Open Access

Nonlinear optomechanical detection for Majorana fermions via a hybrid nanomechanical system

Nanoscale Research Letters20149:166

DOI: 10.1186/1556-276X-9-166

Received: 8 January 2014

Accepted: 29 March 2014

Published: 5 April 2014


The pursuit for detecting the existence of Majorana fermions is a challenging task in condensed matter physics at present. In this work, we theoretically propose a novel nonlinear optical method for probing Majorana fermions in the hybrid semiconductor/superconductor heterostructure. Our proposal is based on a hybrid system constituted by a quantum dot embedded in a nanomechanical resonator. With this method, the nonlinear optical Kerr effect presents a distinct signature for the existence of Majorana fermions. Further, the vibration of the nanomechanical resonator will enhance the nonlinear optical effect, which makes the Majorana fermions more sensitive to be detected. This proposed method may provide a potential supplement for the detection of Majorana fermions.


Majorana fermions Nanomechanical resonator Coherent nonlinear optical spectroscopy


The search for Majorana fermions (MFs) in hybrid nanostructures of condensed matter systems has become an important topic in quantum information processing. Unlike the usual Dirac particles, MFs obey non-Abelian statistics, which will open the potential applications in topological quantum computation [13]. In recent years, a number of systems that might host MFs in solid-state scenarios have been proposed. Several typical proposals include atoms trapped in optical lattices [4, 5], heterostructures of topological insulators and superconductor [6, 7], carbon-based materials [8], p-wave superconductors [911], and graphene or graphene-like materials [12]. Beyond these proposals, one promising scheme is to use semiconducting nanowires (such as InAs and InSb nanowires) with strong spin-orbit coupling placed in proximity with a superconductor and biased with an external magnetic field [13, 14]. After the prediction that Majorana bound states (MBSs) can be observed in the hybrid semiconductor/superconductor heterostructure, various experiments have indeed reported signatures of MFs in such systems recently [1520].

Since MFs are their own antiparticles, they are predicted to appear in tunneling spectroscopy experiments as zero-bias peaks [2123]. Such peaks have been observed in several experiments and have been interpreted as the signatures of MFs [1519]. Unfortunately, a zero-bias anomaly might also occur under similar conditions due to a Kondo resonance once the magnetic field has suppressed the superconducting gap enough to permit the screening of a localized spin [18, 24], and these experiments are not spatially resolved to detect the position of the MFs. Additionally, in many instances, the presence of disorder can also result in spurious zero-bias anomalies even when the system is not topological [2527]. Except zero-bias conductance peak, the Josephson effect is another signature which can demonstrate Majorana particles in the hybrid semiconductor-superconductor junction [20, 28, 29]. However, most of the recent experiments proposed and carried out have focused on electrical scheme, and the observation of Majorana signature based on electrical methods still remains a subject of debate. Meanwhile, other effective methods, such as optical technique [30, 31], for detecting MFs in the hybrid semiconductor/superconductor heterostructure have received less attention until now.

In recent years, nanostructures such as quantum dots (QDs) and nanomechanical resonators (NRs) have been obtained significant progress in modern nanoscience and nanotechnology. QD, as a simple stationary atom with well optical property [32], lays the foundation for numerous possible applications [33]. On the other hand, NRs are applied to ultrasensitive detection of mechanical signal [34], mass [35, 36], mechanical displacements [37], and spin [38] due to their high natural frequencies and large quality factors [39]. Further, the hybrid system where a QD is coupled to the NR also attracts much interest [4042]. Based on the advantages of QD or NR, several groups propose a scheme for detecting MFs via the QD [4348] or the NR [49] coupled to the nearby MFs. Here, we will propose an optical scheme to detect the existence of MFs in such a hybrid semiconductor/superconductor heterostructure via a hybrid QD-NR system.

In the present article, we consider a scheme closed to that of the recent experiment by Mourik et al. [15]. Compared with zero-bias peaks and the Josephson effect, we adopt an optical pump-probe technique to detect MFs. The nonlinear optical Kerr effect, as a distinct signature for demonstrating the existence of MFs in the hybrid semiconductor/superconductor heterostructure, is the main result of this work. Further, in our system (see Figure 1), the NR as a phononic cavity will enhance the nonlinear optical effect significantly, which makes MFs more sensitive to be detected.
Figure 1

Sketch of the proposed setup for optically detecting MFs. An InSb semiconductor nanowire (SNW) with strong spin-orbit interaction (SOI) in an external aligned parallel magnetic field B is placed on the surface of a bulk s-wave superconductor (SC). The two green stars at the ends of the nanowire represent a pair of MFs. The nearby MF is coupled to a semiconductor QD embedded in a nanomechanical resonator under a strong pump laser and a weak probe laser simultaneously. The inset is an energy-level diagram of a semiconductor QD coupled to MFs and NR.

Model and theory

Figure 1 presents the schematic setup that will be studied in this work. An InSb semiconductor nanowire with spin-orbit coupling in an external aligned parallel magnetic field B is placed on the surface of a bulk s-wave superconductor (SC). A MF pair is expected to locate at the ends of nanowire. To detect MFs, we employ a hybrid system in which an InAs semiconductor QD is embedded in a GaAs NR. By applying a strong pump laser and a weak probe laser to the QD simultaneously, one could probe the MFs via optical pump-probe technique [30, 31].

Benefitting from recent progress in nanotechnology, the quantum nature of a mechanical resonator can be revealed and manipulated in the hybrid system where a single QD is coupled to a NR [4042]. In such a hybrid system, the QD is modeled as a two-level system consisting of the ground state |g〉 and the single exciton state |e x〉 at low temperatures [50, 51]. The Hamiltonian of the QD can be described as H QD = ω QD S z with the exciton frequency ωQD, where S z is the pseudospin operator. In a structure of the NR where the thickness of the beam is much smaller than its width, the lowest-energy resonance corresponds to the fundamental flexural mode that will constitute the resonator mode [40]. We use a Hamiltonian of quantum harmonic oscillator H m = ω m b + b with the frequency ω m and the annihilation operator b of the resonator mode to describe the eigenmode. Since the flexion induces extensions and compressions in the structure [52], this longitudinal strain will modify the energy of the electronic states of QD through deformation potential coupling. Then the coupling between the resonator mode and the QD is described by ω m η S z ( b + + b ) , where η is the coupling strength between the resonator mode and QD [40]. Therefore, the Hamiltonian of the hybrid QD-NR system is H QD-NR = ω QD S z + ω m b + b + ω m η S z ( b + + b ) .

Since several experiments [1520] have reported the distinct signatures of MFs in the hybrid semiconductor/superconductor heterostructure via electrical methods, we assure that the MFs may exist in these hybrid systems under some appropriate conditions. Based on these experimental results, in the present article, we will try to demonstrate the MFs by using nonlinear optical method. As each MF is its own antiparticle, one can introduce a MF operator γMF such that γ MF = γ MF and γ MF 2 = 1 to describe MFs. Supposing the QD couples to γMF1, the Hamiltonian of the hybrid system [4346] is H MF = iℏ ω MF γ MF1 γ MF2 / 2 + iℏg ( S - - S + ) γ MF1 , where S± are the pseudospin operators. To detect the existence of MFs, it is helpful to switch from the Majorana representation to the regular fermion one via the exact transformation γ MF1 = f M + + f M and γ MF2 = i ( f M + - f M ) . f M and f M + are the fermion annihilation and creation operators obeying the anti-commutative relation f M , f M + = 1 . Accordingly, in the rotating wave approximation [53], H M can be rewritten as H MF = ω MF ( f M + f M - 1 / 2 ) + iℏg ( S - f M + - S + f M ) , where the first term gives the energy of MF at frequency ωMF, and ω MF = ε MF e - l / ξ with the wire length (l) and the superconducting coherent length (ξ). This term is small and can approach zero as the wire length is large enough. The second term describes the coupling between the right MF and the QD with coupling strength g, where the coupling strength depends on the distance between the hybrid QD-NR system and the hybrid semiconductor/superconductor heterostructure. Compared with electrical detection scheme which the QD is coupled to MF via the tunneling, here in our optical scheme, the exciton-MF coupling is mainly due to the dipole-dipole interaction. Since in current experiments the distance between QD and MF can be adjusted to locate the distance by about several tens of nanometers. In this case, the tunneling between the QD and MF can be neglected. It should be also noted that the term of non-conservation for energy, i.e. iℏg ( S - f M - S + f M + ) , is generally neglected. We have made the numerical calculations (not shown in the following figures) and shown that the effect of this term is too small to be considered in our theoretical treatment, especially for calculating the nonlinear optical properties of the QD.

The optical pump-probe technology includes a strong pump laser and a weak probe laser [54], which provides an effective way to investigate the light-matter interaction. Based on the optical pump-probe scheme, the linear and nolinear optical effects can be observed via the probe absorption spectrum. Xu et al. [30] have obtained coherent optical spectroscopy of a strongly driven quantum dot without a nanomechanical resonator. Recently, this optical pump-probe scheme has also been demonstrated experimentally in a cavity optomechanical system [31]. In terms of this scheme, we apply a strong pump laser and a weak probe laser to the QD embedded in the NR simultaneously. The Hamiltonian of the QD coupled to the pump laser and probe laser is given by [54] H QD-L = - µ E pu ( S + e - i ω pu t + S - e i ω pu t ) - µ E pr ( S + e - i ω pr t + S - e i ω pr t ) , where µ is the dipole moment of the exciton, ωpu (ωpr) is the frequency of the pump (probe) laser, and Epu (Epr) is the slowly varying envelope of the pump (probe) laser. Therefore, one can obtain the total Hamiltonian of the hybrid system as H=HQD-NR+HMBS+HQD-L.

According to the Heisenberg equation of motion and introducing the corresponding damping and noise terms, in a rotating frame at the pump laser frequency ωpu, we derive the quantum Langevin equations of the coupled system as follows:
S ̇ z = - Γ 1 S z + 1 2 + i Ω pu S + - S - - g S - f M + + S + f M + i µ E pr ( S + e - iδt - S - e iδt ) ,
S ̇ - = - [ i ( Δ pu + ω m ηN ) + Γ 2 ] S - - 2 i µ E pr e - iδt S z + 2 ( gf M - i Ω pu ) S z + F ̂ in ( t ) ,
f ̇ M = - ( i Δ MF + κ MF / 2 ) f M + g S - + ξ ̂ MF ( t ) ,
N ̈ + γ m N ̇ + ω m 2 N = - 2 ω m 2 η S z + ξ ̂ ( t ) ,

where N=b++b. Γ1 (Γ2) is the exciton relaxation rate (dephasing rate), κMF (γ m ) is the decay rate of the MF (nanomechanical resonator). Δpu=ωQD-ωpu is the detuning of the exciton frequency and the pump frequency, Ω pu = µ E pu / is the Rabi frequency of the pump field, and δ=ωpr-ωpu is the probe-pump detuning. ΔMF=ωMF-ωpu is the detuning of the MF frequency and the pump frequency. F ̂ in ( t ) is the δ-correlated Langevin noise operator, which has zero mean F ̂ in ( t ) = 0 and obeys the correlation function F ̂ in ( t ) F ̂ in ( t ) = δ ( t - t ) . The resonator mode is affected by a Brownian stochastic force with zero mean value, and ξ ̂ ( t ) has the correlation function ξ ̂ + ( t ) ξ ̂ ( t ) = γ m ω m 2 π ω e - ( t - t ) [ 1 + coth ( ℏω 2 κ B T ) ] , where k B and T are the Boltzmann constant and the temperature of the reservoir, respectively. MFs have the same correlation relation as the resonator mode. Actually, we have neglected the regular fermions (i.e. normal electrons) in the nanowire that interact with the QD in the above discussion. To describe the interaction between the normal electrons and the QD, we use the tight-binding Hamiltonian of the whole wire as [55, 56] H QD-e = ω QD S z + k ω k c k + c k + ℏζ k ( c k + S - + S + c k ) , where c k and c k are the regular fermion annihilation and creation operators with energy ω k and momentum ℏk obeying the anti-commutative relation c k , c k = 1 and ζ is the coupling strength between the normal electrons and QD (here, for simplicity, we have neglected the k-dependence of ζ as in [57]).

To go beyond weak coupling, the Heisenberg operator can be rewritten as the sum of its steady-state mean value and a small fluctuation with zero mean value: S z = S 0 z + δ S z , S - = S 0 - + δ S - , f M =fM 0+δ f M and N=N0 +δ N. Since the driving fields are weak, but classical coherent fields, we will identify all operators with their expectation values, and drop the quantum and thermal noise terms [31]. Simultaneously, inserting these operators into the Langevin equations (Equations 1 to 4) and neglecting the nonlinear term, we can obtain two equation sets about the steady-state mean value and the small fluctuation. The steady-state equation set consisting of fM 0, N0 and S 0 - is related to the population inversion ( w 0 = 2 S 0 z ) of the exciton which is determined by Γ 1 ( w 0 + 1 ) [ ( Δ MF 2 + κ MF 2 / 4 ) ( Δ pu 2 + Γ 2 2 + ω m 2 η 4 w 0 2 - 2 ω m Δ pu η 2 w 0 ) + g 2 w 0 2 ( g 2 - 2 ω m Δ MF η 2 + 2 Δ pu Δ MF - Γ 2 κ MF ) ] + 4 Ω pu 2 w 0 Γ 2 ( Δ MF 2 + κ MF 2 / 4 ) = 0 . For the equation set of small fluctuation, we make the ansatz [54] δ S z = S + z e - iδt + S - z e iδt , 〈δ S-〉=S+e-i δ t+S-e i δ t , 〈δ f M 〉=fM+e-i δ t+fM-e i δ t , and 〈δ N〉=N+e-i δ t+N-e i δ t . Solving the equation set and working to the lowest order in Epr but to all orders in Epu, we can obtain the nonlinear optical susceptibility as χ eff ( 3 ) ( ω pr ) = µ S - ( ω pr ) / ( 3 E pu 2 E pr ) = Σ 3 χ ( 3 ) ( ω pr ) , where Σ 3 = µ 4 / ( 3 3 Γ 2 3 ) and χ(3)(ωpr) is given by
χ ( 3 ) ( ω pr ) = ( d 2 + h 4 d 1 ) d 3 h 6 - iw 0 d 3 h 4 ( h 4 h 5 d 3 d 1 - d 4 d 2 ) Ω pu 2 Γ 2 3 ,

where b1=g/[i(ΔMF-δ)+κMF/2], b2=g/[ i(ΔMF+δ)+κMF/2], b 3 = 2 ω m 2 η / ( δ 2 + γ m - ω m 2 ) , h 4 = [ ( i Ω pu - gf M 0 ) - gS 0 - b 1 ] / ( Γ 1 + ) , h 5 = - [ ( i Ω pu + gf M 0 ) + gS 0 - b 2 ] / ( Γ 1 + ) , h 6 = iS 0 - / ( Γ 1 + ) , d 1 = 2 ( gf M 0 - i Ω pu ) - i ω m η S 0 - b 3 , d2=i(Δpu-δ+ω m η N0)+Γ2-g b1w0-d1h2, d 3 = 2 ( gf M 0 - i Ω pu ) - i ω m η S 0 - b 3 , d4=i(Δpu+δ+ω m η N0)+Γ2-g b2w0-d3h5 (where O indicates the conjugate of O). The quantum Langevin equations of the normal electrons coupled to the QD have the same form as MFs; therefore, we omit its derivation and only give the numerical results in the following.

Numerical results and discussions

For illustration of the numerical results, we choose the realistic hybrid systems of the coupled QD-NR system [40] and the hybrid semiconductor/superconductor heterostructure [1517, 20]. For an InAs QD in the coupled QD-NR system, the exciton relaxation rate Γ1=0.3 GHz, the exciton dephasing rate Γ2=0.15 GHz. The physical parameters of GaAs nanomechanical resonator are (ω m , m, Q)=(1.2 GHz, 5.3×10-15 g, 3×104), where m and Q are the effective mass and quality factor of the NR, respectively. The decay rate of the NR is γ m = ω m /Q=4×10-5 GHz. The coupling strength between quantum dot and nanomechanical resonator is η=0.06. For MFs in the the hybrid semiconductor/superconductor heterostructure, there are no experimental values for the lifetime of the MFs and the coupling strength between the exciton and MFs in the recent literature. However, according to a few experimental reports [1517], it is reasonable to assume that the lifetime of the MFs is κMF=0.1 MHz. Since the coupling strength between the QD and nearby MFs is dependent on their distance, we also expect the coupling strength g=0.03 GHz via adjusting the distance between the QD-NR hybrid structure and the nanowire.

Firstly, we consider the case that there is no coupling between the QD and NR (η=0), i.e. only a single QD is coupled to the nanowire. Figure 2 plots the optical Kerr coefficient R e(χ(3)) as a function of the probe detuning Δpr. In Figure 2, the blue curve indicates the nonlinear optical spectrum without the QD-MF coupling, and the red one shows the result with the QD-MF coupling g=0.03 GHz. It is obvious that when the MFs are presented at the ends of the nanowire, the two sharp sideband peaks will appear in the optical Kerr spectrum of the QD. The physical origin of this result is due to the QD-MF coherent interaction, which makes the resonant enhancement of the optical Kerr effect in the QD. This result also implies that the sharp peaks in the nonlinear optical spectrum may be the signature of MFs at the ends of the nanowire. Because there also includes normal electrons in the nanowire, in order to determine whether or not this signature (i.e. the sharp peaks) is the true MFs, we plot the inset of Figure 2, which uses the tight binding Hamiltonian to describe the normal electrons. In the figure, the parameters of normal electrons are chosen the same as MFs so that we can compare with the case of MFs. From the figure, we can observe that there is no sharp peak and only a nearly zero line in the spectrum (see the green line in the inset). This result demonstrates that the coupling between the QD and the normal electrons in the nanowire can be neglected in our theoretical treatment. In this case, one may utilize the optical Kerr effect in QD to detect the existence of MFs provided that the QD is close enough to the ends of the nanowire.
Figure 2

Optical Kerr coefficient as function of probe detuning Δ pr with two different QD-MF coupling strengths. The inset shows the result for the normal electrons in the nanowire that couple to the QD at the coupling strength ζ=0.03 GHz. The parameters used are Γ1=0.3 GHz, Γ2=0.15 GHz, η=0, γ m =4×10-5 GHz, ω m =1.2 GHz, κMF=0.1 MHz, Ω pu 2 = 0.01 GHz2, ΔMF=-0.5 GHz, and Δpu=0.5 GHz.

Secondly, we turn on the coupling to the NR (η≠0) and then plot the optical Kerr coefficient as a function of probe detuning Δpr for η=0.06 as shown in Figure 3. Taking the coupling between the QD and NR into consideration, the other two sharp peaks located at ±ω m will also appear. The red and blue curves correspond to the optical Kerr coefficient with and without the QD-MF coupling, respectively. Without the QD-MF coupling, the two sharp peaks locate at the resonator frequency of nanomechanical resonator induced by its vibration, i.e. two peaks are at Δpr=±1.2 GHz as shown in Figure 3. The physical origin of this result is due to mechanically induced coherent population oscillation (MICPO), which makes quantum interference between the resonator and the beat of the two optical fields via the QD when the probe-pump detuning is equal to the resonator frequency [58]. Turning on the QD-MF coupling, in addition to two sharp peaks located at ±1.2 GHz, the other two sideband peaks induced by the QD-MF coupling appear at Δpr=±0.5 GHz simultaneously.
Figure 3

The optical Kerr coefficient as a function of the probe detuning Δ pr for η =0 . 06. The other parameters used are the same as Figure 2.

To illustrate the advantage of the NR in our system, we adjust the detuning ΔMF=-0.5 GHz to ΔMF=-1.2 GHz, in this case, the location of the two sideband peaks induced by the QD-MF coupling coincides with the two sharp peaks induced by the vibration of NR, so the NR is resonant with the coupled QD-MF system and makes the coherent interaction of QD-MF more strong. Figure 4 gives the result of the optical Kerr coefficient as a function of probe detuning with or without the QD-NR coupling for the QD-MF coupling g=0.03 GHz. The blue and red curves correspond to η=0 and η=0.06, respectively. It is obvious that the role of NR is to narrow and to increase the optical Kerr effect. In this case, the NR as a phonon cavity will enhance the sensitivity for detecting MFs.
Figure 4

Optical Kerr coefficient as a function of probe detuning Δ pr with η =0 and η =0 . 06. g=0.03 GHz and ΔMF=-1.2 GHz. The other parameters used are the same as Figure 2.


We have proposed a nonlinear optical method to detect the existence of Majorana fermions in semiconductor nanowire/superconductor hybrid structure via a single quantum dot coupled to a nanomechanical resonator. The optical Kerr effect may provide another supplement for detecting Majorana fermions. Due to the nanomechanical resonator, the nonlinear optical effect becomes much more significant and then enhances the detectable sensitivity of Majorana fermions. Finally, we hope that our proposed scheme can be realized experimentally in the future.



The authors gratefully acknowledge support from the National Natural Science Foundation of China (No. 10974133 and No. 11274230).

Authors’ Affiliations

Department of Physics and Astronomy, Shanghai Jiao Tong University


  1. Nayak C, Simon SH, Stern A, Freedman M, Das SS: Non-Abelian anyons and topological quantum computation. Rev Mod Phys 2008, 80: 1083. 10.1103/RevModPhys.80.1083View Article
  2. Beenakker CWJ: Search for Majorana fermions in superconductors. Annu Rev Condens Matter Phys 2013, 4: 113. 10.1146/annurev-conmatphys-030212-184337View Article
  3. Stanescu TD, Tewari S: Majorana fermions in semiconductor nanowires: fundamentals, modeling, and experiment. J Phys Condens Matter 2013, 25: 233201. 10.1088/0953-8984/25/23/233201View Article
  4. Diehl S, Rico E, Baranov MA, Zoller P: Topology by dissipation in atomic quantum wires. Nat Phys 2011, 7: 971. 10.1038/nphys2106View Article
  5. Jiang L, Kitagawa T, Alicea J, Akhmerov AR, Pekker D, Refael G, Cirac JI, Demler E, Lukin MD, Zoller P: Majorana fermions in equilibrium and in driven cold-atom quantum wires. Phys Rev Lett 2011, 106: 220402.View Article
  6. Fu L, Kane CL: Superconducting proximity effect and Majorana fermions at the surface of a topological insulator. Phys Rev Lett 2008, 100: 096407.View Article
  7. Tanaka Y, Yokoyama T, Nagaosa N: Manipulation of the Majorana fermion, Andreev reflection, and Josephson current on topological insulators. Phys Rev Lett 2009, 103: 107002.View Article
  8. Klinovaja J, Gangadharaiah S, Loss D: Electric-field-induced Majorana Fermions in Armchair Carbon Nanotubes. Phys Rev Lett 2012, 108: 196804.View Article
  9. Read N, Green D: Paired states of fermions in two dimensions with breaking of parity and time-reversal symmetries and the fractional quantum Hall effect. Phys Rev B 2000, 61: 10267. 10.1103/PhysRevB.61.10267View Article
  10. Potter AC, Lee PA: Majorana end states in multiband microstructures with Rashba spin-orbit coupling. Phys Rev B 2011, 83: 094525.View Article
  11. Wong CLM, Liu J, Law KT, Lee PA: Majorana flat bands and unidirectional Majorana edge states in gapless topological superconductors. Phys Rev B 2013, 88: 060504(R).View Article
  12. Chamon C, Hou C-Y, Mudry C, Ryu S, Santos L: Masses and Majorana fermions in graphene. Phys. Scr 2012, T146: 014013.View Article
  13. Lutchyn RM, Sau JD, Das SS: Majorana fermions and a topological phase transition in semiconductor-superconductor heterostructures. Phys Rev Lett 2010, 105: 077001.View Article
  14. Oreg Y, Refael G, von Oppen F: Helical liquids and Majorana bound states in quantum wires. Phys Rev Lett 2010, 105: 177002.View Article
  15. Mourik V, Zuo K, Frolov SM, Plissard SR, Bakkers EPAM, Kouwenhoven LP: Signatures of Majorana fermions in hybrid superconductorsemiconductor nanowire devices. Science 2012, 336: 1003. 10.1126/science.1222360View Article
  16. Deng MT, Yu CL, Huang GY, Larsson M, Caroff P, Xu HQ: Anomalous zero-bias conductance peak in a Nb-InSb Nanowire-Nb hybrid device. Nano Lett 2012, 12: 6414. 10.1021/nl303758wView Article
  17. Das A, Ronen Y, Most Y, Oreg Y, Heiblum M, Shtrikman H: Zero-bias peaks and splitting in an Al-InAs nanowire topological superconductor as a signature of Majorana fermions. Nat Phys 2012, 8: 887. 10.1038/nphys2479View Article
  18. Lee EJH, Jiang X, Aguado R, Katsaros G, Lieber CM, De FS: Zero-bias anomaly in a nanowire quantum dot coupled to superconductors. Phys Rev Lett 2012, 109: 186802.View Article
  19. Churchill HOH, Fatemi V, Grove-Rasmussen K, Deng MT, Caroff P, Xu HQ, Marcus CM: Superconductor-nanowire devices from tunneling to the multichannel regime: zero-bias oscillations and magnetoconductance crossover. Phys Rev B 2013, 87: 241401.View Article
  20. Rokhinson LP, Liu XY, Furdyna JK: The fractional a. c. Josephson effect in a semiconductor-superconductor nanowire as a signature of Majorana particles. Nat Phys 2012, 8: 795. 10.1038/nphys2429View Article
  21. Law KT, Lee PA, Ng TK: Majorana fermion induced resonant Andreev reflection. Phys Rev Lett 2009, 103: 237001.View Article
  22. Flensberg K: Tunneling characteristics of a chain of Majorana bound states. Phys Rev B 2010, 82: 180516.View Article
  23. Wimmer M, Akhmerov AR, Dahlhaus JP, Beenakker CWJ: Quantum point contact as a probe of a topological superconductor. New J Phys 2011, 13: 053016. 10.1088/1367-2630/13/5/053016View Article
  24. Finck ADK, Van Harlingen DJ, Mohseni PK, Jung K, Li X: Anomalous modulation of a zero-bias peak in a hybrid Nanowiresuperconductor device. Phys Rev Lett 2013, 110: 126406.View Article
  25. Liu J, Potter AC, Law KT, Lee PA: Zero-bias peaks in the tunneling conductance of spin-orbit-coupled superconducting wires with and without Majorana end-states. Phys Rev Lett 2012, 109: 267002.View Article
  26. Pikulin DI, Dahlhaus JP, Wimmer M, Schomerus H, Beenakker CWJ: A zero-voltage conductance peak from weak antilocalization in a Majorana nanowire. New J Phys 2012, 14: 125011. 10.1088/1367-2630/14/12/125011View Article
  27. Bagrets D, Altland A, Class D: Spectral peak in Majorana quantum wires. Phys Rev Lett 2012, 109: 227005.View Article
  28. Williams JR, Bestwick AJ, Gallagher P, Hong SS, Cui Y, Bleich AS, Analytis JG, Fisher IR, Goldhaber-Gordon D: Unconventional Josephson effect in hybrid superconductor-topological insulator devices. Phys Rev Lett 2012, 109: 056803.View Article
  29. Pekker D, Hou C-Y, Manucharyan VE, Demler E: Proposal for coherent coupling of Majorana zero modes and superconducting Qubits using the 4 π Josephson effect . Phys Rev Lett 2013, 111: 107007.View Article
  30. Xu X, Sun B, Berman PR, Steel DG, Bracker AS, Gammon D, Sham LJ: Coherent optical spectroscopy of a strongly driven quantum dot. Science 2007, 317: 929. 10.1126/science.1142979View Article
  31. Weis S, Rivière R, Deleglise S, Gavartin E, Arcizet O, Schliesser A, Kippenberg TJ: Optomechanically induced transparency. Science 2010, 330: 1520. 10.1126/science.1195596View Article
  32. Jundt G, Robledo L, Högele A, Fält S, Imamǒglu A: Observation of dressed Excitonic states in a single quantum dot. Phys Rev Lett 2008, 100: 177401.View Article
  33. Urbaszek B, Marie X, Amand T, Krebs O, Voisin P, Maletinsky P, Högele A, Imamoğlu A: Nuclear spin physics in quantum dots: an optical investigation. Rev Mod Phys 2013, 85: 79. 10.1103/RevModPhys.85.79View Article
  34. Lassagne B, Tarakanov Y, Kinaret J, Garcia-Sanchez D, Bachtold A: Coupling mechanics to charge transport in carbon nanotube mechanical resonators. Science 2009, 325: 1107. 10.1126/science.1174290View Article
  35. Tamayo J, Kosaka PM, Ruz JJ, Paulo AS, Calleja M: Biosensors based on nanomechanical systems. Chem Soc Rev 2013, 42: 1287. 10.1039/c2cs35293aView Article
  36. Li JJ, Zhu KD: All-optical mass sensing with coupled mechanical resonator systems. Phys Rep 2013, 525: 223. 10.1016/j.physrep.2012.11.003View Article
  37. LaHaye MD, Buu O, Camarota B, Schwab KC: Approaching the quantum limit of a nanomechanical resonator. Science 2004, 304: 74. 10.1126/science.1094419View Article
  38. Rugar D, Budakian R, Mamin HJ, Chui BW: Single spin detection by magnetic resonance force microscopy. Nature 2004, 430: 329. 10.1038/nature02658View Article
  39. Poot M, van der Zant HSJ: Mechanical Systems in the Quantum Regime. Phys Rep 2013, 511: 273.View Article
  40. Wilson-Rae I, Zoller P, Imamoḡlu A: Laser cooling of a nanomechanical resonator mode to its quantum ground state. Phys Rev Lett 2004, 92: 075507.View Article
  41. Bennett SD, Cockins L, Miyahara Y, Grütter P, Clerk AA: Strong electromechanical coupling of an atomic force microscope cantilever to a quantum dot. Phys Rev Lett 2010, 104: 017203.View Article
  42. Yeo I, de Assis P-L, Gloppe A, Dupont-Ferrier E, Verlot P, Malik NS, Dupuy E, Claudon J, Gérard J-M, Auffèves A, Nogues G, Seidelin S, Poizat J-Ph, Arcizet O, Richard M: Strain-mediated coupling in a quantum dot-mechanical oscillator hybrid system. Nat Nanotech 2014, 9: 106.View Article
  43. Liu DE, Baranger HU: Detecting a Majorana-fermion zero mode using a quantum dot. Phys Rev B 2011, 84: 201308(R).View Article
  44. Flensberg K: Non-Abelian operations on Majorana fermions via single-charge control. Phys Rev Lett 2011, 106: 090503.View Article
  45. Leijnse M, Flensberg K: Scheme to measure Majorana fermion lifetimes using a quantum dot. Phys Rev B 2011, 84: 140501(R).View Article
  46. Pientka F, Kells G, Romito A, Brouwer PW, von Oppen F: Enhanced zero-bias Majorana peak in the differential tunneling conductance of disordered multisubband quantum-wire/superconductor junctions. Phys Rev Lett 2012, 109: 227006.View Article
  47. Sau JD, Das SS: Realizing a robust practical Majorana chain in a quantum-dot-superconductor linear array. Nat Commun 2012, 3: 964.View Article
  48. Fulga IC, Haim A, Akhmerov AR, Oreg Y: Adaptive tuning of Majorana fermions in a quantum dot chain. New J Phys 2013, 15: 045020. 10.1088/1367-2630/15/4/045020View Article
  49. Walter S, Schmidt TL, Børkje K, Trauzettel B: Detecting Majorana bound states by nanomechanics. Phys Rev B 2011, 84: 224510.View Article
  50. Zrenner A, Beham E, Stufler S, Findeis F, Bichler M, Abstreiter G: Coherent properties of a two-level system based on a quantum-dot photodiode. Nature 2002, 418: 612. 10.1038/nature00912View Article
  51. Stufler S, Ester P, Zrenner A, Bichler M: Quantum optical properties of a single In x Ga1-xAs-GaAs quantum dot two-level system . Phys Rev B 2005, 72: 121301.View Article
  52. Graff KF: Wave Motion in Elastic Solids Dover. New York: Dover Publications; 1991.
  53. Ridolfo A, Stefano OD, Fina N, Saija R, S. Savasta S: Quantum plasmonics with quantum dot-metal nanoparticle molecules: influence of the Fano effect on photon statistics. Phys Rev Lett 2010, 105: 263601.View Article
  54. Boyd RW: Nonlinear Optics. San Diego, CA: Academic; 1992.
  55. Mahan GD: Many-Partcle Physics. New York: Plenum Press; 1992.
  56. Nadj-Perge S, Drozdov IK, Bernevig BA, Yazdani A: Proposal for realizing Majorana fermions in chains of magnetic atoms on a superconductor. Phys Rev B 2013, 88: 020407(R).View Article
  57. Hewson AC: The Kondo Problem to Heavy Fermions. New York: Cambridge University Press; 1993.View Article
  58. Li JJ, Zhu KD: A tunable optical Kerr switch based on a nanomechanical resonator coupled to a quantum dot. Nanotechnol 2010, 21: 205501. 10.1088/0957-4484/21/20/205501View Article


© Chen and Zhu; licensee Springer. 2014

This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.