3,757 research outputs found
Multiple ionization of neon by soft X-rays at ultrahigh intensity
At the free-electron laser FLASH, multiple ionization of neon atoms was
quantitatively investigated at 93.0 eV and 90.5 eV photon energy. For ion
charge states up to 6+, we compare the respective absolute photoionization
yields with results from a minimal model and an elaborate description. Both
approaches are based on rate equations and take into acccout a Gaussian spatial
intensity distribution of the laser beam. From the comparison we conclude, that
photoionization up to a charge of 5+ can be described by the minimal model. For
higher charges, the experimental ionization yields systematically exceed the
elaborate rate based prediction.Comment: 10 pages, 3 figure
Magneto-Optical Trap for Thulium Atoms
Thulium atoms are trapped in a magneto-optical trap using a strong transition
at 410 nm with a small branching ratio. We trap up to atoms at
a temperature of 0.8(2) mK after deceleration in a 40 cm long Zeeman slower.
Optical leaks from the cooling cycle influence the lifetime of atoms in the MOT
which varies between 0.3 -1.5 s in our experiments. The lower limit for the
leaking rate from the upper cooling level is measured to be 22(6) s. The
repumping laser transferring the atomic population out of the F=3 hyperfine
ground-state sublevel gives a 30% increase for the lifetime and the number of
atoms in the trap.Comment: 4 pages, 6 figure
A perturbation of DC electric field caused by light ion adhesion to aerosols during the growth in seismic-related atmospheric radioactivity
International audienceThe influence of variations in conductivity and external electric current variations in the lower atmosphere on DC electric field over a seismic region is investigated. The external current is formed with the occurrence of convective upward transport of charged aerosols and their gravitational sedimentation in the atmosphere. This effect is related with the occurrence of ionization source due to seismic-related emanation of radon and other radioactive elements into the lower atmosphere. An increase in atmosphere radioactivity level results in the appearance of additional sources of ionization, and altitude dependence of the ion formation rate is calculated. Ionization source varies the atmospheric conductivity and the external current through appearance of ions with equilibrium number density and their adhesion to aerosols. We have calculated the perturbation of conductivity and external electric current as a function of altitude. Variation of conductivity and external current in the lower atmosphere leads to a perturbation of electric current which flows in the global atmosphere-ionosphere circuit. Finally, perturbations of DC electric field both on the Earth's surface and in the ionosphere are estimated
The detection of lengthened objects by pulse altimeter
The algorithm of lengthened objects detection is based on statistical processing of reflected pulse altimeter signal. We use method of maximum posteriori probability to make a decision. Minimum of maximum posteriori probability accorded with lengthened objects position. We use this fact to detect their position. This algorithm allows to realize autonomic navigation. In this paper it is shown two cases of the algorithm realization. The first method is based on the typical regime of radar altimeter and the second is based on the application of the Dopplerβs filtration. The results of flight experiments are introduced in this article, which approved the correctness of the created algorithm.ΠΠ»Π³ΠΎΡΠΈΡΠΌ ΠΎΠ±Π½Π°ΡΡΠΆΠ΅Π½ΠΈΡ ΠΏΡΠΎΡΡΠΆΠ΅Π½Π½ΡΡ
ΠΎΠ±ΡΠ΅ΠΊΡΠΎΠ² ΠΎΡΠ½ΠΎΠ²Π°Π½ Π½Π° ΡΡΠ°ΡΠΈΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΠΎΠ±ΡΠ°Π±ΠΎΡΠΊΠ΅ ΠΎΡΡΠ°ΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ ΡΠΈΠ³Π½Π°Π»Π° ΠΈΠΌΠΏΡΠ»ΡΡΠ½ΠΎΠ³ΠΎ ΡΠ°Π΄ΠΈΠΎΠ²ΡΡΠΎΡΠΎΠΌΠ΅ΡΠ°. ΠΠ»Ρ ΠΏΡΠΈΠ½ΡΡΠΈΡ ΡΠ΅ΡΠ΅Π½ΠΈΡ ΠΈΡΠΏΠΎΠ»ΡΠ·ΡΠ΅ΡΡΡ ΠΌΠ΅ΡΠΎΠ΄ ΠΌΠ°ΠΊΡΠΈΠΌΡΠΌΠ° Π°ΠΏΠΎΡΡΠ΅ΡΠΈΠΎΡΠ½ΠΎΠΉ Π²Π΅ΡΠΎΡΡΠ½ΠΎΡΡΠΈ. ΠΠΈΠ½ΠΈΠΌΡΠΌ ΠΌΠ°ΠΊΡΠΈΠΌΡΠΌΠ° Π°ΠΏΠΎΡΡΠ΅ΡΠΈΠΎΡΠ½ΠΎΠΉ Π²Π΅ΡΠΎΡΡΠ½ΠΎΡΡΠΈ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅Ρ ΠΏΠΎΠ»ΠΎΠΆΠ΅Π½ΠΈΠ΅ Π³ΡΠ°Π½ΠΈΡ ΠΏΡΠΎΡΡΠΆΠ΅Π½Π½ΠΎΠ³ΠΎ ΠΎΠ±ΡΠ΅ΠΊΡΠ°. Π ΡΡΠ°ΡΡΠ΅ ΠΏΠΎΠΊΠ°Π·Π°Π½Ρ Π΄Π²Π° ΡΠ΅ΠΆΠΈΠΌΠ°, ΡΠ΅Π°Π»ΠΈΠ·ΡΡΡΠΈΠ΅ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½ΡΠΉ Π°Π»Π³ΠΎΡΠΈΡΠΌ: ΡΠΈΠΏΠΎΠ²ΠΎΠΉ ΡΠ΅ΠΆΠΈΠΌ ΡΠ°Π±ΠΎΡΡ Π ΠΠ‘ ΠΈ ΡΠ΅ΠΆΠΈΠΌ Π΄ΠΎΠΏΠ»Π΅ΡΠΎΠ²ΡΠΊΠΎΠΉ ΡΠΈΠ»ΡΡΡΠ°ΡΠΈΠΈ. ΠΡΠΈΠ²Π΅Π΄Π΅Π½Ρ ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ Π½Π°ΡΡΡΠ½ΡΡ
ΠΈΡΠΏΡΡΠ°Π½ΠΈΠΉ, ΠΏΠΎΠ΄ΡΠ²Π΅ΡΠ΄ΠΈΠ²ΡΠΈΠ΅ ΠΏΡΠ°Π²ΠΈΠ»ΡΠ½ΠΎΡΡΡ ΡΠ°Π·ΡΠ°Π±ΠΎΡΠ°Π½Π½ΠΎΠ³ΠΎ Π°Π»Π³ΠΎΡΠΈΡΠΌΠ°
- β¦