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doi:10.1016/j.neuropharm.2006.09.022
www3.eng.cam.ac.uk/~go223/Publications/ujfalussy07.pdf8 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, -
Theta oscillation-coupled dendritic spiking integrates inputs on a…
www3.eng.cam.ac.uk/~go223/Publications/huhn05.pdf8 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 -
doi:10.1016/j.neuroscience.2004.03.043
www3.eng.cam.ac.uk/~go223/Publications/hajos04.pdf8 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-. -
doi:10.1016/j.tics.2010.01.003
www3.eng.cam.ac.uk/~go223/Publications/fiser10.pdf8 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 -
Skyrmions in Condensed Matter Systems
www.tcm.phy.cam.ac.uk/~nrc25/SEMINARS/skyrmions_damtp_2010.pdf10 Nov 2010: n21 n. 22 n. 23 n. 24 = 1. Q = mn. -
Density Waves and Supersolidity in Rapidly Rotating Atomic Fermi ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.99.190409.pdf12 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]. -
Skyrmions in the Moore-Read State at � ¼ 52Arkadiusz ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.104.086801.pdf12 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]. -
Composite Fermion Theory for Bosonic Quantum Hall States on ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.103.105303.pdf12 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. -
Paired Composite Fermion Phase of Quantum Hall Bilayers at ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevLett.101.176803.pdf12 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] -
Magnetic multipole analysis of kagome and artificial spin-ice dipolar …
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.80.140409.pdf12 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. -
Fractional quantum Hall state at � = 14 in ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.79.245325.pdf12 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. -
Trial wave functions for � = 12 +12 quantum ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.79.125106.pdf12 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. -
Composite fermions in a negative effective magnetic field: A ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevB.72.045344.pdf12 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 -
PHYSICAL REVIEW A 82, 063625 (2010) Condensed ground states ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevA.82.063625.pdf30 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. -
Pairing in ultracold Fermi gases in the lowest Landau ...
www.tcm.phy.cam.ac.uk/~gm360/papers/source-free/PhysRevA.79.033609.pdf12 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. -
Tale 6 The Kramers’ Phase and Laplace’s Method The ...
www.tcm.phy.cam.ac.uk/~dek12/tales/Tale-06.pdf11 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). -
NATURAL SCIENCES TRIPOS Part II Wednesday 13 January 2010 ...
www.tcm.phy.cam.ac.uk/~cc726/TP1/ExamFiles/exam10sol.pdf25 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. -
phmain
www.tcm.phy.cam.ac.uk/~bds10/phase/tripans.pdf4 Apr 2010: 24. (a) Applying the Hubbard-Stratonovich transformation, the classical partition func-tion is given by. -
phmain
www.tcm.phy.cam.ac.uk/~bds10/phase/gl.pdf4 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. -
arX iv:1 004. 1300 v1 [ mat h-ph ] ...
www.statslab.cam.ac.uk/~yms/BCSS3.pdf16 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. -
arX iv:0 907. 1459 v1 [ mat h-ph ] ...
www.statslab.cam.ac.uk/~yms/BCSS2.pdf16 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 -
J Stat Phys (2010) 138: 553–566DOI 10.1007/s10955-009-9883-1…
www.statslab.cam.ac.uk/~yms/BCSS1.pdf16 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 -
oheads_lectures.dvi
www.statslab.cam.ac.uk/~rrw1/opt/oheads_lectures4up.pdf28 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;. -
oheads_lectures.dvi
www.statslab.cam.ac.uk/~rrw1/opt/oheads_lectures.pdf28 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;. -
History of the Diet Problem
www.statslab.cam.ac.uk/~rrw1/opt/diet_history.html15 Apr 2010: Stigler's guess for the optimal solution was off by only 24 cents per year. -
L.dvi
www.statslab.cam.ac.uk/~rrw1/oc/L2010a4.pdf25 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. -
Maximum likelihood estimation of a multidimensional log-concave…
www.statslab.cam.ac.uk/~rjs57/CSSFinalLV.pdf24 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 -
ODE approximations to some Markov chain models Perla Sousi ...
www.statslab.cam.ac.uk/~ps422/smithknight1.pdf10 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. -
IMS CollectionsHigh Dimensional Probability V: The Luminy VolumeVol.…
www.statslab.cam.ac.uk/~nickl/Site/__files/IMSCOLL522.pdf26 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 -
Adaptive estimation of a distribution function and its density in…
www.statslab.cam.ac.uk/~nickl/Site/__files/BEJ239.pdf19 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. -
Confidence bands in density estimation
www.statslab.cam.ac.uk/~nickl/Site/__files/AOS738.pdf19 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 -
PLAQUETTES, SPHERES, AND ENTANGLEMENT GEOFFREY R. GRIMMETT AND…
www.statslab.cam.ac.uk/~grg/papers/USsphere11.pdf17 Aug 2010: F. Sidorenko, Percolation theoryand some applications, Itogi Nauki i Techniki (Series of Probability Theory,Mathematical Statistics, Theoretical Cybernetics) 24 (1986), 53–110. -
SHARP THRESHOLDS FOR THE RANDOM-CLUSTER AND ISING MODELS BENJAMIN ...
www.statslab.cam.ac.uk/~grg/papers/boxUS.pdf9 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. -
Proportional fairness and product form
www.statslab.cam.ac.uk/~frank/TALKS/ima2010.pdf27 Apr 2010: First cut constraint. Second cut constraint. Product form. Outline. Slide Number 24. -
18 Heavy traffic on a controlled motorway F. P. ...
www.statslab.cam.ac.uk/~frank/PAPERS/KingFest/kwroad.pdf24 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}. -
1 Explicit Congestion Control:charging, fairness and…
www.statslab.cam.ac.uk/~frank/PAPERS/ecc.pdf14 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. -
Sheet1
www.statslab.cam.ac.uk/~chris/DATAPAK/SomeSP.xls20 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. -
www.statslab.cam.ac.uk/~chris/DATAPAK/SomeSP.txt
www.statslab.cam.ac.uk/~chris/DATAPAK/SomeSP.txt20 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 -
www.phase-trans.msm.cam.ac.uk/mtdataarchive/sp11-tcfe-fcc-bcc-cem.txt
www.phase-trans.msm.cam.ac.uk/mtdataarchive/sp11-tcfe-fcc-bcc-cem.txt7 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 -
www.phase-trans.msm.cam.ac.uk/mtdataarchive/SP11-sgte-fcc-bcc.txt
www.phase-trans.msm.cam.ac.uk/mtdataarchive/SP11-sgte-fcc-bcc.txt7 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 -
www.phase-trans.msm.cam.ac.uk/mtdataarchive/SP11-sgte-fcc-bcc-cementit…
www.phase-trans.msm.cam.ac.uk/mtdataarchive/SP11-sgte-fcc-bcc-cementite.txt7 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 -
www.phase-trans.msm.cam.ac.uk/mtdataarchive/Salman.txt
www.phase-trans.msm.cam.ac.uk/mtdataarchive/Salman.txt7 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 -
www.phase-trans.msm.cam.ac.uk/mtdataarchive/paraequilibrium.txt
www.phase-trans.msm.cam.ac.uk/mtdataarchive/paraequilibrium.txt7 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? -
Harry.txt
www.phase-trans.msm.cam.ac.uk/mtdataarchive/Pandit2.pdf7 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. -
Harry1.txt
www.phase-trans.msm.cam.ac.uk/mtdataarchive/Pandit1.pdf7 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. -
mucg84_boron_mod
www.phase-trans.msm.cam.ac.uk/mtdataarchive/mucg84_boron.pdf7 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 -
www.phase-trans.msm.cam.ac.uk/mtdataarchive/IF.txt
www.phase-trans.msm.cam.ac.uk/mtdataarchive/IF.txt7 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 -
www.phase-trans.msm.cam.ac.uk/mtdataarchive/hojo.txt
www.phase-trans.msm.cam.ac.uk/mtdataarchive/hojo.txt7 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 -
www.phase-trans.msm.cam.ac.uk/mtdataarchive/Francis_MTTTDATA.txt
www.phase-trans.msm.cam.ac.uk/mtdataarchive/Francis_MTTTDATA.txt7 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. -
www.phase-trans.msm.cam.ac.uk/mtdataarchive/FeNiMnC_paraequilibrium/al…
www.phase-trans.msm.cam.ac.uk/mtdataarchive/FeNiMnC_paraequilibrium/alloy3_para2.txt7 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
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