... Tij v i v j -- [.. ... M · · · = ±n! det(ij ) dx1 · · · dx2n , dim M = 2n. n k 27. n () gij . ... f : +y ) f : (x, y ) x = cos ; y = sin ; ) f : (u, v ) (x, y ) x = u2 - v 2 ; y = 2uv ; f : (p, q , r) (x, y ) x = pq + r; y = 2(pq + r). 4. ) x2 dx + xy 3 dy ; ) x dy dz + 3y dx dz ; dy y dx ) x x2 -y2 . ... r, , z ) 100 r00 2 i 0 , ) tij = 0 r ) tj = 0 r 0. 001 001 ~j 5. , i k - i k ~ (1, 2), j (1, 2) . ... 13. ) , ) ds2 = y (dx2 + dy 2 ). ) r(u, v ) = (u cos v , u sin v , hv ). 2 2 ) ds2 = dx2 +dy . ...

Åùå â ðàçäåëå: (Ïîêàçàòü âñå ðåçóëüòàòû (>28) - dfgm.math.msu.su/ )

• http://dfgm.math.msu.su/files/skopenkov/dubask.pdf
• http://dfgm.math.msu.su/files/0ngit/oshemkov/00ngit.pdf
• http://dfgm.math.msu.su/files/0students/2014-kr3-timonina.pdf

Embedding formulae for Laplace-Beltrami problems on the sphere with a cut. ... Introduction We are considering the scalar problem of plane wave diffraction by a quarter-plane. ... Applying the BesselSommerfeld technique he has obtained the following formula for the diffraction co efficient: ^ i f ( , 0 ) = e-i g ( , 0, ) d, (1 ) where 0 and are directions of incidence and scattering, is the separation parameter and g is the Green's function of the of the spherical problem. ...

Åùå â ðàçäåëå: (Ïîêàçàòü âñå ðåçóëüòàòû (>32) - acoustics.phys.msu.ru/ )

• http://acoustics.phys.msu.su/teachers/gusev_files/nano1.pdf
• http://acoustics.phys.msu.su/teachers/shanin_files/~shanin/papers/cone_asymptotics.pdf
• http://acoustics.phys.msu.su/teachers/shanin_files/~shanin/papers/proc02.pdf

... RELAX module commonmod parameter ( n_max = 1000, nmax_in_sphere = 100,max_atomov = 10) parameter (PI180=3.141592653/180.) character text character(2) atom_name character(6) name_atoms character(6) name_ XYZ character(6) name_sort( n_max ) integer N_atoms ,num_W,num_atom_name integer IP( n_max ) integer print_coord,print_coordg,print_coord_sphera,print_wi_all,print_wi_vozr,print_wi_name integer print_coord_atom,print_coord n_max = 1000 - . ... XYZ_NEW(m,1) = X_NEW(L) + i*1. ...

Åùå â ðàçäåëå: (Ïîêàçàòü âñå ðåçóëüòàòû (>3) - cryst.geol.msu.ru/ )

... It describes the package for power series treatment, and the pro- cedures for building a normal form and normalizing transformations. ... The basic idea of the method of normal form is the use of \local" coordinate transformation to simplify the equations that describe the dynamics of the system under consideration. In other words, with the method of normal forms, one seeks a near-identity coordinate transformation in which the dynamical system takes the simplest form or so-called normal form. ...

Åùå â ðàçäåëå: (Ïîêàçàòü âñå ðåçóëüòàòû (>4) - acat02.sinp.msu.ru/ )

... We designed a prototype of a direction-sensitive optical mo dule (DOM) and we accordingly mo dified the simulation and reconstruction codes [2] currently used by the ANTARES Collaboration to study the response of the detector. The DOM is based on a position-sensitive photomultiplier coupled to a light guide system such that all the Cherenkov light arriving from the same direction is fo cussed on a reduced area of the photo catho de. ... Left: standard optical module; right: DOM. ...

Åùå â ðàçäåëå: (Ïîêàçàòü âñå ðåçóëüòàòû (>7) - antares.sinp.msu.ru/ )

• http://antares.sinp.msu.ru/docs/INFN%20-%20NEMO.pdf

... Applications of Molecular Mechanics to Metal Complexes" . ... Molecular mechanics study of the mixed-ligand lanthanide complexes using Gillespie-Kepert model . ... Within MM-GK, the same parameters are applicable to complexes of different coordination numbers/polyhedra. ... Gillespie-Kepert model . ... Using derived computational parameters, we calculated the geometry of 39 lanthanide ion nonaaqua complexes, 6 octaaqua complexes and 18 beta- diketonate and aqua-beta-diketonate complexes. ...

Åùå â ðàçäåëå: (Ïîêàçàòü âñå ðåçóëüòàòû (>2) - analyt.chem.msu.ru/ )

A Particle Physics Tour with CompHEP Jeffrey D. Richman April 26, 2006 Outline Introduction Getting, installing, and running CompHEP; references Using CompHEP; particle content in SM and SUSY; limitations of CompHEP; exclusive vs. inclusive processes; intermediate states "Observables" in particle physics: decay rates, cross sections,.. ... Specify decay or scattering process 2. ... CM energy for e+e- bb Interfering amplitudes Cross section vs. ... CM energy Cross section vs. ...

Åùå â ðàçäåëå: (Ïîêàçàòü âñå ðåçóëüòàòû (>5) - comphep.sinp.msu.ru/ )

• http://comphep.sinp.msu.ru/_media/download/hep-ph-0208011.pdf
• http://comphep.sinp.msu.ru/_media/manual-3.3.pdf

... The discreteness of pair number ns implies that the values of fs are multiples of 0.16 Hz for the chosen value of T . ... As the authors do not have any information on the later examinations of these 3 22 Table 2: Classification of sub jects into categories corresponding to different risk levels for developing schizophrenia based on the analysis of F3 and F4 EEG signals : I - healthy , II - conditionally healthy , III - susceptible to schizophrenia , IV - highly susceptible to ...

29. http://beams.chem.msu.ru/doc/FizKhim6_05LarinLO.pdf