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22 Nov 2003: 3ZXMe"V Z-y/cNl13PN5@/E36A-(69%36AO=14&-OP-EA-E54(I1R5R"M+([$R$'"?AO 14&5436NO&14&-_huA>3[1 ... 3PAx18&-7+)9%(6A-PJ OP-E3u:-E$'"%/73PA()9 ([A-"?$(@$ 1R54(6"?OP&G19%"?A-PJ u3>M14&-$ 1454(6"VO&1 9%"?A-!

7 Jan 2019: E A B1C91JW XMY ZMY[ 4]HH_H a11M HaH bHcd e J f3 249 7 3 A 9 249 0 5 F3 :hgGikjl mn lhop l@q jl r op ... op l t u /1: 0 9 xHS43 0 9 I@JyMB10<7 849: 9 A B24I=0 BHI s 7 849A 9 27 0 9B1ThC/1: : 3 : /17z iw n :

7 Jan 2002: E A B1C91JW XMY ZMY[ 4]HH_H a11M HaH bHcd e J f3 249 7 3 A 9 249 0 5 F3 :hgGikjl mn lhop l@q jl r op ... op l t u /1: 0 9 xHS43 0 9 I@JyMB10<7 849: 9 A B24I=0 BHI s 7 849A 9 27 0 9B1ThC/1: : 3 : /17z iw n :

12 Aug 2010: Inbrief, we find a second order phase transition near d 1from the CF-BCS phase at larger d, which has zero 111order parameter (OP), to a phase with nonzero 111 OP ... mix with composite bosons (CB’s) and the presenceof CB’s yields nonzero 111 OP.

18 Oct 2003: " # $. %'&()-,/.02143658790;:=<>.@?:A.@?B7C.DE5FG.IHJ0;:K79?:9F02,MLJNO5P1Q1SR TU1479)05PF/1K3V0;:$1W.X.YHBZ[.@?/1;]51$Z7_1K0;0aA1bRCTc7dZe1gfBF/.I3 Fh7S)i587g79)0 5]79j.@1K<i)02:QZek</:W021W1Q?:W0

5 Mar 2004: then our parti le moves aperiodi ally. In the op-posite limit!

9 Oct 2009: z. From this. definition, confirm that The choice z = x iy (as op-posed to z = x iy) is madeon purely aesthetic grounds – seethe wavefunction below.

8 Oct 2009: Û †ÂÛ = R[Â]. Such unitary transformations are said to be symmetries of a general op-erator Ô(p̂, r̂) if. ... i! θên L. ]. As we have seen, time translations are generated by the time evolution op-erator, Û (t) = exp[ i!Ĥt].

24 Aug 2020: However, in ferroelectrics the motion of the atoms in op-tical modes leads to the emergence of electric dipoles.

18 Oct 2003: "$#% &(')-,/.1032457698:8;=<?>A@8;CBD>A;FEHGI69JLKNMO<D;=PQBDJ7GRJ EHBD>TSG76UJWVYX >[Z5IB?J7GI>FE]PQB;=E]8_;C<;=8[X7JYB?a66UJb;C5 Ec<NMdE/BDJfehg<?J78F69G E]>jiBHkE]8j6UJl8[5YB?P9PU</iminBo;FE]>]pqij57<r8AEG EOs ;=5utv698w

24 Aug 2020: ηαβ. r)pαβ(r), pαβ is a polynomial whose parameters are op-timized in VMC, and Lηαβ is a cutoff length.

30 Jul 2019: ultracold atomic gases [13] promises un-paralleled experimental accuracy, presenting an ideal op-portunity to revisit the structure of the superconductingground state of spin-imbalanced Fermi gases.

24 Aug 2020: Asnickel-base superalloys have been intensely studied sincethe 1930’s [12, 26–84] and there are over 120 commerciallyavailable alloys for different specialist applications, the op-timizing program showed that there ... The points show experimental

10 Oct 2012: He con-tributed to many areas of mathematics. example is the kinetic energy op-erator T̂ =. Pn. p̂2n. 2m , where p̂n isthe momentum operator acting onthe n-th particle. ... have described a physical systemin terms of a theory involving a continuum of

24 Aug 2020: ultracold atomic gases [13] promises un-paralleled experimental accuracy, presenting an ideal op-portunity to revisit the structure of the superconductingground state of spin-imbalanced Fermi gases.

8 Oct 2009: Writing the plane wavefunction φ(r, t) = Aei(prEt)/!, where A is a constant, we can recover theenergy-momentum invariant by adding a constant mass term to the wave

12 Aug 2010: The loop pattern op-timizes the local dipolar energy, in that each dimer is ori-ented favorably with respect to its four nearest neighbors anddue to the convergent nature of the

26 Feb 2018: As well as this the indi-vidual cavity-qubit systems are surrounded by their ownradiation shields made from a special alloy Amumetalthat is annealed in a dry Hydrogen atmosphere for

14 Jan 2013: Current insights in the analytic theory of fractional Cherninsulators rely on the analysis of the projected density op-erator algebra [18,19] or of emergent symmetries in the exactmany-body spectrum

10 Nov 2013: ô = λ=0 |λ〉oλ〈λ|, oλ = 〈λ|ô|λ〉e.g. k.e., |λ〉 |p〉 and op = p2/2m. ... Lecture X: Many-body (Coherent State) Path Integral. Having obtained a complete coherent state basis for the creation and annihilation op-erators, we could

18 Nov 2009: Secondly, to ensure that the field op-erator φ̂(x) obeys the Klein-Gordon equation,10 we require φ̂(k) 2πδ(k2 m2).Taking these conditions together, we require.

24 Jun 2012: cyi cyi cici; (1). where cyi and ci are boson creation and annihilation op-erators on lattice site i, J is the hopping energy, and U is the.

24 Aug 2020: GREPHYSICAL REVIEW APPLIED 12, 034024 (2019). Au-Ge Alloys for Wide-Range Low-Temperature On-Chip Thermometry. J.R.A. Dann,1, P.C. Verpoort,1 J. Ferreira de Oliveira,1,2 S.E. Rowley,1,2 A. Datta,3 S. Kar-Narayan,3C.J.B. Ford,1 G.J. Conduit,1 and V.

28 Sep 2021: 2] R. C. Reed, A. Mottura, D. J. Crudden, Alloys-By-Design: Towards Op-timization of Compositions of Nickel-based Superalloys, in: Superalloys2016, 2016, pp.

22 Jan 2024: The authors are grateful to D.V. Averin for fruitfuldiscussions. Samples were fabricated by the Microelec-tronics Laboratory of the Jet Propulsion Laboratory, op-erated by the California Institute of Technology

27 Jul 2019: INVERSE PROTEIN FOLDING. HIERARCHICAL OPTIMISATION. AND TIE KNOTS. Thomas M A Fink. st johns college. university of cambridge. a dissertation. submitted for the degree. of doctor of philosophy at the. university of cambridge. T O M Y M O T H E R.

2 Apr 2015: Default value is 0.01eV. 5.4.3 real(kind=dp) :: scissor op. Value of the scissor operator.

12 Aug 2010: As usual, the fermion op-erators have anticommutation relations ci. † , cj = i, j.

24 Aug 2020: Collective phenomena in correlated. semiconductors, degenerate Fermi. gases, and ferroelectrics. G.J. Conduit. Selwyn College. University of Cambridge. April 2009. This thesis is submitted. for the degree of. Doctor of Philosophy. i. Collective

13 Feb 2019: B. Littlewood and P. Eastham, inProceedings of the NATO Advanced Research Workshop “Op-tical Properties of Semiconductor Nanostructures”, NATO Sci-ences High Technology Series, Kluwer, 2000.

24 Oct 2022: S O FT AND HARD E L AS T I C I T Y O F. L I Q UI D C RYS T AL E L AS T O ME RS. S O F T A N D H A R D E L A S T I C I T Y O F. L I Q U I D C R Y S T A L E L A S T O M E R S. John Simeon Biggins. corpus christi college. university of cambridge. a

12 Aug 2010: 3 numerical operations, whereas the wave func-tions from Ref. 34 require explicit antisymmetrization, anoperation that requires much computation power with an op-eration count scaling exponentially with the system size.

5 Feb 2019: QUANTUM MONTE CARLO. CALCULATIONS OF. ELECTRONIC EXCITATIONS. By. Andrew James Williamson. Robinson College, Cambridge. Theory of Condensed Matter Group. Cavendish Laboratory. Madingley Road. Cambridge. CB3 0HE. A dissertation submitted for the.

5 Feb 2019: Linear-scaling methods in ab initio. quantum-mechanical calculations. A dissertation submitted for the degree of. Doctor of Philosophy. at the University of Cambridge. Peter David Haynes. Christ's College, Cambridge. July 1998. Preface. This