Iodine photodissociation laser system Perun II

A construction and exploitation of a medium size iodine photodissociation laser system Perun II is reported. This laser produced pulses of infrared light (=1.315m) up to 50 J in energy and 300 ps in duration. The diameter of the beam is 82 mm. The beam divergence is about 4×10^–4 rad. The laser beam can be focused in a focal spot of a power density exceeding 10¹⁴ W/cm². The resuls of measurements of basic plasma parameters on an Al foil target are also presented. A recent improvement of the system includes a conversion to the second harmonic by a DKDP crystal.Presented at bilateral international seminar of High Temperature Laser Plasma and High Gain Iodine Lasers held on 4 July 1991 in the Inst. of Physics, Czechosl. Acad. Sci., in Prague (organized by Division of Optics of the Inst. of Physics, Czechosl. Acad. Sci., and Physical Section (Plasma Division) of the Union of Czech Mathematicians and Physicists.     

Optical bremsstrahlung of relativistic particles in a transparent medium and its relation to the Vavilov-čerenkov radiation

The classical formula for the intensity of the optical bremsstrahlung (OB) emitted by a charged particle moving in a transparent medium with a velocity above the Vavilov-erenkov radiation (VCR) threshold is analysed in the paper.The erenkov properties acquired by the OB atn>1 are shown to be independent of the constant velocity of the particles. All OB properties (including its erenkov character) are explained using interference of prompt bremsstrahlungs that appear during acceleration of a particle and are introduced in the formulation of the problem.The authors are very thankful to Prof. B. M. Bolotovsky and Prof. A. A. Tyapkin for useful discussions of this paper.     

Elastic constants of the alloys Cd1−x Zn x (x<0.3%) and their temperature dependence

The temperature dependence of elastic constants of Cd_1–x Zn _x alloys, havingx=0.021, 0·042 and 0·233 at.%, has been measured in the temperature range from 4·2 to 300 K by the pulse-echo-overlap ultrasonic method. The adiabatic compressibilities and the Debye temperatures have been calculated. All elastic constants with the exception ofc ₄₄ increase slightly with the growing concentration of Zn.The summary of this paper was presented on the 7^th Conference on Ultrasonic Methods in ilina, September 11^th–13^th, 1980.     

Selectrode—the universal ion-selective electrode : Part VII. A valinomycin-based potassium electrode with nonporous polymer membrane and solid-state inner reference system

A potassium electrode utilizing a solution of valinomycin in diphenylether and a porous membrane is compared with selectrodes in which the diphenylether has been replaced by a suitable plasticizer and the porous membrane support by a polymer net-work. The development of the polymer membrane allows the use of simplified selectrode construction with a “solid-state” calomel reference system; Rules for a successful choice of a suitable solvent-polymer combination are suggested and used for development of new Polyvinylchloride- and polyurethane-based membranes.     

Study of radioactive labelled chromium (III) ion adsorption on stearic acid monomolecular layer

A study of chromium(III) ion adsorption on a stearic acid monomolecular layer (MML), spread on the surface of a⁵¹CrCl₃ aqueous solution, is presented. From the analysis of the experimental results it can be concluded that MML saturation is achieved at CrCl₃ concentrations above 10^?6M. When the maximum adsorption pH value of Cr(III) ions on MML is 6.7, MML is completely ionized and chromium ion is bonded as Cr(OH) ₂ ⁺ . The kinetics of Cr(III) ion adsorption on MML could be expressed as A^S=A _∞ ^S (1?e^{?k t}).     

The separation of some Bi- and tervalent cations on zirconium phosphate columns

Summary On small columns filled with the inorganic cation-exchanger zirconium phosphate, Zn²⁺-Cd²⁺ were quantitatively and Ni²⁺-Co²⁺ partly separated. The exchanger was in the NH₄+ form, and 0.5–4N NH₄Cl served as eluent. With the exchanger in the H+ form, U0₂ ²⁺ was separated from bivalent cations and ferric iron by stepwise elution with 0.1, 0.5 and 4N HCl solutions.

---

Zusammenfassung An kleinen Säulen des anorganischen Kationenaustauschers Zirkoniumphosphat wurden Zn²⁺ und Cd²⁺ quantitativ, Ni²⁺ und Co²⁺ teilweise getrennt. Der Austauscher lag in der NH₄+-Form vor, 0,5-bis 4-n Ammoniumchlorid diente als Eluent. Mit der H+-Form des Austauschers wurde UO₂ ²⁺ von zweiwertigen Kationen und von Fe³⁺ durch schrittweise Elution mit 0,1-, 0,5- und 4-n Salzsäure getrennt.

---

Résumé On a séparé Zn²⁺-Cd²⁺ quantitativement et Ni²⁺-Co²⁺ partiellement sur de petites colonnes remplies de phosphate de zirconium comme échangeur minéral cationique. L'échangeur se trouvait sous forme NH₄+ et l'on a pris NH₄Cl 0,5-4N comme éluant. Avec l'échangeur sous forme H⁺, on a séparé UO₂ ²⁺ des cations bivalents et de l'ion ferrique par élution graduelle avec des solutions chlorhydriques 0,1, 0,5 et 4N.

     

On the Interaction of Two Finite-Dimensional Quantum Systems

Interaction of quantum system S ^a described by the generalised × eigenvalue equation A| _s =E _s S ^a | _s (s=1,...,) with quantum system S ^b described by the generalised n×n eigenvalue equation B| _i = _i S ^b | _i (i=1,...,n) is considered. With the system S ^a is associated -dimensional space X ^a and with the system S ^b is associated an n-dimensional space X _n ^b that is orthogonal to X ^a . Combined system S is described by the generalised (+n)×(+n) eigenvalue equation [A+B+V]| _k = _k [S ^a +S ^b +P]| _k (k=1,...,n+) where operators V and P represent interaction between those two systems. All operators are Hermitian, while operators S ^a ,S ^b and S=S ^a +S ^b +P are, in addition, positive definite. It is shown that each eigenvalue _{k i} of the combined system is the eigenvalue of the × eigenvalue equation . Operator in this equation is expressed in terms of the eigenvalues _i of the system S ^b and in terms of matrix elements _s |V| _i and _s |P| _i where vectors | _s form a base in X ^a . Eigenstate | _k ^a of this equation is the projection of the eigenstate | _k of the combined system on the space X ^a . Projection | _k ^b of | _k on the space X _n ^b is given by | _k ^b =( _k S ^b –B)^–1(V– _k P})| _k ^a where ( _k S ^b –B)^–1 is inverse of ( _k S ^b –B) in X _n ^b . Hence, if the solution to the system S ^b is known, one can obtain all eigenvalues _{k i} } and all the corresponding eigenstates | _k of the combined system as a solution of the above × eigenvalue equation that refers to the system S ^a alone. Slightly more complicated expressions are obtained for the eigenvalues _{k i} } and the corresponding eigenstates, provided such eigenvalues and eigenstates exist.