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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.

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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

2 Jul 2024: Finally, as can also be seen in Fig. 3 the nCFl of the op-timized MS1 and YM1 wave functions are noticeably largerthan one in some cases and are negative in

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