High Speed Integrated Circuits for High Speed Coherent Optical Communications

With the development of (sub) THz transistor technologies, high speed integrated circuits up to sub-THz frequencies are now feasible. These high speed and wide bandwidth ICs can improve the performance of optical components, coherent optical fiber communication, and imaging systems. In current optical systems, electrical ICs are used primarily as driving amplifiers for optical modulators, and in receiver chains including TIAs, AGCs, LPFs, ADCs and DSPs. However, there are numerous potential applications in optics using high speed ICs, and different approaches may be required for more efficient, compact and flexible optical systems.This dissertation will discuss three different approaches for optical components and communication systems using high speed ICs: a homodyne optical phase locked loop (OPLL), a heterodyne OPLL, and a new WDM receiver architecture.The homodyne OPLL receiver is designed for short-link optical communication systems using coherent modulation for high spectral efficiency. The phase-locked coherent receiver can recover the transmitted data without requiring complex back-end digital signal processing to recover the phase of the received optical carrier. The main components of the homodyne OPLL are a photonic IC (PIC), an electrical IC (EIC), and a loop filter. One major challenge in OPLL development is loop bandwidth; this must be of order 1 GHz in order for the loop to adequately track and suppress the phase fluctuations of the locked laser, yet a 1 GHz loop bandwidth demands small (<100 ps) propagation delays if the loop is to be stable. Monolithic integration of the high-speed loop components into one electrical and one photonic IC decreases the total loop delay. We have designed and demonstrated an OPLL with a compact size of 10 × 10 mm2, stably operating with a loop bandwidth of 1.1 GHz, a loop delay of 120 ps, a pull-in time of 0.55 μs and lock time of <10 ns. The coherent receiver can receive 40 Gb/s BPSK data with a bit error rate (BER) of <10-7, and operates up to 35 Gb/s with BER 10-12.The thesis also describes heterodyne OPLLs. These can be used to synthesize optical wavelengths of a broad bandwidth (optical wavelength synthesis) with narrow linewidth and with fast frequency switching. There are many applications of such narrow linewidth optical signal sources, including low phase noise mm-wave and THz-signal sources, wavelength-division-multiplexed optical transmitters, and coherent imaging and sensor systems. The heterodyne OPLL also has the same stability issues (loop delay and sensitivity) as the homodyne OPLL. In the EIC, a single sideband mixer operating using digital design principles (DSSBM) enables precisely controlled sweeping of the frequency of the locked laser, with control of the sign of the frequency offset. The loop's phase and frequency difference detector (PFD) uses digital design techniques to make the OPLL loop parameters only weakly sensitive to optical signal levels or optical or electrical component gains. The heterodyne OPLL operates stably with a loop bandwidth of 550 MHz and loop delay of <200 ps. An initial OPLL design exhibited optical frequency (wavelength) synthesis from -6 GHz to -2 GHz and from 2 GHz to 9 GHz. An improved OPLL reached frequency tuning up to 25 GHz. The homodyne OPLL exhibits -110 dBc/Hz phase noise at 10 MHz offset and -80 dBc/Hz at 5 kHz offset.Finally, the thesis describes a new WDM receiver architecture using broadband electrical ICs. In the proposed WDM receiver, a set of received signals at different optical wavelengths are mixed against a single optical local oscillator. This mixing converts the WDM channels to electrical signals in the receiver photocurrent, with each WDM signal being converted to an RF sub-carrier of different frequency. An electrical IC then separately converts each sub-carrier signal to baseband using single-sideband mixers and quadrature local oscillators. The proposed receiver needs less complex hardware than the arrays of wavelength-sensitive receivers now used for WDM, and can readily adjust to changes in the WDM channel frequencies. The proposed WDM receiver concept was demonstrated through several system experiments. Image rejection of greater than 25 dB, adjacent channel suppression of greater than 20 dB, operation with gridless channels, and six-channel data reception at a total 15 Gb/s (2.5 Gb/s BPSK × 6-channels) were demonstrated

The effects of Thomson scattering and chemical mixing on early-time light curves of double peaked type IIb supernovae

Previous numerical simulations of double-peaked SNe IIb light curves have demonstrated that the radius and mass of the hydrogen-rich envelope of the progenitor star can significantly influence the brightness and timescale of the early-time light curve around the first peak. In this study, we investigate how Thomson scattering and chemical mixing in the SN ejecta affect the optical light curves during the early stages of the SNe IIb using radiation hydrodynamics simulations. By comparing the results from two different numerical codes (i.e., \stella{} and \snec{}), we find that the optical brightness of the first peak can be reduced by more than a factor of 3 due to the effect of Thomson scattering that causes the thermalization depth to be located below the Rosseland-mean photosphere, compared to the corresponding case where this effect is ignored. We also observe a short-lived plateau-like feature lasting for a few days in the early-time optical light curves of our models, in contrast to typical observed SNe IIb that show a quasi-linear decrease in optical magnitudes after the first peak. A significant degree of chemical mixing between the hydrogen-rich envelope and the helium core in SN ejecta is required to reconcile this discrepancy between the model prediction and observation. Meanwhile, to properly reproduce the first peak, a significant mixing of \nifs{} into the hydrogen-rich outermost layers should be restricted. Our findings indicate that inferring the SN IIb progenitor structure from a simplified approach that ignores these two factors may introduce substantial uncertainty.Comment: 28 pages, 21 figures, accepted for Ap

Ectopic adrenal gland tissue in the left ovary of an elderly woman: a case report

Ectopic adrenal gland in the ovary is very rare case, and even more rarer in older women. We reported a case of ectopic adrenal tissue as an incidental finding in left ovary from a 68-year-old woman. She presented with bearing down sensation due to uterine prolapse for 5 years. Upon physical examination, uterine prolapse grade III, cystocele, and rectocele were observed. Ultrasonography findings showed 0.69 cm intramural myoma, and no specific findings were found in the bilateral adnexae. She underwent a total laparoscopic hysterectomy, bilateral salpingo-oophorectomy, and anterior-posterior repair. The final pathologic diagnosis of the case was ectopic adrenal gland tissue in the left ovary and uterine leiomyoma. No eventful reactions were observed during hospitalization and after discharge. Although ectopic adrenal gland rarely occurs in elderly women and in the pelvic ovaries, it has a risk of neoplastic transformation and accompanying germ cell tumor and sex cord tumor. Hence, if the ectopic adrenal gland tissue is suspected during surgery, the tissue should be removed. Additionally, by closely examining the contralateral ovary, determining whether other lesions are suspected is necessary. If the other lesions including germ cell tumor or sex cord tumor are suspected, a biopsy of the contralateral ovarian tissue should be performed. Thus, gynecologists must have knowledge about ectopic adrenal gland tissues

Comparative Neutronics Analysis of DIMPLE S06 Criticality Benchmark with Contemporary Reactor Core Analysis Computer Code Systems

A high-leakage core has been known to be a challenging problem not only for a two-step homogenization approach but also for a direct heterogeneous approach. In this paper the DIMPLE S06 core, which is a small high-leakage core, has been analyzed by a direct heterogeneous modeling approach and by a two-step homogenization modeling approach, using contemporary code systems developed for reactor core analysis. The focus of this work is a comprehensive comparative analysis of the conventional approaches and codes with a small core design, DIMPLE S06 critical experiment. The calculation procedure for the two approaches is explicitly presented in this paper. Comprehensive comparative analysis is performed by neutronics parameters: multiplication factor and assembly power distribution. Comparison of two-group homogenized cross sections from each lattice physics codes shows that the generated transport cross section has significant difference according to the transport approximation to treat anisotropic scattering effect. The necessity of the ADF to correct the discontinuity at the assembly interfaces is clearly presented by the flux distributions and the result of two-step approach. Finally, the two approaches show consistent results for all codes, while the comparison with the reference generated by MCNP shows significant error except for another Monte Carlo code, SERPENT2open0

Axial strain dependence of all-fiber acousto-optic tunable filters

We report the axial strain dependence of two types of all-fiber acousto-optic tunable filters based on flexural and torsional acoustic waves. Experimental observation of the resonant wavelength shift under applied axial strain could be explained by theoretical consideration of the combination of acoustic and optical effects. We discuss the possibility of suppressing the strain effect in the filters, or conversely, the possibility of using the strain dependence for wavelength tuning or strain sensors