# bib

id: pip-207
author: Bagnoli, Franco
title: Commentary on "Critical phenomena in the spreading of opinion consensus and disagreement"
date: 2014-08-29
pages: 1
extension: .pdf
mime: application/pdf
words: 506
sentence: 26
flesch: 69
cache: cache/pip-207.pdf
txt: txt/pip-207.txt
summary:
  ics of the model corresponds to that of annihilat- ing random walkers, like in the voter model, except that in this case there are two types of walkers that do not annihilate among themselves. The second point is about the correspondence with annihilating random walks.


id: pip-217
author: Wilson, T. J.; Pfeifer, C. R.; Meysingier, N.; Durian, D. J.
title: Reply to the Commentary on "Granular discharge rate for submerged hoppers"
date: 2014-10-28
pages: 2
extension: .pdf
mime: application/pdf
words: 756
sentence: 40
flesch: 67
cache: cache/pip-217.pdf
txt: txt/pip-217.txt
summary:
  A terminal surge has now been seen for dry grains in air [3], so the effect is of broader interest. The latter is for large grains, in which case the fluid drag scales as speed-squared and the inter- stitial fluid flow must be somewhat turbulent.


id: pip-12
author: Fort, Hugo
title: Commentary on "A note on the consensus time of mean-field majority-rule dynamics"
date: 2009-10-16
pages: 2
extension: .pdf
mime: application/pdf
words: 787
sentence: 45
flesch: 62
cache: cache/pip-12.pdf
txt: txt/pip-12.txt
summary:
  Mass media sig- nals, advertising and propaganda operating over the individuals play an important role in opinion formation and can have an important impact. Population dynamics.


id: pip-208
author: Chacoma, A.; Zanette, Damián H.
date: 2014-08-29
pages: 2
extension: .pdf
mime: application/pdf
words: 946
sentence: 49
flesch: 61
cache: cache/pip-208.pdf
txt: txt/pip-208.txt
title:
  Reply to the Commentary on "Critical phenomena in the spreading of opinion consensus and disagreement"

summary:
  http://dx.doi.org/10.4279/PIP.060005 www.papersinphysics.org ISSN 1852-4249 Reply to the Commentary on “Critical phenomena in the spreading of opinion consensus and disagreement” A. Chacoma,1 D. H. Zanette1, 2∗ 1. [1] F Bagnoli, Commentary on “Critical phenom- ena in the spreading of opinion consensus and disagreement”, Pap. Phys. 6, 060004 (2014).


id: pip-16
author: Zanette, Damián H.
title: Answer to the Commentary on "A note on the consensus time of mean-field majority-rule dynamics"
date: 2009-10-16
pages: 2
extension: .pdf
mime: application/pdf
words: 928
sentence: 47
flesch: 62
cache: cache/pip-16.pdf
txt: txt/pip-16.txt
summary:
  To my knowledge, population dynamics has not been addressed in the context of MR model. Either random or deterministic time-dependent effects, such as stochastic fluctuations in the rules that govern single consensus events or population dynamics, are certainly worth considering.


id: pip-216
author: Staron, Lydie
title: Commentary on "Granular discharge rate for submerged hoppers"
date: 2014-10-28
pages: 3
extension: .pdf
mime: application/pdf
words: 1325
sentence: 69
flesch: 64
cache: cache/pip-216.pdf
txt: txt/pip-216.txt
summary:
  Many interesting open ques- tions remain, and certainly the work in progress by the same team will bring original new material to understand what happens during the discharge of granular flows - be it dry or immersed. In other words, taller columns would still coincide with the discharge of dense granular flow, while shorter columns may imply the discharge of a dense suspension.


id: pip-163
author: Forgan, E. M.
title: Commentary on "Graphite and its hidden superconductivity"
date: 2013-12-09
pages: 3
extension: .pdf
mime: application/pdf
words: 1749
sentence: 87
flesch: 55
cache: cache/pip-163.pdf
txt: txt/pip-163.txt
summary:
  [7] T Scheike, W Bhlmann, P Esquinazi, J Barzola-Quiquia, A Ballestar, A Setzer, Can doping graphite trigger room temperature su- perconductivity? Unless and until graphite samples can be produced which exhibit the Meissner effect for a volume fraction of at least 1%, and which show direct evidence of quantum coherence (hysteresis which might arise from Josephson networks or from other causes is not direct evidence), I expect that the scientific community at large will not accept that graphite exhibits high-temperature supercon- ductivity.


id: pip-222
author: Ferrari, Fabiano A. S.; Viana, Ricardo L.
title: Two distinct desynchronization processes caused by lesions in globally coupled neurons
date: 2015-03-25
pages: 5
extension: .pdf
mime: application/pdf
words: 2472
sentence: 138
flesch: 65
cache: cache/pip-222.pdf
txt: txt/pip-222.txt
summary:
  [9] P Moretti, M A Muñoz, Griffiths phases and the stretching of criticality in brain networks, Nat. Panel (a) shows a fully connected network, panels (b) and (c) show the effect of lesions type 1 and type 2, respectively.


id: pip-169
author: Bonzi, Edgardo; Grad, Gabriela; Maggi, Alicia; Muñoz, Marta
title: Study of the characteristic parameters of the normal voices of Argentinian speakers
date: 2014-07-12
pages: 5
extension: .pdf
mime: application/pdf
words: 2566
sentence: 158
flesch: 68
cache: cache/pip-169.pdf
txt: txt/pip-169.txt
summary:
  Normal voices have a low level of noise and high HNR. [2] T Cervera, J L Miralles, J González-Álvarez, Acoustical analysis of Spanish vowels produced by laryngectomized subjects, J. Speech Lang.


id: pip-19
author: Mariotti, Alejandro David; Brandaleze, Elena; Buscaglia, Gustavo C.
date: 2010-01-08
pages: 7
extension: .pdf
mime: application/pdf
words: 3275
sentence: 169
flesch: 64
cache: cache/pip-19.pdf
txt: txt/pip-19.txt
title:
  Parametric study of the interface behavior between two immiscible liquids flowing through a porous medium

summary:
  [8] Y Efendiev, T Houb, Multiscale finite element methods for porous media flows and their ap- plications, Appl. (2009) / A. D. Mariotti et al. Figure 5: Stationary interface profiles modifying the fluid 1 viscosity without the gravity effect.


id: pip-215
author: Arévalo, Roberto
title: Commentary on "Jamming transition in a two-dimensional open granular pile with rolling resistance"
date: 2014-10-27
pages: 5
extension: .pdf
mime: application/pdf
words: 3636
sentence: 205
flesch: 71
cache: cache/pip-215.pdf
txt: txt/pip-215.txt
summary:
  It was found that the data on avalanche size could be fit with the same expression than in the 3D case, with val- ues Regarding the 3D silo, the conclusion that there exists a criti- cal outlet size is based on the good fit of the data on avalanche size by Eq.


id: pip-166
author: Bonzi, Edgardo; Grad, Gabriela; Barrea, Raúl
date: 2014-02-13
pages: 6
extension: .pdf
mime: application/pdf
words: 3431
sentence: 179
flesch: 69
cache: cache/pip-166.pdf
txt: txt/pip-166.txt
title:
  Experimental determination of L X-ray fluorescence cross sections for elements with 45 < Z < 50 at 10 keV

summary:
  The L X-ray cross sections were measured with monoenergetic excitation beam at 10 keV. We report cross sections for each spectral line, according to the resolution of the Si(Li) solid state detector used to resolve individual component lines of the spectral emission. This work Puri Krause Figure 2: Comparison of Lα cross sections.


id: pip-219
author: Mort, Paul
title: Characterizing flowability of granular materials by onset of jamming in orifice flows
date: 2015-04-21
pages: 8
extension: .pdf
mime: application/pdf
words: 3754
sentence: 175
flesch: 56
cache: cache/pip-219.pdf
txt: txt/pip-219.txt
summary:
  The range of orifice sizes used with the Flodex included: 2.0, 2.5, 3.0, 3.5, 4, 5, 6, 7, 8, 9, 10, 12, 14, 16, 18 and 20 mm. In other words, the granular flow behavior is consistent for orifice sizes above the jamming onset, but subtle differences in the gran- ular characteristics and frictional properties have a significant effect on the onset of jamming.


id: pip-10
author: Campo, M. G.
title: Structural and dynamic properties of SPC/E water
date: 2010-02-18
pages: 7
extension: .pdf
mime: application/pdf
words: 3603
sentence: 187
flesch: 60
cache: cache/pip-10.pdf
txt: txt/pip-10.txt
summary:
  [28] M G Campo, G L Ferri, G B Roston, q- exponential distribution in time correlation function of water hydrogen bonds, Braz. The thermodynamic behavior of water presents important differences compared with those of the other substances, and many of the characteristics of such behavior are often attributed to the existence of hydrogen bonds between water molecules.


id: pip-186
author: Banerjee, Rahul; Kanjilal, S.
title: Influence of surface tension on two fluids shearing instability
date: 2014-11-25
pages: 8
extension: .pdf
mime: application/pdf
words: 4255
sentence: 216
flesch: 72
cache: cache/pip-186.pdf
txt: txt/pip-186.txt
summary:
  http://dx.doi.org/10.4279/PIP.060006 www.papersinphysics.org ISSN 1852-4249 Influence of surface tension on two fluids shearing instability Rahul Banerjee,1∗ S. Kanjilal1 Using extended Layzer’s potential flow model, we investigate the effects of surface tension on the growth of the bubble and spike in combined Rayleigh-Taylor and Kelvin-Helmholtz instability.


id: pip-135
author: Assaneo, María Florencia; Trevisan, Marcos A.
title: Revisiting the two-mass model of the vocal folds
date: 2013-06-25
pages: 7
extension: .pdf
mime: application/pdf
words: 3937
sentence: 220
flesch: 65
cache: cache/pip-135.pdf
txt: txt/pip-135.txt
summary:
  In particular, the action of the thyroarytenoid and the cricothyroid muscles control the thickness and the stiffness of folds. The blue and green lines represent folds of cycles (saddle-node bifurcations in the map).


id: pip-214
author: Parisi, Daniel R.; Negri, Pablo A
title: Sequential evacuation strategy for multiple rooms toward the same means of egress
date: 2014-12-02
pages: 8
extension: .pdf
mime: application/pdf
words: 4813
sentence: 234
flesch: 65
cache: cache/pip-214.pdf
txt: txt/pip-214.txt
summary:
  From these data, it is possible to calcu- late several outputs; in the present work we focused on evacuation times. [4] D R Parisi, C Dorso, Microscopic dynamics of pedestrian evacuation, Physica A 354, 608 (2005).


id: pip-127
title: Enhancement of photoacoustic detection of inhomogeneities in polymers
date: 2013-07-05
pages: 8
extension: .pdf
mime: application/pdf
words: 4943
sentence: 226
flesch: 66
cache: cache/pip-127.pdf
txt: txt/pip-127.txt
author:
  Grondona, P.; Di Rocco, H. O.; Iriarte, D. I.; Pomarico, J. A.; Ranea-Sandoval, Héctor F.; Bilmes, G. M.

summary:
  The �duciary pattern engraved on one of the faces of some samples consists of �ve grooves of approximately 1 mm width and 0.2 mm deep, �lled with thick black paint, separated by stripes of material which retain the natural turbid white color of the polymer (which we call �clear� for short) of 1 mm, whose lengths are approximately 70% the length of the face. Circles are for cavity �lled with water in clear samples.


id: pip-212
author: Wilson, T. J.; Pfeifer, C. R.; Mesyngier, N.; Durian, D. J.
title: Granular discharge rate for submerged hoppers
date: 2014-10-28
pages: 7
extension: .pdf
mime: application/pdf
words: 4899
sentence: 261
flesch: 72
cache: cache/pip-212.pdf
txt: txt/pip-212.txt
summary:
  Grain discharge rate data are plotted in Fig. 1(d), on top of prior data for an open-topped hopper with no liquid pumping. Recently, we have found excellent agreement with the Beverloo equation for up to three [11] and four [12] decades in discharge rate for spherical grains.


id: pip-164
author: Esquinazi, P.
title: Reply to the Commentary on "Graphite and its hidden superconductivity"
date: 2013-12-09
pages: 7
extension: .pdf
mime: application/pdf
words: 4985
sentence: 235
flesch: 55
cache: cache/pip-164.pdf
txt: txt/pip-164.txt
summary:
  Reply: A possible answer to this comment might be that the superconductivity at graphite interfaces has not only a ten times larger critical tempera- ture but also ten times larger activation energies as in cuprate materials. Whether this is applicable in the case of supercon- ductivity at graphite interfaces has to be seen.


id: pip-200
author: Magalhães, Caio F. M.; Atman, Allbens P.F.; Combe, Gaël; Moreira, José G.
title: Jamming transition in a two-dimensional open granular pile with rolling resistance
date: 2014-10-27
pages: 9
extension: .pdf
mime: application/pdf
words: 5443
sentence: 302
flesch: 64
cache: cache/pip-200.pdf
txt: txt/pip-200.txt
summary:
  [20], the authors have revealed evidence of self-organized criticality (SOC) by measuring the internal avalanches resulting from the opening of an orifice at the bottom of granular piles. Recently, a simulation study on discharges of granular piles with open bound- aries


id: pip-21
author: Kunik, D.; Pietrasanta, L. I.; Martínez, O. E.
date: 2010-01-11
pages: 10
extension: .pdf
mime: application/pdf
words: 5625
sentence: 293
flesch: 64
cache: cache/pip-21.pdf
txt: txt/pip-21.txt
title:
  Surface Percolation and Growth. An alternative scheme for breaking the diffraction limit in optical patterning

summary:
  When the volume dye concentration is very large (1 mM and Figure 4: Height of the lines as a function of the exposition time for samples with dye concentration of 50 µM (squares) and 100 µM (circles). (2009) / D. Kunik et al. Figure 7: Fit of the data for the sample made at 100 µM dye concentration.


id: pip-185
author: Chacoma, Andrés; Zanette, Damián H.
title: Critical phenomena in the spreading of opinion consensus and disagreement
date: 2014-08-29
pages: 9
extension: .pdf
mime: application/pdf
words: 5393
sentence: 262
flesch: 62
cache: cache/pip-185.pdf
txt: txt/pip-185.txt
summary:
  The upper panel of Fig. 2 shows numerical results for the probability of final full consensus Pcons, de- termined as the fraction of realizations that ended in full consensus out of 103 runs, as a function of n+(0) and for several population sizes N. The curve is the analytic prediction given above. In summary, while spreading of consensus and disagreement on a two-dimensional lattice bears superficial qualitative similarity with the one- dimensional case, the probability that the popula- tion reaches full collective consensus in two dimen- −2 0 2 4 6 0.0 0.2 0.4 0.6 0.8 1.0 L = 90 L = 120 L = 150 L = 180 L = 210 P c o n s L 0.93 (0.984 − p D ) 10 100 0.01 0.1 w id th L Figure 9: Collapse of numerical results for the prob- ability of reaching full consensus, Pcons, on a two- dimensional lattice with pC = 1 and n+(0)


id: pip-20
author: Kadanoff, Leo P.
title: Expansions for eigenfunction and eigenvalues of large-$n$ Toeplitz matrices
date: 2010-10-19
pages: 9
extension: .pdf
mime: application/pdf
words: 6136
sentence: 369
flesch: 75
cache: cache/pip-20.pdf
txt: txt/pip-20.txt
summary:
  One conventional way of �nding eigenvalues is through the use of an extremal principle. and it obeys ∞∑ k=−∞ Kj,kψ 0 k = φ − j + φ + j, (6) which holds for all integer values of j. Here, the matrix K is Kj,k = Tj−k − �δj,k (7) Eq.


id: pip-22
author: Arabshahi, H.; Binesh, A.
title: Light effect in photoionization of traps in GaN MESFETs
date: 2009-12-17
pages: 5
extension: .pdf
mime: application/pdf
words: 2698
sentence: 131
flesch: 61
cache: cache/pip-22.pdf
txt: txt/pip-22.txt
summary:
  Trapping of hot electron behavior by trap centers located in buffer layer of a wurtzite phase GaN MESFET has been simulated using an ensemble Monte Carlo simulation. 2 Department of Physics, Payam-e-Nour University, Fari- man, Iran. layers and have a significant effect on GaN devices.


id: pip-227
author: Ré, Miguel A.; Bustos, Natalia C.
title: Reaction rate in an evanescent random walkers system
date: 2015-04-07
pages: 6
extension: .pdf
mime: application/pdf
words: 3043
sentence: 196
flesch: 68
cache: cache/pip-227.pdf
txt: txt/pip-227.txt
summary:
  Other mag- nitudes, such as time dependent reaction rates or survival probabilities of the reactives, can be de- rived from the APD. If we assume an initially uniform concentration in the ECTRW, c0, the concentration at time t is c (t) = c0e −ηt, (10) i.e., it remains uniform but decays exponentially.


id: pip-206
author: Lengyel, Iván M.; Soroldoni, Daniele; Oates, Andrew C.; Morelli, Luis G.
date: 2014-12-02
pages: 11
extension: .pdf
mime: application/pdf
words: 6513
sentence: 392
flesch: 66
cache: cache/pip-206.pdf
txt: txt/pip-206.txt
title:
  Nonlinearity arising from noncooperative transcription factor binding enhances negative feedback and promotes genetic oscillations

summary:
  A B 1 2 3 4 N 1 2 3 4 N k � k ✁ Figure 2: Schematic representation of a promoter with multiple binding sites, numbered from 1 to N. Transcriptional repressors (orange squares) bind and unbind from binding sites (numbered platforms) at the promoter of a gene (light blue stretch). One way to increase nonlinearity would be cooperative binding of repressors to regulatory binding sites at the pro- moter


id: pip-223
author: Cascallares, G.; Gleiser, Pablo
title: What season suits you best? Seasonal light changes and cyanobacterial competition
date: 2015-04-17
pages: 6
extension: .pdf
mime: application/pdf
words: 3127
sentence: 173
flesch: 64
cache: cache/pip-223.pdf
txt: txt/pip-223.txt
summary:
  Even near the equator, where day length changes are very small through the whole year, they are used to synchronize reproductive activities with an- nual events. [10]. Using this as a motivation, we will test how day length variation plays a role in the competition be- tween different strains of cyanobacteria. II.


id: pip-112
author: Porasso, Rodolfo D.; López Cascales, José J.
title: A criterion to identify the equilibration time in lipid bilayer simulations
date: 2012-11-10
pages: 10
extension: .pdf
mime: application/pdf
words: 6222
sentence: 302
flesch: 64
cache: cache/pip-112.pdf
txt: txt/pip-112.txt
summary:
  A criterion to identify the equilibration time in lipid bilayer simulations Rodolfo D. Porasso,1∗ J.J. López Cascales,2 With the aim of establishing a criterion for identifying when a lipid bilayer has reached steady state using the molecular dynamics simulation technique, lipid bilayers of different composition in their liquid crystalline phase were simulated in aqueous solution in pres- ence of CaCl2 as electrolyte, at different concentration levels. In this sense, for both type of lipid bilayers, we have studied the temporal evolution of some lipids properties, such as the surface area per lipid, the deuterium order parameter, the lipid hydration and the lipid-calcium coordination.


id: pip-263
author: Perfetti, Mauro
date: 2015-07-07
pages: 2
extension: .pdf
mime: application/pdf
words: 923
sentence: 38
flesch: 53
cache: cache/pip-263.pdf
txt: txt/pip-263.txt
title:
  Commentary on "An intermediate state between the kagome-ice and the fully polarized state in Dy$_2$Ti$_2$O$_7$"

summary:
  [2] J P C Ruff, R G Melko, M J P Gingras, Finite- temperature transitions in dipolar spin ice in a large magnetic field, Phys. O7 spin ice: A test case for emergent clusters in a frustrated magnet, Phys.


id: pip-228
author: Rosso, Osvaldo Anibal; Olivares, Felipe; Plastino, Angelo
title: Noise versus chaos in a causal Fisher-Shannon plane
date: 2015-04-14
pages: 6
extension: .pdf
mime: application/pdf
words: 3373
sentence: 183
flesch: 62
cache: cache/pip-228.pdf
txt: txt/pip-228.txt
summary:
  A second group of chaotic maps, constituted by: the Gauss map (7), linear congruential generator (4), dissipative stan- dard map (18), Sinai map (20) and Arnold’s cat map, is localized near the right-lower corner of the H×F plane, that is in the range 0.95 ≤ H ≤ 1.0 and 0 These chaotic maps are grouped as a) Noninvertible maps: (1) Logistic map; (2) Sine map; (3) Tent map; (4) Linear congruential generator; (5) Cubic map; (6) Ricker’s popu- lation model; (7) Gauss map; (8) Cusp map; (9) Pinchers map; (10) Spence map; (11) Sine- circle map; b) Dissipative maps: (12) Hénon map; (13) Lozi map; (14) Delayed logistic map; (15) Tinker- bell map; (16) Burgers’ map; (17) Holmes cubic map; (18) Dissipative standard map; (19) Ikeda map; (20) Sinai map; (21) Discrete predator-prey map, c) Conservative maps: (22) Chirikov standard map; (23) Hénon area-preserving quadratic map; (24) Arnold’s cat map; (25) Gingerbread- man map; (26) Chaotic web map; (27) Lorenz three-dimensional chaotic map; Even when the present list of chaotic maps is not exhaustive, it could be taken as representative of common chaotic systems


id: pip-147
author: Zylberberg, Ariel D; Paz, Luciano; Roelfsema, Pieter R; Dehaene, Stanislas; Sigman, Mariano
title: A neuronal device for the control of multi-step computations
date: 2013-08-13
pages: 14
extension: .pdf
mime: application/pdf
words: 8318
sentence: 429
flesch: 58
cache: cache/pip-147.pdf
txt: txt/pip-147.txt
summary:
  As we show later, this can be accomplished by the se- quential firing of production neurons. The successive steps of the counting routine are gov- erned by firing of production neurons.


id: pip-23
author: Zarragoicoechea, G. J.; Meyra, A. G.; Kuz, V. A.
title: Multilayer approximation for a confined fluid in a slit pore
date: 2010-03-16
pages: 6
extension: .pdf
mime: application/pdf
words: 3000
sentence: 155
flesch: 68
cache: cache/pip-23.pdf
txt: txt/pip-23.txt
summary:
  From these equations, giving as input the wall separation L and the mean density ρ∗ = ρσ3, it is constructed a system of (n − 1) non-linear equa- tions with (n − 1) unknowns (layer densities and widths) to be numerically solved. Figure 1: Density profiles for a n=9 layer model of a confined fluid in a slit pore (solid symbols).


id: pip-128
author: Romano, Sergio; Sigman, Mariano; Figueira, Santiago
title: $LT^2C^2$ : A language of thought with Turing-computable Kolmogorov complexity
date: 2013-03-01
pages: 14
extension: .pdf
mime: application/pdf
words: 8654
sentence: 459
flesch: 64
cache: cache/pip-128.pdf
txt: txt/pip-128.txt
summary:
  This work extends on previous efforts to combine notions of Kolmogorov complexity theory and algorithmic information theory to psychology, by explicitly proposing a language which may describe the patterns of human thoughts. Mathematical theory of random- ness The idea behind Kolmogorov complexity theory is to study the length of the descriptions that a formal language can produce to identify a given string.


id: pip-229
author: Zangara, Pablo R.; Levstein, P. R.; Pastawski, H. M.
date: 2015-07-14
pages: 9
extension: .pdf
mime: application/pdf
words: 5728
sentence: 341
flesch: 62
cache: cache/pip-229.pdf
txt: txt/pip-229.txt
title:
  Role of energy uncertainties in ergodicity breaking induced by competing interactions and disorder. A dynamical assessment through the Loschmidt echo

summary:
  Since the sensitivity to initial conditions does not apply to quantum systems, the quantum signature of dynamical chaos had to be found as an instability of an evolution towards per- turbations in the Hamiltonian [11]. Last, but not least, in state-of-the- art NMR [51, 52], the high temperature correla- tion functions, like the LE, are privileged witnesses for the onset of phase transitions [53] that could hint the appearance of Many-Body Localization [45, 51, 54].


id: pip-258
title: An intermediate state between the kagome-ice and the fully polarized state in Dy$_2$Ti$_2$O$_7$
date: 2015-06-25
pages: 7
extension: .pdf
mime: application/pdf
words: 4171
sentence: 215
flesch: 63
cache: cache/pip-258.pdf
txt: txt/pip-258.txt
author:
  Grigera, S. A.; Borzi, R.; Slobinsky, D. G.; Gibbs, A. S.; Higashinaka, R.; Maeno, Y.; Grigera, T. S.

summary:
  S. A. Grigera et al. Figure 1: Real (left) and Imaginary (right) parts of the ac-susceptibility as a function of temperature and magnetic field, for temperatures between 50 mK and 6000 mK and magnetic fields between -4 and 4 T. Results and Discussion Figure 1 shows the real (∆χ′, left) and imaginary (∆χ′′, right) parts of the ac-susceptibility χ as a function of temperature and magnetic field in the whole area of interest.


id: pip-138
author: Kuperman, Marcelo N.
title: Invited review: Epidemics on social networks
date: 2013-06-26
pages: 17
extension: .pdf
mime: application/pdf
words: 10823
sentence: 619
flesch: 60
cache: cache/pip-138.pdf
txt: txt/pip-138.txt
summary:
  [56,57], the authors analyze the structure of di�erent networks of sexual encounters, to �nd that it has a pattern of contact closely related to a power law. [15] F G Ball, P Donnelly, Strong approximations for epidemic models, Stoch.


id: pip-39
author: Ehrhardt, Torsten
title: Commentary on "Expansions for Eigenfunctions and Eigenvalues of large-$n$ Toeplitz Matrices"
date: 2010-10-19
pages: 2
extension: .pdf
mime: application/pdf
words: 1108
sentence: 66
flesch: 64
cache: cache/pip-39.pdf
txt: txt/pip-39.txt
summary:
  [1] is concerned with the problem of describing the asymptotics of the eigenvalues and eigenvectors of Toeplitz matrices, Tn(φ) = (φj−k) n−1 j,k=0, as the matrix size n goes to infinity. The problem of the asymptotics of the eigenval- ues of Toeplitz matrices has a long history and is a multi-faceted and difficult topic.


id: pip-280
author: Sevilla, Diego
title: Bayesian regression of piecewise homogeneous Poisson processes
date: 2015-12-18
pages: 6
extension: .pdf
mime: application/pdf
words: 2665
sentence: 147
flesch: 65
cache: cache/pip-280.pdf
txt: txt/pip-280.txt
summary:
  (2) For a Poisson process with rate r, the likelihood of a segment Dij is P(Dij|r) = j∏ t=i+1 rnt e−r nt! . It can be used to analyze data of several physical processes which follow the Poisson distribution (e.g., detec- tion of photons in X-ray Astronomy, particles in nuclear disintegration, etc.), if sudden changes in detection rates are suspected. II.


id: pip-148
author: Wio, Horacio S.; Deza, Roberto R.; Escudero, Carlos; Revelli, Jorge A.
title: Invited review: KPZ. Recent developments via a variational formulation
date: 2014-01-13
pages: 16
extension: .pdf
mime: application/pdf
words: 9439
sentence: 542
flesch: 67
cache: cache/pip-148.pdf
txt: txt/pip-148.txt
summary:
  Equation (1) is stated in the sense of Itô. The {ξi(t)}, i = 1, . . . Equation (3) and the normalization condition en- sure that Φ is bounded from below.


id: pip-239
author: Slobinsky, Demian; Pugnaloni, Luis Ariel
date: 2015-03-09
pages: 9
extension: .pdf
mime: application/pdf
words: 5965
sentence: 294
flesch: 61
cache: cache/pip-239.pdf
txt: txt/pip-239.txt
title:
  Wang-Landau algorithm for entropic sampling of arch-based microstates in the volume ensemble of static granular packings

summary:
  Since arches are sets of grains that stabilize each other, these are the basic units of mechanically stable struc- tures in the packing. We have considered, as an example, a model of a two-dimensional (2D) granular system composed of disks where arches are assumed to take a single pos- sible structure and the arch–arch interactions (due to the interlocking of arches) is neglected.


id: pip-130
author: Esquinazi, Pablo
title: Invited review: Graphite and its hidden superconductivity
date: 2013-12-09
pages: 19
extension: .pdf
mime: application/pdf
words: 12079
sentence: 609
flesch: 59
cache: cache/pip-130.pdf
txt: txt/pip-130.txt
summary:
  We review experimental results, from transport to magnetization measurements, on dif- ferent graphite samples, from bulk oriented graphite, thin graphite films to transmission electron microscope lamellae, that indicate the existence of granular superconductivity at temperatures above 100 K. The accumulated evidence speaks for a localization of the superconducting phase(s) at certain interfaces embedded in semiconducting crystalline regions with Bernal stacking order. The impact of well defined two-dimensional in- terfaces inside graphite samples [7, 8] had not been realized until recent studies of the transport proper- ties as a function of thickness of the graphite sample provided a link to the microstructure of the sam- ples obtained by transmission electron microscope (TEM) studies.


id: pip-429
author: Zhang, Yisi S
title: Commentary on "Modeling temperature manipulation in a circular model of birdsong production"
date: 2018-01-19
pages: 2
extension: .pdf
mime: application/pdf
words: 938
sentence: 52
flesch: 56
cache: cache/pip-429.pdf
txt: txt/pip-429.txt
summary:
  Why would the model undergo a qualitative change between different syllable types? On the other hand, it proposes alternative generators of song timing.


id: pip-231
author: Zuriguel, Iker
title: Invited review: Clogging of granular materials in bottlenecks
date: 2014-12-15
pages: 13
extension: .pdf
mime: application/pdf
words: 7871
sentence: 416
flesch: 64
cache: cache/pip-231.pdf
txt: txt/pip-231.txt
summary:
  The goal in all these works was finding a ratio of the outlet to particle size that could guaran- tee the absence of clogging. While for horizontal and vertical slots the ratio of slot width to parti- cles size are 3.3 and 4.6 respectively, for horizon- tal circular outlets the ratio of orifice diameter to particle size is 6.4.


id: pip-279
author: Gago, Paula A.; Maza, Diego; Pugnaloni, Luis A.
title: Ergodic-nonergodic transition in tapped granular systems: The role of persistent contacts
date: 2016-01-12
pages: 7
extension: .pdf
mime: application/pdf
words: 4118
sentence: 201
flesch: 65
cache: cache/pip-279.pdf
txt: txt/pip-279.txt
summary:
  We show that the tap intensity beyond which sampling by tapping becomes ergodic coincides with the forcing necessary to break all particle–particle contacts during each tap. Licence: Creative Commons Attribution 3.0 DOI: http://dx.doi.org/10.4279/PIP.080001 www.papersinphysics.org ISSN 1852-4249 Ergodic–nonergodic transition in tapped granular systems:


id: pip-428
author: Forinash, Kyle; Wisman, Raymond
title: Smartphone audio port data collection cookbook
date: 2018-06-06
pages: 4
extension: .pdf
mime: application/pdf
words: 1850
sentence: 91
flesch: 60
cache: cache/pip-428.pdf
txt: txt/pip-428.txt
summary:
  K. Forinash et al. range of peak amplitudes produced by the cir- cuit of Fig. 1 and the corresponding temper- atures, an equation fitted to that amplitude vs. temperature data can convert the circuit amplitude output to temperature. II. put to the microphone input; the speaker output is a wave which peak amplitude at the microphone input varies with the variable resistor, greater re- sistance resulting in lower peak amplitude.


id: pip-410
author: Llamas Bello, César; Vegas, Jesús; González Rebollo, Miguel Ángel; González Delgado, Manuel Ángel
title: Open-source sensors system for doing simple physics experiments
date: 2018-04-07
pages: 4
extension: .pdf
mime: application/pdf
words: 2256
sentence: 104
flesch: 54
cache: cache/pip-410.pdf
txt: txt/pip-410.txt
summary:
  Un- like commercial sensor systems, this one constitutes an extensible and customizable platform that can be modified by adding other sensors and includ- ing other software characteristics. We initially decided to include sensors in the platform that measure kinematic magnitudes: ac- celerometer, gyroscope, distance sensor and light- gate sensors.


id: pip-28
author: Grecco, H. E.; Martínez, O. E.
date: 2011-01-05
pages: 9
extension: .pdf
mime: application/pdf
words: 5024
sentence: 256
flesch: 57
cache: cache/pip-28.pdf
txt: txt/pip-28.txt
title:
  Experimental determination of distance and orientation of metallic nanodimers by polarization dependent plasmon coupling

summary:
  Additionally, it is important to mention that various factors such as a non-monodisperse or non-spherical population of particles will have an incidence in the recovery of dimer distance, size and orientation from model based fittings. A negative control sam- ple was prepared in the same way but omitting the incubation of gold nanoparticles.


id: pip-367
author: Wolk, Brian Jonathan
date: 2017-01-14
pages: 6
extension: .pdf
mime: application/pdf
words: 3228
sentence: 181
flesch: 69
cache: cache/pip-367.pdf
txt: txt/pip-367.txt
title:
  An alternative derivation of the Dirac operator generating intrinsic Lagrangian local gauge invariance

summary:
  In standard vector analysis, vector �eld operators operate on scalar �elds [15]. Introduction of a vector �eld Aµ that couples to the Dirac �eld ψ must then be introduced in order to satisfy the imposed local symmetry constraint


id: pip-234
author: Uñac, Rodolfo O.; Sales, José L.; Gargiulo, María V.; Vidales, Ana M.
title: Density distribution of particles upon jamming after an avalanche in a 2D silo
date: 2015-04-29
pages: 11
extension: .pdf
mime: application/pdf
words: 6677
sentence: 340
flesch: 68
cache: cache/pip-234.pdf
txt: txt/pip-234.txt
summary:
  The decrease of the density at small distances from the center, especially for A = 1.1 and 2.0, is a purely 0 20 40 60 80 100 0.0 0.1 0.2 0.3 0.4 0.5 0.1 0.2 0.3 0.4 0.5 (b) R D is ks d en si ty (a) Figure 3: Particle density vs. the distance of the ring to the center, using the cell depicted in Fig. 2(a). et al. 0 20 40 60 80 100 120 140 160 180 0.2 0.3 0.4 0.5 0.6 0.3 0.4 0.5 0.6 (b) (º) D is ks d en si ty (a) Figure 4: Particle density vs. the inclination an- gle of the sector respect to the horizontal, for three values of A. (a) Initial packing behavior.


id: pip-37
author: Zanette, Damián H.
title: SIR epidemics in monogamous populations with recombination
date: 2011-03-25
pages: 7
extension: .pdf
mime: application/pdf
words: 3785
sentence: 200
flesch: 58
cache: cache/pip-37.pdf
txt: txt/pip-37.txt
summary:
  This process of couple recombination can compensate the instantaneous disconnection of the interaction pattern and thus allow for the propagation of the infection. Monogamous populations with couple recombination Suppose now that, at any given time, each agent in the population has exactly just one neighbor or, 030001-2 Papers in Physics, vol.


id: pip-388
author: Núñez Fernández, Yuriel; Hallberg, Karen
title: An efficient impurity-solver for the dynamical mean field theory algorithm
date: 2017-08-01
pages: 7
extension: .pdf
mime: application/pdf
words: 3283
sentence: 202
flesch: 66
cache: cache/pip-388.pdf
txt: txt/pip-388.txt
summary:
  [25] D J Garćıa, K Hallberg, M J Rozenberg, Dy- namical mean field theory with the density ma- trix renormalization group, Phys. Rev. Lett. 93, 246403 (2004). [13] A Georges, G Kotliar, Hubbard model in in- finite dimensions, Phys.


id: pip-416
author: González Delgado, Manuel Ángel; Gómez, Alfonso; González Rebollo, Miguel Ángel
title: Smartphones on the air track. Examples and difficulties
date: 2018-06-06
pages: 4
extension: .pdf
mime: application/pdf
words: 2678
sentence: 114
flesch: 55
cache: cache/pip-416.pdf
txt: txt/pip-416.txt
summary:
  i. Elastic collisions between carts in a hor- izontal air track This is a simple experiment that is done by using two carts, each with a smartphone measuring its acceleration, allowing us to check the momentum conservation in a collision between two bodies. Figure 1 shows the results of one of such ex- periments corresponding to an elastic collision be- tween two bodies (cart plus smartphone) of similar masses.


id: pip-341
author: Dey, Dayasindhu; Maiti, Debasmita; Kumar, Manoranjan
date: 2016-11-18
pages: 7
extension: .pdf
mime: application/pdf
words: 4510
sentence: 267
flesch: 69
cache: cache/pip-341.pdf
txt: txt/pip-341.txt
title:
  An efficient density matrix renormalization group algorithm for chains with periodic boundary condition

summary:
  [21] S Östlund, S Rommer, Thermodynamic limit of density matrix renormalization, Phys. Rev. Lett. [27] D Rossini, V Giovannetti, R Fazio, Spin- supersolid phase in Heisenberg chains: A char- acterization via matrix product states with pe- riodic boundary conditions, Phys.


id: pip-415
author: Allerdt, Andrew; Feiguin, Adrian E.
title: Dilute antiferromagnetism in magnetically doped phosphorene
date: 2017-12-31
pages: 6
extension: .pdf
mime: application/pdf
words: 2994
sentence: 199
flesch: 64
cache: cache/pip-415.pdf
txt: txt/pip-415.txt
summary:
  The case of magnetic impurities is considerably 090008-1 PAPERS IN PHYSICS, VOL. [22] C A Büsser, G B Martins, A E Feiguin, Lanczos transformation for quantum impurity problems in d-dimensional lattices: Application to graphene nanoribbons, Phys.


id: pip-47
author: Coniglio, Antonio; Pica Ciamarra, Massimo
title: Commentary on “Effect of temperature on a granular pile”
date: 2010-11-17
pages: 3
extension: .pdf
mime: application/pdf
words: 1446
sentence: 72
flesch: 66
cache: cache/pip-47.pdf
txt: txt/pip-47.txt
summary:
  Here, µ and σ are the friction coefficient and the shear stress of a gran- ular system, while ε measures the strength of the attractive force between thermal particles, and T is the temperature. In this structure, all inter–particle forces are equal in magnitude, and the net force acting on each particle is zero.


id: pip-278
author: Suárez, G. P.; Hoyuelos, Miguel; Chialvo, Dante R.
title: Invited review: Fluctuation-induced transport. From the very small to the very large scales
date: 2016-04-09
pages: 12
extension: .pdf
mime: application/pdf
words: 6526
sentence: 359
flesch: 65
cache: cache/pip-278.pdf
txt: txt/pip-278.txt
summary:
  [35] M Kostur, J Luczka, Multiple current reversal in Brownian ratchets, Phys. G. P. Suárez et al. U(x) x λ Q   Figure 2: Typical ratchet potential U(x).


id: pip-275
title: How we move is universal: Scaling in the average shape of human activity
date: 2015-11-18
pages: 7
extension: .pdf
mime: application/pdf
words: 4374
sentence: 210
flesch: 64
cache: cache/pip-275.pdf
txt: txt/pip-275.txt
author:
  Chialvo, Dante; Gonzalez Torrado, Ana María; Gudowska-Nowak, Ewa; Ochab, Jeremi K.; Montoya, Pedro; Nowak, Maciej A.; Tagliazucchi, Enzo

summary:
  al. 102 103 104 T 102 103 104 105 <S > 100 101 102 103 104 105 S,Wt,T 10-3 10-2 10-1 100 C C D F S Wt T A B α' τ' µ + 1 Figure 2: Scaling of activity events in a single subject (same dataset as in Fig. 1). Here we establish the presence of universality in motor activity fluctuations based on the empirical study of a month of con- tinuous wristwatch accelerometer recordings.


id: pip-380
author: Zanette, Damián H.
title: Self-sustained oscillations with delayed velocity feedback
date: 2017-03-30
pages: 7
extension: .pdf
mime: application/pdf
words: 4060
sentence: 220
flesch: 59
cache: cache/pip-380.pdf
txt: txt/pip-380.txt
summary:
  Since a purely linear mechanical system can- not display stable periodic motion, this kind of feedback force must necessarily be compensated by some nonlinear contribution from the oscillator dynamics itself. Em- phasis is put on the effects of time delays in the 090003-1 Papers in Physics, vol. 9, art.


id: pip-477
title: Pressure-induced Lifshitz transition in FeSe$_{0.88}$S$_{0.12}$ probed via $^{77}$Se-NMR
date: 2019-06-18
pages: 4
extension: .pdf
mime: application/pdf
words: 1893
sentence: 108
flesch: 67
cache: cache/pip-477.pdf
txt: txt/pip-477.txt
author:
  Kuwayama, T.; Matsuura, K.; Mizukami, Y.; Kasahara, S.; Matsuda, Y.; Shibauchi, T.; Uwatoko, Y.; Fujiwara, N.

summary:
  [2] J P Sun, K Matsuura, G Z Ye, Y Mizukami, M Shimozawa, K Matsubayashi, M Yamashita, T Watashige, S Kasahara, Y Matsuda, J Q Yan, B C Sales, Y Uwatoko, J G Cheng, T Shibauchi, Dome-shaped magnetic order com- peting with high-temperature superconductivity at high pressures in FeSe, Nat. Tc in- creases up to ∼ 27 K at 3.0 GPa from Tc ∼ 9 K at ambient pressure.


id: pip-284
author: López Grande, Ignacio H.; Schmiegelow, Christian T.; Larotonda, Miguel A.
title: Autonomous open-source hardware apparatus for quantum key distribution
date: 2016-01-21
pages: 8
extension: .pdf
mime: application/pdf
words: 4647
sentence: 221
flesch: 59
cache: cache/pip-284.pdf
txt: txt/pip-284.txt
summary:
  [16] N Lütkenhaus, Security against individual at- tacks for realistic quantum key distribution, Phys. Under normal operation conditions, the three parameters are constant through a typi- cal one hour and a half experiment, with a relative dispersion on their average values below 2 × 10−2 for key rate, 7 × 10−3 for bit bias and 2 × 10−3 for QBER (statistics obtained over 20 kbit partitions from a total 1.9 Mbit key).


id: pip-400
author: Ghosh, Sudeep; Roy, Ankhi
title: An improvement to the measurement of Dalitz plot parameters
date: 2017-12-31
pages: 8
extension: .pdf
mime: application/pdf
words: 4180
sentence: 227
flesch: 67
cache: cache/pip-400.pdf
txt: txt/pip-400.txt
summary:
  http://dx.doi.org/10.4279/PIP.090009 www.papersinphysics.org ISSN 1852-4249 An improvement to the measurement of Dalitz plot parameters S. Ghosh,1∗ A. Roy1† Precise measurement of the Dalitz plot parameters of the η′ → η π+ π− decay gives a better insight of the dynamics of the heavy pseudo-scalar meson. Dalitz plot parameters of the η′ → η π+ π− decay from the BESIII [12] experiment were used as input parameters for the generated events.


id: pip-475
author: Fujiwara, N.; Takeuchi, M.; Kuwayama, T.; Nakagawa, S.; Iimura, S.; Matsuishi, S.; Hosono, H.
title: Nuclear magnetic resonance on $LaFeAsO_{0.4}H_{0.6}$ at 3.7 GPa
date: 2019-06-04
pages: 4
extension: .pdf
mime: application/pdf
words: 1903
sentence: 107
flesch: 65
cache: cache/pip-475.pdf
txt: txt/pip-475.txt
summary:
  [3] M Hiraishi, S Iimura, K M Kojima, J Ya- maura, H Hiraka, K Ikeda, P Miao, Y Ishikawa, S Torii, M Miyazaki, I Yamauchi, A Koda, K Ishii, M Yoshida, J Mizuki, R Kadono, R Kumai, T Kamiyama, T Otomo, Y Murakami, S Matsuishi, H Hosono, Intro- duction to solid state physics, Nat. Phys. 10, 300 (2014). The R1 and R2 lines at ambient pressure, 3.0 and 3.7 GPa are shown in Fig.


id: pip-35
author: Perotti, Juan I.; Billoni, Orlando V.; Tamarit, Francisco A.; Cannas, Sergio A.
title: Stability as a natural selection mechanism on interacting networks
date: 2010-10-20
pages: 10
extension: .pdf
mime: application/pdf
words: 6078
sentence: 327
flesch: 62
cache: cache/pip-35.pdf
txt: txt/pip-35.txt
summary:
  While this suggests the presence of an underlying preferential attachment rule mecha- nism, a detailed analysis has shown that this is not Figure 4: Average network size as a function of the time measured in number of trials for b = 2 and q = 3. In Fig. 2, we plotted the connectivity for differ- ent biological networks across three orders of mag- nitude of network size scales, using data collected from the literature.


id: pip-49
author: Fedorenko, Andrei
date: 2011-01-12
pages: 3
extension: .pdf
mime: application/pdf
words: 1496
sentence: 81
flesch: 59
cache: cache/pip-49.pdf
txt: txt/pip-49.txt
title:
  Commentary on "Anisotropic finite-size scaling of an elastic string at the depinning threshold in a random-periodic medium"

summary:
  The latter takes place also in random field spin systems and states that a d-dimensional disordered system at zero tem- perature is equivalent to all orders in perturbation theory to a pure system in d−2 dimensions at finite temperature. The picture for finite systems is more involved.


id: pip-478
title: Fluorine chemistry at extreme conditions: Possible synthesis of $HgF_4$
date: 2019-02-27
pages: 6
extension: .pdf
mime: application/pdf
words: 3100
sentence: 151
flesch: 61
cache: cache/pip-478.pdf
txt: txt/pip-478.txt
author:
  Pravica, Michael G.; Schyck, Sarah; Harris, Blake; Cifligu, Petrika; Kim, Eunja; Billinghurst, Brant

summary:
  Our observation differs somewhat from the predictions of Botana et al. of a 38–73 GPa pres- sure range of stability [1] but given the challenges associated with connecting theory and experiment at high pressure and given the complex chemistry occurring during and after hard x-ray irradiation and at high pressures, our results are nevertheless encouraging. 110001-4 Papers in Physics, vol. 3. We note in passing that we performed a purely high pressure mid-IR study of just the XeF2 + HgF2 mixture (see Fig. 5) and found no evidence of any significant spectral changes (with the excep- tion of a phase transition near 5 GPa from HgF2) demonstrating that x-ray irradiation in combina- tion with high pressure is necessary to produce the interesting features observed in Fig.


id: pip-50
author: Roy, Sukhdev
date: 2011-01-13
pages: 3
extension: .pdf
mime: application/pdf
words: 1588
sentence: 77
flesch: 49
cache: cache/pip-50.pdf
txt: txt/pip-50.txt
title:
  Commentary on "Experimental determination of distance and orientation of metallic nanodimers by polarization dependent plasmon coupling"

summary:
  Gold nanoparticles have stimulated tremendous research interest due to their unique optical proper- ties. The authors address the important problem of experimental determination of distance and orien- tation of gold nanoparticles by measuring scatter- ing by illumination with polarized light.


id: pip-120
author: Fernández, M. L.; Otero, M.; Schweigmann, N.; Solari, H. G.
date: 2013-03-25
pages: 25
extension: .pdf
mime: application/pdf
words: 15971
sentence: 791
flesch: 65
cache: cache/pip-120.pdf
txt: txt/pip-120.txt
title:
  A mathematically assisted reconstruction of the initial focus of the yellow fever outbreak in Buenos Aires (1871)

summary:
  The immi- grants occupied large houses where they rented a room, usually for an entire family, a housing that was known as �conventillo� and was the dominant form of housing in some districts such as San Telmo, where the epidemic started [20]. Developmental Rate coe�cients The developmental rates that correspond to egg hatching, pupation, adult emergence and the gonotrophic cycles were evaluated using the results of the thermodynamic model developed by Sharp and DeMichele


id: pip-336
author: Lisandrini, Franco Thomas; Lobos, Alejandro Martín; Dobry, Ariel Oscar; Gazza, Claudio Javier
title: Topological quantum phase transition in strongly correlated Kondo insulators in 1D
date: 2016-09-30
pages: 10
extension: .pdf
mime: application/pdf
words: 6373
sentence: 323
flesch: 63
cache: cache/pip-336.pdf
txt: txt/pip-336.txt
summary:
  [11] M Dzero, K Sun, P Coleman, V Galitski, The- ory of topological Kondo insulators, Phys. Rev. B 85, 045130 (2012). From this perspective, our toy-model Hamiltonian H al- lows to explore a transtition from topological to non-topological Kondo insulators, and to gain a valuable insight of the TQPT. III.


id: pip-466
title: Temperature-dependent transport measurements with Arduino
date: 2018-11-02
pages: 8
extension: .pdf
mime: application/pdf
words: 4764
sentence: 225
flesch: 56
cache: cache/pip-466.pdf
txt: txt/pip-466.txt
author:
  Hilberer, A.; Laurent, G.; Lorin, A.; Partier, A.; Bobroff, J.; Bouquet, F.; Even, C.; Fischbach, J. M.; Marrache-Kikuchi, Claire Akiko; Monteverde, M.; Pilett, B.; Quay, Q.

summary:
  There is a wide variety of temperature sensors, depending on the temperature range of interest. We will also review some ba- sic techniques to ensure a proper thermal contact between the sample and the thermometer. i. Sensors types a. Built-in Arduino sensors There are a number of temperature sensors that are generally sold with standard Arduino kits.


id: pip-352
author: Gómez, Edgar Arturo; Hernández, José David; Vinck Posada, Herbert
title: Green's functions technique for calculating the emission spectrum in a quantum dot-cavity system
date: 2016-12-23
pages: 13
extension: .pdf
mime: application/pdf
words: 7413
sentence: 380
flesch: 69
cache: cache/pip-352.pdf
txt: txt/pip-352.txt
summary:
  More- over, it allows overcoming the inherent theoretical difficulties associated with the direct application of the quantum regression theorem in open quantum systems. I. Introduction The measurement and control of light produced by quantum systems have been the focus of interest of the cavity quantum electrodynamics [1, 2].


id: pip-485
author: Ishigaki, K.; Gouchi, J.; Nagasaki, S.; Cheng, J. G.; Uwatoko, Y.
title: Development of two-stage multi-anvil apparatus for low-temperature measurements
date: 2019-08-12
pages: 6
extension: .pdf
mime: application/pdf
words: 2795
sentence: 147
flesch: 62
cache: cache/pip-485.pdf
txt: txt/pip-485.txt
summary:
  The ap- plication of high pressure can induce structural or electronic phase transitions or precisely tune the structural and physical properties. In comparison with DAC, multianvil-type (MA) apparatus can maintain bet- ter pressure homogeneity even if the PTM becomes solidified at low temperature and/or high pressure [6].


id: pip-54
author: Jais, Pablo M.; von Bilderling, Catalina; Bragas, Andrea V.
date: 2011-06-09
pages: 5
extension: .pdf
mime: application/pdf
words: 2766
sentence: 167
flesch: 68
cache: cache/pip-54.pdf
txt: txt/pip-54.txt
title:
  Plasmon-enhanced second harmonic generation in semiconductor quantum dots close to metal nanoparticles

summary:
  NP samples were prepared by placing a drop of the NP solution on a glass substrate until the sol- vent evaporated. The observations can be attributed to the en- hancement of the nonlinear field around the QDs due to silver NP plasmon resonance at 2ω.


id: pip-513
author: Rezaei, Z.; Farokhi, B.
title: Theory of terahertz Smith-Purcell radiation from a cylindrical grating
date: 2019-10-08
pages: 7
extension: .pdf
mime: application/pdf
words: 3475
sentence: 233
flesch: 76
cache: cache/pip-513.pdf
txt: txt/pip-513.txt
summary:
  The effect of beam thickness (∆) on growth rate is depicted in Fig. Z. Rezaei et al. momentum equation for electron beams:


id: pip-44
author: Bustingorry, Sebastián; Kolton, Alejandro B.
date: 2010-12-20
pages: 11
extension: .pdf
mime: application/pdf
words: 6739
sentence: 337
flesch: 61
cache: cache/pip-44.pdf
txt: txt/pip-44.txt
title:
  Anisotropic finite-size scaling of an elastic string at the depinning threshold in a random-periodic medium

summary:
  Since the periodicity can often be experimentally tuned in such periodic systems it is thus worth studying in detail the geometry of critical interfaces of size L as a function of M with periodic boundary conditions, and thus com- plement the study of the critical force in such sys- tems This property is relevant as w2 fluctuates even in the thermodynamic limit for critical interfaces with a positive roughness expo- nent [42].


id: pip-482
title: Structural correlations in $Cs_2CuCl_4$: Pressure dependence of electronic structures
date: 2019-06-21
pages: 7
extension: .pdf
mime: application/pdf
words: 4061
sentence: 211
flesch: 66
cache: cache/pip-482.pdf
txt: txt/pip-482.txt
author:
  Jara, Enrique; Barreda-Argüeso, Jose Antonio; González, Jesus Antonio; Valiente, Rafael; Rodriguez, Fernando

summary:
  Single crystal dimensions (ambient pressure): 80 × 80 × 22 µm3. usually increases by decreasing the Cu–Cl bond distance, R, whereas the dihedral angle tends to decrease with pressure, approaching the Td angle (109.47o) under high compression. Vol- ume and pressure dependences of the elec- tronic, vibrational, and crystal structures of Cs2CoCl4: Identification of a pressure-induced piezochromic phase at high pressure, Phys. Rev. B 95, 014110 (2017).


id: pip-36
author: Divoux, Thibaut
title: Invited review: Effect of temperature on a granular pile
date: 2010-11-17
pages: 16
extension: .pdf
mime: application/pdf
words: 9836
sentence: 564
flesch: 66
cache: cache/pip-36.pdf
txt: txt/pip-36.txt
summary:
  [87] P Ribiere, P Richard, P Philippe, D Bideau, R Delanay, On the existence of stationary state during granular compaction, Eur. Phys. In particular, how can we compare the aging effects observed in vibrated granular piles and described in [89] to the one described here ?


id: pip-539
author: Mahmood, Rana S.; Salman, Sabah A.; Bakr, Nabeel Ali
title: The electrical and mechanical properties of Cadmium chloride reinforced PVA:PVP blend films
date: 2020-10-30
pages: 8
extension: .pdf
mime: application/pdf
words: 4529
sentence: 189
flesch: 57
cache: cache/pip-539.pdf
txt: txt/pip-539.txt
summary:
  The dielectric loss fac- tor of the pure PVA:PVP polymer blend films and polymer blend films reinforced by CdCl2·H2O salt was calculated at different weight ratios (10 wt%, 20 wt%, 40 wt%) at room temperature and within the frequency range of 100 Hz – 1 MHz, as shown in Fig. The effect of the salt weight ratio on the mechanical properties of the salt-reinforced PVA:PVP polymer blend films was also studied.


id: pip-531
author: Bazaziyan, Behnaz; Bozorgmehr, Mohammad Reza ; Momen-Heravi, Mohammad ; Beyramabadi, S. Ali
date: 2020-08-21
pages: 9
extension: .pdf
mime: application/pdf
words: 4762
sentence: 291
flesch: 61
cache: cache/pip-531.pdf
txt: txt/pip-531.txt
title:
  Flavodoxin in a binary surfactant system consisting of the nonionic 1-decanoyl-rac-glycerol and the zwitterionic lauryldimethylamine-N-oxide: Molecular dynamics simulation approach

summary:
  [4] C R Babu, P F Flynn, A J Wand, Validation of protein structure from preparations of en- capsulated proteins dissolved in low viscosity fluids, J. Am. Flavodoxin in sys- tem A has the smallest Rg and in system C the highest Rg.


id: pip-57
author: Fernández, E.; Fernández, R. J.; Bilmes, Gabriel Mario
title: Natural and laser-induced cavitation in corn stems: On the mechanisms of acoustic emissions
date: 2012-05-10
pages: 8
extension: .pdf
mime: application/pdf
words: 4329
sentence: 270
flesch: 67
cache: cache/pip-57.pdf
txt: txt/pip-57.txt
summary:
  Air seeding induced by the heating at pit membranes under CW laser irradiation should also be taken into account as an initial stage in laser induced cavitation inception. E. Fernández et al. sion technique to measure xylem cavitation


id: pip-515
author: Cifre, I.; Zarepour, M.; Horovitz, S. G. ; Cannas, S. A.; Chialvo, D. R.
date: 2020-06-18
pages: 8
extension: .pdf
mime: application/pdf
words: 5060
sentence: 249
flesch: 58
cache: cache/pip-515.pdf
txt: txt/pip-515.txt
title:
  Further results on why a point process is effective for estimating correlation between brain regions

summary:
  To answer this we analyze BOLD time series from the brain of a subject during an experiment in which fMRI data are collected at rest Figure 2 illus- trates, for those unfamiliar to the subject, three examples of typical BOLD time series that are usu- ally recorded from the brain.


id: pip-484
date: 2019-06-21
pages: 10
extension: .pdf
mime: application/pdf
words: 6843
sentence: 367
flesch: 69
cache: cache/pip-484.pdf
txt: txt/pip-484.txt
author:
  Francisco-López, Adrián; Han, Bo; Lagarde, Delphine; Marie, Xavier; Urbaszek, Bernhard; Robert, Cedric; Goñi, Alejandro

title:
  On the impact of the stress situation on the optical properties of $WSe_2$ monolayers under high pressure

summary:
  [18] R S Alencar, K D A Saboia, D Machon, G Montagnac, V Meunier, O P Ferreira, A San- Miguel, A G Souza Fihlo, Atomic-layer MoS2 on SiO2 under high pressure: [29] D Machon, C Bousige, R Alencar, A Torres- Dias, F Balima, J Nicolle, G S Pinheiro, A G Souza Filho, A San-Miguel, Raman scatter- ing studies of graphene under high pressure, J. Raman Spectrosc.


id: pip-65
date: 2012-02-13
pages: 8
extension: .pdf
mime: application/pdf
words: 4321
sentence: 255
flesch: 75
cache: cache/pip-65.pdf
txt: txt/pip-65.txt
author:
  Caldarola, Martín; Bettachini, Víctor A.; Rieznik, Andrés A.; Konig, Pablo G.; Masip, Martín E.; Grosz, Diego F.; Bragas, Andrea V.

title:
  High-speed tunable photonic crystal fiber-based femtosecond soliton source without dispersion pre-compensation

summary:
  Chirped pump pulses The effect over the soliton produced by the chirp of pump pulses was studied systematically by in- troducing a known amount of extra glass path on the second prism of the compressor. The figure shows that more power is always re- quired to attain the same shift when pump pulses are heavily chirped. 0 20 40 60 80 P [mW] 0 100 200 300 400 ∆ λ s [ n m ] 0 fs 2 7400 fs 2 Figure 8: Soliton wavelength shift for chirped (full squares) and TL pump pulses (empty squares) vs pump pulse power.


id: pip-638
author: Ré, Miguel Ángel; Aguirre Varela, Guillermo Gabriel
title: A method for continuous-range sequence analysis with Jensen-Shannon divergence
date: 2021-02-05
pages: 10
extension: .pdf
mime: application/pdf
words: 5002
sentence: 286
flesch: 63
cache: cache/pip-638.pdf
txt: txt/pip-638.txt
summary:
  For real value data sets (or the discrete type with a wide range) estimation of MI by frequency of appearance is not applica- ble. We generated 100 data sets, sam- pling 1000 (x,y) pairs from the distribution in (10) with different values of ym or σg, and from the joint distribution µ (x= 1,y)


id: pip-8
author: Zanette, Damián H.
title: A note on the consensus time of mean-field majority-rule dynamics
date: 2009-09-11
pages: 4
extension: .pdf
mime: application/pdf
words: 2156
sentence: 118
flesch: 67
cache: cache/pip-8.pdf
txt: txt/pip-8.txt
summary:
  In order to validate this analysis, numerical sim- ulations of MFMR dynamics have been performed for population sizes ranging from 102 to 105. If the size distribution of the groups of agents selected at each evolution step de- cays fast enough, one reobtains the logarithmic an- alytical result for constant group sizes.


id: pip-733
title: Observation of atmospheric scintillation during the 2020 total eclipse in northern Patagonia
date: 2022-11-04
pages: 7
extension: .pdf
mime: application/pdf
words: 4361
sentence: 216
flesch: 60
cache: cache/pip-733.pdf
txt: txt/pip-733.txt
author:
  Schmiegelow, Christian T.; Drechsler, Martín; Filgueira, Lautaro E.; Nuñez Barreto, Nicolás A.; Meconi, Franco

summary:
  [1] E. Gaviola, On shadow bands at total eclipses of the sun, Popular Astronomy 56, 353 (1948). [5] J. P. Madhani, G. E. Chu, C. V. Gomez, S. Bartel, R. J. Clark, L. W. Coban, M. Hart- man, E. M. Potosky, S. M. Rao, and D. A. Turnshek, Observation of eclipse shadow bands using high altitude balloon and ground based photodiode arrays, Journal of Atmospheric and Solar-Terrestrial Physics, 211, 105420 (2020).


id: pip-597
author: Abdel-Latif, Ahmed; Kassab, Maged ; Sayyed, M. I.; Tekin, H. O.
title: Optimizing the shielding properties of strength-enhanced concrete containing marble
date: 2020-09-08
pages: 9
extension: .pdf
mime: application/pdf
words: 5080
sentence: 265
flesch: 60
cache: cache/pip-597.pdf
txt: txt/pip-597.txt
summary:
  (2014) found that using marble powder as a partial replacement for cement or sand improves the physical properties of concrete [9]. V. Conclusions The following conclusions can be drawn: � The replacement of cement by marble waste powder enhances compressive strength, as re- placing 10 % of cement with marble powder (CM3) led to an increase of 10 % in com- pressive strength with respect to the measured value for reference sample CM1.


id: pip-78
author: González, Rafael; Page, Ricardo; Sartarelli, Andrés Salvador
title: Beltrami flow structure in a diffuser. Quasi-cylindrical approximation
date: 2012-03-07
pages: 7
extension: .pdf
mime: application/pdf
words: 3675
sentence: 203
flesch: 74
cache: cache/pip-78.pdf
txt: txt/pip-78.txt
summary:
  [2] R González, A Costa, E S Santini, On a varia- tional principle for Beltrami flows, Phys. In the quasi-cylindrical approximation, the steady flow in the transition expansion region corresponding to a solid body rotation with uniform axial flow as inlet flow has the same Beltrami flow structure as in the pipe down- stream, which is compatible with the bound- ary conditions.


id: pip-774
author: Chou, Yu-Ching; Huang, Weihan
date: 2022-04-12
pages: 8
extension: .pdf
mime: application/pdf
words: 4500
sentence: 324
flesch: 63
cache: cache/pip-774.pdf
txt: txt/pip-774.txt
title:
  A novel singularity-free black hole with nonlinear magnetic monopole: Hawking radiation and quantum correction

summary:
  Y. C. Chou et al. Qm = 1 4π ∫ F. (7) We found it extremely difficult to construct a solu- tion to analyze black holes with hadronic charges. VI Hawking radiation Hawking radiation is a quantum effect of black holes, in which the quantum tunneling effect causes parti- cles in black holes to pass through the event horizon.


id: pip-578
author: Barrere, Nicasio; Brum, Javier ; L'her, Alexandre; Sarasúa, Gustavo L.; Cabeza, Cecilia
title: Vortex dynamics under pulsatile flow in axisymmetric constricted tubes
date: 2020-06-16
pages: 14
extension: .pdf
mime: application/pdf
words: 6885
sentence: 357
flesch: 57
cache: cache/pip-578.pdf
txt: txt/pip-578.txt
summary:
  Received: 20 February 2020, Accepted: 25 May 2020 Edited by: S. Rafai Reviewed by: J. A. Isler Licence: Creative Commons Attribution 4.0 DOI: https://doi.org/10.4279/PIP.120002 www.papersinphysics.org ISSN 1852-4249 Vortex dynamics under pulsatile flow in axisymmetric constricted tubes Nicasio Barrere1*, Javier Brum1, Alexandre L’her1, Gustavo L. Sarasúa1, Cecilia Cabeza1 Improved understanding of how vortices develop and propagate under pulsatile flow can shed important light on the mixing and transport processes occurring in such systems, in- cluding the transition to turbulent regime. The analysis led to a scaling law equation for maximum vortex displacement as a function of a dimensionless variable dependent on the system parameters Re and α. I. Introduction Research on the dynamics of pulsatile flows through constricted regions has multiple applications in biomedical engineering and medicine.


id: pip-677
author: Nguyen, Thanh Tien; Le Vo Phuong Thuan; Tran Yen Mi
date: 2021-05-11
pages: 9
extension: .pdf
mime: application/pdf
words: 5001
sentence: 254
flesch: 62
cache: cache/pip-677.pdf
txt: txt/pip-677.txt
title:
  An ab initio study of small gas molecule adsorption on the edge of N-doped sawtooth penta-graphene nanoribbons

summary:
  The paper is organized as follows: the subject and research objectives are presented in the in- troduction section; in section II the computational methods are discussed; section III contains the re- sults and discussion of the electronic and trans- port properties of N:SSPGNR with the adsorbed Figure 2: Adsorption configurations of C-H- N:SSPGNR consist of: a) C-H-N:SSPGNR, b) isolated gas molecules and c) configurations of C-H-N:SSPGNR after adsorption gas molecules. / N. T. Tien et al. Table 1: Adsorption orientations and corresponding numbers for the adsorption structures of CO, CO2 and NH3 on the edge of N:SSPGNR Gas Configurations Adsorption orientations Notation of N:SSPGNR CO C-H-N:SSPGNR Vertical to C and O is downward COCH1 Vertical to C and O is upward COCH2 H-N-N:SSPGNR Vertical to N and O is downward COHN1 Vertical to Nintro and O is upward COHN2 C-N-N:SSPGNR Vertical to C and O is downward COCN1 Vertical to C and O is upward COCN2 Vertical to N and O is downward COCN3 Vertical to N and O is upward COCN4 CO2 C-H-N:SSPGNR Vertical to C CO2CH1 Horizontal to C and CO2 perpendicular to PG CO2CH2 Horizontal to C and CO2 parallel to PG CO2CH3 H-N-N:SSPGNR Vertical to N CO2HN1 Horizontal to N and CO2 perpendicular to PG CO2HN2 Horizontal to N and CO2 parallel to PG CO2HN3 C-N-N:SSPGNR Vertical to C CO2CN1 Horizontal to C and CO2 perpendicular to PG CO2CN2 Horizontal to C and CO2 parallel to PG CO2CN3 Vertical to N CO2CN4 Horizontal to N and CO2 perpendicular to PG CO2CN5 Horizontal to N and CO2 parallel to PG CO2CN6 NH3 C-H-N:SSPGNR Gas molecule is downward NH3CH1 Gas molecule is upward NH3CH2 H-N-N:SSPGNR Gas molecule is downward NH3HN1 Gas molecule is upward NH3HN2 C-N-N:SSPGNR Gas molecule is downward NH3CN1 Gas molecule is upward NH3CN2 Gas molecule is downward NH3CN3 Gas molecule is upward NH3CN4 III Results and Discussion


id: pip-7
author: Sartarelli, Salvador A.; Szybisz, Leszek
title: Correlation between asymmetric profiles in slits and standard prewetting lines
date: 2009-09-07
pages: 9
extension: .pdf
mime: application/pdf
words: 4929
sentence: 309
flesch: 73
cache: cache/pip-7.pdf
txt: txt/pip-7.txt
summary:
  Asymmetric density profiles are found for fluid confined in a slit built up of two identical planar walls leading to the spontaneous symmetry breaking (SSB) effect. Figure 3: Examples of density profiles of Ar ad- sorbed on a surface of Li at T = 114 K displayed as a function of the distance from the wall located at z∗ = 0.


id: pip-716
author: Mathew, Prijil; Mathews, Sajith T; Issac, Paul; Kurian, P J
title: Experimental study on the similarity of gas discharge in low-pressure Argon gaps
date: 2022-03-08
pages: 9
extension: .pdf
mime: application/pdf
words: 5206
sentence: 306
flesch: 68
cache: cache/pip-716.pdf
txt: txt/pip-716.txt
summary:
  When we considered similar discharge gaps, the radius r, gap length d and gas pressure p fulfilled the conditions of p1r1 = p2r2 Received: 20 May 2021, Accepted: 7 October 2021 Edited by: A. B. Márquez Licence: Creative Commons Attribution 4.0 DOI: https://doi.org/10.4279/PIP.140004 www.papersinphysics.org ISSN 1852-4249 Experimental study on the similarity of gas discharge in low-pressure Argon gaps Prijil Mathew1∗, Sajith T. Mathews1, Paul Issac1, P. J. Kurian1 Through experiments and theoretical analysis, we investigated the similarity of gas dis- charge in low-pressure Argon gaps between two plane-parallel electrodes.


id: pip-64
author: de Souza, Mario Everaldo
title: Calculation of almost all energy levels of baryons
date: 2011-08-08
pages: 13
extension: .pdf
mime: application/pdf
words: 7339
sentence: 495
flesch: 89
cache: cache/pip-64.pdf
txt: txt/pip-64.txt
summary:
  [1] which has calcula- tion of baryon energy levels and magnetic moments of baryons using approximate wavefunctions. |mz1| + 2r2 + |mz2| and k = 2r3 + |mz3| = 0, and thus we obtain |mz1| + |mz2|


id: pip-782
author: Cantor, David; Cárdenas-Barrantes, Manuel; Orozco, Luisa Fernanda
title: Bespoke particle shapes in granular matter
date: 2022-04-22
pages: 8
extension: .pdf
mime: application/pdf
words: 4905
sentence: 291
flesch: 49
cache: cache/pip-782.pdf
txt: txt/pip-782.txt
summary:
  (a) (b) Figure 1: Examples of structures built using non-convex particles: a) coastal barrier (public image by Pok Rie [20]) and b) aggregate wall (with permission of Karola Dierichts [21]). of non-convex shapes and the mechanical character- ization of assemblies either in standard equipment or non-conventional devices (e.g., large-scale shear boxes [37, 38]). To correctly match non-convex particle shapes to applications, a series of challenges need to be over- come.


id: pip-778
author: Hurley, Ryan; Zhai, Chongpu
date: 2022-03-05
pages: 9
extension: .pdf
mime: application/pdf
words: 5195
sentence: 297
flesch: 49
cache: cache/pip-778.pdf
txt: txt/pip-778.txt
title:
  Challenges and opportunities in measuring time-resolved force chain evolution in 3D granular materials

summary:
  The statis- tics, fluctuations, and organization of force chains – inter-particle forces with magnitudes greater than the average in a cohesion-less material – have been linked to: material stresses [4]; electrical and me- chanical energy transport [5–8]; mechanical failure via particle fracture and inter-particle slip [9, 10]; mechanical failure of confining vessels due to stress ∗rhurley6@jhu.edu †zhaichongpu@xjtu.edu.cn 1 Mechanical Engineering, Johns Hopkins University, Bal- timore, MD 21218, USA. 2 Hopkins Extreme Materials Institute, Johns Hopkins University, Baltimore, MD 21218, USA. In energetic materials, force chains that develop during rapid compaction are also thought to nucleate hot-spots that eventually lead to ma- terial ignition [48].


id: pip-9
author: Longone, P.; Linares, D. H.; Ramirez-Pastor, A. J.
date: 2009-11-17
pages: 7
extension: .pdf
mime: application/pdf
words: 4092
sentence: 222
flesch: 61
cache: cache/pip-9.pdf
txt: txt/pip-9.txt
title:
  The effect of the lateral interactions on the critical behavior of long straight rigid rods on two-dimensional lattices

summary:
  Finally, it is worth pointing out that: (1) the be- havior of the order parameter in Fig. 3 clearly indi- cates that the transition from the low-density dis- ordered phase to the intermediate-density ordered phase is an isotropic to nematic phase transition (when all the words have the usual meaning). The effect of the lateral interactions on the critical behavior of long straight rigid rods on two-dimensional lattices P. Longone,1 D. H. Linares,1 A. J. Ramirez-Pastor1∗ Using Monte Carlo simulations and finite-size scaling analysis, the critical behavior of attractive rigid rods of length k (k-mers) on square lattices has been studied.


id: pip-729
author: Panthi, Narayan; Bhandari, Indra ; Koirala, Ishwar
title: Thermophysical behavior of mercury-lead liquid alloy
date: 2022-04-01
pages: 11
extension: .pdf
mime: application/pdf
words: 5945
sentence: 308
flesch: 58
cache: cache/pip-729.pdf
txt: txt/pip-729.txt
summary:
  Similarly, concentration-dependent surface tension and vis- cosity of binary liquid alloys are investigated, these being the most desirable in metallurgical research for specifying the surface and transport properties of liquid mixtures: as such, scientists are attempt- ing to investigate these aspects by proposing several models [10–16] . III Results and discussion i Thermodynamic and microscopic proper- ties Generally, the properties of binary liquid alloys de- pend on temperature, composition, and pressure.


id: pip-641
author: Barberis, Lucas
title: Radial percolation reveals that Cancer Stem Cells are trapped in the core of colonies
date: 2021-04-09
pages: 11
extension: .pdf
mime: application/pdf
words: 7183
sentence: 361
flesch: 61
cache: cache/pip-641.pdf
txt: txt/pip-641.txt
summary:
  [2] C A M La Porta, S Zapperi, J P Sethna, Senescent cells in growing tumors: Popula- tion dynamics and cancer stem cells, PLoS Comput. [3] N A Lobo, Y Shimono, D Qian, M F Clarke, The biology of cancer stem cells, Annu.


id: pip-61
author: Pugnaloni, Luis Ariel; Damas, José; Zuriguel, Iker; Maza, Diego
date: 2011-08-25
pages: 13
extension: .pdf
mime: application/pdf
words: 8087
sentence: 420
flesch: 68
cache: cache/pip-61.pdf
txt: txt/pip-61.txt
title:
  Master curves for the stress tensor invariants in stationary states of static granular beds. Implications for the thermodynamic phase space

summary:
  We will use the expressions equilibrium state, steady state or simply state to refer to the collection of all configurations gener- ated by using a given external excitation after any transient has disappeared. Notice, however, that the same values of φ, Σ and its fluctuations, ∆φ and ∆Σ, are observed for the steady state of low Γ obtained before and after the 800 pulses of high Γ. Unless otherwise stated, all the results we present in what follows correspond to steady states.


id: pip-687
title: Physical distance characterization using pedestrian dynamics simulation
date: 2022-01-28
pages: 14
extension: .pdf
mime: application/pdf
words: 8237
sentence: 391
flesch: 65
cache: cache/pip-687.pdf
txt: txt/pip-687.txt
author:
  Parisi, Daniel R.; Patterson, Germán A.; Pagni, Lucio; Osimani, Agustina; Bacigalupo, Tomas; Godfrid, Juan; Bergagna, Federico M.; Rodriguez Brizi, Manuel; Momesso, Pedro; Gomez, Fermin L.; Lozano, Jimena; Baader, Juan M.; Ribas, Ignacio; Astiz Meyer, Facundo P.; Di Luca, Miguel; Barrera, Nicolas E.; Keimel Álvarez, Ezequiel M.; Herran Oyhanarte, Maite M.; Pingarilho, Pedro R.; Zuberbuhler, Ximena; Gorostiaga, Felipe

summary:
  Considering that: (a) The parameter we choose to maintain constant during each simulation is the allowed capacity N, and this capacity is reached at the beginning of each simulation in a very short time compared to other processes, and (b) all agents have the same number of items on their list, and thus the required time to complete it is similar on average, the first group of N agents will go to the checkout points at nearly the same time, generat- ing high checkout demand and long queues. This will provide efficient navigation to prevent poten- tial collisions with other agents and obstacles.


id: pip-883
author: Syiem, Elisheba ; Kharwanlang, Regenel Son
date: 2023-06-16
pages: 10
extension: .pdf
mime: application/pdf
words: 6675
sentence: 311
flesch: 75
cache: cache/pip-883.pdf
txt: txt/pip-883.txt
title:
  Study of hysteresis in the ferromagnetic random field 3-state clock model in two and three dimensional periodic lattices at zero temperature and in the presence of dilution and an absorbing state

summary:
  In this plot, for example at the h value along the red vertical line, CD gives the range of random fields where spins with one nearest neighbor in second state Sb and the remaining three in the first state Sa remain in the first state Sa at h. The range -0.8 -0.7 -0.6 -0.5 -0.4 -0.3 -0.2 -0.1 0 -0.8 -0.7 -0.6 -0.5 -0.4 -0.3 -0.2 -0.1 0 M a g n e ti z a ti o n Applied Field Figure 10: Jumps in magnetization in 3D lattice in increasing field for J = 0.1 (violet), J = 0.15 (green) and J = 0.2 (light blue), L = 1000. 150003-6 Papers in Physics, vol. The minor hysteresis loops for the 3D lattice 0 0.05 0.1 0.15 0.2 0.25 0.3 0.35 0.4 -0.5 -0.4 -0.3 -0.2 -0.1 0 0.1 0.2 0.3 0.4 0.5 F ra c ti o n o f s p in s a t th e s e c o n d s ta te Applied Field Figure 8: Trajectory of the fraction of spins at the second state in increasing and decreasing field in 3D for J = 0.257, Sa = −0.75, Sb = 0.0, Sc = 0.75, L = 1000. -0.8 -0.6 -0.4 -0.2 0 0.2 -0.5 -0.4 -0.3 -0.2 -0.1 0 0.1 0.2 M a g n e ti z a ti o n Applied Field Figure 9: Jumps in magnetization in 2D lattice in increasing field for J = 0.25 (violet), J = 0.3 (green) and J = 0.35 (light blue), L = 3000.


id: pip-87
author: Perez, Alejandro
title: Invited review: The new spin foam models and quantum gravity
date: 2012-05-25
pages: 37
extension: .pdf
mime: application/pdf
words: 20763
sentence: 1342
flesch: 74
cache: cache/pip-87.pdf
txt: txt/pip-87.txt
summary:
  Spin foam models are defini- tions of the path integral formulation of quantum general relativity and are expected to be the co- variant counterpart of the background independent canonical quantization of general relativity known as loop quantum gravity [1–3]. The importance of coherent states in spin foam models was put forward in Ref.


# url

id: pip-539
domain: www.researchgate.net
url:
  https://www.researchgate.net/profile/ahmed_hashim19/publication/310141127_synthesis_and_characterization_of_carbon_nanotubes-polystyrene_composites/links/5829a5d808aef00c20560d04.pdf


id: pip-539
domain: www.researchgate.net
url:
  https://www.researchgate.net/publication/248708227_effect_of_reinforcing_by_magnesium_oxide_particles_on_thermal_conductivity_and_mechanical_properties_of_vinyl_ester_resin


id: pip-774
domain: www.researchgate.net
url:
  https://www.researchgate.net/profile/tommaso-de-lorenzo/publication/283489779_investigating_static_and_dynamic_non-singular_black_holes/links/563a421d08aeed0531dcacdf/investigating-static-and-dynamic-non-singular-black-holes.pdf


id: pip-782
domain: www.researchgate.net
url:
  https://www.researchgate.net/profile/bas-reedijk/publication/275960407_design_of_concrete_armour_layers/links/554b8c450cf21ed213594b1a/design-of-concrete-armour-layers.pdf


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id: pip-539
sid: 165
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entity:
  https://doi.org/10.3390/polym9110622 https://doi.org/10.3390/polym9110622 https://www.ijsr.net/archive/v7i1/art20177355.pdf


id: pip-539
sid: 192
eid: 2
type: PERSON
entity:
  https://doi.org/10.1177/096739111502300805 https://doi.org/10.1177/096739111502300805 https://www.uotechnology.edu.iq/tec_magaz/volume282010/no.4.2010/researches/text


id: pip-539
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eid: 1
type: PERSON
entity:
  https://www.researchgate.net/publication/248708227_effect_of_reinforcing_by_magnesium_oxide_particles_on_thermal_conductivity_and_mechanical_properties_of_vinyl_ester_resin https://www.researchgate.net/publication/248708227_effect_of_reinforcing_by_magnesium_oxide_particles_on_thermal_conductivity_and_mechanical_properties_of_vinyl_ester_resin https://www.researchgate.net/publication/248708227_effect_of_reinforcing_by_magnesium_oxide_particles_on_thermal_conductivity_and_mechanical_properties_of_vinyl_ester_resin


id: pip-531
sid: 271
eid: 1
type: ORG
entity:
  http://doi.org/10.1093/bioinformatics/bth248 http://doi.org/10.1073/pnas.90.9.3835 http://doi.org/10.1073/pnas.90.9.3835


id: pip-515
sid: 267
eid: 1
type: PERSON
entity:
  https://doi.org/10.1615/int.j.uncertaintyquantification.2011003089 https://doi.org/10.1615/int.j.uncertaintyquantification.2011003089 https://people.sc.fsu.edu/~jburkardt https://doi.org/10.1103/physrevlett.94.018102 https://doi.org/10.1016/j.neuroimage.2010.08.063


id: pip-515
sid: 267
eid: 2
type: PERSON
entity:
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id: pip-733
sid: 97
eid: 3
type: PERSON
entity:
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id: pip-733
sid: 206
eid: 2
type: PERSON
entity:
  https://doi.org/10.1016/0021-9169(72)90144-4 https://doi.org/10.1016/0021-9169(72)90144-4 https://doi.org/10.1109/aero.2019.8741706 https://doi.org/10.1109/aero.2019.8741706


id: pip-733
sid: 209
eid: 2
type: ORG
entity:
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id: pip-638
sid: 288
eid: 3
type: PRODUCT
entity:
  https://doi.org/10.1016/j.physa.2006.12.051 https://aip.scitation.org/doi/abs/10.1063/1.4999613 https://aip.scitation.org/doi/abs/10.1063/1.4999613 https://www.jstor.org/stable/4144429 https://www.jstor.org/stable/4144429 10.1109


id: pip-597
sid: 209
eid: 1
type: PERSON
entity:
  https://doi.org/10.1016/j.conbuildmat.2013.09.005 https://doi.org/10.1016/j.conbuildmat.2013.09.005 https://doi.org/10.1016/j.conbuildmat.2010.07.002


id: pip-597
sid: 261
eid: 5
type: ORG
entity:
  https://doi.org/10.1016/j.anucene.2014.09.044 https://doi.org/10.1016/j.anucene.2014.09.044 https://doi.org/10.18576/jrna/020203


id: pip-597
sid: 263
eid: 2
type: PERSON
entity:
  https://dx.doi.org/10.26808/rs.ed.i8v4.02 http://www.scirp.org/journal/paperinformation.aspx?paperid=59708&#abstract http://www.scirp.org/journal/paperinformation.aspx?paperid=59708&#abstract https://doi.org/10.1093/rpd/nci192 https://doi.org/10.1093/rpd/nci192


id: pip-677
sid: 252
eid: 2
type: MONEY
entity:
  https://doi.org/10.1039/c7cp03404k https://doi.org/10.1063/1.5035385 https://doi.org/10.1016/j.physe.2019.113572 https://doi.org/10.1016/j.physe.2019.113572


id: pip-578
sid: 317
eid: 2
type: ORG
entity:
  https://doi.org/10.1098/rspb.1971.0019 https://doi.org/10.1161/01.atv.5.3.293 https://doi.org/10.1161/01.atv.5.3.293


id: pip-578
sid: 359
eid: 3
type: TIME
entity:
  https://doi.org/10.1146/annurev.fluid.29.1.399 https://doi.org/10.1146/annurev.fluid.29.1.399 https://doi.org/10.1017/s0022112097008410


id: pip-716
sid: 270
eid: 3
type: PERSON
entity:
  https://doi.org/10.1063/1.4976848 https://doi.org/10.1063/1.4976848 https://doi.org/10.1088/0963-0252/9/4/301 https://doi.org/10.1088/0963-0252/9/4/301


id: pip-716
sid: 274
eid: 1
type: ORG
entity:
  https://doi.org/10.1063/1.1388204 https://doi.org/10.1016/s0584-8547(01)00406-2 https://doi.org/10.1088/0256-307x/31/7/075201 https://doi.org/10.1088/0256-307x/31/7/075201


id: pip-716
sid: 275
eid: 1
type: GPE
entity:
  https://doi.org/10.1063/1.4866016 https://doi.org/10.1109/tps.2018.2889796 https://doi.org/10.1109/tps.2018.2889796 https://doi.org/10.1063/1.870572


id: pip-120
sid: 635
eid: 2
type: ORG
entity:
  estadistica de la mortalidad ocasionada por la epidemia de �ebre amarilla durante los meses de enero


id: pip-782
sid: 145
eid: 1
type: PERSON
entity:
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id: pip-782
sid: 194
eid: 5
type: ORG
entity:
  https://www.pexels.com/photo/aerial-view-of-breakwater-with-concrete-dolosse-5854657/ https://www.pexels.com/photo/aerial-view-of-breakwater-with-concrete-dolosse-5854657/


id: pip-782
sid: 199
eid: 1
type: PERSON
entity:
  https://doi.org/10.1111/j.1365-3091.1964.tb00271.x https://doi.org/10.1111/j.1365-3091.1964.tb00271.x


id: pip-782
sid: 256
eid: 2
type: PERSON
entity:
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id: pip-782
sid: 258
eid: 1
type: PERSON
entity:
  https://www.icevirtuallibrary.com/doi/abs/10.1680/aigev1.32644.0035 https://www.icevirtuallibrary.com/doi/abs/10.1680/aigev1.32644.0035 https://doi.org/10.1007/s11440-011-0151-6 https://doi.org/10.1007/s11440-011-0151-6


id: pip-782
sid: 262
eid: 3
type: PERSON
entity:
  https://doi.org/10.1016/j.crme.2017.12.009 https://doi.org/10.1016/0045-7825(94)90112-0 https://doi.org/10.1016/0045-7825(94)90112-0 https://doi.org/10.1016/s0045-7825(99)00338-2 https://doi.org/10.1016/s0045-7825(99)00338-2


id: pip-782
sid: 313
eid: 1
type: MONEY
entity:
  140007-8 https://doi.org/10.1103/physreve.99.062903 https://doi.org/10.1103/physreve.99.062903 https://doi.org/10.1103/physrevlett.124.208003 https://doi.org/10.1103/physrevlett.124.208003


id: pip-778
sid: 45
eid: 3
type: ORG
entity:
  latexit sha1_base64="tdhtje8astejqtp4ssnauw2jujc=">aaab63icbvbns8naej3ur1q/qh69lbbbu0mkqmecf48v7ae0owy2m3bpbhj2j0ij/qtepcji1t/kzx/jps1bwx8mpn6bywzekehh0hw/ndlg5tb2tnm3srd


id: pip-778
sid: 45
eid: 4
type: ORG
entity:
  latexit sha1_base64="zwpv2do4eabdwv8f2ryspkuakw0=">aaab83icbvdlssnafl2pr1pfvzdubovgqirs1gxbjcsk9gfnkjpppb06k4szg6ge


id: pip-778
sid: 156
eid: 1
type: PERSON
entity:
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id: pip-778
sid: 201
eid: 2
type: PERSON
entity:
  https://doi.org/10.1002/grl.50813 https://doi.org/10.1002/grl.50813 https://doi.org/10.1063/1.367429


id: pip-778
sid: 203
eid: 1
type: PERSON
entity:
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id: pip-778
sid: 267
eid: 1
type: GPE
entity:
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id: pip-778
sid: 270
eid: 1
type: PERSON
entity:
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id: pip-778
sid: 272
eid: 1
type: PERSON
entity:
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id: pip-729
sid: 319
eid: 1
type: PERSON
entity:
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id: pip-729
sid: 349
eid: 1
type: PERSON
entity:
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id: pip-641
sid: 298
eid: 2
type: ORG
entity:
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id: pip-641
sid: 300
eid: 1
type: ORG
entity:
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id: pip-641
sid: 300
eid: 2
type: ORG
entity:
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id: pip-641
sid: 345
eid: 1
type: LOC
entity:
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id: pip-641
sid: 345
eid: 2
type: ORG
entity:
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id: pip-641
sid: 347
eid: 1
type: PERSON
entity:
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id: pip-641
sid: 348
eid: 1
type: EVENT
entity:
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id: pip-883
sid: 356
eid: 2
type: ORG
entity:
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id: pip-883
sid: 358
eid: 1
type: GPE
entity:
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id: pip-687
sid: 340
eid: 1
type: DATE
entity:
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# pos

id: pip-778
sid: 45
tid: 44
pos: NUM
token:
  4czj14balbgdaw+juyxsxvpeimqtf9z03qz6hgwssfvwap4qlluzrmfusjqrjxs8wtc3jhlrejy20rqrjqf09kvbkzu4htvbqnztxlxf+8forhrz+jkemrr2y5kewlwzjkj5or0jyhnflcmrb2vsimvfognp6kdcfbfxmddbp177reeliqnrtfhgu4g3o4ba9uoan30ii2mjjam7zcm6ocf+fd+vi2lpxi5ht+wpn8ar6njj8=</latexit

lemma:
  4czj14balbgdaw+juyxsxvpeimqtf9z03qz6hgwssfvwap4qlluzrmfusjqrjxs8wtc3jhlrejy20rqrjqf09kvbkzu4htvbqnztxlxf+8forhrz+jkemrr2y5kewlwzjkj5or0jyhnflcmrb2vsimvfognp6kdcfbfxmddbp177reeliqnrtfhgu4g3o4ba9uoan30ii2mjjam7zcm6ocf+fd+vi2lpxi5ht+wpn8ar6njj8=</latexit


id: pip-778
sid: 45
tid: 49
pos: PROPN
token:
  sha1_base64="to9trxjlk1nmzgiduidqyjskhqy=">aaab7xicbvdlsgnbeoynrxhfuy9ebopgkewgir4dxjxgma9ilja7mu3gzgozmrxckn

lemma:
  sha1_base64="to9trxjlk1nmzgiduidqyjskhqy=">aaab7xicbvdlsgnbeoynrxhfuy9ebopgkewgir4dxjxgma9ilja7mu3gzgozmrxckn


id: pip-778
sid: 45
tid: 59
pos: NOUN
token:
  dtqbjmjhtgeoxilasjsce0mxthligklxumlfurviqwly6yicp0c27fz9ebif14vtffnmdgzpjzkslwupxxzheavoyhtlfg+dqqtzdytiiyxxss6geouhgd15xxsrlwderv2f1vp1pi4inag53ajavxda+6gcs0g8ajp8apvnvjevhfvy9la8pkzu

lemma:
  dtqbjmjhtgeoxilasjsce0mxthligklxumlfurviqwly6yicp0c27fz9ebif14vtffnmdgzpjzkslwupxxzheavoyhtlfg+dqqtzdytiiyxxss6geouhgd15xxsrlwderv2f1vp1pi4inag53ajavxda+6gcs0g8ajp8apvnvjevhfvy9la8pkzu


id: pip-778
sid: 45
tid: 87
pos: NOUN
token:
  rqmypyqhigt1ji+5yboz1sjyjlpk4pu8isykr3zvqurvdz42elwobmwyoiesbyvivmovycyqoyzqcb2koots+rl4n9ep8xw1s9elktii7zcfkasyezyx8liam5qziyhtat7k2etqildg0

lemma:
  rqmypyqhigt1ji+5yboz1sjyjlpk4pu8isykr3zvqurvdz42elwobmwyoiesbyvivmovycyqoyzqcb2koots+rl4n9ep8xw1s9elktii7zcfkasyezyx8liam5qziyhtat7k2etqildg0


id: pip-778
sid: 45
tid: 96
pos: PROPN
token:
  sha1_base64="zwpv2do4eabdwv8f2ryspkuakw0=">aaab83icbvdlssnafl2pr1pfvzdubovgqirs1gxbjcsk9gfnkjpppb06k4szg6ge

lemma:
  sha1_base64="zwpv2do4eabdwv8f2ryspkuakw0=">aaab83icbvdlssnafl2pr1pfvzdubovgqirs1gxbjcsk9gfnkjpppb06k4szg6ge


id: pip-778
sid: 45
tid: 102
pos: PROPN
token:
  chhupt7pmcttjldzihpdc6nhuss8jqil76wauxvk3g0nd3o/+8s1eun8inoub4qoyhejrtfkvj9mmpdhvck6g1rrbt1dgkwtrya1knaavl9sngwkx8gknabvuskgoduomoszip8znli2ospetzsmipsgx9w8ixdwgzio0fbfsbbq70roltftfdpjrxfsvr25+j

lemma:
  chhupt7pmcttjldzihpdc6nhuss8jqil76wauxvk3g0nd3o/+8s1eun8inoub4qoyhejrtfkvj9mmpdhvck6g1rrbt1dgkwtrya1knaavl9sngwkx8gknabvuskgoduomoszip8znli2ospetzsmipsgx9w8ixdwgzio0fbfsbbq70roltftfdpjrxfsvr25+j


