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Journal articles on the topic 'Band 5'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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1

Warda, Bint Ashraf, and Ahmed Noor Munaz. "Concrete Property Analysis with the Perspective of “5-10-14-18” and “5-10-18-22” Band Gradation." Applied Mechanics and Materials 84-85 (August 2011): 101–5. http://dx.doi.org/10.4028/www.scientific.net/amm.84-85.101.

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Recent concrete specifications often require the use of combined aggregate gradation that meets the “8-18” band gradation. But theoretically “8-18” band covers a wide range of aggregate variation which may result in variable properties of concrete. To avoid this drawback, two new band gradations were proposed, these are, “5-10-14-18” and “5-10-18-22” bands. This paper analyses different aspects of these proposed bands through a number of concrete mix results.

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2

Piltz, Burghard. "MünchKomm/HGB, Band 5." Internationales Handelsrecht 18, no. 6 (December 1, 2018): 267–68. http://dx.doi.org/10.9785/ihr-2018-180613.

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3

Milosevic, Nenad, Bojan Dimitrijevic, Dejan Drajic, Zorica Nikolic, and Milorad Tosic. "LTE and WiFi co-existence in 5 GHz unlicensed band." Facta universitatis - series: Electronics and Energetics 30, no. 3 (2017): 363–73. http://dx.doi.org/10.2298/fuee1703363m.

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Since the future mobile networks will require significantly higher data throughput, and the Long-Term Evolution (LTE) licensed bands are already occupied, the frequency band extension and the data rate increase may be achieved by using some of the available unlicensed bands. The most appropriate unlicensed band for this purpose lies in 5 GHz frequency range. However, this unlicensed band is already occupied by WiFi networks and a special attention has to be paid to coordinate these two different networks in the shared spectrum usage. Therefore, this paper considers the shared access co-existence in 5 GHz unlicensed band between uncoordinated LTE and WiFi networks. More precisely, it considers the influence of the LTE downlink transmission on the performance of the WiFi networks. The experimental results show that the LTE significantly degrades the WiFi network performance, which means that some of the coordination algorithms have to be employed.

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4

Belitsky, V., M. Bylund, V. Desmaris, A. Ermakov, S. E. Ferm, M. Fredrixon, S. Krause, et al. "ALMA Band 5 receiver cartridge." Astronomy & Astrophysics 611 (March 2018): A98. http://dx.doi.org/10.1051/0004-6361/201731883.

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We describe the design, performance, and commissioning results for the new ALMA Band 5 receiver channel, 163–211 GHz, which is in the final stage of full deployment and expected to be available for observations in 2018. This manuscript provides the description of the new ALMA Band 5 receiver cartridge and serves as a reference for observers using the ALMA Band 5 receiver for observations. At the time of writing this paper, the ALMA Band 5 Production Consortium consisting of NOVA Instrumentation group, based in Groningen, NL, and GARD in Sweden have produced and delivered to ALMA Observatory over 60 receiver cartridges. All 60 cartridges fulfil the new more stringent specifications for Band 5 and demonstrate excellent noise temperatures, typically below 45 K single sideband (SSB) at 4 K detector physical temperature and below 35 K SSB at 3.5 K (typical for operation at the ALMA Frontend), providing the average sideband rejection better than 15 dB, and the integrated cross-polarization level better than –25 dB. The 70 warm cartridge assemblies, hosting Band 5 local oscillator and DC bias electronics, have been produced and delivered to ALMA by NRAO. The commissioning results confirm the excellent performance of the receivers.

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5

Wang, Jyh Liang, Tsang Yen Hsieh, Chuan Chou Hwang, and Mei Hui Wang. "Monopole Patch Antenna with Dual Band of 2.4 and 5 GHz Designed for Wireless LAN Applications." Applied Mechanics and Materials 421 (September 2013): 173–76. http://dx.doi.org/10.4028/www.scientific.net/amm.421.173.

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A compact prototype of dual band monopole antenna has been fabricated on PCB with small overall size of 36.6 mm×47 mm. By the trial of simulation to tune the dimensions of PCB, an optimum design of antenna can be obtained. Dual resonances excited in 2.4 and 5 GHz bands. For return loss more than 9.6 dB, the achieved bandwidths are 2.41 to 2.77 GHz in 2.4 GHz band and 5.11 to 5.83 GHz in 5 GHz band. The return loss ( ) can keep larger than 9.6dB within the bands of 2.4 and 5 GHz.

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6

Bonatsos, Dennis, D. Lenis, D. Petrellis, and P. A. Terziev. "W(5): Wobbling Mode in the Framework of the X(5) Model." HNPS Proceedings 13 (February 20, 2020): 214. http://dx.doi.org/10.12681/hnps.2971.

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Using in the Bohr Hamiltonian the approximations leading to the Bohr and Mot- telson description of wobbling motion in even nuclei, a W(5) model for wobbling bands, coexisting with a X(5) ground state band, is obtained. Separation of vari ables is achieved by assuming that the relevant potential has a sharp minimum at 70, which is the only parameter entering in the spectra and B(E2) transition rates (up to overall scale factors). B(E2) transition rates exhibit the features expected in the wobbling case.

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7

A., Ikhsani, Sudjono P., Firdayati M., and Marselina M. "Identification and analysis of shoreline changes over fishermen settlement along the coast of sungaibuntu and cemarajaya village, Karawang Regency, West Java." Transport and Communications Science Journal 72, no. 1 (January 25, 2021): 95–106. http://dx.doi.org/10.47869/tcsj.72.1.11.

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Shoreline changes, that occur along the coast, gives negative effects to the environment and also social-economic activities on the fishermen’s livelihood. Study about shoreline changes, its trends, and its causes are important for the development of economic and sanitation vulnerability assessment on fishermen community caused by shoreline changes. Thus, environmental sustainability criteria within the local scale and specific to fishermen community takes into account and the implementation of the instrument become more appropriate to reduce the undesirable effects. This research aims to identifying and analysing shoreline changes trend and its factors over the fishermen settlement area along the coast of Sungaibuntu and Cemarajaya village, Karawang Regency, West Java. Data used in this study are Landsat-7 1999, 2002, 2007, and 2012 as well as Landsat-8 2017. To enhance Landsat-7 images, band 2-4-5 are used, meanwhile Landsat-8 employs band 3-5-6. Later, the shoreline was extracted by applying band rationing techniques, Band2/Band5 for Landsat-7 and Band3/Band6 for Landsat-8. The rate of shoreline changes along the coast of Sungaibuntu is -0.15 m/yr and -2.89 m/yr along Cemarajaya. The periodic phenomena that affect shoreline changes consist of tidal range with a mean value of 0.796 m, significant wave height (Hs) of 0 - 2.9 m with the dominant direction heading to the southeast, and also sea level rise (SLR). Besides, there is an anthropogenic factor of land use and land cover changes as the significant feature shown by the managed system of ponds, cropland, farmland, paddy field, along with the settlement. As for the instrument development of economic and sanitation vulnerability on fishermen community, it is important to take shoreline changes rate and its causes into account and consider it as vulnerability criteria.

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8

Choi, Munyong, Hyunho Wi, Byeonggwi Mun, Yonghyun Yoon, Hyunwoo Lee, and Byungje Lee. "A Compact Frequency Reconfigurable Antenna for LTE Mobile Handset Applications." International Journal of Antennas and Propagation 2015 (2015): 1–10. http://dx.doi.org/10.1155/2015/764949.

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A compact (8 × 62 × 5 mm3; 2.48 cc) frequency reconfigurable antenna that uses electrical switching with PIN diodes is proposed for the low frequency LTE band (699 MHz–862 MHz), high frequency LTE band (2496 MHz–2690 MHz), GSM850/900 bands (824 MHz–960 MHz), and DCS/PCS/WCDMA bands (1710 MHz–2170 MHz). The penta-band PIFA is first designed for GSM850/900/DCS/PCS/WCDMA bands by using two slits and ground pins within a limited antenna volume (8 × 54.6 × 5 mm3; 2.18 cc). The frequency reconfigurable antenna based on this penta-band PIFA is thus proposed to additionally cover all LTE bands. The proposed antenna has two PIN diodes with an optimal location. For State 1 (PIN diode 1: ON state, PIN diode 2: OFF state), the proposed antenna covers the low frequency LTE band, DCS/PCS/WCDMA bands, and high frequency LTE band. For State 2 (PIN diode 1: OFF state, PIN diode 2: ON state), the antenna covers the GSM850/900 bands. Simulated and measured results show that the total efficiency of the proposed antenna was greater than 40% for all operating frequency bands.

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9

Liu, Gongye, Li Li, Xianfeng Li, Yingjun Ma, Yanxin Zhao, Dong Yang, Congbo Li, et al. "Yrast Band in122I and Band Termination." Plasma Science and Technology 14, no. 5 (May 2012): 412–14. http://dx.doi.org/10.1088/1009-0630/14/5/17.

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10

Allen, G., J. J. Remedios, D. A. Newnham, K. M. Smith, and P. S. Monks. "Improved mid-infrared cross-sections for peroxyacetyl nitrate (PAN) vapour." Atmospheric Chemistry and Physics 5, no. 1 (January 17, 2005): 47–56. http://dx.doi.org/10.5194/acp-5-47-2005.

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Abstract. Absorption spectra of peroxyacetyl nitrate (PAN, CH3C(O)OONO2) vapour at room temperature (295K) have been measured in the mid-infrared range, 550-2200cm-1 (18.2-4.55µm), using a Fourier Transform infrared spectrometer at instrument resolutions of 0.25 and 0.03cm-1 (unapodised). Between five and eight measurements were obtained for each spectral band of PAN in the pressure range 0.24-2.20mb showing good agreement with Beer's law. Both cross-section data and integrated absorption intensities for the five principal bands in the PAN spectra in this spectral range have been derived with peak cross-sections of the 794, 1163, 1302, 1741 and 1842cm-1 bands measured to be 0.95(±0.02), 1.21(±0.03), 0.92(±0.02), 2.39(±0.06) and 0.74(±0.03) (x10-18cm2molecule-1) respectively. Band intensities and band centre absorptivities are also reported for four weaker PAN absorption bands in the mid infrared for the first time. These observations are the highest spectral resolution measurements of PAN bands reported in the infrared to date. For three of the five strongest bands, the absolute integrated absorption intensities are in excellent agreement with previous studies. A 4.8% lower integrated intensity was found for the 1741cm-1νas(NO2) PAN absorption band, possibly as a result of the removal in this work of spectra affected by acetone contamination, while a 10.6% higher intensity was determined for the 1163cm-1ν(C-O) absorption band. No resolution of fine structure in the PAN absorption bands was observed at the resolutions studied. The confirmation of absorption cross-sections and estimated errors in this work will allow more accurate investigations of PAN using infrared spectroscopy, particularly for remote sensing of PAN in the atmosphere.

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11

Jain, Poonam, and Samit K. Mandal. "Band head spin for triaxial super-deformed bands in 165,167Lu." EPJ Web of Conferences 177 (2018): 03002. http://dx.doi.org/10.1051/epjconf/201817703002.

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We use VMI model for the prediction of band head spin of Triaxial Super- Deformed (TSD) rotational bands. The calculated and observed transition energies are agreed well when an accurate band head spin (I0) is predicted. The results are in good agreement with the experimentally known values of spin and transition energies. In the present paper, we have reported the band head spin of TSD bands for Lu isotope. This method brings comprehensive interpretation for spin assignment of TSD bands which could help in designing future experiments for these bands. Thus, we have reported the band head spin value of 5 TSD rotational band of Lu isotope.

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12

van Peteghem, P. P. J. L. "Band 5: Reichsstädte, 1: Frankfurt am Main; Band 6: Reichsstädte, 2: Köln." Tijdschrift voor Rechtsgeschiedenis / Revue d'Histoire du Droit / The Legal History Review 75, no. 1 (2007): 68–71. http://dx.doi.org/10.1163/157181907781602863.

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13

Ali, M., T. Sittironnarit, H. S. Hwang, R. A. Sadler, and G. J. Hayes. "Wide-Band/Dual-Band Packaged Antenna for 5–6 GHz WLAN Application." IEEE Transactions on Antennas and Propagation 52, no. 2 (February 2004): 610–15. http://dx.doi.org/10.1109/tap.2004.823992.

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14

Fan, Shuaiqi, and Ziguang Chen. "Electric potential and energy band in ZnO nanofiber tuned by local mechanical loading." Applied Mathematics and Mechanics 42, no. 6 (May 19, 2021): 787–804. http://dx.doi.org/10.1007/s10483-021-2736-5.

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AbstractRecent success in strain engineering has triggered tremendous interest in its study and potential applications in nanodevice design. In this paper, we establish a coupled piezoelectric/semiconducting model for a wurtzite structure ZnO nanofiber under the local mechanical loading. The energy band structure tuned by the local mechanical loading and local length is calculated via an eight-band k · p method, which includes the coupling of valance and conduction bands. Poisson’s effect on the distribution of electric potential inversely depends on the local mechanical loading. Numerical results reveal that both the applied local mechanical loading and the local length exhibit obvious tuning effects on the electric potential and energy band. The band gap at band edges varies linearly with the applied loading. Changing the local length shifts the energy band which is far away from the band edges. This study will be useful in the electronic and optical enhancement of semiconductor devices.

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15

Abubakirov, Edward B., Alexey V. Chirkov, Gregory G. Denisov, Yury M. Guznov, Sergey Yu Kornishin, Alexander N. Leontyev, Oleg P. Plankin, et al. "W-Band 5 MW Pulse Relativistic Gyrotron." IEEE Transactions on Electron Devices 64, no. 4 (April 2017): 1865–67. http://dx.doi.org/10.1109/ted.2017.2664106.

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16

Yang, Li-Ming, Guo-Yong Fang, Jing Ma, Eric Ganz, and Sang Soo Han. "Band Gap Engineering of Paradigm MOF-5." Crystal Growth & Design 14, no. 5 (April 24, 2014): 2532–41. http://dx.doi.org/10.1021/cg500243s.

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17

Zihl, Joseph. "Visuelle Wahrnehmungsstörungen. Fortschritte der Neuropsychologie Band 5." Zeitschrift für Neuropsychologie 17, no. 3 (January 2006): 205. http://dx.doi.org/10.1024/1016-264x.16.3.205.

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18

Chander, G., D. L. Helder, and W. C. Boncyk. "Landsat-4/5 Band 6 relative radiometry." IEEE Transactions on Geoscience and Remote Sensing 40, no. 1 (2002): 206–10. http://dx.doi.org/10.1109/36.981362.

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19

Holtgrave, E. A. "Zahn-, Mund-, Kieferheilkunde, Band 5: Kieferorthopädie, Parodontologie." Fortschritte der Kieferorthopädie 51, no. 1 (January 1990): 60. http://dx.doi.org/10.1007/bf02165214.

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20

Hollender, Martin. "Jahrbuch für Buch- und Bibliotheksgeschichte Band 5." Zeitschrift für Bibliothekswesen und Bibliographie 68, no. 2 (April 15, 2021): 4–9. http://dx.doi.org/10.3196/1864295020682106.

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21

Jeong, Tae Hun, and Dong Geun Jeong. "Frequency Band Selection for WLAN Using Multiple Bands of 5 GHz/60 GHz." Journal of Korean Institute of Communications and Information Sciences 39A, no. 12 (December 31, 2014): 718–28. http://dx.doi.org/10.7840/kics.2014.39a.12.718.

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22

Tilstra, Lieuwe G., Martin de Graaf, Ping Wang, and Piet Stammes. "In-orbit Earth reflectance validation of TROPOMI on board the Sentinel-5 Precursor satellite." Atmospheric Measurement Techniques 13, no. 8 (August 18, 2020): 4479–97. http://dx.doi.org/10.5194/amt-13-4479-2020.

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Abstract. The goal of the study described in this paper is to determine the accuracy of the radiometric calibration of the TROPOMI instrument in flight, using its Earth radiance and solar irradiance measurements, from which the Earth reflectance is determined. The Earth reflectances are compared to radiative transfer calculations. We restrict ourselves to clear-sky observations as these are less difficult to model than observations containing clouds and/or aerosols. The limiting factor in the radiative transfer calculations is then the knowledge of the surface reflectance. We use OMI and SCIAMACHY surface Lambertian-equivalent reflectivity (LER) information to model the reflectivity of the Earth's surface. This Lambertian, nondirectional description of the surface reflection contribution results in a relatively large source of uncertainty in the calculations. These errors can be reduced significantly by filtering out geometries for which we know that surface LER is a poor approximation of the real surface reflectivity. This filtering is done by comparing the OMI/SCIAMACHY surface LER information to MODIS surface BRDF information. We report calibration accuracies and errors for 21 selected wavelength bands between 328 and 2314 nm, located in TROPOMI spectral bands 3–7. All wavelength bands show good linear response to the intensity of the radiation and negligible offset problems. Reflectances in spectral bands 5 and 6 (wavelength bands 670 to 772 nm) have good absolute agreement with the simulations, showing calibration errors on the order of 0.01 or 0 %–3 %. Trends over the mission lifetime, due to instrument degradation, are studied and found to be negligible at these wavelengths. Reflectances in bands 3 and 4 (wavelength bands 328 to 494 nm), on the other hand, are found to be affected by serious calibration errors, on the order of 0.004–0.02 and ranging between 6 % and 10 %, depending on the wavelength. The TROPOMI requirements (of 2 % maximal deviation) are not met in this case. Trends due to instrument degradation are also found, being strongest for the 328 nm wavelength band and almost absent for the 494 nm wavelength band. The validation results obtained for TROPOMI spectral band 7 show behaviour that we cannot fully explain. As a result, these results call for more research and different methods to study the calibration of the reflectance. It seems plausible, though, that the reflectance for this particular band is underestimated by about 6 %. A table is provided containing the final results for all 21 selected wavelength bands.

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23

Huang, Xianglei, Jason N. S. Cole, Fei He, Gerald L. Potter, Lazaros Oreopoulos, Dongmin Lee, Max Suarez, and Norman G. Loeb. "Longwave Band-By-Band Cloud Radiative Effect and Its Application in GCM Evaluation." Journal of Climate 26, no. 2 (January 15, 2013): 450–67. http://dx.doi.org/10.1175/jcli-d-12-00112.1.

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Abstract The cloud radiative effect (CRE) of each longwave (LW) absorption band of a GCM’s radiation code is uniquely valuable for GCM evaluation because 1) comparing band-by-band CRE avoids the compensating biases in the broadband CRE comparison and 2) the fractional contribution of each band to the LW broadband CRE (fCRE) is sensitive to cloud-top height but largely insensitive to cloud fraction, thereby presenting a diagnostic metric to separate the two macroscopic properties of clouds. Recent studies led by the first author have established methods to derive such band-by-band quantities from collocated Atmospheric Infrared Sounder (AIRS) and Clouds and the Earth’s Radiant Energy System (CERES) observations. A study is presented here that compares the observed band-by-band CRE over the tropical oceans with those simulated by three different atmospheric GCMs—the GFDL Atmospheric Model version 2 (GFDL AM2), NASA Goddard Earth Observing System version 5 (GEOS-5), and the fourth-generation AGCM of the Canadian Centre for Climate Modelling and Analysis (CCCma CanAM4)—forced by observed SST. The models agree with observation on the annual-mean LW broadband CRE over the tropical oceans within ±1 W m−2. However, the differences among these three GCMs in some bands can be as large as or even larger than ±1 W m−2. Observed seasonal cycles of fCRE in major bands are shown to be consistent with the seasonal cycle of cloud-top pressure for both the amplitude and the phase. However, while the three simulated seasonal cycles of fCRE agree with observations on the phase, the amplitudes are underestimated. Simulated interannual anomalies from GFDL AM2 and CCCma CanAM4 are in phase with observed anomalies. The spatial distribution of fCRE highlights the discrepancies between models and observation over the low-cloud regions and the compensating biases from different bands.

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24

OBUKURO, YUKI, KENJI OBATA, SHIGENORI MATSUSHIMA, MASAO ARAI, and KENKICHIRO KOBAYASHI. "PREPARATION AND CHARACTERIZATION OF SrO-Bi2O3 COMPLEX OXIDE." Functional Materials Letters 05, no. 02 (June 2012): 1260015. http://dx.doi.org/10.1142/s1793604712600156.

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The Sr 2 Bi 2 O 5 powders were prepared by a malonic acid complex method and a solid-state reaction. These powders were characterized by X-ray diffraction, UV-vis diffuse reflectance spectra and specific surface area measurements. In a malonic acid complex method, the Sr 2 Bi 2 O 5 phase of high purity was obtained at 700°C in air and its specific surface area was calculated to be 2.74 m2/g. From UV-vis measurements, it was confirmed that Sr 2 Bi 2 O 5 is a direct band gap material and its optical band gap is ca. 3.1 eV. The first-principles energy band calculation showed that the energy bands of Sr 2 Bi 2 O 5 crystal have a wide dispersion near the valence band maximum and the conduction band minimum. The Sr 2 Bi 2 O 5 powders showed a distinct photocatalytic decomposition of methylene blue under visible light irradiation (a wavelength ≥ 420 nm).

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25

Parkinson, David, Elizabeth C. Coscia, and Nigel W. Daw. "Identification and localization of 5-hydroxytryptamine receptor sites in macaque visual cortex." Visual Neuroscience 2, no. 5 (May 1989): 515–25. http://dx.doi.org/10.1017/s0952523800012402.

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AbstractThe two main receptor subtypes for 5-hydroxytryptamine (5HT) were measured and localized in visual cortical areas of macaque monkey. [3H]5HT was used to label all 5HT-1 receptor subtypes and [3H]ketanserin was used to label 5HT-2 receptors. Both receptor types could be demonstrated in membranes prepared from macaque primary visual cortex. The specificity of these ligands for 5HT-1 or 5HT-2 receptors was demonstrated by the pharmacological profile of inhibitors of the specific binding. 5HT-1A receptor sites were detected by displacement experiments and by direct labeling with [3H]8-hydroxy-2(di-n-propylamino) tetralin 8OH-DPAT. Receptor autoradiography showed that the distribution of these receptor subtypes varied from one part of visual cortex to another. 5HT-1 receptors, labeled with [3H]5HT were present in several bands through layer IV of primary visual cortex with the densest band seen in and above layer IVA: another band was in lower layer VI. The band in layer VI was predominantly 5HT-1A sites. There were two main bands of 5HT-2 receptor sites, the most prominent around the IV/V boundary, and the other extending from layer IVA upwards. Adjacent areas showed 5HT receptors in a broad band corresponding to layer IV. 5HT-1A sites were found in superficial layers of adjacent areas, except V2. These layering patterns did not correspond precisely with cytoarchitectonic layering, nor with the pattern of 5HT-containing presynaptic fibres in published reports. It is important, therefore, in considering the role of the 5HT-containing neurons in cortical function to take account not only of the anatomy of the presynaptic terminals, but also of the postsynaptic receptors upon which the released transmitter will act, and their location within the cortex.

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26

Hwang, S. H., J. I. Moon, W. I. Kwak, and S. O. Park. "Printed compact dual band antenna for 2.4 and 5 GHz ISM band applications." Electronics Letters 40, no. 25 (2004): 1568. http://dx.doi.org/10.1049/el:20046579.

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27

Bykov, Alexander D., Olga V. Naumenko, Maxim A. Smirnov, Leonid N. Sinitsa, Linda R. Brown, Joy Crisp, and David Crisp. "The infrared spectrum of H2S from 1 to 5 μm." Canadian Journal of Physics 72, no. 11-12 (November 1, 1994): 989–1000. http://dx.doi.org/10.1139/p94-130.

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The absorption spectra of H2S from 2000 to 11 147 cm−1 have been obtained with spectral resolutions of 0.006, 0.012, and 0.021 cm−1 using the Fourier transform spectrometer at Kitt Peak National Observatory. The transitions of 21 bands have been assigned for the first time and 9 others reanalyzed so that accurate energy levels, band origins, and rotational parameters could be determined. The analysis of these data revealed some remarkable features in the energy spectrum, e.g., fourfold clustering of rotational levels belonging to the symmetric and asymmetric components of local mode manifolds at a high degree of stretching excitation. This paper reports fitted vibrational parameters and predicted band origins of H232S up to 12 735 cm−1. It also presents the degenerate rotational constants and upper state energies of (301)–(202) and (311)–(212) at 1 μm as illustrations of clustering in the local mode limit.

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28

Bonatsos, Dennis, D. Lenis, N. Minkov, D. Petrellis, P. P. Raychev, and P. A. Terziev. "Variational procedure leading from Davidson potentials to the E(5)and X(5) critical point symmetries." HNPS Proceedings 13 (February 20, 2020): 10. http://dx.doi.org/10.12681/hnps.2952.

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Davidson potentials of the form β^2 + β0^4/β^2, when used in the original Bohr Hamiltonian for γ-independent potentials bridge the U(5) and 0(6) symmetries. Using a variational procedure, we determine for each value of angular momentum L the value of β0 at which the derivative of the energy ratio RL = E(L)/E(2) with respect to β0 has a sharp maximum, the collection of RL values at these points forming a band which practically coincides with the ground state band of the E(5) model, corresponding to the critical point in the shape phase transition from U(5) to Ο(6). The same potentials, when used in the Bohr Hamiltonian after separating variables as in the X(5) model, bridge the U(5) and SU(3) symmetries, the same variational procedure leading to a band which practically coincides with the ground state band of the X(5) model, corresponding to the critical point of the U(5) to SU(3) shape phase transition. A new derivation of the Holmberg-Lipas formula for nuclear energy spectra is obtained as a by-product.

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29

JING, LONG-LONG, LI-YU HUANG, DENG-FENG HUANG, JIE NIU, and ZHENG ZHONG. "AMPLITUDE OF LOW FREQUENCY FLUCTUATION AT DIFFERENT FREQUENCY BANDS IN EARLY AMNESTIC MILD COGNITIVE IMPAIRMENT: RESULTS FROM ADNI." Journal of Innovative Optical Health Sciences 05, no. 01 (January 2012): 1150003. http://dx.doi.org/10.1142/s1793545811500039.

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We used resting-state functional magnetic resonance imaging (fMRI) to determine whether there are any abnormalities in different frequency bands between amplitude of low-frequency fluctuations (ALFF) and fractional ALFF (fALFF) and between 10 early amnestic mild cognitive impairment (EMCI) patients and eight normal controls participating in the Alzheimer's Disease Neuroimaging Initiative (ADNI). We showed widespread difference in ALFF/fALFF between two frequency bands (slow-4: 0.027–0.073 Hz, slow-5: 0.01–0.027 Hz) in many brain areas including posterior cingulate cortex (PCC), medial prefrontal cortex (MPFC), suprasellar cistern (SC) and ambient cistern (AC). Compared to the normal controls, the EMCI patients showed increased ALFF values in PCu , cerebellum, occipital lobe and cerebellum posterior lobe in frequency band slow-4. While in frequency band slow-5, the EMCI patients showed decreased ALFF values in temporal lobe, left cerebrum and middle temporal gyrus5. Moreover, the EMCI patients showed increased fALFF values in frontal lobe and inferior frontal gyrus in band slow-5. While in frequency band slow-4, the EMCI patients showed decreased fALFF values in limbic lobe, cingulate gyrus and corpus callosum. These results demonstrated that EMCI patients had widespread abnormalities of amplitude of LFF in different frequency bands.

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30

Kumar, P., and J. L. Masa-Campos. "Dual Polarized Monopole Patch Antennas for UWB Applications with Elimination of WLAN Signals." Advanced Electromagnetics 5, no. 1 (May 1, 2016): 46. http://dx.doi.org/10.7716/aem.v5i1.305.

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This paper presents the design, fabrication and measurement of dual polarized microstrip patch antennas for ultra wideband (UWB) applications with notch at 5-6 GHz band. The proposed antenna rejects the wireless local area network (WLAN) signals and work properly in the entire remaining ultra-wideband. Two antennas are designed for two different frequency bands of ultra wideband and both antennas together produce the entire ultra wideband with notch at 5-6 GHz band. The antennas are fed by a 50 coaxial probe and the entire design is optimized using CST Microwave Studio. The bandwidth of 3.1-5 GHz is achieved by the optimized design of Antenna-1 and the bandwidth of 6 -10.6 GHz is achieved by the optimized design of Antenna-2. The bandwidth of the optimized combined antenna is 3.1-10.6 GHz with elimination of the 5-6 GHz band. Both antennas are simulated, developed and measured. The simulated and measured results are presented. The two designed dual polarized antennas i.e. Antenna-1 and Antenna-2 can be used for 3.1-5 GHz band and 6-10.6 GHz band dual polarized applications, respectively, and the combined antenna structure can be used for UWB dual polarized applications with elimination of 5-6 GHz band signals.

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31

Reddy, B. Jagannadha, and Ray L. Frost. "Near Infrared Spectroscopy of Aurichalcite (Zn,Cu2+)5(CO3)2(OH)6." Journal of Near Infrared Spectroscopy 15, no. 2 (April 2007): 115–21. http://dx.doi.org/10.1255/jnirs.722.

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In this endeavour, near infrared spectroscopy studies show evidence of variable composition in aurichalcite minerals of zinc copper carbonate hydroxides. The observation of a broad feature in the electronic part of the spectrum around 11,500 cm−1 (870 nm) is a strong indication of Cu2+ substitution for Zn2+ in the mineral. Overtones of OH vibrations in the spectra from 7250 to 5400 cm−1 (1380–1850 nm) show strong hydrogen bonding in these carbonates. A band common to spectra of all carbonates appears near 5400 cm−1 (1850 nm) due to the combination of both OH-stretching and HOH-bending vibrations, which may be attributed to adsorbed water. Aurichalcite minerals display a spectral sequence of five absorption bands with variation of both band positions and intensities and this is the chief spectral feature observed in the range 5200–5100 cm−1 (1920–2380 nm) due to vibrational processes of the carbonate ion. The frequency shift of carbonate bands suggests the effect of divalent cations and/or variations of the Zn/Cu ratio in aurichalcite minerals.

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32

Allen, G., J. J. Remedios, and K. M. Smith. "Low temperature mid-infrared cross-sections for peroxyacetyl nitrate (PAN) vapour." Atmospheric Chemistry and Physics 5, no. 11 (November 24, 2005): 3153–58. http://dx.doi.org/10.5194/acp-5-3153-2005.

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Abstract. Laboratory absorption spectra of peroxyacetyl nitrate (PAN, CH3C(O)OONO2) vapour have been measured in the mid-infrared range 550 cm-1 to 1400 cm-1 (18.2 to 7.14 µm) at both 250 K and 273 K, using a Fourier transform infrared spectrometer at a nominal spectral resolution of 0.25 cm-1 (unapodised). In addition, the 1600 cm-1 to 2200 cm-1 (6.25 to 4.54 µm) spectral region has been measured at 250 K. Cross-sectional data at each temperature, as well as integrated band intensities and peak infrared absorptivities for nine absorption bands of PAN in this spectral range, have been derived from a total of twelve separately measured PAN transmission spectra. A general increase in the peak absorption cross-section for all bands is noted with decreasing temperature, with cross-sectional increases in the range 6% (for the 1842 cm-1 band) and 30% (for the 991 cm-1 band) at 250K, relative to those previously reported at 295K. Differences in integrated band intensities range from -22% to +16% for the 1741 cm-1 and 991 cm-1 bands respectively over the same temperature range. These new absorption cross-sections for PAN are the first to be reported at temperatures below 295 K, allowing the possibility of improved retrievals of the atmospherically important PAN species from remotely sensed infrared spectra of the cold upper troposphere. These new cross-sectional data accompany this paper as an electronic supplement.

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33

Schweiger, Gottfried, Martina Schmidhuber, and Michael Zichy. "Editorial zu Band 5, Heft 1, (Juli) 2018." Zeitschrift für Praktische Philosophie 5, no. 1 (July 2018): 13–14. http://dx.doi.org/10.22613/zfpp/5.1.0.

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34

Hosseinzadeh, Navid, and Ali Medi. "Wideband 5 W Ka-Band GaAs Power Amplifier." IEEE Microwave and Wireless Components Letters 26, no. 8 (August 2016): 622–24. http://dx.doi.org/10.1109/lmwc.2016.2587834.

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35

Barsi, Julia A., Simon J. Hook, John R. Schott, Nina G. Raqueno, and Brian L. Markham. "Landsat-5 Thematic Mapper Thermal Band Calibration Update." IEEE Geoscience and Remote Sensing Letters 4, no. 4 (October 2007): 552–55. http://dx.doi.org/10.1109/lgrs.2007.896322.

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36

Dudin, Gertrud, Denis Alexander, Fayrouz Talj, Mary Deeb, Salim Musallam, and Vazken M. Der Kaloustian. "Interstitial deletion of band q12 of chromosome 5." Clinical Genetics 25, no. 5 (April 23, 2008): 455–58. http://dx.doi.org/10.1111/j.1399-0004.1984.tb02016.x.

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37

Darwish, Ali Mohamed, K. Boutros, B. Luo, Benjamin D. Huebschman, E. Viveiros, and H. Alfred Hung. "AlGaN/GaN $Ka$-Band 5-W MMIC Amplifier." IEEE Transactions on Microwave Theory and Techniques 54, no. 12 (December 2006): 4456–63. http://dx.doi.org/10.1109/tmtt.2006.883599.

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38

Chander, G., D. L. Helder, B. L. Markham, J. D. Dewald, E. Kaita, K. J. Thome, E. Micijevic, and T. A. Ruggles. "Landsat-5 TM reflective-band absolute radiometric calibration." IEEE Transactions on Geoscience and Remote Sensing 42, no. 12 (December 2004): 2747–60. http://dx.doi.org/10.1109/tgrs.2004.836388.

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39

Helder, D. L., T. A. Ruggles, J. D. Dewald, and S. Madhavan. "Landsat-5 Thematic Mapper reflective-band radiometric stability." IEEE Transactions on Geoscience and Remote Sensing 42, no. 12 (December 2004): 2730–46. http://dx.doi.org/10.1109/tgrs.2004.839088.

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40

Kobayashi, Kazuaki, Hirokazu Takaki, Masato Shimono, Nobuhiko Kobayashi, and Kenji Hirose. "Electronic band structure of TiN/MgO-4 × 4 and 5 × 5 nanostructures." Japanese Journal of Applied Physics 58, SB (February 25, 2019): SBBH06. http://dx.doi.org/10.7567/1347-4065/aafc9a.

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41

Jiang, Fei, Yin-Quan Ye, Jin-Min Zuo, Xin Huang, Chen Yu, and Xian-Jun Zeng. "Frequency-specific oscillations synchronization in primary angle-closure glaucoma." Acta Radiologica 61, no. 4 (August 31, 2019): 537–48. http://dx.doi.org/10.1177/0284185119870975.

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Background Previous neuroimaging studies demonstrated that patients with primary angle-closure glaucoma were accompanied by abnormal neuronal activity. Purpose To investigate frequency-dependent local oscillations synchronization in primary angle-closure glaucoma using the regional homogeneity method. Material and Methods In total, 37 individuals with primary angle-closure glaucoma (20 men, 17 women) and 37 normal-sighted controls (20 men, 17 women) closely matched in age, sex, and education underwent resting-state MRI scans. We compared the different regional homogeneity values in full band (0.01–0.08 Hz) and two different frequency bands (slow-4: 0.027–0.073 Hz and slow-5: 0.010–0.027 Hz) between two groups. Results Compared to the normal-sighted group, the primary angle-closure glaucoma group showed decreased regional homogeneity values in the left calcarine and left postcentral in full band. The primary angle-closure glaucoma group showed increased regional homogeneity values in the bilateral superior medial frontal lobe in the slow-4 band. The primary angle-closure glaucoma group exhibited decreased regional homogeneity values in the right calcarine in the slow-5 band. Specifically, we found that the regional homogeneity values in the right superior frontal lobe were greater in the slow-4 than in the slow-5 band, whereas regional homogeneity in the left calcarine, right pallidum, left inferior occipital gyrus, left superior occipital gyrus, left postcentral/angular gyrus, left paracentral lobule, left superior parietal gyrus, and right precuneus gyrus were greater in the slow-5 than in the slow-4 band. Conclusion Primary angle-closure glaucoma groups showed abnormal regional homogeneity in visual network (calcarine) and default mode network (superior medial frontal lobe) at two frequency bands. Moreover, the regional homogeneity signals in slow-5 band showed closely related to the severity of individuals with primary angle-closure glaucoma.

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42

"Analytiker Taschenbuch, Band 5." Journal of Chromatography A 351 (January 1986): 609–10. http://dx.doi.org/10.1016/s0021-9673(01)83550-0.

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43

"Sachwortverzeichnis Band 5, 1998." Complementary Medicine Research 5, no. 6 (1998): 317–18. http://dx.doi.org/10.1159/000021164.

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"Sachwortverzeichnis Band 5, 2010." Breast Care 5, no. 6 (2010): 443–44. http://dx.doi.org/10.1159/000323642.

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"Inhalt Band 5, 2010." Breast Care 5, no. 6 (2010): VII—X. http://dx.doi.org/10.1159/000323646.

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46

"Sachwortregister Band 5, 1995." Verhaltenstherapie 5, no. 4 (1995): 271. http://dx.doi.org/10.1159/000258955.

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47

"Band 21, Heft 5." Schweizerische Zeitschrift für Ganzheitsmedizin / Swiss Journal of Integrative Medicine 21, no. 5 (2009): 221. http://dx.doi.org/10.1159/000314183.

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"Inhalt Band 5, 2004." Dermatology and Psychosomatics / Dermatologie und Psychosomatik 5, no. 4 (2004): V—VI. http://dx.doi.org/10.1159/000083076.

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"Sachwortverzeichnis Band 5, 2004." Dermatology and Psychosomatics / Dermatologie und Psychosomatik 5, no. 4 (2004): 214. http://dx.doi.org/10.1159/000083110.

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50

Giordanetti, Piero, and Werner Stark. "Band 5: Kritik der Urteilskraft." Kant-Studien 91, s1 (2000). http://dx.doi.org/10.1515/kant.2000.91.s1.35.

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