2,425 research outputs found
Wave Functions and Energy Terms of the SCHR\"Odinger Equation with Two-Center Coulomb Plus Harmonic Oscillator Potential
Schr\"odinger equation for two center Coulomb plus harmonic oscillator
potential is solved by the method of ethalon equation at large intercenter
separations. Asymptotical expansions for energy term and wave function are
obtained in the analytical form.Comment: 4 pages, no figures, LaTeX, submitted to PR
Damping Rotor Nutation Oscillations in a Gyroscope with Magnetic Suspension
A possibility of an effective damping of rotor nutations by modulating the field of the moment transducers in synchronism with the nutation frequency is considered. The algorithms for forming the control moments are proposed and their application is discussed
Quantal Two-Centre Coulomb Problem treated by means of the Phase-Integral Method I. General Theory
The present paper concerns the derivation of phase-integral quantization
conditions for the two-centre Coulomb problem under the assumption that the two
Coulomb centres are fixed. With this restriction we treat the general
two-centre Coulomb problem according to the phase-integral method, in which one
uses an {\it a priori} unspecified {\it base function}. We consider base
functions containing three unspecified parameters and .
When the absolute value of the magnetic quantum number is not too small, it
is most appropriate to choose . When, on the other hand,
is sufficiently small, it is most appropriate to choose .
Arbitrary-order phase-integral quantization conditions are obtained for these
choices of . The parameters and are determined from the
requirement that the results of the first and the third order of the
phase-integral approximation coincide, which makes the first-order
approximation as good as possible.
In order to make the paper to some extent self-contained, a short review of
the phase-integral method is given in the Appendix.Comment: 23 pages, RevTeX, 4 EPS figures, submitted to J. Math. Phy
Spectra of Doubly Heavy Quark Baryons
Baryons containing two heavy quarks are treated in the Born-Oppenheimer
approximation. Schr\"odinger equation for two center Coulomb plus harmonic
oscillator potential is solved by the method of ethalon equation at large
intercenter separations. Asymptotical expansions for energy term and wave
function are obtained in the analytical form. Using those formulas, the energy
spectra of doubly heavy baryons with various quark compositions are calculated
analytically.Comment: 19 pages, latex2e, published at PRC61(2000)04520
Relativistic dynamical polarizability of hydrogen-like atoms
Using the operator representation of the Dirac Coulomb Green function the
analytical method in perturbation theory is employed in obtaining solutions of
the Dirac equation for a hydrogen-like atom in a time-dependent electric field.
The relativistic dynamical polarizability of hydrogen-like atoms is calculated
and analysed.Comment: 15 pages, 3 figures (not included, but hard copies are available upon
request
ΠΡΡΠ»Π΅Π΄ΠΎΠ²Π°Π½ΠΈΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΠΎΠ² ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΠΎΡΠΈΡΡΡΡ Π²ΡΠΏΠ»Π°Π²Π»ΡΠ΅ΠΌΡΡ ΠΌΠΎΠ΄Π΅Π»Π΅ΠΉ, ΠΏΡΠΈΠΌΠ΅Π½ΡΠ΅ΠΌΡΡ Π΄Π»Ρ ΠΈΠ·Π³ΠΎΡΠΎΠ²Π»Π΅Π½ΠΈΡ Π²ΡΡΠΎΠΊΠΎΡΠΎΡΠ½ΠΎΠ³ΠΎ Π»ΠΈΡΡΡ
Aerospace, manufacturing, and shipbuilding industries strive to enhance their competitiveness by optimizing material utilization and improving production processes. The investment casting process offers the capability to fabricate intricate and precise components using a diverse range of alloys. However, this method is not without its drawbacks, including high manufacturing costs and a significant rate of defective castings, which can reach up to 30 %. These defects primarily arise from the stresses imposed on the wax patterns and ceramic molds, leading to their distortion. To address this issue, efforts have been made to reduce stress by employing compacted wax powders for the production of investment patterns. However, stress relaxation in the wax patterns remains a concern as it can result in elastic deformation of the compacted material and subsequent alterations in the final product dimensions. To mitigate this issue, a series of tests were conducted with the objective of studying stress relaxation under constant compression strain, as described by the Kohlrausch equation. The obtained results provide valuable insights that enable the prediction of the ultimate dimensions of patterns created using different grades of wax.ΠΠΎΠ½ΠΊΡΡΠ΅Π½ΡΠΎΡΠΏΠΎΡΠΎΠ±Π½ΠΎΡΡΡ ΡΠΎΠ²ΡΠ΅ΠΌΠ΅Π½Π½ΡΡ
ΠΏΡΠ΅Π΄ΠΏΡΠΈΡΡΠΈΠΉ ΠΌΠ°ΡΠΈΠ½ΠΎ-, ΡΡΠ΄ΠΎ- ΠΈ Π°Π²ΠΈΠ°ΡΡΡΠΎΠ΅Π½ΠΈΡ Π²ΠΎ ΠΌΠ½ΠΎΠ³ΠΎΠΌ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅ΡΡΡ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎ- ΠΈ ΡΠ½Π΅ΡΠ³ΠΎΡΡΡΠ΅ΠΊΡΠΈΠ²Π½ΠΎΡΡΡΡ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΠΉ, Π½Π°ΠΏΡΠ°Π²Π»Π΅Π½Π½ΡΡ
Π½Π° ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΠ΅ ΠΊΠΎΠ½ΡΡΡΡΠΊΡΠΈΠΉ ΠΈ ΡΠ·Π»ΠΎΠ² Π΄Π΅ΡΠ°Π»Π΅ΠΉ ΠΎΡΠ²Π΅ΡΡΡΠ²Π΅Π½Π½ΠΎΠ³ΠΎ Π½Π°Π·Π½Π°ΡΠ΅Π½ΠΈΡ. ΠΡΠΈΠΌΠ΅Π½Π΅Π½ΠΈΠ΅ Π»ΠΈΡΡΡ ΠΏΠΎ Π²ΡΠΏΠ»Π°Π²Π»ΡΠ΅ΠΌΡΠΌ ΠΌΠΎΠ΄Π΅Π»ΡΠΌ (ΠΠΠ) ΠΎΠ±Π΅ΡΠΏΠ΅ΡΠΈΠ²Π°Π΅Ρ ΠΏΠΎΠ»ΡΡΠ΅Π½ΠΈΠ΅ Π·Π°Π³ΠΎΡΠΎΠ²ΠΎΠΊ ΠΏΠΎΠ²ΡΡΠ΅Π½Π½ΠΎΠΉ ΡΠ°Π·ΠΌΠ΅ΡΠ½ΠΎΠΉ ΠΈ Π³Π΅ΠΎΠΌΠ΅ΡΡΠΈΡΠ΅ΡΠΊΠΎΠΉ ΡΠΎΡΠ½ΠΎΡΡΠΈ, ΡΠ»ΠΎΠΆΠ½ΠΎΠΉ ΠΏΡΠΎΡΡΡΠ°Π½ΡΡΠ²Π΅Π½Π½ΠΎΠΉ ΠΊΠΎΠ½ΡΠΈΠ³ΡΡΠ°ΡΠΈΠΈ ΠΈΠ· ΡΠΈΡΠΎΠΊΠΎΠΉ Π½ΠΎΠΌΠ΅Π½ΠΊΠ»Π°ΡΡΡΡ ΡΠΏΠ»Π°Π²ΠΎΠ². Π Π½Π΅Π΄ΠΎΡΡΠ°ΡΠΊΠ°ΠΌ ΠΠΠ ΡΠ»Π΅Π΄ΡΠ΅Ρ ΠΎΡΠ½Π΅ΡΡΠΈ ΠΌΠ½ΠΎΠ³ΠΎΡΡΠ°Π΄ΠΈΠΉΠ½ΠΎΡΡΡ ΠΏΡΠΎΡΠ΅ΡΡΠ° ΠΈ Π²ΡΡΠΎΠΊΡΡ ΡΡΠΎΠΈΠΌΠΎΡΡΡ ΠΊΠΎΠ½Π΅ΡΠ½ΠΎΠ³ΠΎ ΠΏΡΠΎΠ΄ΡΠΊΡΠ°, ΡΡΠΎ ΠΏΡΠ΅Π΄ΠΏΠΎΠ»Π°Π³Π°Π΅Ρ Π½Π΅Π΄ΠΎΠΏΡΡΡΠΈΠΌΠΎΡΡΡ Π±ΡΠ°ΠΊΠ°, Π΄ΠΎΠ»Ρ ΠΊΠΎΡΠΎΡΠΎΠ³ΠΎ ΠΌΠΎΠΆΠ΅Ρ Π΄ΠΎΡΡΠΈΠ³Π°ΡΡ 30 %. ΠΡΠ°ΠΊ Π² ΠΠΠ ΠΏΡΠ΅ΠΈΠΌΡΡΠ΅ΡΡΠ²Π΅Π½Π½ΠΎ Π²ΡΠ·Π²Π°Π½ ΡΠ΅ΠΏΠ»ΠΎΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΈΠΌΠΈ ΡΠ²Π»Π΅Π½ΠΈΡΠΌΠΈ, ΡΠΎΠΏΡΠΎΠ²ΠΎΠΆΠ΄Π°ΡΡΠΈΠΌΠΈ ΡΡΠ΄ ΡΠ΅Ρ
Π½ΠΎΠ»ΠΎΠ³ΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΎΠΏΠ΅ΡΠ°ΡΠΈΠΉ ΠΈ ΠΎΠ±ΡΡΠ»ΠΎΠ²Π»ΠΈΠ²Π°ΡΡΠΈΠΌΠΈ Π½Π°Π»ΠΈΡΠΈΠ΅ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ Π² ΡΡΡΡΠΊΡΡΡΠ΅ Π²ΠΎΡΠΊΠΎΠΎΠ±ΡΠ°Π·Π½ΡΡ
ΠΈ ΠΊΠ΅ΡΠ°ΠΌΠΈΡΠ΅ΡΠΊΠΈΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ², ΡΡΠΎ ΠΎΠΏΡΠ΅Π΄Π΅Π»ΡΠ΅Ρ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΎΠ½Π½ΡΠ΅ ΠΏΡΠΎΡΠ΅ΡΡΡ Π² Π²ΡΠΏΠ»Π°Π²Π»ΡΠ΅ΠΌΡΡ
ΠΌΠΎΠ΄Π΅Π»ΡΡ
ΠΈ ΠΎΠ±ΠΎΠ»ΠΎΡΠΊΠΎΠ²ΡΡ
ΡΠΎΡΠΌΠ°Ρ
. ΠΠ»Ρ ΡΡΡΡΠ°Π½Π΅Π½ΠΈΡ Π½Π΅Π³Π°ΡΠΈΠ²Π½ΠΎΠ³ΠΎ Π²Π»ΠΈΡΠ½ΠΈΡ ΡΠ΅ΠΏΠ»ΠΎΡΠΈΠ·ΠΈΡΠ΅ΡΠΊΠΎΠ³ΠΎ ΡΠ°ΠΊΡΠΎΡΠ° ΠΈ ΡΠ½ΠΈΠΆΠ΅Π½ΠΈΡ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ Π² ΡΡΡΡΠΊΡΡΡΠ°Ρ
ΠΏΡΠΎΠΌΠ΅ΠΆΡΡΠΎΡΠ½ΡΡ
ΠΈΠ·Π΄Π΅Π»ΠΈΠΉ ΠΏΡΠΎΡΠ΅ΡΡΠ°, Π²ΡΠΏΠ»Π°Π²Π»ΡΠ΅ΠΌΡΠ΅ ΠΌΠΎΠ΄Π΅Π»ΠΈ ΡΠΎΡΠΌΠΈΡΡΡΡ ΠΏΡΠ΅ΡΡΠΎΠ²Π°Π½ΠΈΠ΅ΠΌ ΠΏΠΎΡΠΎΡΠΊΠΎΠ² Π²ΠΎΡΠΊΠΎΠΎΠ±ΡΠ°Π·Π½ΡΡ
ΠΌΠΎΠ΄Π΅Π»ΡΠ½ΡΡ
ΠΊΠΎΠΌΠΏΠΎΠ·ΠΈΡΠΈΠΉ. ΠΡΠΈ ΡΡΠΎΠΌ Π½Π΅ΡΠ΅ΡΠ΅Π½Π½ΡΠΌ ΠΎΡΡΠ°Π΅ΡΡΡ Π²ΠΎΠΏΡΠΎΡ ΡΠ΅Π»Π°ΠΊΡΠ°ΡΠΈΠΈ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ Π² ΠΏΡΠ΅ΡΡΠΎΠ²ΠΊΠ°Ρ
, ΠΏΡΠΈΠ²ΠΎΠ΄ΡΡΠΈΡ
ΠΊ ΡΠΏΡΡΠ³ΠΎΠΌΡ ΠΎΡΠΊΠ»ΠΈΠΊΡ ΡΠΏΠ»ΠΎΡΠ½Π΅Π½Π½ΠΎΠ³ΠΎ ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»Π° ΠΈ, ΠΊΠ°ΠΊ ΡΠ»Π΅Π΄ΡΡΠ²ΠΈΠ΅, ΠΈΠ·ΠΌΠ΅Π½Π΅Π½ΠΈΡ ΡΠ°Π·ΠΌΠ΅ΡΠΎΠ² ΠΏΠΎΠ»ΡΡΠ°Π΅ΠΌΠΎΠ³ΠΎ ΠΈΠ·Π΄Π΅Π»ΠΈΡ. ΠΠΎΠΈΡΠΊ Π²Π°ΡΠΈΠ°Π½ΡΠΎΠ² Π½Π°ΠΈΠ±ΠΎΠ»Π΅Π΅ ΡΠ°ΡΠΈΠΎΠ½Π°Π»ΡΠ½ΠΎΠ³ΠΎ ΡΠ΅ΠΆΠΈΠΌΠ° ΡΠΎΡΠΌΠΈΡΠΎΠ²Π°Π½ΠΈΡ ΠΏΡΠ΅ΡΡΠΎΠ²ΠΊΠΈ ΠΏΡΠΈΠ²Π΅Π» ΠΊ Π½Π΅ΠΎΠ±Ρ
ΠΎΠ΄ΠΈΠΌΠΎΡΡΠΈ ΠΏΡΠΎΠ²Π΅Π΄Π΅Π½ΠΈΡ ΡΠ΅ΡΠΈΠΈ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠΎΠ², Π² ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΠ΅ ΠΊΠΎΡΠΎΡΡΡ
ΠΏΡΠ΅Π΄ΠΏΠΎΠ»Π°Π³Π°Π΅ΡΡΡ Π΄ΠΎΡΡΠΈΠΆΠ΅Π½ΠΈΠ΅ ΡΠ΅Π»Π°ΠΊΡΠ°ΡΠΈΠΈ Π½Π°ΠΏΡΡΠΆΠ΅Π½ΠΈΠΉ Ο Π² ΡΡΠ»ΠΎΠ²ΠΈΡΡ
ΠΏΠΎΡΡΠΎΡΠ½Π½ΠΎΠΉ Π΄Π΅ΡΠΎΡΠΌΠ°ΡΠΈΠΈ ΡΠΆΠ°ΡΠΈΡ, ΠΎΠΏΠΈΡΡΠ²Π°Π΅ΠΌΠΎΠ³ΠΎ ΡΡΠ°Π²Π½Π΅Π½ΠΈΠ΅ΠΌ ΠΠΎΠ»ΡΡΠ°ΡΡΠ°. ΠΠΎΠ»ΡΡΠ΅Π½Π½ΡΠ΅ Π² Ρ
ΠΎΠ΄Π΅ ΡΠΊΡΠΏΠ΅ΡΠΈΠΌΠ΅Π½ΡΠ° ΡΠ΅Π·ΡΠ»ΡΡΠ°ΡΡ ΠΏΠΎΠ·Π²ΠΎΠ»ΡΡ ΠΏΡΠΎΠ³Π½ΠΎΠ·ΠΈΡΠΎΠ²Π°ΡΡ ΠΊΠΎΠ½Π΅ΡΠ½ΡΠ΅ ΡΠ°Π·ΠΌΠ΅ΡΡ ΠΏΡΠ΅ΡΡΠΎΠ²ΠΎΠΊ ΠΈ ΡΡΠΎΡΠΌΠΈΡΠΎΠ²Π°ΡΡ ΠΌΠ°ΡΠ΅ΠΌΠ°ΡΠΈΡΠ΅ΡΠΊΡΡ ΠΌΠΎΠ΄Π΅Π»Ρ ΠΏΡΠΎΡΠ΅ΡΡΠ°, Π°ΠΊΡΡΠ°Π»ΡΠ½ΡΡ Π΄Π»Ρ ΡΠΈΡΠΎΠΊΠΎΠΉ Π½ΠΎΠΌΠ΅Π½ΠΊΠ»Π°ΡΡΡΡ Π²ΠΎΡΠΊΠΎΠΎΠ±ΡΠ°Π·Π½ΡΡ
ΠΌΠΎΠ΄Π΅Π»ΡΠ½ΡΡ
ΠΌΠ°ΡΠ΅ΡΠΈΠ°Π»ΠΎΠ², ΠΏΡΠΈΠΌΠ΅Π½ΡΠ΅ΠΌΡΡ
Π² ΠΠΠ
Glass capillary X-ray lens: fabrication technique and ray tracing calculations
A new method for producing a compound refractive X-ray lens is described. The lens is designed as glass capillary "lled by a set of concave individual lenses. The method is appropriate for the preparation of 10}1000 spherical lenses in a glass capillary with a diameter of 0.1}1 mm. Lens aberrations are considered and simple formulas for spot size are derived. Ray-tracing simulations on the focusing experiments using 18 keV X-rays are reported. ( 2000 Elsevier Science B.V. All rights reserved
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