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target plasma
On the possibility of target plasma ignition under the conditions of inertial nuclear fusion
      
The thermonuclear gain G for bulk and spark ignitions are calculated using a mathematical simulation of thermonuclear combustion in a DT plasma of laser targets for various parameters of the target plasma and (isobaric and isochoric) ignitors.
      
Good agreement with experimental data is obtained when the main population channels of these states are taken into account for typical values of cluster-target plasma parameters.
      
A hot target plasma is obtained in the end cell of the AMBAL-M device with the use of an end gas-discharge plasma source.
      
The dynamics of the ion temperature of the target plasma in a gas-dynamic trap during high-power neutral beam injection is measured by using the Rutherford scattering technique.
      
The target plasma with a density of ~1015 cm-3 was produced in a solenoid with a field of 4.8 T and was heated by a highpower electron beam with an electron energy of ~1 MeV, a duration of ~7 s, and a total energy of 120-150 kJ.
      
This value substantially exceeds the energy density yielded by the target plasma; i.e., the energy is concentrated across the magnetic field onto a dense plasma bunch produced from the evaporated particle.
      
For a comparison of our results we examine effects of ion-ion correlations on the stopping power of a rigid ion lattice moving through a target plasma within dielectric response theory.
      
In recent years, the emphasis has been put on target plasma lipid concentrations for dietary and drug therapy.
      
Results: Of the 20 patients, 18 attained the target plasma concentration, and 16 of these achieved this initially or with just one dose adjustment.
      
peak power density of CO2 laser radiation focussed into an underdense and homogeneous target plasma of large extent.
      
A parameterised charge distribution is used as target plasma.
      
It is shown that superpositions of spherical Gaussian charge distributions as target plasma are sufficient to simulate various structures in proton imaging measurements, which makes this method very flexible.
      
An improved approach for hydrogen analysis in metal samples using single laser-induced gas plasma and target plasma at helium at
      
Spherical mode structure of the irradiation nonuniformity of 5.6% with MLA is estimated with cos3 θ distribution of absorption coefficient in the target plasma.
      
It is established that a rather quiescent target plasma with controlled density within the range of (2 × 108-2 × 1012)cm-3 and temperature 2-3 eV is accumulated in the trap.
      
It is established that a rather quiescent target plasma with controlled density within the range of (2 × 108-2 × 1012) cm-3 and temperature 2-3eV is accumulated in the trap.
      
The system employed a pharmacokinetic model working in real time to deliver any selected target plasma concentration of alfentanil.
      
The entry of enveloped viruses into host cells is accomplished by fusion ofthe viral envelope and target plasma membrane and is mediated by fusionproteins.
      
The target plasma temperature is about 200 eV at the beam-injection position and falls to 5 eV or less in the end region.
      
 

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