispersed soft X-ray emission. The production of ions after radiative decay is observed to increase from practically nothing at the O 1s ? p ⁄ excitation to the appearance of CO þ 2 , CO + , C + and O + ions when core-valence double excitations and O 1s shake-up transitions are induced. De-excitation pathways involving radiative decay from different core-hole states are discussed in order to interpret the results. A weak CO 2þ 2 signal is attributed to the radiative Auger effect.
Journal of Physics B, 2011
Oxygen Is excitation and ionization processes in the CO2 molecule have been studied with dispersed and non-dispersed fluorescence spectroscopy as well as with the vacuum ultraviolet (VUV) photon-photoion coincidence technique. The intensity of the neutral O emission line at 845 nm shows particular sensitivity to core-to-Rydberg excitations and core-valence double excitations, while shape resonances are suppressed. In contrast, the partial fluorescence yield in the wavelength window 300-650 nm and the excitation functions of selected 0 + and C + emission lines in the wavelength range 400-500 nm display all of the absorption features. The relative intensity of ionic emission in the visible range increases towards higher photon energies, which is attributed to O Is shake-off photoionization. VUV photon-photoion coincidence spectra reveal major contributions from the C + and 0 + ions and a minor contribution from C 2+. No conclusive changes in the intensity ratios among the different ions are observed above the O Is threshold. The line shape of the VUV-0 + coincidence peak in the mass spectrum carries some information on the initial core excitation.
The Journal of Physical Chemistry A, 1998
The photodissociation of Co(CO) 3 NO was studied near 225 nm. Apparent two-photon dissociation of the parent compound produces Co* in a number of excited states that emit in the range of 340-360 nm. Both quartet and doublet states of Co* are observed, implying the existence of spin-conserving and nonspinconserving dissociation channels. Assignment of the Co* emission is used to calculate an upper limit for the average metal-ligand bond dissociation energy of 36.2-38.6 kcal/mol with no spin-conservation restrictions and 41.2-43.9 kcal/mol with spin-conservation restrictions. The Co* emission intensities are used to determine the relative populations of particular J and spin states and to demonstrate that J states within a particular LS configuration are statistically populated. The NO photoproduct was detected by fluorescence excitation spectroscopy. The NO appears to follow dual Boltzmann statistics with rotational temperatures of 580 ( 70 K for E rot < 500 cm -1 and 2800 ( 300 K for E rot > 500 cm -1 .
physica status solidi (RRL) - Rapid Research Letters, 2011
Journal of Electron Spectroscopy and Related Phenomena, 2000
Ab initio MO calculations were performed for three lowest doublet P states of CO using the multireference 2 1 configuration interaction method. Some spectroscopic constants were evaluated also for other low-lying states. For the X S , 2 2 1 A P, and B S states, the calculated spectroscopic constants are in very good agreement with experimental data within the 2 limit of experimental accuracy. In the photoelectron spectra, a series of the vibrational progression assigned to the D 2 P state persists up to v 5 9, whereas the calculated adiabatic potential energy holds only three vibrational levels below a barrier 2 at R 5 1.44 A, which results from an avoided crossing with the upper state, third P. The observed progression was analyzed 2 in terms of the resonant states obtained from the coupling of two strongly interacting diabatic states, second and third P.
Journal of Physical Chemistry C, 2009
Linear response time-dependent hybrid density functional theory has been applied for the first time to describe optical transitions characteristic of Co 2+-and Mn 2+-doped ZnO quantum dots (QDs) with sizes up to 300 atoms (∼1.8 nm diam) and to investigate QD size effects on the absorption spectra. Particular attention is given to charge-transfer (CT or "photoionization") excited states. For both dopants, CT transitions are calculated to appear at sub-band-gap energies and extend into the ZnO excitonic region. CT transitions involving excitation of dopant d electrons to the ZnO conduction band occur lowest in energy, and additional CT transitions corresponding to promotion of ZnO valence band electrons to the dopant d orbitals are found at higher energies, consistent with experimental results. The CT energies are found to depend on the QD diameter. Analysis of excited-state electron and hole density distributions shows that, for both CT types, the electron and hole are localized to some extent around the impurity ion, which results in "heavier" photogenerated carriers than predicted from simple effective mass considerations. In addition to CT transitions, the Co 2+-doped ZnO QDs also exhibit characteristic d-d excitations whose experimental energies are reproduced well and do not depend on the size of the QD.
Physical Review B, 1990
We have performed resonance photoemission, angle-resolved photoemission, and core-level photoemission studies of single-crystalline CoO. On the one hand, strong correlation effects among the d electrons are observed, as signaled by a strong reduction of Co 3d bandwidths and satellites in both the valence band and the cation core levels. On the other hand, the oxygen states are found to be very bandlike, as indicated by strong dispersions of oxygen states in the valence band and the lack of oxygen satellites. We give estimations of 30 and 1.5 for U/8'(Coulomb interaction divided by bandwidth) ratio of Co 3d bands and 0 2p bands, respectively. By comparing the experimental and theoretical F. versus k relation, we show that the density-functiona1 band calculation works well for the oxygen bands but not for the Co bands. We argue that CoO is not a band insulator, but a charge-transfer insulator. We have also observed the effects of local magnetic order on the electronic structure. Finally, we suggest a guideline on calculating the band structure of CoO: introducing a mechanism that reduces the Co 3d bandwidth by 25% while still retaining the other essential features of the band calculation.
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