The integral equations for the process γ→3π and K→3π are derived by the Tamm-Dancoff method. The resonance properties of these process are determined completely by the two pion scattering amplitudes. Our approximate solution for the process K→3π is identical with that obtained by Khuri and Treiman using the method of dispersion relations.
The integral equations for the process γ→3π and K→3π are derived by the Tamm-Dancoff method. The resonance properties of these process are determined completely by the two pion scattering amplitudes. Our approximate solution for the process K→3π is identical with that obtained by Khuri and Treiman using the method of dispersion relations.
Roothaan's LCAO-SCF method is extented to the problem of an infinite long-chain, conjugated molecule. A system of non-linear integral equation is obtained. The nature of the equation as well as the question of the existence of anomalous solutions are discussed. Finally, we suggest a methed of linearization and approximations.
Roothaan's LCAO-SCF method is extented to the problem of an infinite long-chain, conjugated molecule. A system of non-linear integral equation is obtained. The nature of the equation as well as the question of the existence of anomalous solutions are discussed. Finally, we suggest a methed of linearization and approximations.
A stabilized high voltage power supply for an electrostatic analyzer is described in this paper. The design principle has been analyzed in some detail. The output voltage of this instrument may be varied continuously from ± 5 kv to ±20 kv. Within this range the voltage stability is better than ±0.015% for about 3 hours. The ripple voltage is one part in 16,000. This instrument had since served normally for more than two years and was shown to be sufficiently simple and reliable both in operation and maintenance.
A stabilized high voltage power supply for an electrostatic analyzer is described in this paper. The design principle has been analyzed in some detail. The output voltage of this instrument may be varied continuously from ± 5 kv to ±20 kv. Within this range the voltage stability is better than ±0.015% for about 3 hours. The ripple voltage is one part in 16,000. This instrument had since served normally for more than two years and was shown to be sufficiently simple and reliable both in operation and maintenance.
A method to inject beams of H2+ and H° simultaneously into a magnetic mirror system is proposed. From an analysis of the flow of the neutral residual gas in the system the general equation for the rate of accumulation of fast protons is obtained. Parametric study of the condition for exponential build up of the proton density gives results different from those of Post and others.
A method to inject beams of H2+ and H° simultaneously into a magnetic mirror system is proposed. From an analysis of the flow of the neutral residual gas in the system the general equation for the rate of accumulation of fast protons is obtained. Parametric study of the condition for exponential build up of the proton density gives results different from those of Post and others.
The time resolution process of excitation intensity of spectral lines in the spark light source is measured. In the spark, operating under the critical damping state, with flash time at about 2×10-6 Sec., the ion lines of higher excitation potential first appear and appear shortly. Experiments show that, as to time, two lines, All and MoⅡ, piled up at 3961.5?, may be fully seperated, providing the possibility to avoid the interferences and to use the sensitive line as spectrum analysis.
The time resolution process of excitation intensity of spectral lines in the spark light source is measured. In the spark, operating under the critical damping state, with flash time at about 2×10-6 Sec., the ion lines of higher excitation potential first appear and appear shortly. Experiments show that, as to time, two lines, All and MoⅡ, piled up at 3961.5?, may be fully seperated, providing the possibility to avoid the interferences and to use the sensitive line as spectrum analysis.
A measurement for the time resolution limit produced by a photomultiplier, with the accuracy of ± 2～5×10-9 Sec., has been made. With the aid of a hydrogen lamp, illuminating at 5～8×10-8 Sec., the flight time of photoelectrons of serveral kinds of photomultiplier has been determined by employing the oscilloscopic method; an investigation as to the effect of the outer circuit of RCA-5819 for resolution time has been made and the better working state suitable for instant observation for the spectrum excitation process has also been determined.
A measurement for the time resolution limit produced by a photomultiplier, with the accuracy of ± 2～5×10-9 Sec., has been made. With the aid of a hydrogen lamp, illuminating at 5～8×10-8 Sec., the flight time of photoelectrons of serveral kinds of photomultiplier has been determined by employing the oscilloscopic method; an investigation as to the effect of the outer circuit of RCA-5819 for resolution time has been made and the better working state suitable for instant observation for the spectrum excitation process has also been determined.