We have studied the nonlinear current-voltage characteristic of a two dimensional lattice Coulomb gas by Monte Carlo simulation. We present three different determinations of the power-law exponent $a(T)$ of the nonlinear current-voltage characteristic, $V
jumpcriteriontellsusthat1/ (k=0)jumpsfrom4TcatT=Tc to0atT=Tc+[9].Apracticaldi cultyforlocatingTcfromMonteCarlodataonsmalllatticeswiththis
procedureisthatextrapolationtothek=0limitrequireslargelattices,asthesmallest
nonzerokis2π/L.Thecorrespondingquantityto1/ (k=0)inthetwodimensionalXY
modeliscalledthehelicitymodulusγ[5].Bothquantitieshavebeenusedtolocatethe
Kosterlitz-ThoulesstransitiontemperatureinMonteCarlocalculations[5,25,19].
InthedataanalysisinthenextsectionweuseanalternativeproceduretolocateTcfrom
thelinearresistance[12].WeobtainthelinearresistanceRfromtheNyquistformulain
Eq.(5)forasequenceofsystemsizesLandtemperaturesT.AccordingtoEq.(6)data
forL2Rfordi erentsystemsizesshouldbecomesystemsizeindependentatthecritical
temperature,whichisourcriteriontolocateTc.Thiscircumventsthedi cultiesofusing
1/ (k=0).ThetwodeterminationsgivewithinerrorbarsthesamevalueforTc.
V.RESULTS
WepresentMonteCarlosimulationresultsforthreedi erentdeterminationsoftheIV
exponenta(T)forthe2DCoulombgasmodel.Theresultsweshowhereareforthechemical
potentialµ=0.0andlatticesizeL=32ifnotdi erentlystated.
A.NonlinearIVexponent
Our rstmethodconsistsinadirectmeasurementoftheelectric eldEinducedbyan
appliedcurrentdensityj.InFig.1aresultsfortheIVcharacteristicofthetwo-dimensional
Coulombgasareshown.Thedashedlineintheln(E)versusln(j)plothasslopethree
andrepresentstheslopeatT=Tcaccordingtotheuniversaljumpcondition[9].The
solidcurvesrepresentresultsfordi erenttemperatures.Forveryhighcurrentthevoltage
responsesaturates.Thisisbecausewhenallattemptstomovethevorticesinthedirection
oftheLorentzforcearealreadyaccepted,furtherincreasingthecurrentcannotgivemore
voltage.Forlowenoughcurrentthereisacrossovertoohmicresistance,whenthecurrent