Results 1 - 7 of 7 for dc---r .
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DC conductivityKey idea: massless mode conserved quantity, express the DCconductivity in terms of r0. ... σDC (r) = limω0. Πiωλ1. r. σDC () = σDC. can show σ′DC (r) = 0!
www-thphys.physics.ox.ac.uk/people/AndreiStarinets/oxford_holography_group/holography_seminar/Seminar/Slides/andrade.pdf- 664k - 20 Feb 2014 - Cached
D D. A A. d d. A A D DC. r rd d. ... r r. qN x dE x d x. qN xE x - E x d.
users.physics.ox.ac.uk/~rtaylor/teaching/devices/lecture1ppt.pdf- 372k - 4 May 2010 - Cached
Asbefore, a basic step requires time of |DC| |R|2 time, and we perform at most |R| basicsteps, so the algorithm requires polynomial time. ... For all r R do S(vr) 4. T DC (T initially contains all the transformations coalition C has)5.
www.cs.ox.ac.uk/people/michael.wooldridge/pubs/mfcs2010.pdf- 198k - 2 Nov 2010 - Cached
DC. 1 i! T 2 Jt (kL). Result for resistivity agrees with memory matrix prediction. ... 1 A. x. µfi!r. h. 0. DC(r). DC =Q2r2h. M2(rh). Universal Conductivity.
www-thphys.physics.ox.ac.uk/people/AndreiStarinets/oxford_holography_group/holography_seminar/Seminar/Slides/blake.pdf- 3063k - 13 Nov 2014 - Cached
with A as indicated above, and consider the SDE. 2:r “ Lr ζ. ... t P r0, T s and measurable withrespect to t for every r P.
people.maths.ox.ac.uk/suli/oseenfp_BC.pdf- 835k - 17 Feb 2018 - Cached
most |DC| |R|2 time. ... As before, a basic step requirestime of |DC| |R|2 time, and we perform at most |R| basic steps, so the algorithmrequires polynomial time.
www.cs.ox.ac.uk/people/michael.wooldridge/pubs/amai2013.pdf- 550k - 18 Apr 2013 - Cached
For r-partite k-systems we introduce the following alternative notion of degree. ... r]k. ), that is, each index set is. represented by equally many edges.
people.maths.ox.ac.uk/keevash/papers/geom-match-journal.pdf- 1179k - 19 May 2014 - Cached
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