John S. Bulmer
University of Cambridge
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Publication
Featured researches published by John S. Bulmer.
Applied Physics Letters | 2014
M. Cahay; P. T. Murray; T. C. Back; Steven B. Fairchild; John J. Boeckl; John S. Bulmer; Krzysztof Koziol; Gregg Gruen; Martin Sparkes; Francisco Orozco; W O'Neill
Hysteresis in the field emission (FE) data of a chemical vapor synthesized carbon nanotube fiber cathode is analyzed in the regime where self-heating effects are negligible. In both the forward and reverse applied field sweeps, various FE modes of operation are identified: including Fowler-Nordheim (FN) tunneling and space-charge limited emission from the fiber tip and FN emission from the fiber sidewall. Hysteresis in the FE data is linked to the difference in the field enhancement factors in the different FE modes of operation in the forward and reverse sweeps and related to changes in the fiber morphology.
IEEE Transactions on Applied Superconductivity | 2009
George A. Levin; Paul N. Barnes; Jose P. Rodriguez; Jake Connors; John S. Bulmer
We will discuss how stability and speed of normal zone propagation in YBCO-coated conductors is affected by interfacial resistance between the superconducting film and the stabilizer. Our numerical simulation has shown that the increased interfacial resistance substantially increases speed of normal zone propagation and decreases the stability margins. Optimization of the value of the resistance may lead to a better compromise between stability and quench protection requirements than what is found in currently manufactured coated conductors.
Superconductor Science and Technology | 2007
George A. Levin; Paul N. Barnes; John S. Bulmer
Abstract : A two-dimensional model is introduced that describes DC current sharing between the superconducting and normal metal layers in a configuration typical of YBCO-coated conductors. The model is used to compare the effectiveness of a surround stabilizer and a more conventional one-sided stabilizer. When the resistance of the interface between the superconductor and the stabilizer is low enough, the surround stabilizer is less effective than the one-sided stabilizer in stabilizing a hairline crack in the superconducting film.
Scientific Reports | 2015
John S. Bulmer; Jon Martens; Lukasz Kurzepa; Tomasz Gizewski; M. Egilmez; M. G. Blamire; Noorhana Yahya; Krzysztof Koziol
Recent progress with tailored growth and post-process sorting enables carbon nanotube (CNT) assemblies with predominantly metallic or semi-conducting concentrations. Cryogenic and microwave measurements performed here show transport dimensionality and overall order increasing with increasing metallic concentration, even in atmospheric doping conditions. By 120 GHz, the conductivity of predominantly semi-conducting assemblies grew to 400% its DC value at an increasing growth rate, while other concentrations a growth rate that tapered off. A generalized Drude model fits to the different frequency dependent behaviors and yields useful quality control parameters such as plasma frequency, mean free path, and degree of localization. As one of the first demonstrations of waveguides fabricated from this material, sorted CNTs from both as-made and post-process sources were inserted into sections of practical micro-strip. With both sources, sorted CNT micro-strip increasingly outperformed the unsorted with increasing frequency-- illustrating that sorted CNT assemblies will be important for high frequency applications.
Journal of Vacuum Science and Technology | 2008
C. Varanasi; John S. Bulmer; L. Brunke; J. Burke; J. Baca; K. Yost; Paul N. Barnes
In this study, metallic constantan (Cu55–Ni44–Mn1wt%) alloy substrates were investigated as an alternate choice of substrates to grow carbon nanotubes (CNTs). No additional catalysts were used other than the as-rolled and annealed substrates to process CNTs on them. High density CNT growth was observed to take place on these substrates when suitable conditions were used in a thermal chemical vapor deposition (CVD) furnace with C2H2 as the carbon precursor. Scanning electron microscopy and transmission electron microscopy on these samples indicated the presence of several micron long CNTs ranging in 20–100nm in diameter. Raman spectra taken from the samples confirmed the presence of G band peaks (peak at ∼1580cm−1) and D band peaks (peak at ∼1320cm−1) commonly observed in CVD grown multiwall CNT samples with varying intensity ratios depending on the processing conditions.
Journal of Applied Physics | 2012
Damir Latypov; John S. Bulmer
A full wave solution to the classical problem of a transient response in an RL circuit is analyzed. We show that when radiation effects are rigorously taken into account, the response differs from a familiar exponential decay. The circuit behaves more like an RLC circuit and can exhibit an underdamped response. As a result of a two way energy transfer between the circuit and the near field in the underdamped regime, despite the radiation losses, current decay may be slower than predicted by the standard RL circuit model. During a transient, when retardation effects become important, inductance can no longer be defined as a coefficient of proportionality between the magnetic flux through the circuit and the current in the circuit. If rate of current decay is nearly constant, one can define a time-dependent generalized inductance which turns into conventional inductance after time D/c, where D is the diameter of the current loop. Connection of this generalized inductance with the radiation damping problem is discussed. The theory developed in this paper has been used to analyze ultra wide band radiation observed during a fast laser triggered superconducting to normal transition of a superconducting switch.
national aerospace and electronics conference | 2011
Damir Latypov; John S. Bulmer
Radiation from superconducting current loops undergoing fast superconducting to normal (S-N) transitions is investigated. We consider 2 geometries: 1) a double loop configuration where current initially circulates in one loop and redirects /shunts to an adjacent loop and 2) A single loop that suddenly becomes resistive globally. For both geometries, we derive delayed integro-differential equations that fully take into account radiation and near field effects. Using a perturbation approach, we tie theory to experiment involving Ultra Wide Band (UWB) radiation from superconducting switches. Next we extrapolate parameters from this model, such as an effective inductance, that make the radiation more efficient. Focusing on the single loop geometry, we move away from the perturbation approach and explore regimes that fully incorporate radiation and the near field. We observe oscillatory behavior that departs from the classic RL circuit. These current oscillations are a result of a two way energy transfer between the circuit and the near field region. Practical applications of this type of a radiation source are also discussed.
Physical Review E | 2009
George A. Levin; Paul N. Barnes; J. P. Rodriguez; J. Connors; John S. Bulmer
We discuss the emergence of a spontaneous temperature and critical current spatial modulation in current-carrying high-temperature superconducting wire. The modulation of the critical current along the wire on a scale of 3-10 mm forces a fraction of the transport current to crisscross the resistive interface between the superconducting film and normal metal stabilizer attached to it. This generates additional heat that allows such a structure to be self-sustainable. Stability and the conditions for experimental observation of this phenomenon are also discussed.
Scientific Reports | 2017
John S. Bulmer; Agnieszka Lekawa-Raus; Dwight G. Rickel; Fedor Balakirev; Krzysztof Koziol
We explored high-field (60 T) magneto-resistance (MR) with two carbon nanotube (CNT) material classes: (1) unaligned single-wall CNTs (SWCNT) films with controlled metallic SWCNT concentrations and doping degree and (2) CNT fiber with aligned, long-length microstructure. All unaligned SWCNT films showed localized hopping transport where high-field MR saturation definitively supports spin polarization instead of a more prevalent wave function shrinking mechanism. Nitric acid exposure induced an insulator to metal transition and reduced the positive MR component. Aligned CNT fiber, already on the metal side of the insulator to metal transition, had positive MR without saturation and was assigned to classical MR involving electronic mobility. Subtracting high-field fits from the aligned fiber’s MR yielded an unconfounded negative MR, which was assigned to weak localization. It is concluded that fluctuation induced tunnelling, an extrinsic transport model accounting for most of the aligned fiber’s room temperature resistance, appears to lack MR field dependence.
Scientific Reports | 2017
John S. Bulmer; Thurid S. Gspann; Francisco Orozco; Martin Sparkes; Hilmar Koerner; A. Di Bernardo; Arkadiusz Niemiec; J. W. A. Robinson; Krzysztof Koziol; James A. Elliott; William O’Neill
Floating catalyst chemical vapor deposition uniquely generates aligned carbon nanotube (CNT) textiles with individual CNT lengths magnitudes longer than competing processes, though hindered by impurities and intrinsic/extrinsic defects. We present a photonic-based post-process, particularly suited for these textiles, that selectively removes defective CNTs and other carbons not forming a threshold thermal pathway. In this method, a large diameter laser beam rasters across the surface of a partly aligned CNT textile in air, suspended from its ends. This results in brilliant, localized oxidation, where remaining material is an optically transparent film comprised of few-walled CNTs with profound and unique improvement in microstructure alignment and crystallinity. Raman spectroscopy shows substantial D peak suppression while preserving radial breathing modes. This increases the undoped, specific electrical conductivity at least an order of magnitude to beyond that of single-crystal graphite. Cryogenic conductivity measurements indicate intrinsic transport enhancement, opposed to simply removing nonconductive carbons/residual catalyst.