Rero Marques Rubinger

Dr. Rero Marques Rubinger

orcid

Research Focus & Metrics

Academic Career Length

30Years (1997-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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1 June 2009 in Journal of Magnetism and Magnetic Materials
Verified
Journal Article
Closed access
VKVladimir Khomchenko
Vladimir Khomchenko
Dmitry A. KiselevDmitry A. Kiselev
Dmitry A. Kiselev
MKM. Kopcewicz
M. Kopcewicz
MMM. Maglione
M. Maglione
Vladimir ShvartsmanVladimir Shvartsman
Vladimir Shvartsman
Andrei KholkinAndrei Kholkin
Andrei Kholkin

10 April 2007 in Sensors and Actuators B: Chemical
Verified
Journal Article
Closed access
CRC.P.L. Rubinger
C.P.L. Rubinger
CMC.R. Martins
C.R. Martins
MPM.-A. De Paoli
M.-A. De Paoli
RRRero Marques Rubinger
Rero Marques Rubinger

1 November 2018 in Solar Energy
Verified
Journal Article
Closed access
DFD.M. Fébba
D.M. Fébba
RRRero Marques Rubinger
Rero Marques Rubinger
Adhimar Flávio OliveiraAdhimar Flávio Oliveira
Adhimar Flávio Oliveira
EBE.C. Bortoni
E.C. Bortoni

1 June 2008 in Physics Letters A
Verified
Journal Article
Closed access
HAHolokx Abreu Albuquerque
Holokx Abreu Albuquerque
RRRero Marques Rubinger
Rero Marques Rubinger
PRPaulo C. Rech
Paulo C. Rech

27 March 2008 in Physical Review B
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Journal Article
Closed access
PDF file
MRM. S. Reis
M. S. Reis
RRRero Marques Rubinger
Rero Marques Rubinger
Nikolai A. SobolevNikolai A. Sobolev
Nikolai A. Sobolev
Manuel ValenteManuel Valente
Manuel Valente
KYK. Yamada
K. Yamada
SGS. Gama
S. Gama
Manganese monophosphate MnP single crystal deserves attention due to its rich magnetic phase diagram, which is quite different depending on the direction of the applied magnetic field. Generally speaking, it has a Curie temperature around 291K and several other magnetic arrangements at low temperatures (cone-, screw-, fan-, and ferromagnetic-type structures). This richness is due to the strong magnetocrystalline anisotropy. In this sense, the present paper makes a thorough description of the influence of this anisotropy on the magnetocaloric properties of this material. From a fundamental view we could point out, among those several magnetic arrangements, the most stable one. On the other hand, from an applied view, we could show that the magnetic entropy change around room temperature ranges from −4.7to−3.2J∕kgK, when the magnetic field (5T) is applied along the easy and hard magnetization directions, respectively. In addition, we have shown that it is also possible to take advantage of the magnetic anisotropy for magnetocaloric applications, i.e., we have found a quite flat magnetic entropy change (with a huge relative cooling power), at a fixed value of magnetic field, only rotating the crystal by 90°.

24 October 2012 in PLOS ONE
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Journal Article
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Mauricio  BaptistaMauricio Baptista
Mauricio Baptista
RRRero Marques Rubinger
Rero Marques Rubinger
EVEmilson R. Viana
Emilson R. Viana
JSJosé C Sartorelli
José C Sartorelli
UPUlrich Parlitz
Ulrich Parlitz
CGCelso Grebogi
Celso Grebogi
The amount of information exchanged per unit of time between two nodes in a dynamical network or between two data sets is a powerful concept for analysing complex systems. This quantity, known as the mutual information rate (MIR), is calculated from the mutual information, which is rigorously defined only for random systems. Moreover, the definition of mutual information is based on probabilities of significant events. This work offers a simple alternative way to calculate the MIR in dynamical (deterministic) networks or between two time series (not fully deterministic), and to calculate its upper and lower bounds without having to calculate probabilities, but rather in terms of well known and well defined quantities in dynamical systems. As possible applications of our bounds, we study the relationship between synchronisation and the exchange of information in a system of two coupled maps and in experimental networks of coupled oscillators.