We provide an article-extract which points out that a microwave-induced modification in the resistance occurs at relatively "high" magnetic fields where the radiation is incapable of producing inter-Landau level excitations and, therefore, that the microwa
ARTICLEINPRESS
R.G.Mani/PhysicaE](]]]])]]]–]]]
3
illustratedbyFigs.3
and4.Atthelowestfrequency,f¼3:35GHz;seeFig.3(a),regularoscillationsdonotappearinRxx;andthemicrowaveradiationseemstoproducemostlynegativemagnetoresistance,suchthattheirra-diatedRxxfallsbelowthedarkRxxat eldswellaboveBf:At eldsaboveBf;theradiationseemsincapableofproducinginter-Landaulevelexcita-tions,andtherefore,anewmechanismappearsnecessarytodescribethislow-fbehavior.AstheradiationenergyattheappliedfinFig.3(a)seems
1.5
1.0)
( xxR0.5
0.0(a)
2.0
1.5
)
( xx1.0
R0.5
0.0Bf (15.6 GHz)
(b)
B (T)
Fig.3.This gureexhibitstheeffectofmicrowaveirradiationonthediagonalresistance,Rxx;atrelativelylowmicrowavefrequencies.(a)Atf¼3:35GHz;theradiationmostlypro-ducesnegativemagnetoresistanceatmagnetic eldswellaboveBf;wheretheradiationseemsincapableofproducinginter-Landaulevelexcitations.(b)Withincreasingf;theradiation-inducedreductioninRxxaboveBfbecomeslesspronouncedasaresistancemaximum,the‘‘ rstresistancemaximum,’’becomesperceptible.
tolieinthevicinityoftheexpectedzero- eldspinsplittingduetotheRashbaandDresselhaustermsinthisGaAs/AlGaAssystem[19],wesuggestthattheobservedlowfbehaviormightre ectradia-tion-inducedmixingbetweenspinlevelsofthesameLandauband,andthemodi cationofthismixing,duetothe eld-inducedZeemanterm.Theeffectofincreasingf;atrelativelylowf;isexhibitedinFig.3(b).Here,oneobservesthatasf