August 28, 2018
Nippon Telegraph and Telephone Corporation
National Institute of Advanced Industrial Science and Technology
Nippon Telegraph and Telephone Corporation (NTT: head office: Chiyoda-ku, Tokyo; president & CEO: Jun Sawada) and the National Institute of Advanced Industrial Science and Technology (AIST: headquarter: Chiyoda-ku, Tokyo; president: Ryoji Chubachi) have developed a novel device technology to control solid-state nuclear magnetic resonance (NMR)*1 with a micromechanical oscillator.
Quantum memory*2 has received much attention in recent quantum technology research for applications to quantum computers, quantum communications, and quantum sensors. Quantum computers are expected to perform ultrafast computation, quantum communications can provide absolutely secure communications protocols, and quantum sensors promise to drastically improve sensor performance. Quantum memory's ability to store quantum superposition states for a long period of time could improve the performance of these quantum technologies. One of the most important candidates for quantum memory is nuclear spin*3 because of its extremely long spin lifetime. NTT and AIST experimentally demonstrated that the NMR frequency in a mechanical oscillator can be controlled by strain induced by its mechanical motion. This method allows us to control the quantum state of a nuclear spin in a desired mechanical element in an integrated array and will play an essential role in the development of solid-state-based quantum memory.
This demonstration was made possible through a collaboration between NTT, which performed device fabrication and measurements, and AIST, which performed data analysis based on precise theoretical modeling. The results were published in “Nature Communications” on August 28, 2018.
This work was partly supported by a MEXT Grant-in-Aid for Scientific Research on Innovative Areas “Science of hybrid quantum systems”.
Nuclear spin is the rotation of an atomic nucleus [Fig. 1(a)], and it shows a precessional motion under a magnetic field [Fig. 1(b)]. Nuclear spin can sustain precessional motion for a long period of time and is expected to be used in various applications, such as quantum memory to store a quantum superposition state and high performance magnetic field sensors. Nuclear magnetic resonance (NMR) is generally used to manipulate the nuclear spin state, where an electromagnetic wave at the NMR frequency is applied under a magnetic field to modify the precessional motion. However, it is hard to use standard NMR techniques for integrated devices because the magnetic field and electromagnetic wave are simultaneously applied to all the devices. Therefore, a novel method to manipulate nuclear spins in individual devices is highly demanded.
The NMR frequency is highly sensitive to the strain applied in a solid, and this property was used to locally manipulate nuclear spins in this experiment. Artificially generating strain at a desired position in a material allows the control of NMR in individual integrated devices. A micromechanical oscillator*4 fabricated using state-of-the-art nanofabrication technology was used to locally generate large strain, and the NMR frequency was controlled by oscillating strain by the resonator's mechanical motion. As a result, we observed not only the modulation of the NMR frequency but also a novel kind of NMR called sideband*5 resonance, which were induced by the mixed effect of electromagnetic waves and oscillating strain.
The mechanical oscillator [Fig. 2(a)] has the shape of a doubly clamped beam*6 and was fabricated by processing GaAs, which is a piezoelectric*7 semiconductor. The mechanical oscillation can be electrically induced through the piezoelectric effect. The motion generates periodic strain at the clamping point [Fig. 2(b)] and modifies the dynamics of nuclear spins in the strained region. In the experiments, we observed not only a shift in the NMR frequency (Fig. 3) but also sideband resonances, where the resonance was confirmed also at two shifted frequencies: blue- and red-detuned from the original NMR frequency (Fig. 4). The theoretical calculation taking into account the influence of oscillating strain on nuclear spin dynamics showed good agreement with the experimental results, proving that the observed phenomenon can be well explained by the effect of mechanical oscillation.
The mechanical oscillators are fabricated using semiconductor nanofabrication technology and can be integration on a tiny semiconductor chip. We can utilize this scheme as a novel platform to integrate quantum memories and sensors by demonstrating nuclear spin control in individual arrayed devices.
(a) A schematic drawing of an atom. The atom is composed of an atomic nucleus at its center and electrons orbiting it. The nucleus has its own rotational motion like the earth and moon. The rotational motion is called nuclear spin. (b) Precession of a nuclear spin. The axis of nuclear spin shows precessional motion when a magnetic field is applied along the tilt direction. The precessional motion of nuclear spin has a proper frequency specified by the kind of atomic nucleus, so that the frequency measurement through nuclear magnetic resonance (NMR) can identify the materials.
(a) An electron microscope false-color image of a micro-mechanical oscillator used to apply strain on nuclear spins. The mechanical flexural motion is induced by applying an alternate voltage on the surface electrode (shown yellow). (b) A schematic drawing showing the generation of strain. The flexural motion of a 50µm-long beam induces periodic strain on the clamping area. (c) A magnified schematic image of strain area of the oscillator. An antenna of electromagnetic wave generates an oscillating magnetic field and induces nuclear magnetic resonance. The change in the nuclear spin state is detected as the change in resistance.
One of the three peaks in the NMR spectrum of 75As (indicated by red circles) shows the frequency shift with the increase of mechanical oscillation amplitude (X0). Other two peaks (blue squares and purple triangles) are not shifted. The theoretical calculation showed good agreement with the experimental results.
Nuclear magnetic resonance was observed also at the sum and difference frequencies (f NMR + f M and f NMR - f M ) of those of original NMR (f NMR) and mechanical resonance (f M) by a mixing effect between oscillating electromagnetic wave and oscillating strain. The new resonance is called sideband resonance, allowing nuclear spin control in individual arrayed devices. (In contrast to Fig. 3, the NMR of 69Ga is shown as the example.)
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