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Cosmological Models in f(R,T) Theory of Gravitation

Cosmological Models in f(R,T) Theory of Gravitation

We have presented tilted cosmological models in f R T ( , ) theory of gravitation without taking any relation between density  and pressure p .The model are expanding, shearing and rotating universe. The model starts with big bang at t  c 1 and the expansion in the model decreases as time increases and the expansion in the model stop at t   .There is a singularity in the model at t  c 1 This singularity is

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Widening the Nexus: From T-R to T-T-R

Widening the Nexus: From T-R to T-T-R

At Sout hampt on Solent Universit y t he inclusive concept of Advanced Scholarship is used t o recognise and support high-level academic endeavour, including research, and t hird st ream (engagement wit h business and communit ies). The ut ilit y of t his approach has been demonst rat ed f or a wide range of act ivit ies and subj ect disciplines. A key f eat ure is t hat Advanced Scholarship act ivit ies are expect ed t o enhance t he st udent experience, hence a t hird st ream-t eaching-research (T-T-R) nexus.
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T r a ns m i s s i o n Ne t w o r kC o ng e s t i o n i n D e r e g ul a t e d W ho l e s a l eE l e ct r i ci t yM a r k e t

T r a ns m i s s i o n Ne t w o r kC o ng e s t i o n i n D e r e g ul a t e d W ho l e s a l eE l e ct r i ci t yM a r k e t

Whenever transmission network congestion occurs in electricity market, it divides the market in different zones and the trading price of electricity will no longer remains the same for t[r]

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On t h e e v o l u t i o n a r yf o r mo f t h ec o n s t r a i n t s in e l e c t r o d y n a m i c s

On t h e e v o l u t i o n a r yf o r mo f t h ec o n s t r a i n t s in e l e c t r o d y n a m i c s

where S could be of a two-surface with arbitrary topology. In the simplest prac- tical case, however, S would have either planar, cylindrical, toroidal or spherical topology. In these cases, we may assume that there exists a smooth real function ρ : Σ → R whose ρ = const level sets give the S ρ leaves of the foliation and that its

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D e r i v a t i o n o f t he L o c a l L o r e nt z G a ug e T r a ns f o r m a t i o n o f a D i r a c Spi no r F i e l d i n Q ua nt um E i ns t e i n- C a r t a n T he o r y

D e r i v a t i o n o f t he L o c a l L o r e nt z G a ug e T r a ns f o r m a t i o n o f a D i r a c Spi no r F i e l d i n Q ua nt um E i ns t e i n- C a r t a n T he o r y

[?] (Einstein-Cartan theory), Mes- siah [?] (non-relativistic quantum mechanics), Bjorken and Drell [?] (relativistic quantum me- chanics), Bjorken and Drell [?] (quantum elec- trodynami[r]

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THE B I R A T I O N A L G E O ME T R YO F T R O P I C A LC O MP A C T I FI C A T I O N S

THE B I R A T I O N A L G E O ME T R YO F T R O P I C A LC O MP A C T I FI C A T I O N S

The phrase “toroidal singularities” means that at each point in the boundary X \ X the variety is locally (in the analytic topology) isomorphic to a possibly singular toric variety. Stat[r]

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Suppl e m e nt a r y m a t e r i a l t o “ H a z e , H ung e r H e s i t a t i o n: D i s a s t e r A i d a f t e r t he 1 7 8 3 L a k i e r upt i o n” : So c i o - e c o no m i c a s pe c t s o f t he L a k i e r upt i o n i n c o nt e m po r a r y r e p

Suppl e m e nt a r y m a t e r i a l t o “ H a z e , H ung e r H e s i t a t i o n: D i s a s t e r A i d a f t e r t he 1 7 8 3 L a k i e r upt i o n” : So c i o - e c o no m i c a s pe c t s o f t he L a k i e r upt i o n i n c o nt e m po r a r y r e po r t s

Þingeyjarsýsla, 16th September 1784: During winter, people from the northern commune could not reach the trade post due to the ice and to lack of horses and hay.. Currently, there is a f[r]

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Sym e t r i c a l D e f o r ma t i o no f T o r o i d a l S h e l l wi t hC i r c u l a r Cr o s s - S e c t i o n

Sym e t r i c a l D e f o r ma t i o no f T o r o i d a l S h e l l wi t hC i r c u l a r Cr o s s - S e c t i o n

We have successfully obtained exact solution of complex form equation for symmetrical deformation of toroidal shells. The research has confirmed that the deformation of all regular shell structure, such cylindrical shell, conical shell, spherical shell and toiroidal shell can be solved by hypergeometric functions. This supports the doctrine of Zurich school of shell theory [1, 2, 7], which predicted that bending deformation of all regular shells can be expressed by the hypergeometric functions. Through numerical comparison study, the mechanics of toroidal shells is quite sensitive to the radius ratio ε = R a . By slightly adjustment of the ratio might get a desired high performance shell structure.
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Frost hardiness of Eucalyptus delegatensis R T  Baker

Frost hardiness of Eucalyptus delegatensis R T Baker

other Eucalyptus species at four sites at different altitudes and the effect of site maximum and minimum temperatures on growth rate and frost hardiness were evaluated.... Determination [r]

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A B S T R A K pdf

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Kegunaan Praktis : 1 Penelitian ini diharapkan dapat bermanfaat dan digunakan sebagai masukan bagi Pemerintah Daerah Kabupaten Tulang Bawang dalam memberikan perlindungan hukum dalam ben[r]

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¨U B S C H - K R A W ON B E R G L U N D - H I T ZM I R R O R S Y ME T R Y

¨U B S C H - K R A W ON B E R G L U N D - H I T ZM I R R O R S Y ME T R Y

In this chapter, we present a toric framework using Gorenstein cones that attempts to unify the two mirror construction frameworks of Batyrev-Borisov and BHK. There has been some work in the past on this approach ([17], [41], and [11]). We provide an alternate approach that is done by using the approach given by [11] and fitting it into an explicit context of toric vector bundles. We take dual Gorenstein cones σ and σ ∨ of index r. In this work, we find fans Σ and Σ ∨ which have corresponding toric varieties X Σ and X Σ ∨ that are vector bundles over two other

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A B S T R A K pdf

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Sebagai salah satu rezim dari TRIPs, IG diatur berdasarkan tujuan utama TRIPs untuk mempromosikan perlindungan yang efektif dan memadai bagai HKI, dan untuk meyakinkan tiap anggota TRIPs[r]

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A B S T R A K pdf

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Dalam penelitian ini akan mengangkat tema tentang Sistem Informasi Pendataan Mahasiswa Fakultas Matematika dan Ilmu Pengetahuan Alam untuk pendataan mahasiswa maupun dosen serta memberik[r]

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A B S T R A K pdf

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Data Flow Diagram adalah suatu model logika data atau proses yang dibuat untuk menggambarkan dari tempat asal data dan tempat tujuan data yang keluar dari sistem, di tempat data disimpan[r]

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L E -C OUN T I N GQ -R OK T H E OR YANDO T H E R EN E R AL I Z A T I ON S O FC L A SSI CALROK T H E OR Y

L E -C OUN T I N GQ -R OK T H E OR YANDO T H E R EN E R AL I Z A T I ON S O FC L A SSI CALROK T H E OR Y

In this model, first introduced in [8], we allow only one rook per column but more than one rook in a given row. We will call an arrangement of rooks, with at most one rook in each column (but possibly more than one rook in a row), an α-rook placement. We will denote the set of all α-rook placements of k rooks on a board B by R (α) k (B). If there are u rooks in a given row, that row has weight

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BIQUOTIENTS WI T HA L MO S TP O S I T I V EC U R V A T U R E

BIQUOTIENTS WI T HA L MO S TP O S I T I V EC U R V A T U R E

Bonnet-Myers Let M n be a complete Riemannian manifold and suppose that the Ricci curvature satisfies Ric ≥ δ > 0. In fact, Brendle and Schoen proved more general rigidity results whi[r]

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Lo c a l i z a t i o n , P a t h i n t e g r a l a n dS u p e r s y m m e t r y

Lo c a l i z a t i o n , P a t h i n t e g r a l a n dS u p e r s y m m e t r y

: Let’s start with a very simple problem: This prob- lem is resolvable by a high school student: Consider a mouse moving over a grid consisting of n rows and m columns. His only possible actions are to advance or step up without ever going back or down. it is well known that counting all the possible trajectories consists of counting the number of anagrams consisting of n times the letter A and m times the letter M. in this case the sum of all possible trajectories is a finite number is the combinations of n among n + m: N T =

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evisiting Co n s t r a i n t so f Fo u r t h - Ge n e r a t i o nQ u a r k s a n dL e p t o n s

evisiting Co n s t r a i n t so f Fo u r t h - Ge n e r a t i o nQ u a r k s a n dL e p t o n s

In recent years the SM4, the upgraded version of SM3 has been in point of attraction by many physicists. After the last piece, Higgs Boson in the SM3, there are many questions in paucity about the masses of next Leptons and Quarks. In SM3, the mass of Higgs Boson is 125.18 ± 0.16 GeV [1], but there is quite an update that we will encounter with the Higgs masses. In SM4, the mass of Higgs Boson is around 115 GeV (we will examine it later) . With the extension of SM3 to SM4, we just add a couple of Leptons and Quarks, Quarks t’ and b’ with isopin of 1 2 and − 1 2 respectively (but that is not the case, we will see it later) and Lepton l’ and its corresponding Neutrino. There are a lot of discussions about the masses and flavor mixing of leptons and quarks. In our model, we will be looking at the current Koide Formula (Hypothesis) [2]: [3]
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T STA73 R STA73 T STA74 R STA74 T STA75

T STA73 R STA73 T STA74 R STA74 T STA75

Group 10 External All Call is not a valid group selection when using these dial codes NOTE: For Group selection and Background Music Programming: Group 1 Group 2 Group 3 Group 4 Group 5 [r]

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Solutions of the neutral differential difference equation αx′(t)+βx′(t−r)+γx(t)+δx(t−r)=f(t)

Solutions of the neutral differential difference equation αx′(t)+βx′(t−r)+γx(t)+δx(t−r)=f(t)

Suppose that an exponential type solution exists to the homogeneous equation 1.1b of the form e The value of will be given as one of the roots of the characteristic equation hg- 0 where [r]

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