5 research outputs found

    Unusual chemical bond and spectrum of beryllium dimer in ground X1Ξ£g+X^1\Sigma_g^+ state

    Full text link
    This review outlines the main results which show the dual nature of the chemical bond in diatomic beryllium molecule in the ground X1Ξ£g+X^1\Sigma_g^+ state. It has been shown that the beryllium atoms are covalently bound at low-lying vibrational energy levels ({\nu}=0-4), while at higher ones ({\nu}=5-11) they are bound by van der Waals forces near the right turning points. High precision ab initio quantum calculations of Be2_2 resulted in the development of the modified expanded Morse oscillator potential function which contains all twelve vibrational energy levels [A.V. Mitin, Chem. Phys. Lett. 682, 30 (2017)]. The dual nature of chemical bond in Be2_2 is evidenced as a sharp corner on the attractive branch of the ground state potential curve. Moreover, it has been found that the Douglas-Kroll-Hess relativistic corrections also show a sharp corner when presented in dependence on the internuclear separation. The difference in energy between the extrapolated and calculated multi-reference configuration interaction energies in dependence on the internuclear separation also exhibits singular point in the same region. The other problems of ab initio quantum calculations of the beryllium dimer are also discussed. Calculated spectrum of vibrational-rotational bound states and new metastable states of the beryllium dimer in the ground state important for laser spectroscopy are presented. The vibration problem was solved for the modified expanded Morse oscillator potential function and for the potential function obtained with Slater-type orbitals [M. Lesiuk et al, Chem. Theory Comput. 15, 2470 (2019)]. The theoretical upper and lower estimates of the spectrum of vibrational-rotational bound states and the spectrum of rotational-vibrational metastable states with complex-valued energy eigenvalues and the scattering length in the beryllium dimer are presented

    ΠœΠ΅Ρ‚ΠΎΠ΄ ΠΊΠΎΠ½Π΅Ρ‡Π½Ρ‹Ρ… элСмСнтов для исслСдования ΠΊΠ²Π°Π½Ρ‚ΠΎΠ²Ρ‹Ρ… систСм Π½Π΅ΡΠΊΠΎΠ»ΡŒΠΊΠΈΡ… частиц : ΡΠΏΠ΅Ρ†ΠΈΠ°Π»ΡŒΠ½ΠΎΡΡ‚ΡŒ 05.13.18 "ΠœΠ°Ρ‚Π΅ΠΌΠ°Ρ‚ΠΈΡ‡Π΅ΡΠΊΠΎΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈΡ€ΠΎΠ²Π°Π½ΠΈΠ΅, числСнныС ΠΌΠ΅Ρ‚ΠΎΠ΄Ρ‹ ΠΈ комплСксы ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌ" : Π°Π²Ρ‚ΠΎΡ€Π΅Ρ„Π΅Ρ€Π°Ρ‚ диссСртации Π½Π° соисканиС ΡƒΡ‡Π΅Π½ΠΎΠΉ стСпСни Π΄ΠΎΠΊΡ‚ΠΎΡ€Π° Ρ„ΠΈΠ·ΠΈΠΊΠΎ-матСматичСских Π½Π°ΡƒΠΊ

    Get PDF
    Π’ диссСртации Ρ€Π°Π·Ρ€Π°Π±ΠΎΡ‚Π°Π½ алгоритмичСский ΠΏΠΎΠ΄Ρ…ΠΎΠ΄ ΠΊ ΠΏΠΎΡΡ‚Ρ€ΠΎΠ΅Π½ΠΈΡŽ Π²Ρ‹Ρ‡ΠΈΡΠ»ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… схСм ΠΌΠ΅Ρ‚ΠΎΠ΄Π° ΠΊΠΎΠ½Π΅Ρ‡Π½Ρ‹Ρ… элСмСнтов высокого порядка точности ΠΈ ΠΌΠ΅Ρ‚ΠΎΠ΄Π° ΠšΠ°Π½Ρ‚ΠΎΡ€ΠΎΠ²ΠΈΡ‡Π° – ΠΏΡ€ΠΈΠ²Π΅Π΄Π΅Π½ΠΈΠ΅ ΠΊ систСмС ΠΎΠ±Ρ‹ΠΊΠ½ΠΎΠ²Π΅Π½Π½Ρ‹Ρ… Π΄ΠΈΡ„Ρ„Π΅Ρ€Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Ρ… ΡƒΡ€Π°Π²Π½Π΅Π½ΠΈΠΉ, ΠΎΡ€ΠΈΠ΅Π½Ρ‚ΠΈΡ€ΠΎΠ²Π°Π½Π½Ρ‹Ρ… Π½Π° Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅ эллиптичСских ΠΊΡ€Π°Π΅Π²Ρ‹Ρ… Π·Π°Π΄Π°Ρ‡ для ΠΌΠ½ΠΎΠ³ΠΎΠΌΠ΅Ρ€Π½ΠΎΠ³ΠΎ уравнСния Π¨Ρ€Π΅Π΄ΠΈΠ½Π³Π΅Ρ€Π° ΠΈ исслСдованиС ΠΊΠ²Π°Π½Ρ‚ΠΎΠ²Ρ‹Ρ… систСм Π½Π΅ΡΠΊΠΎΠ»ΡŒΠΊΠΈΡ… частиц. Π Π°Π±ΠΎΡ‚ΠΎΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡ‚ΡŒ построСнных Π²Ρ‹Ρ‡ΠΈΡΠ»ΠΈΡ‚Π΅Π»ΡŒΠ½Ρ‹Ρ… схСм, созданных числСнных ΠΈ ΡΠΈΠΌΠ²ΠΎΠ»ΡŒΠ½Ρ‹Ρ… (ΠΊΠΎΠΌΠΏΡŒΡŽΡ‚Π΅Ρ€Π½ΠΎβ€“Π°Π»Π³Π΅Π±Ρ€Π°ΠΈΡ‡Π΅ΡΠΊΠΈΡ…) Π°Π»Π³ΠΎΡ€ΠΈΡ‚ΠΌΠΎΠ² ΠΈ Ρ€Π΅Π°Π»ΠΈΠ·ΡƒΡŽΡ‰ΠΈΡ… ΠΈΡ… проблСмно–ориСнтированных комлСксов ΠΏΡ€ΠΎΠ³Ρ€Π°ΠΌΠΌ дСмонстрируСтся числСнным Π°Π½Π°Π»ΠΈΠ·ΠΎΠΌ Ρ‚ΠΎΡ‡Π½ΠΎβ€“Ρ€Π΅ΡˆΠ°Π΅ΠΌΡ‹Ρ… Π·Π°Π΄Π°Ρ‡ ΠΈ эталонных Π·Π°Π΄Π°Ρ‡ с извСстным Ρ€Π΅ΡˆΠ΅Π½ΠΈΠ΅ΠΌ, Π° Ρ‚Π°ΠΊΠΆΠ΅ физичСски интСрСсных ΠΊΠΎΠ½Ρ„ΠΈΠ³ΡƒΡ€Π°Ρ†ΠΈΠΉ ΠΈ рСзонансных процСссов, Π²ΠΎΠ·ΠΌΠΎΠΆΠ½Ρ‹Ρ… Π² ΠΊΠ²Π°Π½Ρ‚ΠΎΠ²ΠΎΠΉ систСмС Π½Π΅ΡΠΊΠΎΠ»ΡŒΠΊΠΈΡ… частиц: фотоабсорбции Π² ансамблях Π°ΠΊΡΠΈΠ°Π»ΡŒΠ½ΠΎβ€“ΡΠΈΠΌΠΌΠ΅Ρ‚Ρ€ΠΈΡ‡Π½Ρ‹Ρ… ΠΊΠ²Π°Π½Ρ‚ΠΎΠ²Ρ‹Ρ… Ρ‚ΠΎΡ‡Π΅ΠΊ, кулоновского рассСяния элСктрона Π² ΠΌΠ°Π³Π½ΠΈΡ‚Π½ΠΎΠΌ ΠΏΠΎΠ»Π΅ ΠΈ Ρ„ΠΎΡ‚ΠΎΠΈΠΎΠ½ΠΈΠ·Π°Ρ†ΠΈΠΈ Π°Ρ‚ΠΎΠΌΠ° Π²ΠΎΠ΄ΠΎΡ€ΠΎΠ΄Π°, рассСяния Π΄Π²ΡƒΡ…Π°Ρ‚ΠΎΠΌΠ½ΠΎΠΉ ΠΌΠΎΠ»Π΅ΠΊΡƒΠ»Ρ‹ Π½Π° ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½ΠΎΠΌ Π±Π°Ρ€ΡŒΠ΅Ρ€Π΅ ΠΈΠ»ΠΈ Π½Π° Π°Ρ‚ΠΎΠΌΠ΅, туннСлирования кластСра Π½Π΅ΡΠΊΠΎΠ»ΡŒΠΊΠΈΡ… тоТдСствСнных ΠΊΠ²Π°Π½Ρ‚ΠΎΠ²Ρ‹Ρ… частиц Ρ‡Π΅Ρ€Π΅Π· ΠΏΠΎΡ‚Π΅Π½Ρ†ΠΈΠ°Π»ΡŒΠ½Ρ‹Π΅ Π±Π°Ρ€ΡŒΠ΅Ρ€Ρ‹ ΠΈ ямы
    corecore