Observation of Hysteretic Transport Due to Dynamic Nuclear Spin Polarization in a GaAs Lateral Double Quantum Dot

We report a new transport feature in a GaAs lateral double quantum dot that emerges only for magnetic field sweeps and shows hysteresis due to dynamic nuclear spin polarization (DNP). This DNP signal appears in the Coulomb blockade regime by virtue of the finite inter-dot tunnel coupling and originates from the crossing between ground levels of the spin triplet and singlet extensively used for nuclear spin manipulations in pulsed gate experiments. The unexpectedly large signal intensity is suggestive of unbalanced DNP between the two dots, which opens up the possibility of controlling electron and nuclear spin states via DC transport.Comment: 5 pages, 4 figure

Stimulated emission from multilayer graphene

Monolayer graphene absorbs $\sim$ 2.3 percent of the incident visible light. This "small" absorption was used to emphasize visual transparency of graphene, but in fact it means that multilayer graphene absorbs sizable fraction of incident light, which causes non-negligible fluorescence. In this paper, we study the light emission properties of multilayer graphene composed of tens to hundreds of layers, because these are informative materials having interesting optical properties correlated closely with fluorescence. For example, it was recently predicted that 87-layer graphene absorbs infrared light at maximum efficiency and 20-layer graphene on silicon substrates exhibits zero reflectance (a total absence of backscattering) at a specific visible light wavelength. By modeling light emissions from multilayer graphene using a transfer matrix method, we could quantitatively explain the measured reflectivity from multilayer graphene on silicon substrates. We found sizable corrections, that cannot be classified as incoherent light emissions, to the reflectance of visible light. The new component originates from stimulated emission caused by absorption at each graphene layer, and it is a coherent sum over the amplitudes coming from all graphene layers with a common phase shift of $\pi$ relative to the incident light. The coherent corrections to the reflectance become dominant for samples thicker than 40-layers and thinner than 160-layers. Multilayer graphene thus functions as a partial coherent light source of various wavelengths and it may have surface-emitting laser applications.Comment: 9 pages, 9 figure

Ultra-Precise Frequency Conversion Using an Electro-Optic-Modulation Frequency Comb

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Optical-referenceless optical frequency counter with twelve-digit absolute accuracy

Abstract A simpler and more accurate measurement of absolute optical frequencies (AOFs) is very important for optical communications and navigation systems. To date, an optical reference has been needed for measuring AOFs with twelve-digit accuracy because of the difficulty in measuring them directly. Here, we focus on an electro-optics-modulation comb that can bridge the vast frequency gap between photonics and electronics. We demonstrate an unprecedented method that can directly measure AOFs to an accuracy of twelve digits with an RF frequency counter by simply delivering a frequency-unknown laser into an optical phase modulator. This could open up a new horizon for optical-referenceless optical frequency metrology. Our method can also simultaneously achieve a 100-fold phase-noise reduction in a conventional signal generator. This corresponds to an increase in the transmission speed of wireless communications of by about seven times

Sub‐30‐fs fibre‐coupled electro‐optic modulation comb at 1.5 μm with a 25‐GHz repetition rate

Abstract The generation of a 24‐fs fibre‐coupled electro‐optic‐modulation (EO) comb at 1.5 μm with a 25‐GHz repetition rate, which is the shortest pulse, is demonstrated. The authors also generated a 2/3‐octave spanning supercontinuum spectrum using precise dispersion‐controlled silicon nitride waveguides. This method can open new horizons to generate a compact and robust carrier‐envelope‐offset‐locked EO comb