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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. -
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
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