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  1. No Access

    Article

    Microwave-Dimensional Measurements of Cylindrical Resonators for Primary Acoustic Thermometry

    Acoustic gas thermometry relies on the fundamental relationship between the speed of sound in a monatomic gas and its thermodynamic temperature. The speed of sound is calculated from the resonance frequencies ...

    R. J. Underwood, G. J. Edwards in International Journal of Thermophysics (2014)

  2. No Access

    Article

    A Novel Comparative Photothermal Method for Measuring Thermal Diffusivity

    A novel comparative method has been developed at the National Physical Laboratory (NPL) to measure the thermal diffusivity of semi-infinite samples without a priori knowledge of the boundary conditions. It is bas...

    M. Broussely, A. P. Levick, G. J. Edwards in International Journal of Thermophysics (2005)

  3. No Access

    Article

    Measurement of the Thermal Diffusivity of Solids with an Improved Accuracy

    A photothermal radiometry technique is being developed at the NPL with the goal of improving the accuracy of thermal diffusivity measurements. The principle is to perform a laser-induced thermal experiment whi...

    C. D. Martinsons, A. P. Levick, G. J. Edwards in International Journal of Thermophysics (2003)

  4. No Access

    Chapter and Conference Paper

    A Unified Framework for Atlas Matching Using Active Appearance Models

    We propose to use statistical models of shape and texture as deformable anatomical atlases. By training on sets of labelled examples these can represent both the mean structure and appearance of anatomy in med...

    T. F. Cootes, C. Beeston, G. J. Edwards in Information Processing in Medical Imaging (1999)

  5. Chapter and Conference Paper

    Active appearance models

    We demonstrate a novel method of interpreting images using an Active Appearance Model (AAM). An AAM contains a statistical model of the shape and grey-level appearance of the object of interest which can gener...

    T. F. Cootes, G. J. Edwards, C. J. Taylor in Computer Vision — ECCV’98 (1998)

  6. Chapter and Conference Paper

    Face recognition using active appearance models

    We present a new framework for interpreting face images and image sequences using an Active Appearance Model (AAM). The AAM contains a statistical, photo-realistic model of the shape and grey-level appearance ...

    G. J. Edwards, T. F. Cootes, C. J. Taylor in Computer Vision — ECCV’98 (1998)

  7. No Access

    Article

    Radiation Damage Mechanisms In Scintillator Materials: Applications to BaF2 and CeF3

    Results from recent radiation damage studies in high quality BaF2 and CeF3 crystals are presented. Optical absorption and electron paramagnetic resonance (EPR) techniques are used to identify specific radiation d...

    L. E. Halliburton, G. J. Edwards in MRS Online Proceedings Library (1994)

  8. No Access

    Article

    A temperature-dependent dispersion equation for congruently grown lithium niobate

    G. J. Edwards, M. Lawrence in Optical and Quantum Electronics (1984)

  9. No Access

    Article

    Stable clocks and the theory of relativity

    G.J. Edwards in Nature (1981)

  10. No Access

    Article

    Frequency of the methane-stabilized He–Ne laser at 88 THz measured to ±3 parts in 1011

    We have measured the frequency of methane-stabilized laser at 88 THz (3.39 µm) (ref. 1), by method which largely eliminates the uncertainties contributed by lower-frequency lasers used as transfer oscillators....

    D. J. E. Knight, G. J. Edwards, P. R. Pearce, N. R. Cross in Nature (1980)

  11. No Access

    Article

    Dislodgeable residues of parathion and carbophenothion in florida citrus: A weather model

    H. N. Nigg, J. C. Allen, R. W. King in Bulletin of Environmental Contamination an… (1978)

  12. No Access

    Article

    Dislodgeable residues of ethion in Florida citrus and relationships to weather variables

    Five different treatments of ethion on Valencia orange trees were compared for decay rates and for ethion monoxon and ethion dioxon production under different environmental conditions. The oxon metabolite leve...

    H. N. Nigg, J. C. Allen, R. F. Brooks in Archives of Environmental Contamination an… (1977)

  13. No Access

    Article

    Measurement of the frequency of the methane-stabilised laser at 3.39 µm and of the R(32) transition of CO2 at 10.17 µm

    ACCURATE, infrared, frequency and wavelength measurements now constitute the best means of determining the speed of light, and provide a link between the standards of length and time. We measured the frequency...

    T. G. BLANEY, C. C. BRADLEY, G. J. EDWARDS, B. W. JOLLIFFE, D. J. E. KNIGHT in Nature (1975)

  14. Article

    Measurement of the speed of light

    WE report here the completion of a determination of the speed of light at the National Physical Laboratory1. The value was obtained from the product of the measured frequency and the wavelength, determined throug...

    T. G. BLANEY, C. C. BRADLEY, G. J. EDWARDS, B. W. JOLLIFFE, D. J. E. KNIGHT in Nature (1974)

  15. Article

    Absolute Frequency Measurement of the R(12) Transition of CO2 at 9.3 µm

    THE frequency of a CO2 laser stabilized to the R(12) transition of CO2 has been measured with an accuracy better than one part in 109. This is part of an experiment at the National Physical Laboratory to determin...

    T. G. BLANEY, C. C. BRADLEY, G. J. EDWARDS, D. J. E. KNIGHT, P. T. WOODS in Nature (1973)

  16. No Access

    Chapter and Conference Paper

    Progress with a Determination of the Speed of Light

    The scheme for measuring the CO2 laser frequency (shown in the Introduction) consists of three separate frequency-mixing experiments using two lower-frequency lasers as transfer oscillators. If an accurate measur...

    T. G. Blaney, C. C. Bradley, G. J. Edwards in Atomic Masses and Fundamental Constants 4 (1972)

  17. No Access

    Chapter and Conference Paper

    Progress with a Determination of the Speed of Light

    Until recently the direct measurement of frequencies in the infra-red spectral region has not been possible because of the lack of suitable detectors and mixers with response times of the order of 10−13 to 10−14 ...

    C. C. Bradley, G. J. Edwards, D. J. E. Knight in Atomic Masses and Fundamental Constants 4 (1972)