Corrugation and Squat Classification and Detection with VGG16 and YOLOv5 Neural Network Models by Mohd Yazed, Muhammad Syukri, Mohd Yunus, Mohd Amin, Ahmad Shaubari, Ezak Fadzrin, Abdul Hamid, Nor Aziati, Amzah, Azmale, Md Ali, Zulhelmi

“…This study presents a novel approach utilizing deep learning models, VGG16 and YOLOv5, for detecting and classifying railway track defects, explicitly focusing on corrugation and squat defects. …”
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Effective 5D BIM requirements for risk mitigation during pre-contract stage. by Nazirul Fariq, Nazirul Fariq, Ismail, Syuhaida, Ab. Rani, Nur Izzati

“…As the development of BIM progresses, there are concerns related to the five-dimensional (5D) BIM procedures in producing deliverables from the cost aspects of the project that adopts BIM technology. …”
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Machine learning, IoT and 5G technologies for breast cancer studies: A review by Saroğlu, Havva Elif, Shayea, Ibraheem, Saoud, Bilal, Azmi, Marwan Hadri, El-Saleh, Ayman A., Saad, Sawsan Ali, Mohammad Alnakhli, Mohammad Alnakhli

“…Moreover, the advent of 5G technology in BC applications promises to revolutionize communication speeds and data transfer, enabling rapid and seamless transmission of large medical datasets. …”
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B cell receptor repertoire kinetics after SARS-CoV-2 infection and vaccination by Kotagiri, P, Mescia, F, Rae, WM, Bergamaschi, L, Tuong, ZK, Turner, L, Hunter, K, Gerber, PP, Hosmillo, M, Hess, C, Clatworthy, MR, Goodfellow, IG, Matheson, NJ, McKinney, EF, Wills, MR, Gupta, RK, Bradley, JR, Bashford-Rogers, RJM, Lyons, PA, Smith, KGC

“…Infection generates a broad distribution of SARS-CoV-2-specific clones predicted to target the spike protein, while a more focused response after vaccination mainly targets the spike's receptor-binding domain. …”

Numerical modelling of detonation reaction zone of nitromethane by EXPLO5 code and wood and kirkwood theory by Štimac, Barbara, Chan, Serene Hay Yee, Kunzel, Martin, Muhamed Suceska

“…The measured particle velocity profile of NM shows the existence of a sharp spike followed by a rapid drop over the first 5-10 ns (fast reaction). …”
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Thermoelectric properties of N-type Bi2Te2.7Se0.3 and P-type Bi0.5Sb1.5Te3 films for micro-cooler applications by Peng, Qi Zhen, San, Ye Ko, Khong, Samuel, Sim, Jonathan, Ezhilvalavan, Santhiagu, Ma, Jan, Hng, Huey Hoon

“…In this paper, we present the fabrication and analysis of thermoelectric thin films deposited by RF-magnetron sputtering from n-type Bi2Te2.7Se0.3 and p-type Bi0.5Sb1.5Te3 targets on a silicon substrate. X-ray diffraction, Scanning electron microscopy combined with energy dispersive spectrometry, electrical resistivity, Seebeck coefficient and thermal diffusivity measurements were used for the thermoelectric thin films characterization. …”
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An open-ended approach to enhance critical thinking skill in mathematics among secondary five normal (academic) pupils by Seoh, Bee Hua.

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AMIC Conference on Asian Communications : the Next Twenty-five Years, Singapore, Jun 1-3, 1996 : [contents]

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The first example of the two‐electron reduction of a phosphaalkyne – synthesis and structural characterisation of the diuranium(IV) pentalene complex [(U{η5‐C5Me5}{η8‐C8H4(SiiPr3‐1,4)2})2(μ‐η2:η1‐tBuCP)] by Tsoureas, N, Kilpatrick, A, Summerscales, OT, Nixon, JF, Cloke, FGN, Hitchcock, PB

“…The facile two‐electron reduction of the phosphaalkyne tBuC≡P by the UIII cyclopentadienyl–pentalene mixed‐sandwich complex [U(η5‐C5Me5){η8‐C8H4(SiiPr3)2}] is reported. A single‐crystal X‐ray structural analysis of the diuranium(IV) product [(U{η5‐C5Me5}{η8‐C8H4(SiiPr3)2})2(μ‐tBuCP)] shows that it contains a slightly unsymmetrical, bridging μ‐η2:η1‐ligated phosphaalkene dianion.…”

Low-cost incubator for live-cell imaging by Goh, Rui Si

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Modified cyclic shift tree denoising technique with fewer number of sweep for wave v detection / by Wan Siti Nur Aminah Wan Abdul Aziz, 1989-, author 612315, Sheikh Hussain Shaikh Salleh, 1958-, supervisor 455474, Fakulti Biosains dan Kejuruteraan Perubatan 538915

Polyethylenimine modified sugarcane bagasse adsorbent for the removal of reactive black 5 and methyl orange dyes / by Nurul Balqis Mohamed, 1994-, author 613693, Norzita Ngadi, 1976-, supervisor 411591, Fakulti Kejuruteraan Kimia Dan Kejuruteraan Tenaga 599090

Polyethylenimine modified sugarcane bagasse adsorbent for the removal of reactive black 5 and methyl orange dyes / by Nurul Balqis Mohamed, 1994- , author 613693

Superhydrophobic surface of Ti6Al4V using direct nanosecond laser texturing by Mohd Harizan, Zul, Mahadzir, Ishak, Aiman, Mohd Halil, Ramdziah, Md Nasir, Moinuddin, Mohammed Quazi

“…The results demonstrate a significant increase in surface roughness profiles such as Sa and Sq by 6 and 5 times, respectively, compared to the untextured surface. …”
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Atmospheric characterization of cold exoplanets using a 1.5-m coronagraphic space telescope by Maire, Anne-Lise, Galicher, Raphael, Boccaletti, Anthony, Baudoz, Pierre, Schneider, Jean, Stam, Daphne, Cahoy, Kerri, Traub, Wes

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Luminosity determination in pp collisions at  √𝑠 = 7 TeV using the ATLAS detector at the LHC by Aad, G., Abbott, B., Abdallah, J., Abdelalim, A. A., Abdesselam, A., Abdinov, O., Abi, B., Abolins, M., Abramowicz, H., Abreu, H., Acerbi, E., Acharya, B. S., Ackers, M., Adams, D. L., Addy, T. N., Adelman, J., Aderholz, M., Adomeit, S., Adragna, P., Adye, T.

“…Residual time- and μ-dependence between the methods is less than 2% for 0<μ<2.5. Absolute luminosity calibrations, performed using beam separation scans, have a common systematic uncertainty of ±11%, dominated by the measurement of the LHC beam currents. …”
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Measurement of the primary Lund jet plane density in proton-proton collisions at √s = 13 TeV by Hayrapetyan, A., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Damanakis, K., Dragicevic, M., Escalante Del Valle, A., Hussain, P. S., Jeitler, M., Krammer, N., Liko, D., Mikulec, I., Schieck, J., Schöfbeck, R., Schwarz, D.

“…The average density of emissions as function of ln(kT/GeV) and ln(R/∆R) is measured for jets with distance parameters R = 0.4 or 0.8, transverse momentum pT > 700 GeV, and rapidity |y| < 1.7. …”
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Search for dark QCD with emerging jets in proton-proton collisions at √𝑠 = 13 TeV by Hayrapetyan, A., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Damanakis, K., Dragicevic, M., Hussain, P. S., Jeitler, M., Krammer, N., Li, A., Liko, D., Mikulec, I., Schieck, J., Schöfbeck, R.

“…A search for “emerging jets” produced in proton-proton collisions at a center-of-mass energy of 13 TeV is performed using data collected by the CMS experiment corresponding to an integrated luminosity of 138 fb−1. …”
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Measurement of diferential ZZ + jets production cross sections in pp collisions at √s = 13 TeV by Hayrapetyan, A., Tumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Damanakis, K., Dragicevic, M., Escalante Del Valle, A., Hussain, P. S., Jeitler, M., Krammer, N., Liko, D., Mikulec, I., Schieck, J., Schöfbeck, R., Schwarz, D., Sonawane, M.

“…Diboson production in association with jets is studied in the fully leptonic final states, pp → (Z/γ*)(Z/γ*) + jets → 2ℓ2ℓ′ + jets, (ℓ, ℓ′ = e or μ) in proton-proton collisions at a center-of-mass energy of 13 TeV. The data sample corresponds to an integrated luminosity of 138 fb−1 collected with the CMS detector at the LHC. …”
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Precision measurement of the W boson mass with the CMS Experiment in pp collisions at √s = 13 TeV by Yang, Tianyu Justin

“…The result of this measurement is m_W = 80, 360.2 ± 2.4 (stat.) ± 9.6 (syst.) MeV,= 80, 360.2 ± 9.9 MeV, which is consistent with the standard model prediction m(SM/W) = 80, 354.5 ± 5.7 MeV.…”
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