154 research outputs found
Inferring possible magnetic field strength of accreting inflows in EXor-type objects from scaled laboratory experiments
Aims. EXor-type objects are protostars that display powerful UV-optical outbursts caused by intermittent and powerful events of magnetospheric accretion. These objects are not yet well investigated and are quite difficult to characterize. Several parameters, such as plasma stream velocities, characteristic densities, and temperatures, can be retrieved from present observations. As of yet, however, there is no information about the magnetic field values and the exact underlying accretion scenario is also under discussion. Methods. We use laboratory plasmas, created by a high power laser impacting a solid target or by a plasma gun injector, and make these plasmas propagate perpendicularly to a strong external magnetic field. The propagating plasmas are found to be well scaled to the presently inferred parameters of EXor-type accretion event, thus allowing us to study the behaviour of such episodic accretion processes in scaled conditions. Results. We propose a scenario of additional matter accretion in the equatorial plane, which claims to explain the increased accretion rates of the EXor objects, supported by the experimental demonstration of effective plasma propagation across the magnetic field. In particular, our laboratory investigation allows us to determine that the field strength in the accretion stream of EXor objects, in a position intermediate between the truncation radius and the stellar surface, should be of the order of 100 G. This, in turn, suggests a field strength of a few kilogausses on the stellar surface, which is similar to values inferred from observations of classical T Tauri stars
Π£Π»ΡΡΡΠ°ΡΠΈΠΎΠ»Π΅ΡΠΎΠ²ΠΎΠ΅ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΠ΅ ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΠΎβΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΈΡ ΡΠ°Π·ΡΡΠ΄ΠΎΠ² Π²ΡΡΠΎΠΊΠΎΠ³ΠΎ Π΄Π°Π²Π»Π΅Π½ΠΈΡ Π² ΠΊΡΠ΅Π½ΠΎΠ½Π΅
Pulsed quartz-jacketed high-pressure xenon lamps, operating in the periodic pulse repetition modes, despite the appearing UV radiation sources of other types, remain a critical component of the processing equipment used in photochemistry, photo-medicine, nanoelectronics, biology, etc. Their main advantages, namely high power and radiation energy are slightly devalued by a relatively low efficiency of the shortwave radiation. Available literature data concerning the influence of various factors on the energy level of short-wave radiation in xenon need to be systematised and generalised because they have been obtained under conditions of uncontrolled quartz-jacketed transmission. The transmission of quartz can degrade after a while and, in addition, undergo great changes during the pulse. Besides, as a rule, in the literature, there is no detailed description of a complete kit of experimental setting. As a result, to analyse the factors affecting the efficiency of studying in the UV range is difficult, and there arises a relevant problem to optimise this type of discharge parameters to increase the efficiency in the range of 220-400 nm. A mathematical model of the radiation source, realistically describing the processes in the xenon plasma and in the stabilising envelope, can be a reliable ground for such a study. The paper shows an impact of the discharge channel diameter and length, the filling pressure of xenon, the pulse duration, the parameters of discharge circuit, and the current of pilot arc on the radiation yield. Based on the simulation-found relationship of internal plasma parameters (temperature distributions, fields of particle concentration and radiation, dynamics of electrical resistance of discharge channel, and plasma emission spectra) with radiation characteristics of discharge, are determined conditions to ensure the greatest radiation yield in the UV region. Β The experimental data prove the computational results. A material obtained gives practice-critical guidelines for development and correct selection of the short-wave radiation source.ΠΠΌΠΏΡΠ»ΡΡΠ½ΡΠ΅ ΠΊΡΠ΅Π½ΠΎΠ½ΠΎΠ²ΡΠ΅ Π»Π°ΠΌΠΏΡ Π²ΡΡΠΎΠΊΠΎΠ³ΠΎ Π΄Π°Π²Π»Π΅Π½ΠΈΡ Π² ΠΊΠ²Π°ΡΡΠ΅Π²ΠΎΠΉ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠ΅, ΡΠ°Π±ΠΎΡΠ°ΡΡΠΈΠ΅ Π² ΡΠ΅ΠΆΠΈΠΌΠ°Ρ
ΠΏΠ΅ΡΠΈΠΎΠ΄ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΡ ΠΈΠΌΠΏΡΠ»ΡΡΠΎΠ², Π½Π΅ΡΠΌΠΎΡΡΡ Π½Π° ΠΏΠΎΡΠ²Π»Π΅Π½ΠΈΠ΅ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠΎΠ² Π£Π€- ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π΄ΡΡΠ³ΠΈΡ
ΡΠΈΠΏΠΎΠ² ΠΎΡΡΠ°ΡΡΡΡ Π²Π°ΠΆΠ½Π΅ΠΉΡΠΈΠΌ ΠΊΠΎΠΌΠΏΠΎΠ½Π΅Π½ΡΠΎΠΌ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΠΎΠ±ΠΎΡΡΠ΄ΠΎΠ²Π°Π½ΠΈΡ, ΠΏΡΠΈΠΌΠ΅Π½ΡΠ΅ΠΌΠΎΠ³ΠΎ Π² ΡΠΎΡΠΎΡ
ΠΈΠΌΠΈΠΈ, ΡΠΎΡΠΎΠΌΠ΅Π΄ΠΈΡΠΈΠ½Π΅, Π½Π°Π½ΠΎΡΠ»Π΅ΠΊΡΡΠΎΠ½ΠΈΠΊΠ΅, Π±ΠΈΠΎΠ»ΠΎΠ³ΠΈΠΈ ΠΈ Ρ.Π΄. ΠΠ»Π°Π²Π½ΡΠ΅ ΠΈΡ
Π΄ΠΎΡΡΠΎΠΈΠ½ΡΡΠ²Π° -Β Π²ΡΡΠΎΠΊΠ°Ρ ΠΌΠΎΡΠ½ΠΎΡΡΡ ΠΈ ΡΠ½Π΅ΡΠ³ΠΈΡ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ - Π½Π΅ΡΠΊΠΎΠ»ΡΠΊΠΎ ΠΎΠ±Π΅ΡΡΠ΅Π½ΠΈΠ²Π°Π΅Ρ ΠΎΡΠ½ΠΎΡΠΈΡΠ΅Π»ΡΠ½ΠΎ Π½ΠΈΠ·ΠΊΠ°Ρ ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π² ΠΊΠΎΡΠΎΡΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠΉ ΠΎΠ±Π»Π°ΡΡΠΈ. ΠΠΌΠ΅ΡΡΠΈΠ΅ΡΡ Π»ΠΈΡΠ΅ΡΠ°ΡΡΡΠ½ΡΠ΅ Π΄Π°Π½Π½ΡΠ΅ ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠΈ ΡΠ°Π·Π»ΠΈΡΠ½ΡΡ
ΡΠ°ΠΊΡΠΎΡΠΎΠ² Π½Π° ΡΡΠΎΠ²Π΅Π½Ρ ΡΠ½Π΅ΡΠ³ΠΈΠΈ ΠΊΠΎΡΠΎΡΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΡΠ°Π·ΡΡΠ΄ΠΎΠ² Π² ΠΊΡΠ΅Π½ΠΎΠ½Π΅ Π½ΡΠΆΠ΄Π°ΡΡΡΡ Π² ΡΠΈΡΡΠ΅ΠΌΠ°ΡΠΈΠ·Π°ΡΠΈΠΈ ΠΈ ΠΎΠ±ΠΎΠ±ΡΠ΅Π½ΠΈΠΈ, Ρ.ΠΊ. ΠΎΠ½ΠΈ ΠΏΠΎΠ»ΡΡΠ΅Π½Ρ Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
Π½Π΅ΠΊΠΎΠ½ΡΡΠΎΠ»ΠΈΡΡΠ΅ΠΌΠΎΠ³ΠΎ Π·Π½Π°ΡΠ΅Π½ΠΈΡ ΠΏΡΠΎΠΏΡΡΠΊΠ°Π½ΠΈΡ ΠΊΠ²Π°ΡΡΠ΅Π²ΠΎΠΉ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΈ. ΠΡΠΎΠΏΡΡΠΊΠ°Π½ΠΈΠ΅ ΠΊΠ²Π°ΡΡΠ° ΠΌΠΎΠΆΠ΅Ρ Π΄Π΅Π³ΡΠ°Π΄ΠΈΡΠΎΠ²Π°ΡΡ ΡΠΎ Π²ΡΠ΅ΠΌΠ΅Π½Π΅ΠΌ ΠΈ, ΠΊΡΠΎΠΌΠ΅ ΡΠΎΠ³ΠΎ,Β ΡΠΈΠ»ΡΠ½ΠΎ ΠΌΠ΅Π½ΡΡΡΡΡ Π² ΡΠ΅ΡΠ΅Π½ΠΈΠ΅ ΠΈΠΌΠΏΡΠ»ΡΡΠ°. ΠΡΠΎΠΌΠ΅ ΡΠΎΠ³ΠΎ,Β Π² Π»ΠΈΡΠ΅ΡΠ°ΡΡΡΠ΅ ΠΎΡΡΡΡΡΡΠ²ΡΠ΅Ρ, ΠΊΠ°ΠΊ ΠΏΡΠ°Π²ΠΈΠ»ΠΎ, Π΄Π΅ΡΠ°Π»ΡΠ½ΠΎΠ΅ ΠΎΠΏΠΈΡΠ°Π½ΠΈΠ΅ ΠΏΠΎΠ»Π½ΠΎΠ³ΠΎ Π½Π°Π±ΠΎΡΠ° ΡΡΠ»ΠΎΠ²ΠΈΠΉ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°. Π ΠΈΡΠΎΠ³Π΅ Π°Π½Π°Π»ΠΈΠ· ΡΠ°ΠΊΡΠΎΡΠΎΠ², Π²Π»ΠΈΡΡΡΠΈΡ
Π½Π°Β ΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡ ΠΈΠ·ΡΡΠ΅Π½ΠΈΡ Π² Π£Π€- ΠΎΠ±Π»Π°ΡΡΠΈ Π·Π°ΡΡΡΠ΄Π½Π΅Π½, ΠΈ Π²ΠΎΠ·Π½ΠΈΠΊΠ°Π΅Ρ Π°ΠΊΡΡΠ°Π»ΡΠ½Π°Ρ Π·Π°Π΄Π°ΡΠ° ΠΎΠΏΡΠΈΠΌΠΈΠ·Π°ΡΠΈΠΈ ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΡΠ°Π·ΡΡΠ΄ΠΎΠ² ΡΠΊΠ°Π·Π°Π½Π½ΠΎΠ³ΠΎ ΡΠΈΠΏΠ° Ρ ΡΠ΅Π»ΡΡ ΡΠ²Π΅Π»ΠΈΡΠ΅Π½ΠΈΡ ΠΠΠ Π² ΠΎΠ±Π»Π°ΡΡΠΈ 220-400 Π½ΠΌ. ΠΠ°Π΄Π΅ΠΆΠ½ΠΎΠΉ ΠΎΡΠ½ΠΎΠ²ΠΎΠΉ Π΄Π»Ρ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ ΡΠ°ΠΊΠΎΠΉ ΡΠ°Π±ΠΎΡΡ ΠΌΠΎΠΆΠ΅Ρ ΡΠ»ΡΠΆΠΈΡΡ ΡΠ°ΡΡΠ΅ΡΠ½ΠΎ- ΡΠ΅ΠΎΡΠ΅ΡΠΈΡΠ΅ΡΠΊΠΎΠ΅ ΠΈΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ Ρ ΠΏΠΎΠΌΠΎΡΡΡΒ ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ° ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ, ΡΠ΅Π°Π»ΠΈΡΡΠΈΡΠ½ΠΎ ΠΎΠΏΠΈΡΡΠ²Π°ΡΡΠ΅ΠΉ ΠΏΡΠΎΡΠ΅ΡΡΡ Π² ΠΏΠ»Π°Π·ΠΌΠ΅ ΠΊΡΠ΅Π½ΠΎΠ½Π° ΠΈ ΡΡΠ°Π±ΠΈΠ»ΠΈΠ·ΠΈΡΡΡΡΠ΅ΠΉ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠ΅. Π ΡΠ°Π±ΠΎΡΠ΅Β ΠΏΠΎΠΊΠ°Π·Π°Π½ΠΎ Π²Π»ΠΈΡΠ½ΠΈΠ΅ Π½Π°Β Π²ΡΡ
ΠΎΠ΄ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π΄ΠΈΠ°ΠΌΠ΅ΡΡΠ° ΠΈ Π΄Π»ΠΈΠ½Ρ ΡΠ°Π·ΡΡΠ΄Π½ΠΎΠ³ΠΎ ΠΊΠ°Π½Π°Π»Π°, Π΄Π°Π²Π»Π΅Π½ΠΈΡ Π½Π°ΠΏΠΎΠ»Π½Π΅Π½ΠΈΡ ΠΊΡΠ΅Π½ΠΎΠ½Π°, Π΄Π»ΠΈΡΠ΅Π»ΡΠ½ΠΎΡΡΠΈ ΠΈΠΌΠΏΡΠ»ΡΡΠ°, ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΡΠ°Π·ΡΡΠ΄Π½ΠΎΠ³ΠΎ ΠΊΠΎΠ½ΡΡΡΠ°, ΡΠΎΠΊΠ° Π΄Π΅ΠΆΡΡΠ½ΠΎΠΉ Π΄ΡΠ³ΠΈ. ΠΠ° ΠΎΡΠ½ΠΎΠ²Π΅ ΡΡΡΠ°Π½Π°Π²Π»ΠΈΠ²Π°Π΅ΠΌΠΎΠΉ ΠΏΡΠΈ ΠΌΠΎΠ΄Π΅Π»ΠΈΡΠΎΠ²Π°Π½ΠΈΠΈ ΡΠ²ΡΠ·ΠΈ Π²Π½ΡΡΡΠ΅Π½Π½ΠΈΡ
ΠΏΠ°ΡΠ°ΠΌΠ΅ΡΡΠΎΠ² ΠΏΠ»Π°Π·ΠΌΡ (ΡΠ΅ΠΌΠΏΠ΅ΡΠ°ΡΡΡΠ½ΡΡ
ΡΠ°ΡΠΏΡΠ΅Π΄Π΅Π»Π΅Π½ΠΈΠΉ, ΠΏΠΎΠ»Π΅ΠΉ ΠΊΠΎΠ½ΡΠ΅Π½ΡΡΠ°ΡΠΈΠΈ ΡΠ°ΡΡΠΈΡ ΠΈ ΡΠ°Π΄ΠΈΠ°ΡΠΈΠΈ, Π΄ΠΈΠ½Π°ΠΌΠΈΠΊΠΈ ΡΠ»Π΅ΠΊΡΡΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠΎΠΏΡΠΎΡΠΈΠ²Π»Π΅Π½ΠΈΡ ΠΊΠ°Π½Π°Π»Π° ΡΠ°Π·ΡΡΠ΄Π° ΠΈ ΡΠΏΠ΅ΠΊΡΡΠΎΠ² ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΏΠ»Π°Π·ΠΌΡ) Ρ ΡΠ°Π΄ΠΈΠ°ΡΠΈΠΎΠ½Π½ΡΠΌΠΈ Ρ
Π°ΡΠ°ΠΊΡΠ΅ΡΠΈΡΡΠΈΠΊΠ°ΠΌΠΈ ΡΠ°Π·ΡΡΠ΄Π° ΠΎΠΏΡΠ΅Π΄Π΅Π»Π΅Π½Ρ ΡΡΠ»ΠΎΠ²ΠΈΡ, ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°ΡΡΠΈΠ΅ Π½Π°ΠΈΠ±ΠΎΠ»ΡΡΠΈΠΉ Π²ΡΡ
ΠΎΠ΄ ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ Π² Π£Π€- ΠΎΠ±Π»Π°ΡΡΠΈ. Π Π΅Π·ΡΠ»ΡΡΠ°ΡΡ Π²ΡΡΠΈΡΠ»Π΅Π½ΠΈΠΉΒ ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠΆΠ΄Π΅Π½Ρ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ°Π»ΡΠ½ΡΠΌΠΈ Π΄Π°Π½Π½ΡΠΌΠΈ. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠΉΠΌΠ°ΡΠ΅ΡΠΈΠ°Π» Π΄Π°Π΅Ρ Π²Π°ΠΆΠ½ΡΠ΅ Π΄Π»Ρ ΠΏΡΠ°ΠΊΡΠΈΠΊΠΈ ΠΎΡΠΈΠ΅Π½ΡΠΈΡΡ Π΄Π»Ρ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠΊΠΈ ΠΈ ΠΏΡΠ°Π²ΠΈΠ»ΡΠ½ΠΎΠ³ΠΎ Π²ΡΠ±ΠΎΡΠ° ΠΈΡΡΠΎΡΠ½ΠΈΠΊΠ° ΠΈΠ·Π»ΡΡΠ΅Π½ΠΈΡ ΠΊΠΎΡΠΎΡΠΊΠΎΠ²ΠΎΠ»Π½ΠΎΠ²ΠΎΠ³ΠΎ Π΄ΠΈΠ°ΠΏΠ°Π·ΠΎΠ½Π°
ΠΠΎΠ²ΡΠ΅ ΠΊΠΎΠΌΠ±ΠΈΠ½Π°ΡΠΈΠΈ ΠΈ Π½Π°Π·Π²Π°Π½ΠΈΡ ΡΠΎΡΡΠ΄ΠΈΡΡΡΡ ΡΠ°ΡΡΠ΅Π½ΠΈΠΉ ΠΠ·ΠΈΠ°ΡΡΠΊΠΎΠΉ Π ΠΎΡΡΠΈΠΈ.
In this paper, we present nomenclatural novelties required in the course of the preparation of the second, revised version of the checklist of vascular plants of Asian Russia. The first version was published in 2012 (Baikov 2012). At the family level, we accepted the modern classification systems (APG IV for flowering plants, PPG I for lycophytes and ferns, and GPG for gymnosperms). At the genus level, we follow the generic concepts applied for particular taxonomic groups according to the Catalogue of Life (COL; https://www.catalogueoflife.org/), version COL23.5. At the species level, we consistently apply the monotypic species concept (also known in Russia as Komarovβs concept). In total, this paper presents one new nothogenus name (Γ Sibirotrisetokoeleria Chepinoga nom. nov., Poaceae) and 156 new names in the rank of species, in 28 families: Amaranthaceae Juss. (1 name), Amaryllidaceae J.Β St.-Hil. (1), Apiaceae Lindl. (2), Asteraceae Bercht. & J.Presl (12), Boraginaceae Juss. (4), Caryophyllaceae Juss. (11), Crassulaceae J.Β St.-Hill. (3), Cyperaceae Juss. (8), Ericaceae Juss. (2), Fabaceae Lindl. (16), Gentianaceae Juss. (1), Geraniaceae Juss. (1), Juncaceae Juss. (1), Lamiaceae Martinov (1), Menyanthaceae Dumort. (1), Orchidaceae Juss. (1), Orobanchaceae Vent. (1), Papaveraceae Juss. (4), Plantaginaceae Juss. (1), Poaceae Barnhart (49), Polygonaceae Juss. (4), Primulaceae Batsch. ex Borkh. (6), Ranunculaceae Juss. (4), Rosaceae Juss. (5), Salicaceae Mirb. (2), Saxifragaceae Juss. (11), Vitaceae Juss. (1), Zygophyllaceae R.Β Br. (2 names)
DETERMINATION OF THE MOLAR RATIO AlCl3/KCl IN THE MELT ZrCl4 β KCl β AlCl3
A method for determining the molar ratio of AlCl3/KCl in the melt ZrCl4-KCl β AlCl3 has been developed. The developed technique was tested on the working melt of the rectification plant of JSC ChMZ. Frozen alloy samples were analyzed by X-ray diffractometry
Orbital effects of a monochromatic plane gravitational wave with ultra-low frequency incident on a gravitationally bound two-body system
We analytically compute the long-term orbital variations of a test particle
orbiting a central body acted upon by an incident monochromatic plane
gravitational wave. We assume that the characteristic size of the perturbed
two-body system is much smaller than the wavelength of the wave. Moreover, we
also suppose that the wave's frequency is much smaller than the particle's
orbital one. We make neither a priori assumptions about the direction of the
wavevector nor on the orbital geometry of the planet. We find that, while the
semi-major axis is left unaffected, the eccentricity, the inclination, the
longitude of the ascending node, the longitude of pericenter and the mean
anomaly undergo non-vanishing long-term changes. They are not secular trends
because of the slow modulation introduced by the tidal matrix coefficients and
by the orbital elements themselves. They could be useful to indepenedently
constrain the ultra-low frequency waves which may have been indirectly detected
in the BICEP2 experiment. Our calculation holds, in general, for any
gravitationally bound two-body system whose characteristic frequency is much
larger than the frequency of the external wave. It is also valid for a generic
perturbation of tidal type with constant coefficients over timescales of the
order of the orbital period of the perturbed particle.Comment: LaTex2e, 24 pages, no figures, no tables. Changes suggested by the
referees include
Molecular and electronic structure of terminal and alkali metal-capped uranium(V) nitride complexes
Determining the electronic structure of actinide complexes is intrinsically challenging because inter-electronic repulsion, crystal field, and spinβorbit coupling effects can be of similar magnitude. Moreover, such efforts have been hampered by the lack of structurally analogous families of complexes to study. Here we report an improved method to Uβ‘N triple bonds, and assemble a family of uranium(V) nitrides. Along with an isoelectronic oxo, we quantify the electronic structure of this 5f1 family by magnetometry, optical and electron paramagnetic resonance (EPR) spectroscopies and modelling. Thus, we define the relative importance of the spinβorbit and crystal field interactions, and explain the experimentally observed different ground states. We find optical absorption linewidths give a potential tool to identify spinβorbit coupled states, and show measurement of UVΒ·Β·Β·UV super-exchange coupling in dimers by EPR. We show that observed slow magnetic relaxation occurs via two-phonon processes, with no obvious correlation to the crystal field
Strongly coupled binuclear uranium-oxo complexes from uranyl oxo rearrangement and reductive silylation
The most common motif in uranium chemistry is the d0f0 uranyl ion [UO2]21 in which the oxo groups are rigorously linear and inert. Alternative geometries, such as the cis-uranyl, have been identified theoretically and implicated in oxo-atom transfer reactions that are relevant to environmental speciation and nuclear waste remediation. Single electron reduction is now known to impart greater oxo-group reactivity, but with retention of the linear OUO motif, and reactions of the oxo groups to form new covalent bonds remain rare. Here, we describe the synthesis, structure, reactivity and magnetic properties of a binuclear uraniumβoxo complex. Formed through a combination of reduction and oxo-silylation and migration from a trans to a cis position, the new butterfly-shaped SiβOUO2UOβSi molecule shows remarkably strong UVβUV coupling and chemical inertness, suggesting that this rearranged uranium oxo motif might exist for other actinide species in the environment, and have relevance to the aggregation of actinide oxide clusters.JRC.E.6-Actinides researc
Small Molecule Activation by Uranium Tris(aryloxides): Experimental and Computational Studies of Binding of N-2, Coupling of CO, and Deoxygenation Insertion of CO2 under Ambient Conditions
Previously unanticipated dinitrogen activation is exhibited by the well-known uranium tris(aryloxide) U(ODtbp)(3), U(OC6H3-Bu-2(t)-2,6)(3), and the tri-tert-butyl analogue U(OTtbp)(3), U(OC6H2-Bu-3(t)-2,4,6)(3), in the form of bridging, side-on dinitrogen complexes [U(OAr)(3)](2)(mu-eta(2):eta(2)-N-2), for which the tri-tert-butyl N-2 complex is the most robust U-2(N-2) complex isolated to date. Attempted reduction of the tris(aryloxide) complex under N-2 gave only the potassium salt of the uranium(III) tetra(aryloxide) anion, K[U(OAr)(4)], as a result of ligand redistribution. The solid-state structure is a polymeric chain formed by each potassium cation bridging two arenes of adjacent anions in an eta(6) fashion. The same uranium tris(aryloxides) were also found to couple carbon monoxide under ambient conditions to give exclusively the ynediolate [OCCO](2-) dianion in [U(OAr)(3)](2)(mu-eta(1):eta(1)-C2O2), in direct analogy with the reductive coupling recently shown to afford [U{N(SiMe3)(2)}(3)](2)(mu-eta(1):eta(1)-C2O2). The related U-III complexes U{N(SiPhMe2)(2)}(3) and U{CH(SiMe3)(2)}(3) however do not show CO coupling chemistry in our hands. Of the aryloxide complexes, only the U(OC6H2-Bu-3(t)-2,4,6)(3) reacts with CO2 to give an insertion product containing bridging oxo and aryl carbonate moieties, U-2(OTtbp)(4)(mu-O)(mu-eta(1):eta(1)-O2COC6H2-Bu-3(t)-2,4,6)(2), which has been structurally characterized. The presence of coordinated N-2 in [U(OTtbp)(3)](2)(N-2) prevents the occurrence of any reaction with CO2, underscoring the remarkable stability of the N-2 complex. The di-tert-butyl aryloxide does not insert CO2, and only U(ODtbp)(4) was isolated. The silylamide also reacts with carbon dioxide to afford U(OSiMe3)(4) as the only uranium-containing material. GGA and hybrid DFT calculations, in conjunction with topological analysis of the electron density, suggest that the U-N-2 bond is strongly polar, and that the only covalent U -> N-2 interaction is pi backbonding, leading to a formal (U-IV)(2)(N-2)(2-) description of the electronic structure. The N-N stretching wavenumber is preferred as a metric of N-2 reduction to the N-N bond length, as there is excellent agreement between theory and experiment for the former but poorer agreement for the latter due to X-ray crystallographic underestimation of r(N-N). Possible intermediates on the CO coupling pathway to [U(OAr)(3)](2)(mu-C2O2) are identified, and potential energy surface scans indicate that the ynediolate fragment is more weakly bound than the ancillary ligands, which may have implications in the development of low-temperature and pressure catalytic CO chemistry
- β¦