cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.5281/zenodo.3375205
title: LBM dynamism analysis with MERIC

description: Lattice Boltzmann method (LBM) application analysis using READEX approach provided by MERIC library. Exhaustive algorithm has been used for state space search. This data has been measured on a single node of TU Dresden Taurus supercomputer powered by two Intel Xeon CPUs E5-2680v3 (codename Haswell). HDEEM system has been used for energy measurement.
description: {"references": ["LBM benchmark repository: https://baltig.infn.it/schifano/d2q37-bench-aos", "MERIC repository: https://code.it4i.cz/vys0053/meric"]}
DOI: 10.5281/zenodo.3375559
title: COMPOSITION Fill Level Sensors Datasets

description: The Smart Waste Management scenario is one of the main use cases of the COMPOSITION EU Project. In this scenario a real-time monitoring framework has set up for the monitoring of bins' fill level in pilot partners' sites. The deployed datasets contains measurement coming from the deployed bins fill level sensors. These datasets are public available after partners, KLEEMANN Hellas SA and ELDIA SA consent to share their data for a period from 1 to 2 months.
description: The first dataset is about indoor bins' fill level monitoring The second dataset is about the fill level monitoring of an outdoors open top container More details about the sensor modules were used for these measurements are available in references sections
description: {"references": ["Sensors modules details: https://www.composition-project.eu/wp-content/uploads/2019/02/D7.7_On-Site_Readiness_Assessment_of_Use_Cases_Based_on_Existing_Sensor_Infrastructure_II.pdf"]}
DOI: 10.5281/zenodo.3375560
title: COMPOSITION Fill Level Sensors Datasets

description: The Smart Waste Management scenario is one of the main use cases of the COMPOSITION EU Project. In this scenario a real-time monitoring framework has set up for the monitoring of bins' fill level in pilot partners' sites. The deployed datasets contains measurement coming from the deployed bins fill level sensors. These datasets are public available after partners, KLEEMANN Hellas SA and ELDIA SA consent to share their data for a period from 1 to 2 months.
description: The first dataset is about indoor bins' fill level monitoring The second dataset is about the fill level monitoring of an outdoors open top container More details about the sensor modules were used for these measurements are available in references sections
description: {"references": ["Sensors modules details: https://www.composition-project.eu/wp-content/uploads/2019/02/D7.7_On-Site_Readiness_Assessment_of_Use_Cases_Based_on_Existing_Sensor_Infrastructure_II.pdf"]}
DOI: 10.5281/zenodo.3375578
title: rdemolgen/MNV-test-data: Published version for journal paper.

description: A BAM file containing five MNVs (Multiple Nucleotide Variants) for the purposes of testing bioinformatics pipelines.
DOI: 10.5281/zenodo.3375579
title: rdemolgen/MNV-test-data: Published version for journal paper.

description: A BAM file containing five MNVs (Multiple Nucleotide Variants) for the purposes of testing bioinformatics pipelines.
DOI: 10.5519/qd.4fgspr0m
title: Query on the Natural History Museum Data Portal (data.nhm.ac.uk) (4402345 records)
DOI: 10.7910/dvn/8a1xo3/1junhi
title: cauliflower-angle-0-trial-1.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/1oq4ei
title: cauliflower-angle-90-trial-6.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/3mgxrd
title: banana-angle-0-trial-0.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/50u9jf
title: cantaloupe-angle-90-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/58poiw
title: apple-angle-90-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/6obyym
title: honeydew-angle-90-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/a3rmqv
title: lettuce-angle-0-trial-3.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/bauz71
title: carrot-angle-0-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/cfttz5
title: lettuce-angle-0-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/ewy6np
title: grape-angle-0-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/fel2lp
title: broccoli-angle-0-trial-6.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/gs4odx
title: cantaloupe-angle-90-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/hsy5dq
title: strawberry-angle-0-trial-6.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/hxqvdy
title: banana-angle-0-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/i93pou
title: cantaloupe-angle-90-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/ixgkhn
title: carrot-angle-90-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/jqip0d
title: honeydew-angle-0-trial-6.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/jxj9vm
title: lettuce-angle-0-trial-2.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/pw0hxi
title: celery-angle-90-trial-3.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/r69nto
title: grape-angle-90-trial-3.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/r6vv8c
title: banana-angle-0-trial-0.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/rogaji
title: grape-angle-0-trial-3.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/slytht
title: apple-angle-90-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/u8mt07
title: banana-angle-0-trial-1.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/xsivsh
title: honeydew-angle-90-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/yiskpe
title: spinach-angle-0-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/yvq6m0
title: cauliflower-angle-0-trial-1.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/z2k1qw
title: pepper-angle-0-trial-1.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/zcxukz
title: celery-angle-0-trial-4.zip

description: :unav
DOI: 10.17632/xgmh9x8yp8.1
title: thermal ductivity and tensile strength of SiC/Al-17Si-3.5Cu

description: thermal ductivity and tensile strength
DOI: 10.25919/5d5f48acb8618
title: Parkes observations for project P1006 semester 2019APRS_15

description: We propose observations with the ultra-wide-bandwidth, low-frequency receiver installed at the Parkes telescope to carry out the first ultra-high time resolution, coherently de-dispersed search for pulsars in globular clusters. We have chosen the 11 most likely clusters for new discoveries. These clusters all have at least three pulsars already known allowing us to have a precise estimate of the pulsar dispersion measures and our observations will provide the first ultra-wide-bandwidth observation of these pulsars. Our observing strategy will enable us to search for extremely narrow pulsars and even pulsars with sub-millisecond periods.
DOI: 10.25919/5d5f48eba29ec
title: Parkes observations for project P958 semester 2019APRS_73

description: Fast radio bursts (FRBs) continue to raise more questions than they answer. Until a few months ago, only one burst – the only one known to repeat - had been localized to a bright radio nebula (either a young supernova remnant or pulsar wind nebulae) in a distant dwarf galaxy. Over the last year searches with the Australian Square Kilometre Array Pathfinder (ASKAP) have detected 28 bursts, two of which have been localised to host galaxies at redshifts &gt; 0.3. These bursts and their hosts are very unlike the repeater, suggesting there may be a dichotomy in the population. Over the next six months we expect to detect another 12 FRBs, which will also have sub-arcsecond localisations. Here we propose to search this population for repeats. Our comprehensive sample and a dense monitoring campaign of well localised bursts, at a fluence limit more than 60 times lower than that of their detections, will either confirm the presence of additional repeating FRBs or the uniqueness of FRB 121102 amongst the population.
DOI: 10.7910/dvn/8a1xo3/2lrkbx
title: grape-angle-0-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/3iwfj8
title: banana-angle-0-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/cy6npz
title: grape-angle-90-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/dphmjm
title: carrot-angle-90-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/e5upyk
title: pepper-angle-0-trial-1.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/fadqvl
title: strawberry-angle-0-trial-6.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/fazu0c
title: carrot-angle-90-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/h5s6u5
title: cauliflower-angle-0-trial-1.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/izovug
title: honeydew-angle-0-trial-6.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/jg2vbo
title: honeydew-angle-0-trial-6.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/kdqwyr
title: lettuce-angle-0-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/l7o6ql
title: celery-angle-90-trial-1.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/n8qjic
title: apple-angle-90-trial-2.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/o153iz
title: broccoli-angle-0-trial-6.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/p0kpud
title: celery-angle-90-trial-3.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/pjnhwb
title: carrot-angle-0-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/qide2c
title: apple-angle-90-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/s8gksk
title: cauliflower-angle-90-trial-6.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/tuadx8
title: celery-angle-0-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/uhnrhg
title: pepper-angle-0-trial-8.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/uwqlfe
title: celery-angle-90-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/w5praa
title: honeydew-angle-90-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/ws9edj
title: kale-angle-0-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/xmbrct
title: red_grape-angle-0-trial-1.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/y5ckyr
title: honeydew-angle-90-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/zs5nug
title: cauliflower-angle-90-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/zvo8eo
title: grape-angle-90-trial-4.zip

description: :unav
DOI: 10.14457/cu.the.2008.1732
title: Preparation of citric acid-doped polyaniline fibrous membrane by electrospinning for ammonia sensing

description: Electrospinning is one of the simplest techniques for obtaining ultrafine fibers with diameter ranging from nanometer to sub-micrometers. In this study, electrospun mats of citric acid-doped polyaniline (PANi) blended polyvinyl alcohol (PVA) were prepared. Due to electrospinning PANi alone is difficult as limited by its molecular weight and solubility, blending PANi with PVA was employed to assist in fiber formation. The morphology, diameter, and structure of electrospun fibers were investigated by Scanning Electron Microscopy (SEM). The fibers had a diameter ranging from 400 nm to 700 nm. To producing fine fibers, the flow rate at 15 mL/min, the diameter of needle at 0.55 mm, the electric potential at 15 kV and distance between the needle and the collection screen at 25 cm were used. The electrospun fibers were regular, straight and uniform. These electrospun mats were then studied for ammonia gas sensing. The decrease of their resistance was observed when exposed to ammonia gas. Additionally, the ammonia sensing of this electrospun mat was reversible. The response time and recovery time were 5 and 10 minutes, respectively. The responses of repeated sensing of ammonia gas were reproducible up to 12 cycles. In the presence of 1 to 100 ppm of ammonia gas, the changes of resistance were well related to the concentration of ammonia gas. In comparison to PANi-PVA membrane by casting, the sensing of ammonia using PANi-PVA electrospun mat was better in sensitivity and shorter in response time and recovery time. In addition, the sensing of ammonia gas in real sample was performed. The concentrations of ammonia gas using PANi-PVA electrospun mat were comparable to those using commercial ammonia sensor.
DOI: 10.15468/vmblvz
title: A new species of the mud shrimp genus Axianassa Schmitt, 1924 (Decapoda: Gebiidea: Laomediidae) from the Ryukyu Islands, southern Japan

description: This dataset contains the digitized treatments in Plazi based on the original journal article Komai, Tomoyuki, Fujita, Yoshihisa (2019): A new species of the mud shrimp genus Axianassa Schmitt, 1924 (Decapoda: Gebiidea: Laomediidae) from the Ryukyu Islands, southern Japan. Zootaxa 4658 (3): 452-460, DOI: https://doi.org/10.11646/zootaxa.4658.3.2
DOI: 10.5281/zenodo.3372755
title: Simulations of shallow water wave turbulence

description: <strong>About</strong> This dataset curates all the simulations used to reproduce the paper: <em>Shallow water wave turbulence</em><br> DOI: 10.1017/jfm.2019.375 The source code and scripts necessary to generate the manuscript are archived at: https://github.com/ashwinvis/augieretal_jfm_2019_shallow_water See the README in the repository above to generate the manuscript <strong>Abstract</strong> The dynamics of irrotational shallow water wave turbulence forced at large scales and dissipated at small scales is investigated. First, we derive the shallow water analogue of the ‘four-fifths law’ of Kolmogorov turbulence for a third-order structure function involving velocity and displacement increments. Using this relation and assuming that the flow is dominated by shocks, we develop a simple model predicting that the shock amplitude scales as \((\epsilon d)^{1/3}\), where \( \epsilon\) is the mean dissipation rate and \(d\) the mean distance between the shocks, and that the \(p\)<sup>th</sup>-order displacement and velocity structure functions scale as \((\epsilon d)^{p/3} r/d\), where \(r\) is the separation. Then we carry out a series of forced simulations with resolutions up to 7680<sup>2</sup>, varying the Froude number,\(F_{f} = (\epsilon L_f)^{1/3}/ c \), where \(L_f\) is the forcing length scale and \(c\) is the wave speed. In all simulations a stationary state is reached in which there is a constant spectral energy flux and equipartition between kinetic and potential energy in the constant flux range. The third-order structure function relation is satisfied with a high degree of accuracy. Mean energy is found to scale approximately as \(E \sim \sqrt{\epsilon L_f c}\), and is also dependent on resolution, indicating that shallow water wave turbulence does not fit into the paradigm of a Richardson–Kolmogorov cascade. In all simulations shocks develop, displayed as long thin bands of negative divergence in flow visualizations. The mean distance between the shocks is found to scale as \( d \sim F_f^{1/2} L_f\). Structure functions of second and higher order are found to scale in good agreement with the model. We conclude that in the weak limit, \(F_f \rightarrow 0 \), shocks will become denser and weaker and finally disappear for a finite Reynolds number. On the other hand, for a given \(F_f\), no matter how small, shocks will prevail if the Reynolds number is sufficiently large.
DOI: 10.5281/zenodo.3372756
title: Simulations of shallow water wave turbulence

description: <strong>About</strong> This dataset curates all the simulations used to reproduce the paper: <em>Shallow water wave turbulence</em><br> DOI: 10.1017/jfm.2019.375 The source code and scripts necessary to generate the manuscript are archived at: https://github.com/ashwinvis/augieretal_jfm_2019_shallow_water See the README in the repository above to generate the manuscript <strong>Abstract</strong> The dynamics of irrotational shallow water wave turbulence forced at large scales and dissipated at small scales is investigated. First, we derive the shallow water analogue of the ‘four-fifths law’ of Kolmogorov turbulence for a third-order structure function involving velocity and displacement increments. Using this relation and assuming that the flow is dominated by shocks, we develop a simple model predicting that the shock amplitude scales as \((\epsilon d)^{1/3}\), where \( \epsilon\) is the mean dissipation rate and \(d\) the mean distance between the shocks, and that the \(p\)<sup>th</sup>-order displacement and velocity structure functions scale as \((\epsilon d)^{p/3} r/d\), where \(r\) is the separation. Then we carry out a series of forced simulations with resolutions up to 7680<sup>2</sup>, varying the Froude number,\(F_{f} = (\epsilon L_f)^{1/3}/ c \), where \(L_f\) is the forcing length scale and \(c\) is the wave speed. In all simulations a stationary state is reached in which there is a constant spectral energy flux and equipartition between kinetic and potential energy in the constant flux range. The third-order structure function relation is satisfied with a high degree of accuracy. Mean energy is found to scale approximately as \(E \sim \sqrt{\epsilon L_f c}\), and is also dependent on resolution, indicating that shallow water wave turbulence does not fit into the paradigm of a Richardson–Kolmogorov cascade. In all simulations shocks develop, displayed as long thin bands of negative divergence in flow visualizations. The mean distance between the shocks is found to scale as \( d \sim F_f^{1/2} L_f\). Structure functions of second and higher order are found to scale in good agreement with the model. We conclude that in the weak limit, \(F_f \rightarrow 0 \), shocks will become denser and weaker and finally disappear for a finite Reynolds number. On the other hand, for a given \(F_f\), no matter how small, shocks will prevail if the Reynolds number is sufficiently large.
DOI: 10.7910/dvn/3kno0s/gd4sxd
title: VitaminA_Banana_23AUG19_Final.xlsx

description: :unav
DOI: 10.7910/dvn/8a1xo3/1ivbfq
title: strawberry-angle-0-trial-6.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/4uyzre
title: pepper-angle-90-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/a8hrg1
title: banana-angle-0-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/b1jnxb
title: apple-angle-90-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/bbc5cd
title: celery-angle-90-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/d2s5gw
title: carrot-angle-0-trial-0.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/f2op2i
title: apple-angle-90-trial-2.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/fquvzh
title: red_grape-angle-90-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/g8acoy
title: kiwi-angle-0-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/hzqyfv
title: kale-angle-0-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/lbyfz2
title: cauliflower-angle-90-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/liepzq
title: kale-angle-0-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/mivcw2
title: pepper-angle-0-trial-8.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/n5ub21
title: lettuce-angle-0-trial-9.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/nj2h3c
title: grape-angle-0-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/obp7z0
title: red_grape-angle-0-trial-1.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/oivkj1
title: carrot-angle-90-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/pioitv
title: apple-angle-0-trial-8.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/pwntw3
title: celery-angle-90-trial-3.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/qojoks
title: carrot-angle-90-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/qpcnxl
title: cauliflower-angle-0-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/sq4jcu
title: celery-angle-90-trial-1.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/tkcqhl
title: kale-angle-0-trial-5.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/vdqehm
title: pepper-angle-0-trial-1.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/vunxgi
title: grape-angle-90-trial-4.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/ypwflf
title: tomato-angle-0-trial-2.zip

description: :unav
DOI: 10.7910/dvn/8a1xo3/zwtg2t
title: apple-angle-90-trial-2.zip

description: :unav
DOI: 10.14457/cu.the.2008.1733
title: Effects of synthesis methods on properties of ABO3 and A2BO4 perovskites

description: Ba0.5Sr0.5Co0.8Fe0.2O3-d(BSCF), La0.7Sr0.3Ga0.7Fe0.2Mg0.1O3-d (LSGFM), La0.8Sr0.2Ga0.8Mg0.15Co0.05O3-d (LSGCM), PrSrCoO4 (PSC), PrSrNiO4 (PSN) were investigated in the scope of reducing their particle sizes to improve the electrical conductivity and thermal expansion coefficient (TEC) for using as a new mixed electronic-ionic conducting materials in solid oxide fuel cells (SOFCs). The compounds were synthesized by sol gel and hydrothermal methods using various chelating agents. Characterized by XRD and SEM, BSCF, LSGFM and LSGCM perovskites showed single phase with cubic ABO3 structure whereas PSC and PSN displayed the tetragonal K2NiF4–type structure. Moreover, the crystallite and particle sizes of the perovskites synthesized by the hydrothermal method were smaller and more homogeneous than those of the sol gel method. Among all of the BSCFs, the BSCF synthesized by the sol gel method using ethylene glycol combined with citric acid as chelating agents showed highest conductivity (61.2 S/cm) at 550oC. For PSC and PSN the maximum conductivity was 202.6 S/cm at 800oC and 854.5 S/cm at 27oC respectively. In case of LSGFM and LSGCM, the values were 0.32 S/cm and 0.0246 S/cm at 800oC. Thermal expansion results, the smallest TEC value of BSCF was in the range of 15.6436-24.4395x10-6(oC) -1. TEC of PSC was 19.7471x10-6(oC) -1 whereas that of PSN was in the range of 11.8786-13.8377x10-6(oC)-1. TEC values of LSGFM and LSGCM were in the ranges of 14.1057-16.6132x10-6(oC)-1and 5.4556-14.0485 x10-6(oC) -1 respectively.
DOI: 10.14457/cu.the.2008.1734
title: 3-D Image reconstruction based on optical interferometry

description: Optical coherence tomography (OCT), based on a vertical scanning Michelson interferometer with a superluminescent diode (SLD), was applied for constructing a surface profile of material. To reduce time-consuming process, a parallel light beam and a CCD camera were set in this OCT. In this technique, each pixel of CCD camera acted as a separated light detector. Interferogram, taken by each pixel of CCD camera, was finally analyzed by two signal analysis methods. For comparing the efficiencies of two signal analysis methods, a continuous wavelet transform (CWT) and a discrete Fourier transform (DFT), surface profiles of a step-height standard plate were first individually determined by these two kinds of signal analysis methods. The result showed that the surface profile, constructed by CWT, was more closed to a real sample surface than the one constructed by DFT. Next, surface cross-sections of three stainless steel plates (Sample No.1, No.2 and No.3) were also defined by analyzing their interferograms with both CWT and DFT. For Sample No.1 and No.2, root-mean-square roughness (Rq) of cross-section, analyzed by CWT, was acceptable by comparing with the one, measured by SP-500 Series of Toray, used as a standard tool. But the uncertainty ranges of Rq for Sample No.3, analyzed with both methods, did not overlap with the ones measured by our standard tool. It was caused by the difference in analysis method and more surface roughness of this Sample No.3. Next, OCT with CWT was applied to construct surface profiles of these three samples, while their surfaces were covered with a cover slide. By comparing the profiles of covered surfaces with the uncovered ones, consistencies of their surface profiles were existed. Finally, this OCT was applied for measuring thickness of a cover slide. It was found that its thickness, measured by our OCT, was significantly closed to the one measured by ULM RUBIN 800 of MAHR.