نتایج جستجو برای: ñ

تعداد نتایج: 579  

2013

μ â q Z K̈ y Å Š z z Z ã Z 0 s Æ ́ z { Z qZ z g „ CÙ Â å Z K̈ y ì 1 : „ å % Š Z z g : „ å ú g ] ƒ C ì X p Z z u Z Ô Æ Z Ô 3, !* y Ô Z z g 7 ~ 1 Z ñ z ) { Æ * x Ð å g } Y ä z Z á ç Ñ } ~ ñ Š Z y TM Š Z g z V Å | (, ~ Š g Š * u ì X Z k ï Ã Z C * á h+ Z y Å 6 g ~ ì X ‚ g ~ i 0+ Ï Z K̈ y Å w q Ý TM ä Æ p Z [ Š Ú z Z à t Š g ] Å z { ‘ t ì X ~ ” h+ Ù ! d Z y 0* c Y @* ì X t TM Š Z g a Z Â Z 0 W Š x ...

2015

› â V » o { ì g Î w Z v | ] · Z v m z Å g z ̄ a #Ö Z v ¬ \ Æ — g Z L Z $ 4 3 ðG G V Æ h ~ Ë ®) Û â N Ð X CÙ › y Å t Š à M g i z ì Z k Š y Z Ð M \ Z v m z Å Å ~ Z k o { Å z Ÿ s# V Å ˆ ì : † | ] Ö Ã Ï n ‚ é ] Ö _ v ^ æ m è Ë ®) ‚ ƒ X æ œ Ú ^ œ â Ø ] Ö Š ß è æ ] Ö r Û ^  è Ê n Ï † æ á e Ë ^  è Þ f n ß ^ ‘ × o ] Ö ×# ä Â × n ä æ ‰ × Ü Ê o œ â Ø ] Ö Ó f ^ ñ † ( æ Ë ^  è Æ n † å ( Ö Ó à Ÿ m Ë ...

2011
Rudolf Kaehr Marcus Kracht

The main differences between symbolic and morphic formal systems: Instead of the Kleene star for the symbolic universes, morphic universes are generated by the Stirling cross. Symbolic substitution and concatenation is preserving production concatenation. Morphic substitution/concatenation is opening up a system of interactive complexions of derivations. Comparison of substitution based product...

Journal: :Fiziolohichnyi zhurnal 2003
G Zubieta-Castillo G R Zubieta-Calleja L Zubieta-Calleja Zubieta-Calleja Nancy

Èñòîðèÿ âîñõîæäåíèé íà Ýâåðåñò ïîêàçûâàåò, ÷òî äàæå íà òàêîé âûñîòå ñóùåñòâóþò ìåõàíèçìû òêàíåâîé àäàïòàöèè, ñïîñîáíûå ïîääåðæèâàòü æèçíü. Åñòü äàííûå, ñâèäåòåëüñòâóþùèå î âîçìîæíîñòè ÷åëîâåêà âûïîëíÿòü òÿæåëóþ ôèçè÷åñêóþ ðàáîòó íà ýêñòðåìàëüíûõ âûñîòàõ. 2 àâãóñòà 2001 ãîäà ôóòáîëüíàÿ êîìàíäà Áîëèâèè óñïåøíî ïîêîðèëà ñàìóþ âûñîêóþ âåðøèíó Áîëèâèè ïèê Ñàéàìà (6542 ì) è ñûãðàëà òàì ôóòáîëüíûé ìàò...

2005
G. PIZZA C. DE VINCI G. LO CONTE A. MAZZUCA V. DI MAIO S. RATINI G. SEVERINI L. BUSUTTI A. P. PALARETI A. GULINO A. VACCA L. MELCHIORRI M. FERRARI L. GIACOMELLI O. R. BARICORDI S. FORZINI R. CAPANNA

In a limited study, comprising only ten patients, we have previously reported that allogeneic irradiated RCC-cell-line cells, engineered to produce IL-2 (ACHN-IL-2), admixed with autologous metastatic formalin-treated tumour cells were used to vaccinate MRCC patients in progression of disease and also receiving IL-2 immunotherapy. The cells, admixed to autologous TC, were administered subcutane...

2002
Elvi Räisänen-Ruotsalainen Kimmo Lasanen M. Sijander Juha Kostamovaara

â ã ä å ae ç å è ç é ê é ë ae ì í î è ï ã ï å é ê é ð ñ å ò ò í ó ï è ï é ê é ð ô ï ö ÷ ì è ø å ã ù ï é ú ê ö ï é ú û ì ü ï ñ í è î ï ò í ä ï ï ö ï

2004
Ashok Das J. Frenkel

We show that the Feynman propagator in the light-cone gauge with the MandelstamLeibbrandt prescription has a logarithmic growth for large ñ · x which is related to the presence of a residual gauge invariance. Furthermore, we show that the retarded propagator for the ñ · A component of the gauge field develops a coordinate dependent mass which is inversely proportional to the magnitude of the tr...

2016
Ivan Gavran

It is clear that Ñ would accept L (N accepts if one branch ends up in the accepting state. Ñ would notice that as rejecting state it would reject as soon as there is one rejecting state because all the states are universal. N rejects if no branch end in an accepting state, i.e., all end up in the rejecting state. But for Ñ that would mean that all the branches are accepting, therefore, it would...

2003
SERGEY ARKHIPOV VICTOR GINZBURG

In this diagram, G is a connected complex semisimple group of adjoint type with Lie algebra g. We fix a Borel subgroup B ⊂ G, write b = Lie B ⊂ g for the corresponding Borel subalgebra, and n for the nilradical of b. Let Ñ := G×B n be the Springer resolution, and CohG×C ∗ (Ñ ) the abelian category ofG×C∗-equivariant coherent sheaves on Ñ , where the group G acts on Ñ by conjugation and C∗ acts ...

2011
Kai Schweda

We report recent results from the ALICE experiment the Large Hadron Collider on open charmed hadron production in pp collisions at ? s “ 2.76 and 7 TeV, and Pb–Pb collisions at sNN “ 2.76 TeV. Open charmed hadrons are kinematically fully reconstructed in the hadronic decay channels D0 Ñ K ́π`, D` Ñ K ́π`π`, and D ̊`p2010q Ñ D0π`and identified through their invariant mass. Combinatorial background ...

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