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8 Jun 2010: Neuropharmacology 52 (2007) 733e743www.elsevier.com/locate/neuropharm. Pharmacological and computational analysis of alpha-subunitpreferential GABAA positive allosteric modulators. on the rat septo-hippocampal activity. Balázs Ujfalussy a,b,

8 Jun 2010: Theta Oscillation-Coupled Dendritic Spiking IntegratesInputs on a Long Time Scale. Zsófia Huhn,1 Gergo” Orbán,1,2 Péter Érdi,1,3 and Máté Lengyel4. ABSTRACT: Persistent neural activity lasting for seconds after transientstimulation has

8 Jun 2010: Mean amplitude of band oscillation (4 –5 Hz,umber of simulations run 24) at different levels of relative strength ofABAergic transmission (diamonds), 100% corresponding to the con-.

8 Jun 2010: It has been found that configural learning in animals[22], causal learning in rats [23] as well as in humaninfants [24] and a vast array of inductive learning phenom-ena fit

10 Nov 2010: n21 n. 22 n. 23 n. 24 = 1. Q = mn.

12 Aug 2010: n 0 1 2 3 4 12cjg<0 0.726(4) 0.86(1) 0.91(1) 0.93(1) 0.95(1) 12cjg>0 1.556(4) 1.24(1) ... This (incompressible) filled LL will appear as astep in the transverse density profile, as measured in situ orin an expansion measurement [24].

12 Aug 2010: function of a polarized filled LL times an additionalfactor describing the spin texture [24]. ... Finite Skyrmions of size K N=2 on thesphere have L S N=2 K [24].

12 Aug 2010: the relation between n andn remains linear [24,25], n n þ , with an offset. ... B. Laughlin, Phys. Rev. Lett. 59, 2095. (1987).[23] Time-reversal symm. is broken explicitly in the model.[24] F.

12 Aug 2010: 24 OCTOBER 2008. 0031-9007=08=101(17)=176803(4) 176803-1 2008 The American Physical Society. ... 24 OCTOBER 2008. 176803-2. CF-Fermi sea state is uniquely defined as filling two CFshells in each layer (at this flux, the pth CF shell has 2porbitals) [3,12]

12 Aug 2010: The data shown here arefor = 0.05 from Monte Carlo simulations on a lattice oflinear size L = 24, with the interaction summed over periodiccopies up to distance = 500 L.

12 Aug 2010: J. Thomson Avenue, Cambridge CB3 0HE, United Kingdom. 4Laboratoire Pierre Aigrain, Ecole Normale Supérieure, CNRS, 24 rue Lhomond, F-75005 Paris, FranceReceived 1 April 2009; published 23 June 2009.

12 Aug 2010: 4 0.99082. 9 24 84 5 104 0.98816. 10 27 319 6 104 0.984311 30 1160 7 104 0.98428 16 8 4 105 0.99872.

12 Aug 2010: 2Laboratoire de Physique Théorique et Mécanique Statistique, 91406 Orsay, FranceReceived 24 February 2005; published 19 July 2005. ... 498045 0.0531 0.065141 5 24 0.49761 0.0484 0.0584 7 18 0.497976 0.0502 0.0642 0.49682 0.0428 0.0608 0.49722 0.0413

30 Dec 2010: 2This was also found in the studies of Ref. [24] (D.K.K. ... not gauge-invariant. Under the transformation (24) the single-particle density operator becomes.

12 Aug 2010: 2Laboratoire de Physique Théorique et Modèles Statistiques, Université Paris-Sud, 91405 Orsay, France3Département de Physique, Laboratoire Pierre Aigrain, ENS, CNRS, 24 rue Lhomond, Paris F-75005, France. ... W. West,Phys. Rev. B 41, 7910 1990. 24 L.

11 Sep 2010: y′′ x2y = λy (24). The asymptote of its solution at |x| is. ... x2. 2. ). (26). into Eq (24) leads to the following equation for Hλ(x) :. {. d2. dx2+ 2x. d. dx λ 1. }. Hλ(x) = 0 (27).

25 Jan 2010: g. aB , ω2B = 12ga. l2(AB). so. ω2B = 12gal2B 24. ... 11. g2. l2ω2B ,. ω4 12gal2ω2 24. 11. g2. l2= 0 ,. and therefore. ω2 = 6ga. l2. 1. 1 2. 33. l2.

4 Apr 2010: 24. (a) Applying the Hubbard-Stratonovich transformation, the classical partition func-tion is given by.

4 Apr 2010: Phase Transitions and Collective Phenomena. 24 CHAPTER 2. GINZBURG-LANDAU PHENOMENOLOGY. Using Eq. ... 32 1.24 0.63Superconductors 0 1/2 1 1/2.

16 Aug 2010: SUHOV. satisfies. (1.24) y /. K(x,n). =1. ΛL(l)(x(l)),. then boxes Λ(n)L (x) and Λ. ... Set β = 1/2, α = 3/2 (cf.1.24). GivenE I and v Znd, the n-particle box ΛL(v) and the corresponding lattice box BL(v)are called.

16 Aug 2010: arX. iv:0. 907. 1459. v1 [. mat. h-ph. ] 9. Jul. 200. 9. Anderson localization in a two-particle. continuous model with an alloy-type external. potential. A. Boutet de Monvel1, V. Chulaevsky2, P. Stollmann3, Y. Suhov4. 1Institut de Mathématiques

16 Aug 2010: Instead, we refer the reader to the monographs [6, 20, 23], the surveys[18, 24] and the recent papers [2, 11] where such bibliography is presented. ... Progress in Math. Phys., vol. 20. Birkhäuser, Basel (2001)24. Veselić, I.: Existence and Regularity

28 Apr 2010: j=31. xij 1,. 14. j=11. xij 26. j=24. xij 1,. 30. ... 36.1FI 31.2FF 27.7HA 22.6HC 38.6MS 12.5MI 73.7BS. 51.7PI 18.6OJ 29.7QP 4.0GS 24.6SM 30.4SE 5.7TK = CARB;.

28 Apr 2010: j=31. xij 1,. 14. j=11. xij 26. j=24. xij 1,. 30. ... 36.1FI 31.2FF 27.7HA 22.6HC 38.6MS 12.5MI 73.7BS. 51.7PI 18.6OJ 29.7QP 4.0GS 24.6SM 30.4SE 5.7TK = CARB;.

15 Apr 2010: Stigler's guess for the optimal solution was off by only 24 cents per year.

25 Nov 2010: 236.5 Calculation of the Gittins index. 24. 6.6 Forward induction policies. ... 24. 7 Average-cost Programming 257.1 Average-cost optimization. 257.2 Example: admission control at a queue.

24 Mar 2010: n = 100 n = 200 n = 500 n = 1000 n = 2000d = 2 1.5 secs (260) 2.9 secs (500) 50 secs (1270) 4 mins (2540) 24 mins (5370)d = 3 6

10 Nov 2010: 23. 4.2.2 Notation. 24. 4.2.3 Defining the rates of individual interactions. ... 24. 4.2.4 Deriving the Markov chain rates. 25. 4.2.5 Example: n = 1.

26 Feb 2010: 24) ch(p, q) ‖p q‖2,λ Ch(p, q). holds for p, q P (t, ζ, D) with t > 1/2 and ζ > 0 (cf. ... Consequently, us-ing (24), the Hellinger-bracketing metric entropy H[](ε, P̄H(n), ‖ ‖2,λ) (with P̄H(n) ={ p : p P̃H(n) }) can be bounded by the L2(T

19 Nov 2010: F. Combining the bounds completes the proof of (24).It remains to prove (25). ... By (19) and (27), we have V ′ c2(λ)nσ 2, and the condition on t together with (24) givesthe result.

19 Feb 2010: The Annals of Statistics2010, Vol. 38, No. 2, 1122–1170DOI: 10.1214/09-AOS738 Institute of Mathematical Statistics, 2010. CONFIDENCE BANDS IN DENSITY ESTIMATION. BY EVARIST GINÉ AND RICHARD NICKL. University of Connecticut and University of

17 Aug 2010: F. Sidorenko, Percolation theoryand some applications, Itogi Nauki i Techniki (Series of Probability Theory,Mathematical Statistics, Theoretical Cybernetics) 24 (1986), 53–110.

9 Feb 2010: Recall from [23, 24] that hc(β) > 0 if and only if β < βc. ... 8.25). Inequality (8.24) holds by the positive association of random-cluster measureswith cluster-weights at least 1.

27 Apr 2010: First cut constraint. Second cut constraint. Product form. Outline. Slide Number 24.

24 Feb 2010: incentives are provided to the larger system [24, 38]. Might some of these ideas transfer to help our understanding of the. ... of rate control algorithms in the Internet [24, 38]. Let I+(n) = {i I : ni > 0}.

14 Feb 2010: the queue size. Instead, as described in [24, 25], protocols act to control the. ... Computer Communication Review, 38 (2008) 51–. 62. [24] G. Raina, D.

20 Jul 2010: 9.42. 55.88. 71.47. 25.74. 71.76. 16.87. 24. 66.91. 83.13. 34.2. 36. ... 13.31. 208.99. 33.94. 31.57. 8.21. 56.9. 69.16. 25. 64. 16.71. 24.39.

20 Jul 2010: 151.51 30.24 24.68 4.08 58.63 69.7 24.57 43.02 12.19 20.11 39.46 73.8 35.04 30.05 29.97 ... 29.96 24.24 4.17 58.27 68.57 24.42 42.2 12.24 19.88 36.65 73.43 34.77 29.87 29.6 28.33

7 Jun 2010: MC_SHP ABSENT PURE SUBSTANCE 23 SIC ABSENT PURE SUBSTANCE 24 MU_PHASE ABSENT SUBLATTICE 25 R_PHASE ABSENT SUBLATTICE 26 CHI_A12 ABSENT SUBLATTICE 27 P_PHASE ABSENT SUBLATTICE 28 ... NORMAL 23 Mo:2LAVES_PHASE_C14 NORMAL 24 Al:1AL4C3 NORMAL 25 Si:1AL4C3

7 Jun 2010: ABSENT PURE SUBSTANCE 22 AL4MN ABSENT PURE SUBSTANCE 23 AL6MN ABSENT PURE SUBSTANCE 24 AL8MN5_D810 ABSENT SUBLATTICE 25 CBCC_A12 ABSENT SUBLATTICE 26 CUB_A13 ABSENT SUBLATTICE 27 HCP_A3 ... 23 Al:1BCC_A2 NORMAL 24 Co:1BCC_A2 NORMAL 25 Cr:1BCC_A2 NORMAL

7 Jun 2010: Date and time of run 20-JUN-2007 16:55:08 070620165458,24 MTDATA 4.73 2002-11-15 14:22, LOG /numerobis/users/hala/mtdata/mt24.log 070620165502,24 ... 32965 on LNX-000-S (UNIX) using sgm000.exe 070620165507,24 MODULE 3 creates MPI file

7 Jun 2010: AL6MN ABSENT PURE SUBSTANCE 24 AL8MN5_D810 ABSENT SUBLATTICE 25 CBCC_A12 ABSENT SUBLATTICE 26 CUB_A13 ABSENT SUBLATTICE 27 HCP_A3 ABSENT SUBLATTICE 28 ALNI_B2 ABSENT PURE SUBSTANCE 29 ... NORMAL 19 Al.692Cr.308AL9CR4_ NORMAL 20 Al.692Cr.308AL9CR4_ NORMAL

7 Jun 2010: UNARY Fe:Cr:MoMONI_DELTA:24:20:12 WARNING: BINARY INTERACTION REJECTED - MISSING? UNARY Fe:Cr:MoMONI_DELTA:24:20:12 WARNING: BINARY INTERACTION REJECTED - MISSING? ... UNARY Cr:Fe:MoMONI_DELTA:24:20:12 WARNING: BINARY INTERACTION REJECTED - MISSING?

7 Jun 2010: 24> tcfe 298.15 6000.00 Cr:Cr:Fe<CHI_A12:24:10:24> tcfe 298.15 6000.00. ... Page 24 of 37Harry.txtPrinted: Wednesday, September 23, 2009 12:34:22. Component Ref.Phase Chem.Pot.

7 Jun 2010: 20 Va:2<FCC_A1> NORMAL 21 Cr:1<FE4N> NORMAL 22 Fe:1<FE4N> NORMAL 23 Mn:1<FE4N> NORMAL 24 C:2<FE4N> NORMAL 25 Cr:1<HCP_A3> ... 24> tcfe 298.15 6000.00 Cr:Cr:Fe<CHI_A12:24:10:24> tcfe 298.15 6000.00.

7 Jun 2010: 1/T / K-1. log. 10k! AlN. BNTiN. TiN: (Turkdogan)log kγ = 5.4 -(15790/T)AlN: ( Gladman)log kγ =1.03 -(6770/T)BN: ( Fountain & Chipman)log kγ = 5.24

7 Jun 2010: SUBSTANCE Type return for more, Q to quit paging : 22 AL3M_DO22:.75:.25 NORMAL PURE SUBSTANCE 23 ALNI_B2:.5:.5 NORMAL PURE SUBSTANCE 24 DIAMOND_A4 NORMAL PURE SUBSTANCE

7 Jun 2010: 1 NORMAL PURE SUBSTANCE Type return for more, Q to quit paging : 22 CRSI2:1:2 NORMAL PURE SUBSTANCE 23 CHI_A12:24:10:24 NORMAL PURE SUBSTANCE 24 ... CR3SI:3:1 absent PURE SUBSTANCE Type return for more, Q to quit paging : 22 CRSI2:1:2 absent PURE

7 Jun 2010: 475. -277. -156. -24. 0.90E-04 0.0377 0.55E-03 0.0205 0.0099 0.0000 0.7669 0.22E04 0.17E03 913. ... 207. -24. -4. 122. 0.94E-04 0.0085 0.15E-03 0.0008 0.0021 0.0000 0.3240 0.28E09 0.26E05 MS= 663.

7 Jun 2010: 1CEMENTITE NORMAL 20 C:2CEMENTITE NORMAL 21 Fe:1CUB_A13 NORMAL 22 Mn:1CUB_A13 NORMAL 23 Ni:1CUB_A13 NORMAL 24 C:2CUB_A13 NORMAL 25 Va:2CUB_A13 NORMAL