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Properties of the Geometric Phase in Electromechanical Oscillations of CarbonNanotubeBased Nanowire Resonators
Nanoscale Research Letters volume 14, Article number: 44 (2019)
Abstract
The geometric phase is an extra phase evolution in the wave function of vibrations that is potentially applicable in a broad range of science and technology. The characteristics of the geometric phase in the squeezed state for a carbonnanotubebased nanowire resonator have been investigated by means of the invariant operator method. The introduction of a linear invariant operator, which is useful for treating a complicated timedependent Hamiltonian system, enabled us to derive the analytical formula of the geometric phase. By making use of this, we have analyzed the time behavior of the geometric phase based on relevant illustrations. The influence of squeezing parameters on the evolution of the geometric phase has been investigated. The geometric phase, in large, oscillates, and the envelope of such oscillation increases over time. The rate of the increase of the geometric phase is large when the parameters, such as the classical amplitude of the oscillation, the damping factor, and the amplitude of the driving force, are large. We have confirmed a very sharp increase of the geometric phase over time in the case that the angular frequency of the system reaches near the resonance angular frequency. Our development regarding the characteristics of the geometric phase is crucial for understanding the topological features in nanowire oscillations.
Introduction
Mechanical vibrations of the smallest resonators, such as carbonnanotubebased (CNTbased) nanowires [1–3], semiconducting nanowires [4], graphenes [5], and levitated particles [6], have been a main research subject in the nanoscience community for over a decade. Active researches regarding electromechanical oscillations of nanowire resonators driven by an external periodic force have been performed in both theoretical and experimental spheres. In particular, CNTbased nanowire resonators have attracted considerable interest as nanoscale mechanical devices due to their extraordinary sensitivities with highquality factors to a small perturbation from surroundings. Suspended CNTbased nanowire resonators are promising candidates for apparatuses measuring a wide range of physical quantities, such as EM waves [2], small forces [7], masses [8], temperatures [9], and noises [10].
Analyses of the quantal phase evolution in nanowire oscillations are required for elucidating underlying features of the system theoretically. Regarding quantum vibrational states of the CNTbased nanowire resonators [11], the geometric phase [12] as well as the usual dynamical phase emerges as a supplementary evolution of the phase. The geometric phase [12] is an anholonomic of a quantum state which can be applicable in diverse fields of physics. Analyses of the geometric phase can be potentially adopted in characterizing nano properties of nanowires, such as the resonance profiles [13, 14], strong quantum vibrations [15, 16], strain relaxation mechanisms [17, 18], the emergence of Dirac magnetoplasmons [19], and the topology of AharonovBohm oscillations [20].
The study of the geometric phase associated with nonadiabatic dynamics may provide an insight for nanomechanical systems, which is necessary for the advancement of accurate simulation techniques [21]. The preparation, manipulation, and detection of quantum states are important factors in quantum technologies. The aim of the present research is to shed light on time behaviors of the geometric phase that takes place in quantum states of nanowire oscillations. To understand the mechanism of CNTbased nanowire vibrations, we will investigate the time evolution of the geometric phase in the squeezed state which is a classicallike quantum state like the coherent state. The merit of the squeezed state is that the uncertainty of a quadrature in that state can be reduced substantially at the expense of rising the uncertainty of the other quadrature, while such uncertainty modulation is impossible in the coherent state. In particular, we will analyze the effects of resonance on the geometric phase. Because the resonant energy is significantly different from the energy of the nonresonant state [22, 23], the topological behavior of the wave function is nontrivial and may be considerably deviated from the one in normal situations. The influence of the change of physical parameters and the squeezing parameters on the evolution of the geometric phase will also be rigorously analyzed. The geometric phases are ubiquitous in dynamical systems [24] and can be applied to various modern technologies, such as quantum computation [25], intensity interferometries [26], photonic multitasking [27], quantumsensing protocols [28], and wavestability measurements [29].
The Hamiltonian of the system involves time functions associated with the damping of the system and the external driving force. Hence, the system is a kind of timedependent Hamiltonian systems (TDHSs) of which quantum mechanical problems are extensively studied up to recently. The time function in the Hamiltonian of a TDHS cannot be separated out from the function of canonical variables in most cases, leading the conventional separation of variables method for solving the Schrödinger equation being unavailable. An alternative powerful method developed for overcoming this difficulty is the invariant operator method which has been introduced by Lewis and Riesenfeld [30, 31]. This method is a very useful mathematical tool when we derive quantum solutions of a TDHS. Many quantum mechanical problems described by TDHSs are investigated based on this method. For instance, they include chaotic particlescattering [32], light propagation in timevarying media [33], control of trapped driven electrons [34], and nonclassicality of quantum nanoelectronic circuits [35]. There is a variety of other methods for quantum mechanical treatments of TDHSs, which include unitary transformation method [36], Lie algebraic method [37], and Hamiltonian estimation method [38].
Regarding that the system is a TDHS, we use the invariant operator method in order to obtain quantum solutions of the system. A linear invariant operator which is represented in terms of the annihilation operator will be introduced. While the annihilation and the creation operators are represented in terms of time due to the timedependence of the system, both the coherent and the squeezed states can be obtained using these ladder operators. The geometric phase of the system will be analytically evaluated by utilizing the wave function in the squeezed state. The time evolution of the geometric phase will be analyzed in detail on the basis of its illustrations depicted with diverse choices of parameters.
Methods
To investigate the geometric phase, we first need to setup the classical equation of motion of the nanowire tip. Because the geometric phase appears in the quantum wave evolution of a TDHS, it is necessary to derive wave functions in a specific quantum state that we manage. We will consider the squeezed state as mentioned in the introductory part. The wave functions in the diverse quantum states of a TDHS, including the squeezed state, can be obtained from the invariant operator method.
The equation of motion for the timedependent amplitude x for a bending mode of a suspended carbon nanotube with an effective mass m is given by [1]
where ω_{0} is the resonant angular frequency, Q the quality factor, f_{d} the electrostatic driving force divided by m, η the nonlinear damping coefficient, and β the Duffing parameter. Let us assume for convenience that the displacement of the tip is sufficiently small relative to the CNTwire length. Then, we can neglect the nonlinear terms in Eq. (1), leading to [2]
The Hamiltonian of the system which yields Eq. (2) is given by
where γ=ω_{0}/Q. The classical solution of Eq. (2) is composed of a complementary function X_{c}(t) and a particular solution X_{p}(t), which are given by
where X_{c,0} is a constant, \(\Omega = \sqrt {\omega _{0}^{2}  \gamma ^{2}/4}\), φ is an arbitrary phase, and
The classical solution in the momentum space is given in a similar way, where the complementary function is \(P_{c} (t) = m e^{\gamma t} \dot {X}_{c}(t)\) and the particular solution is \(P_{p} (t) = m e^{\gamma t} \dot {X}_{p}(t)\). To investigate the geometric phase of the system, we first need to derive quantum solutions. Notice that the Hamiltonian of the system given in Eq. (3) is explicitly dependent on time. In order to derive quantum solutions of the system, we use the invariant operator method [30, 31], which is a useful method when we treat such a timevarying system. An invariant operator \(\hat {I}\) of the system can be derived from the Liouvillevon Neumann equation, which is given by \({d \hat {I}}/{d t} = {\partial \hat {I}}/{\partial t} + \left [\hat {I},\hat {H}\right ]/\left (i\hbar \right) = 0\). Hence, from a rigorous evaluation after inserting Eq. (3) into this equation, we have a linear invariant operator [34] of the form
where \(\hat {A}\) is the annihilation operator that is given by
The hermitian adjoint of Eq. (9), \(\hat {A}^{\dagger }\), is the creation operator.
We can express the eigenvalue equation of \(\hat {A}\) as
By evaluating the above equation, we have the expression of the eigenvalue such that
where A(0)=A_{0}e^{−iφ} with
While the coherent state A〉 is the eigenstate of \(\hat {A}\), the squeezed state is the eigenstate of an operator \(\hat {B}\) that is given by
where μ and ν are complex variables that yield the equation
If we write the eigenvalue equation of \(\hat {B}\) in the form
B〉 is the squeezed state. By solving this equation in the configuration space, we have
Thus, the wave function in the squeezed state has been derived as given in Eq. (16). Quantum features of the system can be clarified on the basis of such analytical description of the wave function. For μ=1 and ν=0, Eq. (16) reduces to the wave function in the coherent state, which is the eigenstate of Eq. (10) in the configuration space. The wave function, Eq. (16), will be used in the next section in order to derive the geometric phase in the squeezed state.
Results and Discussion
It is well known that the phase in the quantum wave evolution involves the geometric phase as well as the dynamical phase. The geometric phase was first discovered by Berry in 1984 [12] for a system evolving cyclically with an adiabatic change. According to the adiabatic theorem in quantum mechanics, an instantaneous eigenstate of a quantum state in a cyclic evolution in the parameter space will remain on the same state later, while there is an additional accumulation of the quantum phase which is the Berry phase. A generalization of the Berry phase in a way that it includes nonadiabatic, noncyclic, and/or nonunitary evolution of the quantum system is the geometric phase.
The geometric phase in the squeezed state is given by
The differentiation of the wave function with respect to time in configuration space becomes
where
Further evaluation after inserting Eq. (18) into Eq. (17) gives
where
The last term in g_{5} that contains (μ−μ^{∗})(ν−ν^{∗}) is inadequate as a phase because this is a purely imaginary number. Hence, we now remove this term by choosing at least one of μ and ν as a real value. This remedy can always be done without loss of generality, because only the relative phase between μ and ν has physical meaning rather than their absolute phases.
From the execution of the integration in Eq. (22), we have
where \(\bar {g}_{i}(t)~(i=3,4,5)\) are given by
with
Thus, we have evaluated the full geometric phase in the squeezed state, which is given by Eq. (28) with Eqs. (23), (24), and (29)–(32).
The time evolution of the geometric phase has been illustrated in Figs. 1, 2, 3, and 4. From Fig. 1, we see that the geometric phase oscillates and the envelope of such oscillation increases over time. The increase of the envelope is greater when A_{0} is large. The pattern of the oscillation becomes gradually irregular as the values of μ and ν increase. Moreover, the amplitude of the oscillation becomes large as time goes by.
The squeezing effects in the squeezed state depending on the squeeze parameter c where c=μ/ν has been investigated in ref. [39]. According to the analysis given in ref. [39] (see Fig. 1(a) in ref. [39]), the squeezed state illustrated in Fig. 2, which corresponds to \(c=\sqrt {2}\), is the qsqueezed state at initial time, while that in Fig. 3, which corresponds to \(c=\sqrt {2}\), is the psqueezed state in the same situation. By comparing Figs. 2 and 3 to each other, we can conclude that the geometric phase in the qsqueezed state is nearly the same as that in the psqueezed state.
The effects of γ on the evolution of the geometric phase can be confirmed from Figs. 2 and 3. The geometric phase increases more rapidly when γ is large. By comparing Figs. 2a and 3a with Figs. 2c and 3c, we can confirm that the geometric phase varies somewhat rapidly when ω is greater than the resonance angular frequency.
The time behavior of the geometric phase at or near the resonant state of the system may be of great interest [22, 23]. Figures 2b and 3b show that the geometric phase increases very rapidly when ω is near the resonance angular frequency. This means that the wave function in this situation varies significantly over time, because the magnitude of the geometric phase is related to the time variation of the wave function. As a matter of fact, the amplitude of the wire oscillation is remarkably augmented at the resonance state. By the way, resonance angular frequencies of suspended CNTbased nanowire resonators are not only high but also widely tunable with very highquality factors [3]. For this reason, the vibrational modes of the system will be kept for a long time until they thoroughly damped out [11].
Figure 4 shows that the geometric phase is also affected by the amplitude of the driving force f_{d}. As f_{d} increases, the increment of the geometric phase in time is rapid.
Conclusion
We have investigated the geometric phase in the squeezed state for the system on the basis of quantum dynamics with the Schrödinger equation. Regarding timedependence of the Hamiltonian that describes the system, the invariant operator method has been introduced, which is a potential tool for deriving quantum solutions in the case where the Hamiltonian is described in terms of time. By means of this method, the analytical formula of the geometric phase for the CNTbased nanowire oscillation has been obtained.
A detailed analysis of the phase effects, which is necessary for a theoretical understanding of the mechanical vibrations, has been carried out. Our development of the geometric phase is a fully quantumbased one with rigorous mathematical evaluations. The geometric phase is sensitive to the change of mechanical parameters and exhibits an oscillation in a large number of cases. The influence of the squeezing parameters on the evolution of the geometric phase has also been analyzed. We have confirmed a strong increase of geometric phase accumulation over time near the resonant angular frequency.
Our results illustrate the time behavior of the geometric phase that appears in the vibration of a CNTbased nanowire. The analysis of the geometric phase given in this work is important for understanding not only topological features of the system but dynamical vibrations of other nanowirebased mechanical oscillators as well. In particular, we have developed phase properties of the resonant state, of which clarification is necessary in the application of the system in quantum information technologies and other quantumbased industries [40]. The similar method and framework used in this research can also be extended to other nano systems, such as superconducting FabryPerot resonators [41], nano cantilevers [42], and qubitresonatoratom hybrid systems [43].
Abbreviations
 CNT:

Carbon nanotube
 EM waves:

Electromagnetic waves
 TDHS:

Timedependent Hamiltonian system
References
Willick K, Tang XS, Baugh J (2017) Probing the nonlinear transient response of a carbon nanotube mechanical oscillator. Appl Phys Lett 111(22):223108.
Tadokoro Y, Ohno Y, Tanaka H (2018) Detection of digitally phasemodulated signals utilizing mechanical vibration of CNT cantilever. IEEE Trans Nanotech 17(1):84–92.
Laird EA, Pei F, Tang W, Steele GA, Kouwenhoven LP (2012) A high quality factor carbon nanotube mechanical resonator at 39 GHz. Nano Lett 12(1):193–197.
Sansa M, FernandezRegulez M, San Paulo A, PerezMurano F (2012) Electrical transduction in nanomechanical resonators based on doubly clamped bottomup silicon nanowires. Appl Phys Lett 101(24):243115.
Will M, Hamer M, Muller M, Noury A, Weber P, Bachtold A, Gorbachev RV, Stampfer C, Guttinger J (2017) High quality factor graphenebased twodimensional heterostructure mechanical resonator. Nano Lett 17(10):5950–5955.
Kiesel N, Blaser F, Delic U, Grass D, Kaltenbaek R, Aspelmeyer M (2013) Cavity cooling of an optically levitated submicron particle. Proc Natl Acad Sci USA 110(35):14180–14185.
Moser J, Güttinger J, Eichler A, Esplandiu MJ, Liu DE, Dykman MI, Bachtold A (2013) Ultrasensitive force detection with a nanotube mechanical resonator. Nat Nanotechnol 8(7):493–496.
Chaste J, Eichler A, Moser J, Ceballos G, Rurali R, Bachtold A (2012) A nanomechanical mass sensor with yoctogram resolution. Nat Nanotechnol 7(5):301–304.
Kuo CY, Chan CL, Gau C, Liu CW, Shiau SH, Ting JH (2007) Nano temperature sensor using selective lateral growth of carbon nanotube between electrodes. IEEE Trans Nanotechnol 6(1):63–69.
de Bonis SL, Urgell C, Yang W, Samanta C, Noury A, VergaraCruz J, Dong Q, Jin Y, Bachtold A (2018) Ultrasensitive displacement noise measurement of carbon nanotube mechanical resonators. Nano Lett 18(8):5324–5328.
Wang H, Burkard G (2016) Creating arbitrary quantum vibrational states in a carbon nanotube. Phys Rev B 94(20):205413.
Berry MV (1984) Quantal phase factors accompanying adiabatic changes. Proc Soc R London Ser A 392(1802):45–57.
Jauregui LA, Pettes MT, Rokhinson LP, Shi L, Chen YP (2015) Gate tunable relativistic mass and Berry’s phase in topological insulator nanoribbon field effect devices. Sci Rep 5:8452.
Erlingsson SI, Bardarson JH, Manolescu A (2018) Thermoelectric current in topological insulator nanowires with impurities. Beilstein J Nanotechnol 9:1156–1161.
Zhang C, Liu Y, Yuan X, Wang W, Liang S, Xiu F (2015) Highly tunable Berry pase and abipolar field effect in topological crystalline insulator Pb _{1x} Sn _{x}Se. Nano Lett 15(3):2161–2167.
Safdar M, Wang Q, Mirza M, Wang Z, Xu K, He J (2013) Topological surface transport properties of singlecrystalline SnTe nanowire. Nano Lett 13(11):5344–5349.
Taraci JL, Hÿtch MJ, Clement T, Peralta P, McCartney MR, Drucker J, Picraux ST (2005) Strain mapping in nanowires. Nanotechnology 16(10):2365–2371.
ConesaBoj S, et al (2014) Plastic and elastic strain fields in GaAsSi coreshell nanowires. Nano Lett 14(4):1859–1864.
Iorio P, Perroni CA, Cataudella V (2017) Plasmons in topological insulator cylindrical nanowires. Phys Rev B 95(23):235420.
Gitsu DV, Huber TE, Konopko LA, Nikolaeva AA (2009) Berry’s phase manifestation in AharonovBohm oscillations in single Bi nanowires. J Phys Conf Ser 150(2):022013.
Ryabinkin IG, JoubertDoriol L, Izmaylov AF (2017) Geometric phase effects in nonadiabatic dynamics near conical intersections. Acc Chem Res 50(7):1785–1793.
Rau ARP, Uskov D (2006) Effective Hamiltonians in quantum physics: resonances and geometric phase. Phys Scr 74(2):C31–C36.
Yuen KW, Fung HT, Cheng KM, Chu MC, Colanero K (2003) The quantum mechanical geometric phase of a particle in a resonant vibrating cavity. J Phys A Math Gen 36(44):11321–11332.
Dennis M, Popescu S, Vaidman L (2010) Quantum phases: 50 years of the Aharonov–Bohm effect and 25 years of the Berry phase. J Phys A Math Theor 43(35):350301.
Song C, et al (2017) Continuousvariable geometric phase and its manipulation for quantum computation in a superconducting circuit. Nat Commun 8:1061.
Wadhawan D, Roychowdhury K, Mehta P, Das S (2018) Multielectron geometric phase in intensity interferometry. Phys Rev B 98(15):155113.
Litchinitser NM (2016) Photonic multitasking enabled with geometric phase. Science 352(6290):1177–1178.
Andersson SB (2003) Geometric phases in sensing and control. Doctorial Dissertation, University of Maryland.
Grudzien CJ, Bridges TJ, Jones CKRT (2016) Geometric phase in the Hopf bundle and the stability of nonlinear waves. Physica D 334:4–18.
Lewis Jr HR (1967) Classical and quantum systems with timedependent harmonicoscillatortype Hamiltonians. Phys Rev Lett 18(13):510–512.
Lewis Jr HR, Riesenfeld WB (1969) An exact quantum theory of the timedependent harmonic oscillator and of a charged particle in a timedependent electromagnetic field. J Math Phys 10(8):1458–1473.
Lai YC, Grebogi C (1991) Chaotic scattering in timedependent Hamiltonian systems. Int J Bifurcat Chaos 1(3):667–679.
Choi JR (2010) Interpreting quantum states of electromagnetic field in timedependent linear media. Phys Rev A 82(5):055803.
Abdalla MS, Choi JR (2007) Propagator for the timedependent charged oscillator via linear and quadratic invariants. Ann Phys(N.Y.) 322(12):2795–2810.
Choi JR (2017) Superposition states for quantum nanoelectronic circuits and their nonclassical properties. Int Nano Lett 7(1):69–77.
Choi JR (2004) Unitary transformation of the timedependent Hamilton system for the linear, the Vshape, and the triangular well potentials into the quadratic Hamiltonian system. J Appl Sci 4(4):636–643.
Dong W, Wu R, Wu J, Li C, Tarn TJ (2015) Optimal control of quantum systems with SU(1,1) dynamical symmetry. Control Theory Tech 13(3):211–220.
de Clercq LE, et al (2015) Estimation of a general timedependent Hamiltonian for a single qubit. Nat Commun 7:11218.
Choi JR (2004) The dependency on the squeezing parameter for the uncertainty relation in the squeezed states of the timedependent oscillator. Int J Mod Phys B 18(16):2307–2324.
Hornyak GL, Moore JJ, Tibbals HF, Dutta J (2009) Fundamentals of nanotechnology. CRC Press, Boca Raton.
Kuhr S, et al (2007) Ultrahigh finesse FabryPérot superconducting resonator. Appl Phys Lett 90(16):164101.
Li P, You Z, Cui T (2012) Graphene cantilever beams for nano switches. Appl Phys Lett 101(9):093111.
Yu D, Kwek LC, Amico L, Dumke R (2017) Superconducting qubitresonatoratom hybrid system. Quantum Sci Technol 2(3):035005.
Funding
This research was supported by the Basic Science Research Program of the year 2018 through the National Research Foundation of Korea (NRF) funded by the Ministry of Education (Grant No.: NRF2016R1D1A1A09919503).
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The datasets used and/or analyzed during the current study are available from the corresponding author on reasonable request.
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The authors declare that they have no competing interests.
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JRC proposed the idea of the research. JRC and SJ cowrote the manuscript. The graphics in the text have been prepared by JRC. Both authors read and approved the final manuscript.
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Choi, J., Ju, S. Properties of the Geometric Phase in Electromechanical Oscillations of CarbonNanotubeBased Nanowire Resonators. Nanoscale Res Lett 14, 44 (2019). https://doi.org/10.1186/s1167101928558
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DOI: https://doi.org/10.1186/s1167101928558
Keywords
 Geometric phase
 Nanowire resonator
 Electromechanical oscillation
 Squeezed state
 Invariant operator
 Phase effect