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1.
J Synchrotron Radiat ; 30(Pt 5): 876-884, 2023 Sep 01.
Article in English | MEDLINE | ID: mdl-37462689

ABSTRACT

Single-crystal chemical vapour deposition (CVD) diamond detectors are an established transmissive synchrotron beamline diagnostic instrument used for beam position and beam intensity monitoring. A recently commercialized alternative is silicon carbide (4H-SiC) devices. These have the potential to provide the same diagnostic information as commercially available single-crystal CVD diamond X-ray beam position monitors, but with a much larger transmissive aperture. At Diamond Light Source an experimental comparison of the performance of single-crystal CVD diamond and 4H-SiC X-ray beam position monitors has been carried out. A quantitative comparison of their performance is presented in this paper. The single-crystal diamond and 4H-SiC beam position monitors were installed in-line along the synchrotron X-ray beam path enabling synchronous measurements at kilohertz rates of the beam motion from both devices. The results of several tests of the two position monitors' performance are presented: comparing signal uniformity across the surface of the detectors, comparing kHz intensity measurements, and comparing kHz beam position measurements from the detectors. Each test is performed with a range of applied external bias voltages. A discussion of the benefits and limitations of 4H-SiC and single-crystal CVD diamond detectors is included.

2.
Sci Rep ; 9(1): 5274, 2019 Mar 27.
Article in English | MEDLINE | ID: mdl-30918345

ABSTRACT

Realtime in situ temperature monitoring in difficult experimental conditions or inaccessible environments is critical for many applications. Non-contact luminescence decay time thermometry is often the method of choice for such applications due to a favorable combination of sensitivity, accuracy and robustness. In this work, we demonstrate the feasibility of an ultrafast PbI2 scintillator for temperature determination, using the time structure of X-ray radiation, produced by a synchrotron. The decay kinetics of the scintillations was measured over the 8-107 K temperature range using monochromatic pulsed X-ray excitation. It is found that lead iodide exhibits a very fast and intense scintillation response due to excitons and donor-acceptor pairs, with the fast decay component varying between 0.08 and 0.5 ns - a feature that can be readily exploited for temperature monitoring. The observed temperature dependence of the decay time is discussed in terms of two possible mechanisms of thermal quenching - transition over activation barrier and phonon-assisted escape. It is concluded that the latter provides a better fit to the experimental results and is consistent with the model of luminescence processes in PbI2. We evaluated the sensitivity and estimated the accuracy of the temperature determination as ca. ±6 K at 107 K, improving to ±1.4 K at 8 K. The results of this study prove the feasibility of temperature monitoring, using ultrafast scintillation of PbI2 excited by X-ray pulses from a synchrotron, thus enabling non-contact in-situ cryothermometry with megahertz sampling rate.

3.
Phys Rev Lett ; 121(5): 054802, 2018 Aug 03.
Article in English | MEDLINE | ID: mdl-30118307

ABSTRACT

We report on the observation of incoherent Cherenkov radiation emitted by a 5.3 GeV positron beam circulating in the Cornell electron-positron storage ring as the beam passes in the close vicinity of the surface of a fused silica radiator (i.e., at a distance larger than 0.8 mm). The shape of the radiator was designed in order to send the Cherenkov photons towards the detector, consisting of a compact optical system equipped with an intensified camera. The optical system allows both the measurements of 2D images and angular distribution including polarization study. The corresponding light intensity has been measured as a function of the distance between the beam and the surface of the radiator and has shown a good agreement with theoretical predictions. For highly relativistic particles, a large amount of incoherent radiation is produced in a wide spectral range. A light yield of 0.8×10^{-3} photon per particle per turn has been measured at a wavelength of 600±10 nm in a 2 cm long radiator and for an impact parameter of 1 mm. This will find applications in accelerators as noninvasive beam diagnostics for both leptons and hadrons.

4.
Opt Lett ; 16(2): 112-4, 1991 Jan 15.
Article in English | MEDLINE | ID: mdl-19773854

ABSTRACT

A novel sensor that uses tapere single-mode fibers is discussed. The tapered single-mode fiber is bent in a simple fixture to increase its sensitivity. Pressure sensors have been fabricated utilizing the bend-sensitive property of the biconically tapered single-mode fibers.

5.
Opt Lett ; 15(21): 1242-4, 1990 Nov 01.
Article in English | MEDLINE | ID: mdl-19771054

ABSTRACT

The modal power distribution technique is applied to a multimode optical fiber embedded in a three-dimensional composite material for real-time characterization and monitoring of the structure. The measurements on the modal power distribution within these fibers, and the subsequent redistribution induced by external perturbation, indicate that the modal power distribution technique is more sensitive than the intensity-modulation technique for smart-structure characterization.

6.
Appl Opt ; 25(15): 2469-70, 1986 Aug 01.
Article in English | MEDLINE | ID: mdl-20453968
7.
Appl Opt ; 18(8): 1167-71, 1979 Apr 15.
Article in English | MEDLINE | ID: mdl-20208903

ABSTRACT

Wave tank measurements on wind driven capillary waves were performed. The height, slope, and frequency content of the capillary waves were measured. The wave heights (trough to crest) were found to be in the 0.06-8.8-mm range for wind speeds in the 2.2-7.6-m/sec range. The distribution of frequencies (wavelengths)depends on wind speed, with more higher frequency waves occurring at higher wind speeds. The rms value of the wave slope plotted against the wind speed is an S-shaped curve with the steeply rising portion starting at ~3 m/sec. The maximum value of the rms wave slope measured in these experiments was 17.5 degrees and occurred at 7.6 m/sec.

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