Готові списки джерел за темами / Probe structure

Добірка наукової літератури з теми "Probe structure"

Автор: Grafiati
Опубліковано: 30 травня 2022
Оновлено: 31 травня 2022

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Статті в журналах з теми "Probe structure"

1

Liu, Yifang, Ruimin Liu, Xiang Wang, Jiaxin Jiang, Wenwang Li, Juan Liu, Shumin Guo, and Gaofeng Zheng. "Electrospun Three-Dimensional Nanofibrous Structure via Probe Arrays Inducing." Micromachines 9, no. 9 (August 24, 2018): 427. http://dx.doi.org/10.3390/mi9090427.

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The fast and precise direct-printing of micro three-dimensional (3D) structures is the important development trend for micro/nano fabrication technique. A novel method with probe arrays was built up to realize the controllable deposition of 3D electrospun nanofibrous structures. Firstly, several 3D nanofibrous structures were built on a single probe and 2-, 3-probes, which indicated that the probe height and probe interval played a key role on the 3D structure morphology. Then, different stereo nanofibrous structures based on multiprobe arrays were achieved accurately and the effects of processing parameters, including the probe height, probe interval, applied voltage and flow rate on the deposition behaviors of electrospun nanofiber over the probe arrays were investigated. The deposition area of 3D electrospun nanofibrous structures decreased with the increase of probe interval, applied voltage, and flow rate. Several 3D nanofibrous structures of special shapes including convex, triangle wave, inverted cone and complex curved surface were demonstrated by controlling the configuration of probe arrays and electrospinning parameters. This work provides an effective and simple way for the construction of 3D electrospun nanofibrous structures, which has great potentials in various medical and industrial applications.
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2

Livanova, Nadezhda, Svetlana Karpova, and Gennady Zaikov. "The Structure of Acrylonitrile-Butadiene Rubbers: Paramagnetic-Probe Study." Chemistry & Chemical Technology 7, no. 1 (March 10, 2013): 69–72. http://dx.doi.org/10.23939/chcht07.01.069.

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3

Chen, Guolong, Zheng Cao, and Weimin Zhang. "A Novel Planar Differential Koch Fractal Eddy Current Probe with Parallel Wound Topological Structure." Journal of Sensors 2021 (June 16, 2021): 1–13. http://dx.doi.org/10.1155/2021/6671189.

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Flexible planar eddy current probes are widely used to detect conductive components with complex surface. In this study, topological transformation is applied to design a differential Koch coil exciting eddy current probe. Two kinds of Koch exciting coils, Koch A and Koch B , were obtained by topological transformation from a three-dimensional differential exciting eddy current probe. Finite element model simulation is conducted to visualize the differences of eddy current distributions induced by the probes and get the defect signal. A detailed comparison is made among the two kinds of Koch eddy current probes and a circular eddy current probe by experiments. The experiments demonstrate that the sensitivity of the Koch A eddy current probe is higher than that of another two probes for detecting the defect which is shorter than the size of the probe. This work provides a novel method for improving the performance of eddy current probes in the coil structure design.
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4

Kimoto, Gunsei, Takehiro Watanabe, Souta Matsusaka, Akio Inoue, and Takaharu Kuroda. "New Development of Contact Probe and Methodology." Advanced Materials Research 126-128 (August 2010): 726–31. http://dx.doi.org/10.4028/www.scientific.net/amr.126-128.726.

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We present a new type of wafer probe card with resin film consisting of two beams. Resin film is embedded on both sides of the probe beam, having a thickness of 4 [μm] and made from polyimide. This proposed probe enables compliant structures with large overdrive to ensure high durability of the structure and controllable scrub motion to assure cleaning process. In this study, Matrix method is introduced for theoretical studies of the probe structure and commercial finite element code is used. Electrical contact resistance is determined by theoretical studies based on Holm's theory and experimentally by our measurement instrumentation respectively. The structure is proven theoretically to get appropriate scrub motion when it undergoes a large overdrive with preferable exhibited contact force. Moreover, all of these mechanical characteristics can be varied to know the values of the character of probes. The methodology having one of the most preferable characters of the contact-probe had been achieved.
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5

Chandler, Darrell P., Gregory J. Newton, Jonathan A. Small, and Don S. Daly. "Sequence versus Structure for the Direct Detection of 16S rRNA on Planar Oligonucleotide Microarrays." Applied and Environmental Microbiology 69, no. 5 (May 2003): 2950–58. http://dx.doi.org/10.1128/aem.69.5.2950-2958.2003.

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ABSTRACT A two-probe proximal chaperone detection system consisting of a species-specific capture probe for the microarray and a labeled, proximal chaperone probe for detection was recently described for direct detection of intact rRNAs from environmental samples on oligonucleotide arrays. In this study, we investigated the physical spacing and nucleotide mismatch tolerance between capture and proximal chaperone detector probes that are required to achieve species-specific 16S rRNA detection for the dissimilatory metal and sulfate reducer 16S rRNAs. Microarray specificity was deduced by analyzing signal intensities across replicate microarrays with a statistical analysis-of-variance model that accommodates well-to-well and slide-to-slide variations in microarray signal intensity. Chaperone detector probes located in immediate proximity to the capture probe resulted in detectable, nonspecific binding of nontarget rRNA, presumably due to base-stacking effects. Species-specific rRNA detection was achieved by using a 22-nt capture probe and a 15-nt detector probe separated by 10 to 14 nt along the primary sequence. Chaperone detector probes with up to three mismatched nucleotides still resulted in species-specific capture of 16S rRNAs. There was no obvious relationship between position or number of mismatches and within- or between-genus hybridization specificity. From these results, we conclude that relieving secondary structure is of principal concern for the successful capture and detection of 16S rRNAs on planar surfaces but that the sequence of the capture probe is more important than relieving secondary structure for achieving specific hybridization.
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6

Zheng, Guanghua, Fei Shui, Jinxin Hu, Xin Liu, and Huazhong Xiao. "Effects of probes with different structures on the flow field and measurement results of imported compressors." Xibei Gongye Daxue Xuebao/Journal of Northwestern Polytechnical University 39, no. 4 (August 2021): 858–64. http://dx.doi.org/10.1051/jnwpu/20213940858.

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In this paper, the measurement accuracy of two different types of total pressure probe and total temperature probe in turboshaft engine compressor inlet channel and the influence of these two probes on the flow field through numerical simulation was studied. At the same time, the influence of the probe structure and installation position on probe measurement results under three typical working conditions of cruise, maximum continuous and takeoff was analyzed. The simulation results showed that the higher the engine inlet flow rate, the greater the measurement error of the probe. Comparing with the total temperature probe, the total pressure probe measurement accuracy is more influenced by the flow rate. The velocity uniformity is less affected by the engine operating conditions and is mainly related to the structure of the inserted probes. The closer the total pressure probe to the support plate, the greater the measurement error. The probe installation position has a small effect on the total pressure loss coefficient at the outlet.
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7

AbdAlla, Ahmed N., Moneer A. Faraj, Fahmi Samsuri, Damhuji Rifai, Kharudin Ali, and Y. Al-Douri. "Challenges in improving the performance of eddy current testing: Review." Measurement and Control 52, no. 1-2 (November 16, 2018): 46–64. http://dx.doi.org/10.1177/0020294018801382.

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Eddy current testing plays an important role in numerous industries, particularly in material coating, nuclear and oil and gas. However, the eddy current testing technique still needs to focus on the details of probe structure and its application. This paper presents an overview of eddy current testing technique and the probe structure design factors that affect the accuracy of crack detection. The first part focuses on the development of different types of eddy current testing probes and their advantages and disadvantages. A review of previous studies that examined testing samples, eddy current testing probe structures and a review of factors contributing to eddy current signals is also presented. The second part mainly comprised an in-depth discussion of the lift-off effect with particular consideration of ensuring that defects are correctly measured, and the eddy current testing probes are optimized. Finally, a comprehensive review of previous studies on the application of intelligent eddy current testing crack detection in non destructive eddy current testing is presented.
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8

Luc Le, Xuan, Han Eul Lee, and Sung-Hoon Choa. "Deformation Behavior of Various Interconnection Structures Using Fine Pitch Microelectromechanical Systems (MEMS) Vertical Probe." Journal of Nanoscience and Nanotechnology 21, no. 5 (May 1, 2021): 2949–58. http://dx.doi.org/10.1166/jnn.2021.19132.

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Recently, fine pitch wafer level packaging (WLP) technologies have drawn a great attention in the semiconductor industries. WLP technology uses various interconnection structures including microbumps and through-silicon-vias (TSVs). To increase yield and reduce cost, there is an increasing demand for wafer level testing. Contact behavior between probe and interconnection structure is a very important factor affecting the reliability and performance of wafer testing. In this study, with a MEMS vertical probe, we performed systematic numerical analysis of the deformation behavior of various interconnection structures, including solder bump, copper (Cu) pillar bump, solder capper Cu bump, and TSV. During probing, the solder ball showed the largest deformation. The Cu pillar bump also exhibited relatively large deformation. The Cu bump began to deform at OD of 10 μm. At OD of 20 μm, bump pillar was compressed, and the height of the bump decreased by 8.3%. The deformation behavior of the solder capped Cu bump was similar to that of the solder ball. At OD of 20 μm, the solder and Cu bumps were largely deformed, and the total height was reduced by 11%. The TSV structure showed the lowest deformation, but exerted the largest stress on the probe. In particular, copper protrusion at the outer edge of the via was observed, and very large shear stress was generated between the via and the silicon oxide layer. In summary, when probing various interconnection structures, the probe stress is less than that when using an aluminum pad. On the other hand, deformation of the structure is a critical issue. In order to minimize damage to the interconnection structure, smaller size probes or less overdrive should be used. This study will provide important guidelines for performing wafer-level testing and minimizing damage of probes and interconnection structures.
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9

Yanagisawa, Keisuke, Ryunosuke Yoshino, Genki Kudo, and Takatsugu Hirokawa. "Inverse Mixed-Solvent Molecular Dynamics for Visualization of the Residue Interaction Profile of Molecular Probes." International Journal of Molecular Sciences 23, no. 9 (April 26, 2022): 4749. http://dx.doi.org/10.3390/ijms23094749.

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To ensure efficiency in discovery and development, the application of computational technology is essential. Although virtual screening techniques are widely applied in the early stages of drug discovery research, the computational methods used in lead optimization to improve activity and reduce the toxicity of compounds are still evolving. In this study, we propose a method to construct the residue interaction profile of the chemical structure used in the lead optimization by performing “inverse” mixed-solvent molecular dynamics (MSMD) simulation. Contrary to constructing a protein-based, atom interaction profile, we constructed a probe-based, protein residue interaction profile using MSMD trajectories. It provides us the profile of the preferred protein environments of probes without co-crystallized structures. We assessed the method using three probes: benzamidine, catechol, and benzene. As a result, the residue interaction profile of each probe obtained by MSMD was a reasonable physicochemical description of the general non-covalent interaction. Moreover, comparison with the X-ray structure containing each probe as a ligand shows that the map of the interaction profile matches the arrangement of amino acid residues in the X-ray structure.
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10

Yanagisawa, Keisuke, Ryunosuke Yoshino, Genki Kudo, and Takatsugu Hirokawa. "Inverse Mixed-Solvent Molecular Dynamics for Visualization of the Residue Interaction Profile of Molecular Probes." International Journal of Molecular Sciences 23, no. 9 (April 26, 2022): 4749. http://dx.doi.org/10.3390/ijms23094749.

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To ensure efficiency in discovery and development, the application of computational technology is essential. Although virtual screening techniques are widely applied in the early stages of drug discovery research, the computational methods used in lead optimization to improve activity and reduce the toxicity of compounds are still evolving. In this study, we propose a method to construct the residue interaction profile of the chemical structure used in the lead optimization by performing “inverse” mixed-solvent molecular dynamics (MSMD) simulation. Contrary to constructing a protein-based, atom interaction profile, we constructed a probe-based, protein residue interaction profile using MSMD trajectories. It provides us the profile of the preferred protein environments of probes without co-crystallized structures. We assessed the method using three probes: benzamidine, catechol, and benzene. As a result, the residue interaction profile of each probe obtained by MSMD was a reasonable physicochemical description of the general non-covalent interaction. Moreover, comparison with the X-ray structure containing each probe as a ligand shows that the map of the interaction profile matches the arrangement of amino acid residues in the X-ray structure.
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Дисертації з теми "Probe structure"

1

Jalloh, Muneer. "Probe diffusion and nanoscale structure in block copylymer hydrogels." Thesis, University of Sheffield, 2010. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.522408.

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2

Shin, Edward Matthew. "Strong gravitational lensing as a probe of galaxy structure." Thesis, University of Cambridge, 2008. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.612310.

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Le, Jenny Vi Le. "Tunable Nanocalipers to Probe Structure and Dynamics in Chromatin." The Ohio State University, 2018. http://rave.ohiolink.edu/etdc/view?acc_num=osu1543163132011865.

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4

Liu, Richard Yufeng. "Oxygen Transport as a Structure Probe for Amorphous Polymeric Systems." Case Western Reserve University School of Graduate Studies / OhioLINK, 2005. http://rave.ohiolink.edu/etdc/view?acc_num=case1103694304.

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5

Hu, Yushan. "OXYGEN TRANSPORT AS A STRUCTURE PROBE FOR HETEROGENEOUS POLYMERIC SYSTEMS." Case Western Reserve University School of Graduate Studies / OhioLINK, 2005. http://rave.ohiolink.edu/etdc/view?acc_num=case1112902488.

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6

Yang, Emma. "Chemical, metabolic and structure-activity relationships to probe abacavir toxicity." Thesis, University of Liverpool, 2014. http://livrepository.liverpool.ac.uk/2008286/.

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Adverse drug reactions (ADRs) are responsible for an increasing number of hospitalised patients, with the large majority of these ADRs classed as either type A or type B. Drug hypersensitivity reactions fall within the type B category and one such drug responsible for this form of ADR is abacavir (ABC). ABC, a nucleoside reverse transcriptase inhibitor, is used to treat the HIV-1 virus. It is responsible for a potentially life-threatening type IV hypersensitivity reaction which occurs in patients bearing the HLA-B*57:01 allele. Although many mechanisms have been proposed, it was the objective of this research to examine all these previous proposals to further extend and develop the mechanism of ABC toxicity. In Chapter 2, deuterated-ABC (D2-ABC) was designed and synthesised where the two 5'-H atoms were replaced with two 5'-D atoms. The design of this analogue was intended to retard the oxidative metabolism of ABC to its aldehyde and carboxylic acid metabolites. The synthesis of this compound was paramount to investigating this metabolism and through a series of metabolic experiments, described in Chapter 3, a kinetic isotope effect between ABC and D2-ABC was determined, ultimately showing an altered metabolism between the two compounds. To investigate binding of ABC within the HLA-B*57:01 protein, analogues of ABC, with alterations at varying positions within the molecule, were required. Using a racemic method, ABC enantiomers were synthesised and ABC’s enantiomer failed to stimulate T-cells in vitro. The creation of further analogues required the development of an asymmetric synthetic route. A total synthetic method was desired to synthesise intermediates to be used in future analogue synthesis. Finally, as described in Chapter 5, a range of 6-position analogues were designed, using a structure-activity relationship method, and synthesised, to further investigate the altered repertoire mechanism. These analogues, consisting of primary and secondary amine and oxy moieties, were subjected to in vitro immunological assays to determine their stimulation of T-cells. Additionally, the synthesised analogues were modelled in silico using molecular docking within the HLA protein. The in silico results assisted in explaining the basis of such T-cell activation/inactivation and will direct future analogue design. IC50 and EC50 values were determined for analogues that presented a negative T-cell response and a compound showing positive values was subjected to further pharmacokinetic testing. The oxidative metabolism of ABC was affected by isotopic substitution, but initial results have shown no altered T-cell stimulation of D2-ABC compared to ABC. This mechanism cannot be discarded, with further investigational work required. However, the synthesised 6-position analogues have assisted in further examining the altered repertoire mechanism and initial findings have enabled further understanding of the binding of ABC within HLA-B*57:01. This mechanism of ABC toxicity appears paramount to others proposed and the results presented in this thesis support this. Additional analogue synthesis and in vivo experiments will assist in confirming this further.
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7

Romero, G. E., S. P. Owocki, A. T. Araudo, R. H. D. Townsend, and P. Benaglia. "Using gamma-rays to probe the clumped structure of stellar winds." Universität Potsdam, 2007. http://opus.kobv.de/ubp/volltexte/2008/1821/.

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Gamma-rays can be produced by the interaction of a relativistic jet and the matter of the stellar wind in the subclass of massive X-ray binaries known as “microquasars”. The relativistic jet is ejected from the surroundings of the compact object and interacts with cold protons from the stellar wind, producing pions that then quickly decay into gamma-rays. Since the resulting gamma-ray emissivity depends on the target density, the detection of rapid variability in microquasars with GLAST and the new generation of Cherenkov imaging arrays could be used to probe the clumped structure of the stellar wind. In particular, we show here that the relative fluctuation in gamma rays may scale with the square root of the ratio of porosity length to binary separation, $sqrt{h/a}$, implying for example a ca. 10% variation in gamma ray emission for a quite moderate porosity, h/a ∼ 0.01.
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8

Vaumousse, David. "An atom probe study of fine scale structure in A1MgSi(Cu)." Thesis, University of Oxford, 2004. http://ethos.bl.uk/OrderDetails.do?uin=uk.bl.ethos.401025.

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9

Orbai, Lucian. "Using nucleic acid chemistry to probe telomeric DNA function and structure /." May be available electronically:, 2007. http://proquest.umi.com/login?COPT=REJTPTU1MTUmSU5UPTAmVkVSPTI=&clientId=12498.

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10

Cavanagh, Molly Christine. "Using the ultrafast pump-probe spectroscopy of atomic anions and the solvated electron to probe solvent structure and solvation dynamics." Diss., Restricted to subscribing institutions, 2008. http://proquest.umi.com/pqdweb?did=1581642021&sid=1&Fmt=2&clientId=1564&RQT=309&VName=PQD.

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Книги з теми "Probe structure"

1

Miller, M. K. Atom probe tomography: Analysis at the atomic level. New York: Kluwer Academic / Plenum Publishers, 2000.

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2

Generating prose: Relations, patterns, structures. New York: Macmillan, 1987.

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3

Duncan, Robert Edward. The structure of rime. San Francisco: Arion Press, 2008.

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4

How to prove it: A structured approach. 2nd ed. New York: Cambridge University Press, 2006.

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5

How to prove it: A structured approach. Cambridge [England]: Cambridge University, 1994.

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6

Hoffman, Greg H. Narrative structure in the later prose of Jurij Trifonov. Ann Arbor: University Microfilms International, 1993.

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7

Style and structure in the prose of Isaak Babel'. Columbus, Ohio: Slavica Publishers, 1986.

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8

Cameron, Kenneth Walter. Emersonʼs prose poem: The structure and meaning of Nature (1836). Hartford (Box A, Station A, Hartford 06106): Transcendental Books, 1988.

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9

The interlace structure of the third part of the prose Lancelot. Woodbridge, Suffolk [England]: D.S. Brewer, 2010.

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10

Telluride International Conference on Spin Observables of Nuclear Probes (1988). Spin observables of nuclear probes. New York: Plenum Press, 1988.

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Частини книг з теми "Probe structure"

1

Seiff, Alvin, and T. C. D. Knight. "The Galileo Probe Atmosphere Structure Instrument." In The Galileo Mission, 203–32. Dordrecht: Springer Netherlands, 1992. http://dx.doi.org/10.1007/978-94-011-2512-3_8.

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2

Wiesendanger, R. "Magnetic-Sensitive Scanning Probe Microscopy." In Magnetism and Structure in Systems of Reduced Dimension, 45–54. Boston, MA: Springer US, 1993. http://dx.doi.org/10.1007/978-1-4899-1519-1_5.

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3

Tobias, Irwin. "Circular Dichroism as a Probe of Tertiary Structure." In Structure and Dynamics of Biopolymers, 31–55. Dordrecht: Springer Netherlands, 1987. http://dx.doi.org/10.1007/978-94-009-3619-5_2.

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4

Thomson, Neil H. "Atomic Force Microscopy of DNA Structure and Interactions." In Applied Scanning Probe Methods VI, 127–64. Berlin, Heidelberg: Springer Berlin Heidelberg, 2007. http://dx.doi.org/10.1007/978-3-540-37319-3_5.

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5

Zuber, Kai. "Neutrinos as a probe of nuclear structure." In Neutrino Physics, 67–110. Third edition. | Boca Raton : CRC Press, 2020. | Series: Series in high energy physics, cosmology & gravitation: CRC Press, 2020. http://dx.doi.org/10.1201/9781315195612-4.

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Uehara, Ryuhei. "Canonical Data Structure for Interval Probe Graphs." In Algorithms and Computation, 859–70. Berlin, Heidelberg: Springer Berlin Heidelberg, 2004. http://dx.doi.org/10.1007/978-3-540-30551-4_73.

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Li, L., and T. Sakurai. "Atomic Structure of 6H-SiC (0001) and (000 $$\bar{1}$$ )." In Advances in Scanning Probe Microscopy, 65–90. Berlin, Heidelberg: Springer Berlin Heidelberg, 2000. http://dx.doi.org/10.1007/978-3-642-56949-4_3.

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8

Thomson, Neil H. "Atomic Force Microscopy of DNA Structure and Interactions." In Biosystems - Investigated by Scanning Probe Microscopy, 389–426. Berlin, Heidelberg: Springer Berlin Heidelberg, 2009. http://dx.doi.org/10.1007/978-3-642-02405-4_14.

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9

Hallgren, S. W., M. Rüdinger, and E. Steudle. "Root hydraulic properties of spruce measured with the pressure probe." In Structure and Function of Roots, 215–22. Dordrecht: Springer Netherlands, 1995. http://dx.doi.org/10.1007/978-94-017-3101-0_28.

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Hill, Walter E., Gregory W. Muth, James M. Bullard, Scott P. Hennelly, Jing Yuan, Wendy T. Grace, Douglas J. Bucklin, Michael A. Van Waes, and Charles M. Thompson. "Chemical Cleavage as a Probe of Ribosomal Structure." In The Ribosome, 257–69. Washington, DC, USA: ASM Press, 2014. http://dx.doi.org/10.1128/9781555818142.ch22.

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Тези доповідей конференцій з теми "Probe structure"

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Kaiser, W. J., L. D. Bell, M. H. Hecht, and L. C. Davis. "A New Scanning Probe Microscopy For Imaging Subsurface Interface Structure." In Scanned probe microscopy. AIP, 1991. http://dx.doi.org/10.1063/1.41424.

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2

Davidovich, M. V., V. P. Meschanov, and N. F. Popova. "Waveguide probe structure on microwave." In 1999 9th International Crimean Microwave Conference 'Microwave and Telecommunication Technology'. Conference Proceedings. IEEE, 1999. http://dx.doi.org/10.1109/crmico.1999.815270.

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3

Bogoslovsky, Andrey V., Ivan S. Kozhevnikov, and Lyubov K. Altunina. "Double-probe viscometer for rheokinetic measurements." In PROCEEDINGS OF THE ADVANCED MATERIALS WITH HIERARCHICAL STRUCTURE FOR NEW TECHNOLOGIES AND RELIABLE STRUCTURES. Author(s), 2018. http://dx.doi.org/10.1063/1.5083279.

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4

Machida, Ryuto, Ryusuke Toda, Keisuke Yoshiki, Shinsuke Hara, Katsumi Irokawa, Hirofumi Miki, Akira Kawazu, and Hiroki I. Fujishiro. "Effect of Types of Ga/Si(111) Reconstructed Structure on Growth Morphology of GaSb Island." In 20th International Colloquium on Scanning Probe Microscopy. Japan Society of Applied Physics, 2013. http://dx.doi.org/10.7567/jjapcp.1.011001.

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5

You, Yong Sing, David A. Reis, and Shambhu Ghimire. "High harmonics from solids probe Angstrom scale structure." In CLEO: QELS_Fundamental Science. Washington, D.C.: OSA, 2016. http://dx.doi.org/10.1364/cleo_qels.2016.ftu1n.3.

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6

Tang, Zhi-Yong, Tian-Hao Song, Li Ding, and Xing-Chang Wei. "A High Frequency Probe with End Launch Structure." In 2020 9th Asia-Pacific Conference on Antennas and Propagation (APCAP). IEEE, 2020. http://dx.doi.org/10.1109/apcap50217.2020.9245958.

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7

Li, Yong, Shuai Wang, ZhaoRui Chu, Jie Tang, Yang Xu, ZhuJun Ai, and HongTao Wang. "A new suspension structure of micro/nano probe." In International Symposium on Precision Engineering Measurement and Instrumentation, edited by Junning Cui, Jiubin Tan, and Xianfang Wen. SPIE, 2015. http://dx.doi.org/10.1117/12.2176017.

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8

Liu, Yifang, Ruimin Liu, Xiang Wang, Jiaxin Jiang, Wenwang Li, Juan Liu, Shumin Guo, and Gaofeng Zheng. "Electrospun Three-Dimensional Nanofibrous Structure via Probe Arrays Inducing." In 2018 IEEE 13th Annual International Conference on Nano/Micro Engineered and Molecular Systems (NEMS). IEEE, 2018. http://dx.doi.org/10.1109/nems.2018.8556954.

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9

Singh, N., B. I. Vashi, and W. C. Leung. "Sheath structure of a probe in a flowing magnetoplasma." In International Conference on Plasma Science (papers in summary form only received). IEEE, 1995. http://dx.doi.org/10.1109/plasma.1995.531724.

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10

Singh, N., and B. Vashi. "Sheath structure near a probe in a flowing plasma." In 1990 Plasma Science IEEE Conference Record - Abstracts. IEEE, 1990. http://dx.doi.org/10.1109/plasma.1990.110695.

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Звіти організацій з теми "Probe structure"

1

Ramsey, G. P. Using spin to probe hadronic structure. Office of Scientific and Technical Information (OSTI), December 1994. http://dx.doi.org/10.2172/515614.

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2

Malkin, A., M. Plomp, T. Leighton, B. Vogelstein, and K. Wheeler. Multi-Probe Investigation of Proteomic Structure of Pathogens. Office of Scientific and Technical Information (OSTI), January 2008. http://dx.doi.org/10.2172/926009.

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3

Shapiro, Daniel Benjamin. Polarized light scattering as a probe for changes in chromosome structure. Office of Scientific and Technical Information (OSTI), October 1993. http://dx.doi.org/10.2172/10107208.

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4

Frieman, J. A., and E. Gaztanaga. The three-point function as a probe of models for large-scale structure. Office of Scientific and Technical Information (OSTI), June 1993. http://dx.doi.org/10.2172/10171918.

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5

Frieman, J. A., and E. Gaztanaga. The three-point function as a probe of models for large-scale structure. Office of Scientific and Technical Information (OSTI), June 1993. http://dx.doi.org/10.2172/6280691.

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6

Leung, Waihung, S. T. Revankar, Yoshihiko Ishii, and Mamoru Ishii. Interfacial area and two-phase flow structure development measured by a double-sensor probe. Office of Scientific and Technical Information (OSTI), June 1992. http://dx.doi.org/10.2172/7291450.

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7

Hsu, Julia. Surface structure and analysis with scanning probe microscopy and electron tunneling spectroscopy. Final report. Office of Scientific and Technical Information (OSTI), May 1998. http://dx.doi.org/10.2172/758935.

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8

Leung, Waihung, S. T. Revankar, Yoshihiko Ishii, and Mamoru Ishii. Interfacial area and two-phase flow structure development measured by a double-sensor probe. Office of Scientific and Technical Information (OSTI), June 1992. http://dx.doi.org/10.2172/10169682.

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9

Peterson, E. S. Electronic excited states as a probe of surface adsorbate structure and dynamics in liquid xenon. Office of Scientific and Technical Information (OSTI), August 1992. http://dx.doi.org/10.2172/7180832.

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10

Peterson, Eric Scott. Electronic excited states as a probe of surface adsorbate structure and dynamics in liquid xenon. Office of Scientific and Technical Information (OSTI), August 1992. http://dx.doi.org/10.2172/10190845.

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