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T. Detmer

Publications and source records attributed to T. Detmer.

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Ab initio calculations with a nonspherical Gaussian basis set: Excited states of the hydrogen molecule

A basis set of generalized nonspherical Gaussian functions (GGTOs) is presented and discussed. As a first example we report on Born-Oppenheimer energies of the hydrogen molecule. Although accurate results have been obtained, we conclude that H_2 is too 'simple' to allow for a substantial gain by using nonspherical functions. We rather expect that these functions may be particularly useful in calculations on large systems. A single basis set of GGTOs was used to simultaneously calculate the potential energy curves of several states within each subspace of {1,3}Σ_{g,u} symmetry. We hereby considerd the entire region of internuclear distances 0.8 < R < 1000 a.u. In particular the results for the fourth up to sixth electronic states show a high accuracy compared to calculations which invoke explicitely correlated functions, e.g. the relative accuracy is at least of the order of magnitude of 10^{-5}a.u. Energies for the 4 ^1Σ_u^+ and 4-6 ^3Σ_u^+ were improved and accurate data for the 6 ^3Σ_g^+, 5 ^1Σ_u^+, and 6 ^1Σ_u^+ state are, to the best of the authors knowledge, presented for the first time. Energy data for the seventh up to the nineth electronic state within each subspace were obtained with an estimated error of the order of magnitude of 10^{-4}a.u. The 7 ^1Σ_g^+ and the 6 ^1Σ_u^+ state were found to exhibit a very broad deep outer well at large internuclear distances.

physics.chem-ph

The hydrogen molecule in magnetic fields: The ground states of the Sigma manifold of the parallel configuration

The electronic structure of the hydrogen molecule is investigated for the parallel configuration. The ground states of the Sigma manifold are studied for ungerade and gerade parity as well as singlet and triplet states covering a broad regime of field strengths from B = 0 up to B = 100a.u. A variety of interesting phenomena can be observed. For the ^1Sigma_g state we found a monotonous decrease of the equilibrium distance and a simultaneously increase of the dissociation energy with growing magnetic field strength. The ^3Σ_g state is shown to develop an additional minimum which has no counterpart in field-free space. The ^1Σ_u state shows a monotonous increase in the dissociation energy with first increasing and than decreasing internuclear distance of the minimum. For this state the dissociation channel is H_2 to H^- + H^+ for magnetic-field strengths B greater than 20a.u. due to the existence of strongly bound H^- states in strong magnetic fields. The repulsive ^3Σ_u state possesses a very shallow van der Waals minimum for magnetic-field strengths smaller than 1.0a.u. within the numerical accuracy of our calculations. The ^1Σ_g and ^3Σ_u states cross as a function of B and the ^3Σ_u state, which is an unbound state, becomes the ground state of the hydrogen molecule in magnetic fields B greater than 0.2a.u. This is of particular interest for the existence of molecular hydrogen in the vicinity of white dwarfs. In superstrong fields the ground state is again a strongly bound state, the ^3Π_u state.

physics.chem-ph

Hydrogen molecule in a magnetic field: The lowest states of the Pi manifold and the global ground state of the parallel configuration

The electronic structure of the hydrogen molecule in a magnetic field is investigated for parallel internuclear and magnetic field axes. The lowest states of the $Π$ manifold are studied for spin singlet and triplet$(M_s = -1) $ as well as gerade and ungerade parity for a broad range of field strengths $0 \leq B \leq 100 a.u.$ For both states with gerade parity we observe a monotonous decrease in the dissociation energy with increasing field strength up to $B = 0.1 a.u.$ and metastable states with respect to the dissociation into two H atoms occur for a certain range of field strengths. For both states with ungerade parity we observe a strong increase in the dissociation energy with increasing field strength above some critical field strength $B_c$. As a major result we determine the transition field strengths for the crossings among the lowest $^1Σ_g$, $^3Σ_u$ and $^3Π_u$ states. The global ground state for $B \lesssim 0.18 a.u.$ is the strongly bound $^1Σ_g$ state. The crossings of the $^1Σ_g$ with the $^3Σ_u$ and $^3Π_u$ state occur at $B \approx 0.18$ and $B \approx0.39 a.u.$, respectively. The transition between the $^3Σ_u$ and $^3Π_u$ state occurs at $B \approx 12.3 a.u.$ Therefore, the global ground state of the hydrogen molecule for the parallel configuration is the unbound $^3Σ_u$ state for $0.18 \lesssim B \lesssim 12.3 a.u.$ The ground state for $B \gtrsim 12.3 a.u.$ is the strongly bound $^3Π_u$ state. This result is of great relevance to the chemistry in the atmospheres of magnetic white dwarfs and neutron stars.

physics.chem-ph