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cond-mat

arxiv:cond-mat/ v2 [cond-mat.other] 3 Nov 2004

arxiv:cond-mat/ v2 [cond-mat.other] 3 Nov 2004

... On the email network we find that small world search strategies using a contact’s position in physical space or in an organizational hierarchy relative to the target can effectively be u[r] ...

20

arxiv: v2 [cond-mat.soft] 21 Dec 2020

arxiv: v2 [cond-mat.soft] 21 Dec 2020

... Conclusion – We studied the mid and large-scale spa- tial correlations in HS packings at Jamming by defining the correlation functions (3) and (2) for the weak forces f and the variation[r] ...

7

arxiv: v2 [cond-mat.stat-mech] 21 Aug 2019

arxiv: v2 [cond-mat.stat-mech] 21 Aug 2019

... Later, Microcanonical Szil´ ard Engines were proposed [30, 31, 32], versions of the Szil´ ard Engine where it is possible to extract energy from a single heat reservoir in a cycle by usi[r] ...

22

arxiv: v2 [cond-mat.mes-hall] 9 Mar 2013

arxiv: v2 [cond-mat.mes-hall] 9 Mar 2013

... Remarkably, we also find that the lowest NDR operation window (the bias range between the current peak and valley) is nearly free to the structural parameters and is always locked around[r] ...

5

arxiv: v1 [cond-mat.mes-hall] 22 Jan 2009

arxiv: v1 [cond-mat.mes-hall] 22 Jan 2009

... We simulated transport in metallic graphene nanoribbons with a rotated gate potential using a non-equilibrium Green function method. 1.) To compare the conductance properties of chiral f[r] ...

9

arxiv: v1 [cond-mat.mes-hall] 5 Jan 2021

arxiv: v1 [cond-mat.mes-hall] 5 Jan 2021

... ‘l.c.’ stands for label of classification (i.e. the values of the gauge invariants) of projective Reps of magnetic little co-groups G 0( k k k ), ‘disp.’ means the dispersion at the vici[r] ...

55

arxiv: v2 [cond-mat.str-el] 16 Feb 2017

arxiv: v2 [cond-mat.str-el] 16 Feb 2017

... 22,23, interesting quantum phases and related field-induced transitions in a strongly frustrated spin-dimer model are revealed. There exist two differ- ent solid orders with checkerboard[r] ...

6

arxiv: v1 [cond-mat.supr-con] 2 Dec 2020

arxiv: v1 [cond-mat.supr-con] 2 Dec 2020

... We have found that in the case of in-plane helical magnetiza- tion h ( y ), evolving along the interface, the calculations reveal nonmonotonic behavior of the critical temperature as a f[r] ...

9

arxiv: v2 [cond-mat.mes-hall] 4 Oct 2018

arxiv: v2 [cond-mat.mes-hall] 4 Oct 2018

... We predict that the tunneling probability in bulk be- comes drastically larger than that by the LZ formula and show that the lattice effect on the LZ problem cannot be neglected for the [r] ...

6

arxiv: v1 [cond-mat.stat-mech] 10 Oct 2016

arxiv: v1 [cond-mat.stat-mech] 10 Oct 2016

... We present computer simulations of three systems of randomly branching polymers in d = 3 dimensions: ideal trees and self-avoiding trees with annealed and quenched connectivities.. In al[r] ...

24

arxiv: v1 [cond-mat.mes-hall] 27 Nov 2020

arxiv: v1 [cond-mat.mes-hall] 27 Nov 2020

... In the double quantum dot we observed Pauli spin blockade, and analyzed the leakage current for both strong and weak interdot tunnel coupling to arrive at estimates for the typical magni[r] ...

10

arxiv: v1 [cond-mat.supr-con] 4 Dec 2020

arxiv: v1 [cond-mat.supr-con] 4 Dec 2020

... strong than in the cuprates [6], and embedded in a metallic environment. While magnetism in these infinite-layer nickelates is still under intense study [13–16], it is then important to [r] ...

7

arxiv:cond-mat/ v4 [cond-mat.soft] 21 Feb 2007

arxiv:cond-mat/ v4 [cond-mat.soft] 21 Feb 2007

... The average energy available for the recombina- tion process raises with temperature, consequently the recombination peak (roughly at the resonance position) moves toward smaller values [r] ...

10

arxiv: v1 [cond-mat.mes-hall] 26 Jul 2019

arxiv: v1 [cond-mat.mes-hall] 26 Jul 2019

... The breakdown of bulk boundary correspondence, as observed in our electric circuit array with a non-reciprocal non-Hermitian admittance profile, relates to a drastic admittance spectral [r] ...

36

arxiv:cond-mat/ v1 [cond-mat.dis-nn] 19 Dec 2002

arxiv:cond-mat/ v1 [cond-mat.dis-nn] 19 Dec 2002

... (14) In this way our transformation has introduced a finite clustering coefficient into the BC ensemble of graphs. In the next section we will apply this transformation to several well k[r] ...

14

arxiv:cond-mat/ v1 [cond-mat.mtrl-sci] 15 Jan 2003

arxiv:cond-mat/ v1 [cond-mat.mtrl-sci] 15 Jan 2003

... In the case of as prepared material the intensity does not change upon fur- ther heating, while a continuous evolution up to our max- imum temperature of 400 K is observed for the chemic[r] ...

5

arxiv:cond-mat/ v1 [cond-mat.stat-mech] 23 Jun 2006

arxiv:cond-mat/ v1 [cond-mat.stat-mech] 23 Jun 2006

... Numerically, an anomalous heat conduction - heat conductivity diverges with system size- has been observed in momentum conserved systems without on-site potential such as the Fermi-Pasta[r] ...

8

arxiv:cond-mat/ v1 [cond-mat.mes-hall] 28 Aug 2000

arxiv:cond-mat/ v1 [cond-mat.mes-hall] 28 Aug 2000

... The conformal mapping of the equation allows a modified but well defined Rayleigh-Schr¨odinger perturbation approach, where the cap height to in-plane radius is used to define the small [r] ...

18

arxiv:cond-mat/ v1 [cond-mat.stat-mech] 26 Oct 2006

arxiv:cond-mat/ v1 [cond-mat.stat-mech] 26 Oct 2006

... The dynamics of this, intrinsically discrete, system can be modelled by methods developed previously, namely, the stochastic Gillespie scheme [7], which allows one to obtain single bubbl[r] ...

7

arxiv:cond-mat/ v1 [cond-mat.stat-mech] 3 Apr 2004

arxiv:cond-mat/ v1 [cond-mat.stat-mech] 3 Apr 2004

... The outline of this work is as follows: After introducing the two fundamental models ( ℓ -ASEP and zero range process) and reviewing some facts about their stationary properties in secti[r] ...

20

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