
Electrically-detected single-spin resonance with Quantum Spin Hall edge states
F. Delgado1and J. Fern´andez-Rossier2,3
1Instituto de estudios avanzados IUDEA, Departamento de F´ısica,
Universidad de La Laguna, C/Astrof´ısico Francisco S´anchez, s/n. 38203, La Laguna and
2International Iberian Nanotechnology Laboratory (INL),
Av. Mestre Jos´e Veiga, 4715-310 Braga, Portugal ,
(Dated: October 7, 2022)
Detection is most often the main impediment to reduce the number of spins in paramagnetic
resonance experiments. Here we propose a new route to carry out electrically-detected spin resonance
of an individual spin, placed at the edge of a quantum spin Hall insulator (QSHI). The edges of
a QSHI host a one dimensional electron gas with perfect spin-momentum locking. Therefore, the
spin relaxation induced by emission of an electron-hole pair at the edge state of the QSHI can
generate current. Here we demonstrate that driving the system with an AC signal, a nonequilibrium
occupation can be induced in the absence of applied bias voltage, resulting in a DC measurable
current. We compute the DC current as a function of the Rabi frequency Ω, the spin relaxation
and decoherence times, T1and we discuss the feasibility of this experiment with state of the art
instrumentation.
PACS numbers: 73.22.Pr, 73.43.Cd, 76.30.-v
I. INTRODUCTION
The sensitivity limit of commonly available electron
paramagnetic resonance (EPR) spectrometers is in the
range of 1013 spins1. This number can be dramatically
reduced in taylored set-ups2. In some special systems,
such as NV-centers, permit one to carry out single-spin
resonance using optical readout, made possible both by
the fact that NV centers are very good single-photon
emitters and their photon yield is spin dependent.3Us-
ing spin-to-charge conversion, electrically detected single
spin resonance has been demonstrated for defects in field
effect-transistors,4quantum dots5,6 and single dopants in
silicon.7Electrically detected single spin resonance with
subatomic spatial resolution has been also demonstrated8
using scanning tunneling microscopy (ESR-STM).
Here we explore the spin-locked edges states of a two
dimensional Quantum Spin Hall insulator9,10 (QSHI) to
accomplish the electrical readout of the spin resonance of
an individual spin sitting on the edge. The edge states of
QSHI are predicted to have a one-to-one relation between
the propagation direction and the spin orientation along
a system-dependent spin quantization axis, see Fig. 1.
As a result, pumping spin along this axis entails elec-
trical current flow. As we discuss below, if a externally
pumped localized spin is exchange coupled to the spin-
locked edges, it will generate a DC current.
Experimental evidences of the spin-locked edge states
in QSHI are indirect. In the absence of magnetic impuri-
ties, edge states should have no backscattering and there-
fore a quantized conductance is expected.11–13 Values of
conductance close to 2e2/h were reported in HgTe/CdTe
quantum wells14 and 1T’ WTe2.15,16 In addition, coher-
ent propagation along the edge with scattering proper-
ties consistent with strong suppression of backscatter-
ing have been observed in bismuth bilayers,17,18 and in
bismuth nanocontacts19. Very relevant for the ensuing
Driving Frequency w
DC Current
J
Bac(t)
e- h+
FIG. 1. Scheme of the device proposed for the electrically-
detected single spin detection. A local spin Sis exchange
coupled to one edge state of a QSHI, where momentum di-
rection and spin orientation are locked, see left inset. When
the system is under the action of an external AC magnetic
field with frequency ωand intensity determined by the Rabi
rate Ω, a frequency-dependent non-equilibrium steady state
occupation is established (see right inset), where one of the
spin transitions ∆Szis favored. This, in turns, leads to a net
DC electrical current along the QSHI edge.
discussion, experiments where magnetic atoms interact
with edge states in bismuth bilayer and produced back-
scattering have been demonstrated20.
The interplay between local spins and the spin-locked
edge states of a QSHI has been widely studied theo-
retically 21–37. Several physical realizations of the lo-
cal spin have been considered, including a confined elec-
tron in a quantum dot29,35, nanomagnets,28 magnetic
atoms,26,27 spin chains36, nuclear spins,25,33,37 and mag-
netic molecules32. Early works focused on the Kondo
effect,21,24 and the influence of magnetic impurities on
conductance22. More recent works have addressed spin-
pumping of local moments at the edges by the helical-
electron spin current.26–29,31,32,34 The reverse problem,
pumping DC current by an external AC excitation of
arXiv:2210.02917v1 [cond-mat.mes-hall] 6 Oct 2022