Search

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 :

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

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.

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