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Journal articles on the topic 'Optical cycle'

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1

Liu, Songyang, Rongqing Tan, Wenning Xu, Fangjin Ning, and Zhiyong Li. "Double-Cycle Alternating-Flow Diode Pumped Potassium Vapor Laser." Photonics 11, no. 5 (2024): 391. http://dx.doi.org/10.3390/photonics11050391.

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A novel double-cycle alternating-flow diode-pumped potassium vapor laser is proposed, theoretically modeled and simulated. The results show that the optical-to-optical efficiency of the laser increases with increasing gas flow rates, although at high flow rates the rate of increase in efficiency decreases. The optical-to-optical efficiency reaches 74.8% at a pump power density of 30 kW/cm2 and a gas flow rate of 50 m/s. The optical-to-optical efficiency of the laser is greater with a narrow linewidth pump and high buffer gas pressure. The optical-to-optical efficiency of a flow gas cell is hig
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2

Leblond, H., and D. Mihalache. "Few-optical-cycle dissipative solitons." Journal of Physics A: Mathematical and Theoretical 43, no. 37 (2010): 375205. http://dx.doi.org/10.1088/1751-8113/43/37/375205.

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3

Poppe, A., R. Holzwarth, A. Apolonski, et al. "Few-cycle optical waveform synthesis." Applied Physics B 72, no. 3 (2001): 373–76. http://dx.doi.org/10.1007/s003400000526.

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4

Wei, Yue, Kai Xu, Yuling Jiang, Heming Zhao, and Gangxiang Shen. "Optimal design for $$p$$ p -Cycle-protected elastic optical networks." Photonic Network Communications 29, no. 3 (2015): 257–68. http://dx.doi.org/10.1007/s11107-015-0490-6.

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5

Altrock, Richard C. "Variations of Coronal Radiations at Optical Wavelengths." International Astronomical Union Colloquium 143 (1994): 172–81. http://dx.doi.org/10.1017/s0252921100024672.

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This paper reviews observations of the variation over long and short time scales of solar coronal flux as observed from ground-based optical observatories. This includes data from Fe X, Fe XIV, Ca XV and the white-light electron corona. The various parameters are compared and contrasted as indicators of global coronal structure and output. The overall envelope of Ca XV minimizes before and during sunspot minimum, begins its slow rise in phase with the solar cycle, but maximizes late with strong 150-day oscillations resulting in values of zero at the local minima. Within the sensitivity of the
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6

Jiménez-Galán, Álvaro, Rui E. F. Silva, Olga Smirnova, and Misha Ivanov. "Sub-cycle valleytronics: control of valley polarization using few-cycle linearly polarized pulses." Optica 8, no. 3 (2021): 277. http://dx.doi.org/10.1364/optica.404257.

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7

Fang Shaobo, 方少波, and 魏志义 Wei Zhiyi. "Sub-Optical-Cycle Coherent Waveform Synthesis." Acta Optica Sinica 39, no. 1 (2019): 0126006. http://dx.doi.org/10.3788/aos201939.0126006.

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8

Shen, Yunfeng, Baicheng Zhang, ZhangYuan Chen, Wanyi Gu, and Anshi Xu. "Leakage cycle in WDM optical networks." Electronics Letters 34, no. 20 (1998): 1961. http://dx.doi.org/10.1049/el:19981352.

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9

Zhao, Taifei. "Optimal capacity assignment for p-cycle in survivable optical mesh networks." Optical Engineering 45, no. 12 (2006): 125005. http://dx.doi.org/10.1117/1.2404917.

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10

Liang, Zhongcheng, Hai Ming, Pei Wang, Jiangying Zhang, Jianping Xie, and Qijing Zhang. "Nonlinearly optical–optical isomerization cycle in azobenzene liquid crystal polymers." Journal of Applied Physics 90, no. 12 (2001): 5866–70. http://dx.doi.org/10.1063/1.1415362.

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11

Borovik, Aleksandr, and Anton Zhdanov. "LOW-POWER SOLAR FLARES OF OPTICAL AND X-RAY WAVELENGTHS FOR SOLAR CYCLES 21–24." Solar-Terrestrial Physics 6, no. 3 (2020): 16–22. http://dx.doi.org/10.12737/stp-63202002.

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Using data obtained in optical and X-ray wavelengths, we have analyzed solar flare activity for cycles 21–24. Over the last three cycles, solar activity is shown to decrease significantly. As compared to solar cycle 21 (the most active over the last 50 years), in cycle 24 2–4-class large optical flares are 4.4 times rarer; 1-class flares, 8.2 times; and S-class small flares, 4.1 times. The number of X-class flares decreased 3.7 times; M-class flares, 3.2 times. This confirms that secular solar activity trends affect peak values of 11-year cycles. It is shown that optical low-power flares can b
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12

Ze Hao, Jing Li, Chuangye Wang, and Jin Yuan. "Performance study of optical triangular-shaped pulse generation with full duty cycle." Chinese Optics Letters 15, no. 11 (2017): 110601. http://dx.doi.org/10.3788/col201715.110601.

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13

Kong, Fanqi, Hugo Larocque, Ebrahim Karimi, P. B. Corkum, and Chunmei Zhang. "Generating few-cycle radially polarized pulses." Optica 6, no. 2 (2019): 160. http://dx.doi.org/10.1364/optica.6.000160.

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14

Liang, Zhihe, and Chunli Xie. "On DRC-cycle covering in optical networks." Journal of High Speed Networks 20, no. 1 (2014): 41–53. http://dx.doi.org/10.3233/jhs-140486.

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15

Mir, Mustafa, Zhuo Wang, Zhen Shen, et al. "Optical measurement of cycle-dependent cell growth." Proceedings of the National Academy of Sciences 108, no. 32 (2011): 13124–29. http://dx.doi.org/10.1073/pnas.1100506108.

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16

Poppe, A., R. Holzwarth, A. Apolonski, et al. "Erratum to: Few-cycle optical waveform synthesis." Applied Physics B 72, no. 8 (2001): 977. http://dx.doi.org/10.1007/s003400100602.

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17

VILLORESI, P., P. BARBIERO, L. POLETTO, et al. "Study of few-optical-cycles generation of high-order harmonics." Laser and Particle Beams 19, no. 1 (2001): 41–45. http://dx.doi.org/10.1017/s0263034601191068.

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The high-order harmonic generation process was studied using laser pump pulses of different duration, down to 7 fs. The time profile of this kind of pulse corresponds to a few optical cycles at the fundamental frequency, and therefore a cycle-to-cycle variation of the maximum amplitude occurs. These facts violate the adiabatic approximation of the generation process, giving rise to new aspects of the physical process. The comparison of results with pulses in the two regimes are reported and discussed. The modeling of the complete generation and propagation process in three dimensions is also p
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18

Song, Li Mei, Guang Xin Xing, Peng Qiang Wang, Jiang Tao Xi, and Qing Hua Guo. "A 3D Measurement Method Based on Three Frequencies PSP." Applied Mechanics and Materials 701-702 (December 2014): 471–74. http://dx.doi.org/10.4028/www.scientific.net/amm.701-702.471.

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This paper proposes a method of global phase unwrapping used in multi-frequency three-dimensional (3D) measurements. In this method, three kinds of optical information which change in accordance with trigonometric function (sine or cosine) to the objects. The optical information cycles is P1, P2 and P3. Each waveform should 4-8 steps phase shifts. Then, calculate the phase value of each cycle. The composited phase value of two cycles and the final composited phase value of three cycles are calculated by image shift of each cycle. Finally, calculate the global phase value of each cycle based on
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19

Borovik, Aleksandr, and Anton Zhdanov. "LOW-POWER SOLAR FLARES OF OPTICAL AND X-RAY WAVELENGTHS FOR SOLAR CYCLES 21–24." Solnechno-Zemnaya Fizika 6, no. 3 (2020): 18–25. http://dx.doi.org/10.12737/szf-63202002.

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Using data obtained in optical and X-ray wavelengths, we have analyzed solar flare activity for cycles 21–24. Over the last three cycles, solar activity is shown to decrease significantly. As compared to solar cycle 21 (the most active over the last 50 years), in cycle 24 2–4-class large optical flares are 4.4 times rarer; 1-class flares, 8.2 times; and S-class small flares, 4.1 times. The number of X-class flares decreased 3.7 times; M-class flares, 3.2 times. This confirms that secular solar activity trends affect peak values of 11-year cycles. It is shown that optical low-power flares can b
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20

Ridente, Enrico, Matthew Weidman, Mikhail Mamaikin, Clemens Jakubeit, Ferenc Krausz, and Nicholas Karpowicz. "Hybrid phase-matching for optical parametric amplification of few-cycle infrared pulses." Optica 7, no. 9 (2020): 1093. http://dx.doi.org/10.1364/optica.395265.

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21

Fananto, Shokhib Zaky, and Samiaji Samiaji. "APPLICATION OF PROBLEM-BASED LEARNING (PBL) MODEL TO IMPROVE THE ACTIVITY OF GRADE VIII STUDENTS IN THE LIGHT AND OPTICAL SYSTEM LEARNING MATERIAL." Jurnal Pembelajaran Sains 6, no. 2 (2022): 99. http://dx.doi.org/10.17977/um033v6i2p99-102.

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Learning based on actual problems experienced by students using problem-based learning models is believed to increase student participation in identifying problems and student activity in solving problems. This study aimed to increase the activeness of class VIII students in the material of light and optical instruments. The subjects of this study were 32 class VIII A students of SMPN 1 Karanggeneng, Lamongan. The study was conducted in the pre-, cycle I, and cycle II stages. Data collection techniques were carried out using activeness observation techniques, cycles I and II tests, and documen
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22

Beetar, John E., M. Nrisimhamurty, Tran-Chau Truong, et al. "Multioctave supercontinuum generation and frequency conversion based on rotational nonlinearity." Science Advances 6, no. 34 (2020): eabb5375. http://dx.doi.org/10.1126/sciadv.abb5375.

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The field of attosecond science was first enabled by nonlinear compression of intense laser pulses to a duration below two optical cycles. Twenty years later, creating such short pulses still requires state-of-the-art few-cycle laser amplifiers to most efficiently exploit “instantaneous” optical nonlinearities in noble gases for spectral broadening and parametric frequency conversion. Here, we show that nonlinear compression can be much more efficient when driven in molecular gases by pulses substantially longer than a few cycles because of enhanced optical nonlinearity associated with rotatio
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23

Retnani, Dewi Ria, Rina Royani, Christopher Beccles, and Abderrachid Afras. "Improving Science Learning Outcomes on Light and Optical Instruments Through Visual Methods in Junior High Schools." Schrödinger: Journal of Physics Education 5, no. 1 (2024): 32–38. http://dx.doi.org/10.37251/sjpe.v5i1.883.

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Purpose of the study: to improve science learning outcomes about light and optical devices through visual methods (learning by observing and describing) in class VIII junior high school students.
 Methodology: This type of research is classroom action research which is carried out in two cycles, namely cycle I and cycle II, each cycle contains planning, implementation, observation and reflection. The data collection method includes tests in the form of questions. Data analysis was carried out by calculating the achievement of learning outcomes for each cycle with an increase in classical
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24

Weigand, R. "Titanium:sapphire laser oscillator delivering two-optical-cycle pulses." Optica Pura y Aplicada 46, no. 2 (2013): 105–10. http://dx.doi.org/10.7149/opa.46.2.105.

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25

Bartels, Randy, Sterling Backus, Gleb Vdovin, Ivan P. Christov, Margaret M. Murnane, and Henry C. Kapteyn. "Sub-Optical-Cycle Coherent Control In Nonlinear Optics." Optics and Photonics News 11, no. 12 (2000): 23. http://dx.doi.org/10.1364/opn.11.12.000023.

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26

Sazonov, S. V. "Few-Cycle Optical Pulses in the Gain Media." Journal of Physics: Conference Series 1283 (July 2019): 012013. http://dx.doi.org/10.1088/1742-6596/1283/1/012013.

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27

Seunarine, K., N. Gadegaard, M. O. Riehle, and C. D. W. Wilkinson. "Optical heating for short hot embossing cycle times." Microelectronic Engineering 83, no. 4-9 (2006): 859–63. http://dx.doi.org/10.1016/j.mee.2005.12.026.

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28

Sansone, G., E. Benedetti, C. Vozzi, S. Stagira, and M. Nisoli. "Attosecond metrology in the few-optical-cycle regime." New Journal of Physics 10, no. 2 (2008): 025006. http://dx.doi.org/10.1088/1367-2630/10/2/025006.

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29

Sokolov, A. V. "Single-cycle optical pulses synchronized with molecular oscillations." Applied Physics B: Lasers and Optics 77, no. 2-3 (2003): 343–47. http://dx.doi.org/10.1007/s00340-003-1232-5.

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30

Menailava, D. N., and M. B. Shundalau. "Optical Cycle Modelling for RbYb and CsYb Molecules." Journal of Applied Spectroscopy 84, no. 4 (2017): 543–48. http://dx.doi.org/10.1007/s10812-017-0508-1.

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31

Manzoni, Cristian, Oliver D. Mücke, Giovanni Cirmi, et al. "Coherent pulse synthesis: towards sub-cycle optical waveforms." Laser & Photonics Reviews 9, no. 2 (2015): 129–71. http://dx.doi.org/10.1002/lpor.201400181.

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32

Szigeti, János, Ricardo Romeral, Tibor Cinkler, and David Larrabeiti. "P-cycle Protection in multi-domain optical networks." Photonic Network Communications 17, no. 1 (2008): 35–47. http://dx.doi.org/10.1007/s11107-008-0141-2.

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33

Chia, Shih-Hsuan, Giovanni Cirmi, Shaobo Fang, Giulio M. Rossi, Oliver D. Mücke, and Franz X. Kärtner. "Two-octave-spanning dispersion-controlled precision optics for sub-optical-cycle waveform synthesizers." Optica 1, no. 5 (2014): 315. http://dx.doi.org/10.1364/optica.1.000315.

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34

Flender, Roland, Adam Borzsonyi, and Viktor Chikan. "The role of asymmetry in few-cycle, mid-IR pulses during THz pulse generation." Journal of Optics 24, no. 4 (2022): 045502. http://dx.doi.org/10.1088/2040-8986/ac5289.

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Abstract The efficiency of terahertz (THz) pulse generation improves at longer driving wavelengths. For this reason, the use of mid-infrared (MIR) sources is more advantageous compared to visible or near-infrared systems. In this work, we investigate how single-color and two-color schemes of MIR pulses with few-cycle pulse durations compare in producing THz pulses. The results reveal that as the duration of the driving pulses decreases, the second harmonic generation crystal can be omitted from the system. Our numerical study pinpointed three regions where the optimal pulse parameters are fund
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35

Toe, May Zin, Wai Kian Tan, Hiroyuki Muto, Go Kawamura, Atsunori Matsuda, and Swee-Yong Pung. "Evaluation of the Structural, Optical and Photoconversion Efficiency of ZnO Thin Films Prepared Using Aerosol Deposition." Applied Sciences 13, no. 3 (2023): 1905. http://dx.doi.org/10.3390/app13031905.

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As compared to other deposition techniques such as atomic layer deposition, chemical vapour deposition and sputtering, aerosol deposition (AD) is a simple and cost-effective technique to produce ZnO thin films. In this work, the effect of deposition cycles on the structural, optical, and photo-conversion efficiency (PCE) of dye sensitized solar cells of ZnO thin films deposited by AD (AZ) was systematically studied. The structural, optical, and PCE% of two-cycle deposited ZnO thin film (AZ-II) exhibited the highest performance. Further increment in deposition cycle caused deterioration in the
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36

Syukria, Mila, and Rani Oktavia. "IMPROVING STUDENTS’ LEARNING OUTCOMES THROUGH PROBLEM-BASED LEARNING MODEL ON LIGHT AND OPTICAL DEVICES TOPIC." SEMESTA: Journal of Science Education and Teaching 7, no. 2 (2024): 83–96. https://doi.org/10.24036/semesta/vol7-iss2/513.

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This study aims to determine the improvement of science learning outcomes of students of SMP Negeri 25 Padang through the application of the Problem Based Learnig (PBL) learning model. The subjects in this study are 33 students. This research is a Class Action Research that refers to the Kemmis and Taggart models. This research was carried out in 3 cycles consisting of planning stages, implementation of actions, observation, and reflection. Research data in the form of cognitive learning outcomes were taken using multiple-choice test and description techniques. The learning outcomes in cycle I
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37

Huang, J., M. Pang, X. Jiang, et al. "Sub-two-cycle octave-spanning mid-infrared fiber laser." Optica 7, no. 6 (2020): 574. http://dx.doi.org/10.1364/optica.389143.

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38

Brida, D., M. Marangoni, C. Manzoni, S. De Silvestri, and G. Cerullo. "Two-optical-cycle pulses in the mid-infrared from an optical parametric amplifier." Optics Letters 33, no. 24 (2008): 2901. http://dx.doi.org/10.1364/ol.33.002901.

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39

So, I. A., A. B. Plachenov, and A. P. Kiselev. "Unidirectional Single-Cycle and Sub-Cycle Pulses." Optics and Spectroscopy 128, no. 12 (2020): 2000–2001. http://dx.doi.org/10.1134/s0030400x20121054.

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40

Alves, Joana, Hugo Pires, Celso P. João, and Gonçalo Figueira. "Multi-mJ Scaling of 5-Optical Cycle, 3 µm OPCPA." Photonics 8, no. 11 (2021): 503. http://dx.doi.org/10.3390/photonics8110503.

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We present the design of an ultrafast optical parametric chirped pulse amplifier (OPCPA) operating at 3 µm yielding few-cycle pulses and multi-mJ output energy. This design demonstrates that with a configuration of a single crystal or combination of crystals (KTA and MgO:LN) it is possible to achieve output energies above the mJ with sufficient bandwidth to allow compression to just 5-optical cycles. Here, we consider a 1 µm mJ-level picosecond chirped pulse amplifier (CPA), a typical pumping source for this type of non-linear amplifiers. Compression with a simple bulk material enables reachin
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41

Georgoulias, A. K., and K. A. Kourtidis. "On the aerosol weekly cycle spatiotemporal variability over Europe." Atmospheric Chemistry and Physics 11, no. 10 (2011): 4611–32. http://dx.doi.org/10.5194/acp-11-4611-2011.

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Abstract. In this work, we focus on the spatial and temporal variability of the aerosol weekly cycle over Europe as these were recorded from TERRA MODIS and AQUA MODIS satellite instruments. Aerosol optical properties retrieved from MODIS TERRA (February 2000–February 2009) and AQUA (July 2002–December 2008) were used to produce an aerosol weekly cycle index. First, the general aerosol optical depth (AOD550 nm) weekly patterns were defined at a 1° × 1° resolution using the satellite-based index and six regions of interest were selected. To remove episodic dust transport events, two different a
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42

Quaas, J., O. Boucher, A. Jones, J. Kieser, and H. Joos. "Exploiting the weekly cycle as observed over Europe to analyse aerosol indirect effects in two climate models." Atmospheric Chemistry and Physics Discussions 9, no. 3 (2009): 11269–85. http://dx.doi.org/10.5194/acpd-9-11269-2009.

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Abstract. A weekly cycle in aerosol pollution and meteorological quantities is observed over Europe. In the present study we exploit this effect to analyse aerosol-cloud-radiation interactions. A weekly cycle is imposed on anthropogenic emissions in two general circulation models that include parameterizations of aerosol cycles and cloud microphysics. It is found that the simulated weekly cycles in sulfur dioxide, sulfate, and aerosol optical depth in both models agree reasonably well with the observed ones indicating model skill in simulating the aerosol cycle. A distinct weekly cycle in clou
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43

Yamashita, Mikio. "Generation of Single-Cycle Optical Pulses and its Prospect." Review of Laser Engineering 33, Supplement (2005): S3—S4. http://dx.doi.org/10.2184/lsj.33.s3.

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44

Wang Yanhai, 王艳海. "Two-Stage Noncollinear Optical Parametric Amplification Approaching Single Cycle." Acta Optica Sinica 35, no. 8 (2015): 0819002. http://dx.doi.org/10.3788/aos201535.0819002.

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45

Brabec, Thomas, and Ferenc Krausz. "Nonlinear Optical Pulse Propagation in the Single-Cycle Regime." Physical Review Letters 78, no. 17 (1997): 3282–85. http://dx.doi.org/10.1103/physrevlett.78.3282.

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46

Zabolotskii, A. A. "Integrable equations of a few cycle optical pulse propagation." European Physical Journal Special Topics 173, no. 1 (2009): 193–222. http://dx.doi.org/10.1140/epjst/e2009-01074-x.

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47

Butuc-Mayer, Filip, Matthew Johnson, Chen-Hao Feng, William Bowden, Richard Hobson, and Ian R. Hill. "Duty cycle engineering for improved optical lattice clock stability." Journal of Physics: Conference Series 2889, no. 1 (2024): 012049. http://dx.doi.org/10.1088/1742-6596/2889/1/012049.

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Abstract We describe a method of duty cycle engineering in optical lattice clocks to reduce clock instability through tailoring of the Dick effect noise contribution. We apply dynamically decoupled interrogation sequences to realise an estimated improvement in single clock instability approaching a factor of two, as well as providing a route to zero dead-time operation for two interleaved clocks which are otherwise unable to reach the required duty cycle. We show through simulations and synchronous measurements of clocks NPL-Sr1 and NPL-Sr2 that a quantum projection noise limited instability &
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48

Kim, Tae Shik, Hyun-Sang Park, Sun-Joo Jang, et al. "Single cardiac cycle three-dimensional intracoronary optical coherence tomography." Biomedical Optics Express 7, no. 12 (2016): 4847. http://dx.doi.org/10.1364/boe.7.004847.

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49

Mennickent, Ronald E., Zbigniew Kołaczkowski, Gojko Djurasevic, M. Diaz, and Ewa Niemczura. "Optical Spectroscopy of V393 Scorpii During its Long Cycle." Proceedings of the International Astronomical Union 7, S282 (2011): 317–18. http://dx.doi.org/10.1017/s1743921311027694.

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AbstractV393 Scorpii is a bright Galactic Double Periodic Variable showing a long photometric cycle of ≈253 days. The ASAS V-band light curve has been disentangled into an orbital and long cycle component. The orbital light curve was modeled with two stellar components and a circumprimary accretion disk. Based on this model, and the careful choice of a template spectrum for the donor, the contribution of the donor to the line+continuum spectrum was removed at every orbital phase. The remaining residual spectra were analyzed. Notable findings are the larger line emissivity observed during the l
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50

Sarma, Amarendra K. "Modulational instability of few-cycle pulses in optical fibers." EPL (Europhysics Letters) 92, no. 2 (2010): 24004. http://dx.doi.org/10.1209/0295-5075/92/24004.

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