EPR spectra of multispin systems. Application to poly-m-p-aniline

P. Juszyński , A. Twardowski , Jacek Gosk , Irena Kulszewicz-Bajer , M Pawłowski , K. Dziatkowski , J. Szczytko


In this communication we present NiceMagnetic, software for simulations and analysis of EPR spectrum and SQUID measurements. Systems of arbitrary number N of spin-only magnetic moments (S ≠ 0 and L = 0) were considered within the lines of the Heisenberg and Zeeman Hamiltonians. Effective algorithms used for the computations are discussed. This includes modified secant method adapted to calculate resonance fields with demanded precision. Finally, application of NiceMagnetic to experimental SQUID magnetization and EPR spectra of poly-m-p-aniline, one of recently synthesized high spin polymers containing unpaired electrons will be presented. As a result, exchange integral between electron and nitrogen nuclei spins (ligand hyperfine interaction) J = 6:3 × 10 -4 cm -1 was estimated.
Author P. Juszyński
P. Juszyński,,
, A. Twardowski
A. Twardowski,,
, Jacek Gosk (FP / HPRD)
Jacek Gosk,,
- High Pressure Research Division
, Irena Kulszewicz-Bajer (FC / CPCT)
Irena Kulszewicz-Bajer,,
- Chair Of Polymer Chemistry And Technology
, M Pawłowski
M Pawłowski,,
, K. Dziatkowski
K. Dziatkowski,,
, J. Szczytko
J. Szczytko,,
Journal seriesActa Physica Polonica A, ISSN 0587-4246, (A 15 pkt)
Issue year2011
Keywords in EnglishArbitrary number; Effective algorithms; EPR spectra; Exchange integrals; Heisenberg; High spins; Hyperfine interactions; Modified Secant method; Resonance field; SQUID magnetization; SQUID measurements; Unpaired electrons, Aniline; Hamiltonians; Magnetic moments; Shellfish, Electron spin resonance spectroscopy
ASJC Classification3100 General Physics and Astronomy
URL http://www.scopus.com/inward/record.url?eid=2-s2.0-79954523174&partnerID=40&md5=44a6e1bbbad583952adb1090121ce985
Score (nominal)15
Publication indicators WoS Citations = 0; Scopus SNIP (Source Normalised Impact per Paper): 2011 = 0.453; WoS Impact Factor: 2011 = 0.444 (2) - 2011=0.404 (5)
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