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Отображаемые элементы 1-10 из 60431
Линейные операторы: примеры и задачи
(Сибирский федеральный университет, 2007)
a238a226
a207a240a232a236a229a240a46 a206a225a238a231a237a224a247a232a236 a247a229a240a229a231 E a235a232a237a229a233a237a238a229 a239a240a238a241a242a240a224a237a241a242a226a238 a241a226a238a225a238a228a45
a237a251a245 a227a229a238a236a229a242a240a...
208a224a241a241a236a238a242a240a232a236 a238a239a229a240a224a242a238a240 a237a224 E a238a239a229a240a224a242a238a240 A(x) = (x,a) a|a|2. a40a49a41 a207a240a238a226a229a240a232a236 a235a232a237a229a233a237a238a241a242a252 a238a239a229a240a224a242a238a...
208a224a241a241a236a238a242a240a232a236 a238a239a229a240a224a242a238a240 a237a224 E a238a239a229a240a224a242a238a240 A(x) = (x,a) a|a|2. a40a49a41 a207a240a238a226a229a240a232a236 a235a232a237a229a233a237a238a241a242a252 a238a239a229a240a224a242a238a...
Исследование эффекта упорядочения узлов в одномерном дискретно-стохастическом алгоритме построения адаптивных сеток
(Сибирский федеральный университет, 2011-07-04)
240a243a234a242a243a240a224 a240a224a241a239a238a235a238a230a229a237a232a255 a243a231a235a238a226a41 a231a224a228a224a229a242a241a255 a234a224a240a242a238a233 Q(M) = {q1,...,qM} a232 a241a232a241a242a229a236a238a233
a237a229a233a240a238a237a238a226 E...
(M) = {e1,...,eM} a40a227a228a229 ei = (qi,xi)a41a44 a238a239a240a229a228a229a235a255a254a249a232a245 a241a238a238a242a226a229a242a241a242a226a232a229 a236a229a230a228a243 a241a229a242a234a224a236a232 X(M) a232 Q(M)a46 a207a240a232a225a235a232a230a229a237a...
(M) = {e1,...,eM} a40a227a228a229 ei = (qi,xi)a41a44 a238a239a240a229a228a229a235a255a254a249a232a245 a241a238a238a242a226a229a242a241a242a226a232a229 a236a229a230a228a243 a241a229a242a234a224a236a232 X(M) a232 Q(M)a46 a207a240a232a225a235a232a230a229a237a...
Dynamical thermalization in isolated quantum dots and black holes
(2017-01)
We study numerically a model of quantum dot with interacting fermions. At strong interactions with small conductance the model is reduced to the Sachdev-Ye-Kitaev black-hole model while at weak interactions and large conductance it describes a...
Оптимальные дискретно-стохастические кубатурные формулы
(Сибирский федеральный университет, 2011-07-04)
238a242a237a238a248a229a237a232a229
D¯θn =
nsummationdisplay
m=1
D(g(ξm)
n2 =
nsummationdisplay
m=1
E(g(ξm)−gm)2
n2 , a227a228a229 gm = Eg(ξm) = µ
d
integraldisplay
Xm
g(x)dx. (5)
a200a231 a242a229a238a240a229a236a251 a238 a241a240a229a228a237a229a236...
stream_source_info bahvalov.pdf.txt stream_content_type text/plain stream_size 33945 Content-Encoding UTF-8 stream_name bahvalov.pdf.txt Content-Type text/plain; charset=UTF-8 a206a239a242a232a236a224a235a252a237a251a229...
stream_source_info bahvalov.pdf.txt stream_content_type text/plain stream_size 33945 Content-Encoding UTF-8 stream_name bahvalov.pdf.txt Content-Type text/plain; charset=UTF-8 a206a239a242a232a236a224a235a252a237a251a229...
Поиск наилучших кубатурных формул для сферы, инвариантных относительно группы вращений тетраэдра
(Сибирский федеральный университет, 2011-07-04)
240 a227a240a243a239a239a251 T a228a235a255 a241a244a229a240a251 a228a238 a50a57a45a227a238 a239a238a240a255a228a234a224 a242a238a247a237a238a241a242a232a46
n N E G L n N E G L n N E G L
2 4 1:9720 Td [5] 12 60 1:1835 T [1] 21 162 1:6219 Th
3 6 2...
244 0:8682 T 9 32 2:2441 Yh [7] 18 124 1:1990 T 27 260 1:5409 Th 10 44 1:4291 Td 19 132 1:0089 Y [9] 28 284 0:3722 T 11 48 1:6928 O [8] 20 148 0:8569 T 29 296 1:7440 Th a199a228a229a241a252E = En+1 a21 a227a235a224a226a237a251a233 a247a235a...
244 0:8682 T 9 32 2:2441 Yh [7] 18 124 1:1990 T 27 260 1:5409 Th 10 44 1:4291 Td 19 132 1:0089 Y [9] 28 284 0:3722 T 11 48 1:6928 O [8] 20 148 0:8569 T 29 296 1:7440 Th a199a228a229a241a252E = En+1 a21 a227a235a224a226a237a251a233 a247a235a...
ANALYSIS OF COMBINED METAL CASTING THERMAL CONDITIONS: THE PRESSING PROCESS DURING CONFORM INSTALLATION
(2017-08)
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A N A L Y S I S O F C O M B I N E D M E T A...
L C A S T I N G T H E R M A L C O N D I T I O N S : T H E P R E S S I N G P R O C E S S D U R I N G C O N F O R M I N S T A L L A T I O N G o r o k h o v Y . V . 1 , S k u r a t o v A . P . 1 , B e l y a e v S . V . 1 , G u b a n o v I . Y . 1 , U...
L C A S T I N G T H E R M A L C O N D I T I O N S : T H E P R E S S I N G P R O C E S S D U R I N G C O N F O R M I N S T A L L A T I O N G o r o k h o v Y . V . 1 , S k u r a t o v A . P . 1 , B e l y a e v S . V . 1 , G u b a n o v I . Y . 1 , U...
CONFORM INSTALLATION STRUCTURAL ELEMENTS DESIGN METHODS
(2017-05)
The technical features in manufacturing press non-ferrous metal articles have been considered via the Conform continuous pressing. Based on an analysis of different types of press equipment, the absence of a connection between the system...
Förster resonance energy transfer between quantum dots and dye immobilized in biopolymer particles
(2018)
We used high adsorption properties of the cationic biopolymer chitosan to synthesize colloidal polymer particles (average size about 0.3 μm) with immobilized CdTe quantum dots (QDs) and organic dye (erythrosin B). A high local concentration...
Stabilization of butyrylcholinesterase by the entrapment into the natural polymer-based gels
(2018)
A new method for obtaining stable butyrylcholinesterase (BuChE) samples based on the enzyme immobilization in starch and gelatin gels followed by drying is proposed. Coimmobilization of BuChE with the thiol group indicator 5,5'-dithiobis(2...
ANION-EXCHANGE SYNTHESIS OF COPPER FERRITE POWDERS
(2018-05)
of the obtained samples were also studied. It
was determined that a ferromagnetically ordered phase is present in the synthesized materials and their magnetic
properties are close to those of bulk CuFe2O4....