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https://homel.vsb.cz/~luk76/publications/LSSC17.pdf
linear problems the arising problems for each frequency separate, which makes it possible to solve for all frequencies, ω = kπ/T , k = 0, 1, 2, · · · , where T
https://www.it4i.cz/o-it4i/infoservis/tiskove-zpravy/it4innovations-posune-hranice-kvantove-optimalizace-vyvine-chytre-korekcni-kody-pomoci-umele-inteligence
řekl hejtman Moravskoslezského kraje Josef Bělica. Projekt v číslech Zahájení: květen 2025 Ukončení: duben 2028 Dotace: 4 680 244 mil. Kč Dotační program: Vouchery
https://www.it4i.cz/o-it4i/infoservis/novinky/it4innovations-posune-hranice-kvantove-optimalizace-vyvine-chytre-korekcni-kody-pomoci-umele-inteligence
řekl hejtman Moravskoslezského kraje Josef Bělica. Projekt v číslech Zahájení: květen 2025 Ukončení: duben 2028 Dotace: 4 680 244 mil. Kč Dotační program: Vouchery
https://www.ekf.vsb.cz/share/static/ekf/www.ekf.vsb.cz/export/sites/ekf/mmfr-history/.content/galerie-dokumentu/2014/sbornik/Valecky.Jiri.pdf
mixture normal distribution, maximum likelihood, EM-algorithm, Monte-Carlo simulation, Markov-Switching. JEL Classification: C1, C13, C52, G1 1 Introduction The Value at Risk (VaR)
https://tses.vsb.cz/Home/tses_article354dafd.pdf?aid=354
different composition for electrodes). The basic supercapacitor concept is illustrated in Fig. 1 (Varghese et al., 2015). Fig.
http://kat354nas3.vsb.cz/icra2018/media/files/0534.pdf
is achieved through a new FBG force sensor which consists of a nitinol tube attached with a FBG strain sensor 1 . The nitinol tube
https://transactions.fs.vsb.cz/2006-2/1547_ROMAN_Monica_BOBASU_Eugen.pdf
power to the system and the half arrow is always pointed outwards these elements. TF, GY, 0 and 1 junctions are junction elements that
https://www.fei.vsb.cz/export/sites/fei/480/.content/galerie-souboru/cps12a_poster.pdf
technique, utilizing a dispersion balanced Mach-Zehnder in- terferometer. The experimental arrangement is shown in Fig. 1. A key part of this setup
https://kf.vsb.cz/Veda/poster/cps12a_poster.pdf
technique, utilizing a dispersion balanced Mach-Zehnder in- terferometer. The experimental arrangement is shown in Fig. 1. A key part of this setup
https://mrl.cs.vsb.cz/people/gaura/dzo/idft_en.pdf
M−1∑ k=0 N−1∑ l=0 F (k, l)ϕk,l(m,n) . (1) The basis ϕk,l is defined as ϕk,l(m,n) = 1√ MN ei2π( mk M +nl N ), k = 0, 1, . . . ,M − 1 a l = 0,
https://transactions.fs.vsb.cz/2010-1/1770.pdf
of zinc molten liquid alloy on pressing piston usually made from grey iron provided with steel rings according to figure 1. It is one
https://www.ekf.vsb.cz/export/sites/ekf/cs/.content/galerie-souboru/SAEI/ukazky/SAEI_VOL15_ukazka.pdf
differences between men and women in the labour force participation rate. According to Table 1–1 the female labour force participation rate
https://transactions.fs.vsb.cz/2012-1/1907.pdf
METHOD USED FOR THE BEAMS ON ELASTIC FOUNDATION – PART 1 (THEORY) METODA KONEČNÝCH DIFERENCÍ POUŽITÁ PRO NOSNÍKY NA PRUŽNÉM PODKLADU – ČÁST 1 (TEORIE) Abstract This article
https://transactions.fs.vsb.cz/2006-2/1545_POPESCU_Dan.pdf
system that we consider is described by equations of the following kind: ( ) ( ) ( ) x f x g x u y h x = + = & (1) in which f(x)
https://transactions.fs.vsb.cz/2009-3/13hor.pdf
independently on the problem size only by adding directly pro- portional number of processors [1]. All the algorithms were implemented into a new library that
http://kat354nas3.vsb.cz/icra2018/media/files/0603.pdf
decreasing function s(t)t∈[0,T ] ∈ [0, 1]. Path parameterizations are also subject to terminal velocity constraints of the form ṡ(T ) ∈ Iend, where Iend is
https://kariernicentrum.vsb.cz/cs/blog
Blog - Kariérní centrum VŠB-TUO Přeskočit na hlavní obsah k+ blog Investiční workshop s deskovou hrou Finanční svoboda Poradenské a kariérní centrum: 26. 1
https://transactions.fs.vsb.cz/2005-2/173.pdf
jak číslicovou simulací, tak i přímo na laboratorním modelu. 1 INTRODUCTION The goal of synthesis is design a control, which ensures
https://kf.vsb.cz/Veda/jcmf/FO2016_reseni.pdf
I). Označme R1 = R2 = R, z rovnic a) – e) pak dostaneme a) ε = I0Ri, b) ε = I1(Ri +R), d) ε = IP ( Ri + R 2 ) , e) ε = IS(Ri + 2R). Elektromotorické napětí zdroje pak vypočteme ze vztahu
http://kat354nas3.vsb.cz/icra2018/media/files/2193.pdf
the environment by the measurement probability density with respect to the radius p(r) := p(r | s, v,M). (1) Consequently, the absolute probability that the ray covers at least distance r