• Title/Summary/Keyword: Photon counting

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Impact of Photon-Counting Detector Computed Tomography on Image Quality and Radiation Dose in Patients With Multiple Myeloma

  • Alexander Rau;Jakob Neubauer;Laetitia Taleb;Thomas Stein;Till Schuermann;Stephan Rau;Sebastian Faby;Sina Wenger;Monika Engelhardt;Fabian Bamberg;Jakob Weiss
    • Korean Journal of Radiology
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    • v.24 no.10
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    • pp.1006-1016
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    • 2023
  • Objective: Computed tomography (CT) is an established method for the diagnosis, staging, and treatment of multiple myeloma. Here, we investigated the potential of photon-counting detector computed tomography (PCD-CT) in terms of image quality, diagnostic confidence, and radiation dose compared with energy-integrating detector CT (EID-CT). Materials and Methods: In this prospective study, patients with known multiple myeloma underwent clinically indicated whole-body PCD-CT. The image quality of PCD-CT was assessed qualitatively by three independent radiologists for overall image quality, edge sharpness, image noise, lesion conspicuity, and diagnostic confidence using a 5-point Likert scale (5 = excellent), and quantitatively for signal homogeneity using the coefficient of variation (CV) of Hounsfield Units (HU) values and modulation transfer function (MTF) via the full width at half maximum (FWHM) in the frequency space. The results were compared with those of the current clinical standard EID-CT protocols as controls. Additionally, the radiation dose (CTDIvol) was determined. Results: We enrolled 35 patients with multiple myeloma (mean age 69.8 ± 9.1 years; 18 [51%] males). Qualitative image analysis revealed superior scores (median [interquartile range]) for PCD-CT regarding overall image quality (4.0 [4.0-5.0] vs. 4.0 [3.0-4.0]), edge sharpness (4.0 [4.0-5.0] vs. 4.0 [3.0-4.0]), image noise (4.0 [4.0-4.0] vs. 3.0 [3.0-4.0]), lesion conspicuity (4.0 [4.0-5.0] vs. 4.0 [3.0-4.0]), and diagnostic confidence (4.0 [4.0-5.0] vs. 4.0 [3.0-4.0]) compared with EID-CT (P ≤ 0.004). In quantitative image analyses, PCD-CT compared with EID-CT revealed a substantially lower FWHM (2.89 vs. 25.68 cy/pixel) and a significantly more homogeneous signal (mean CV ± standard deviation [SD], 0.99 ± 0.65 vs. 1.66 ± 0.5; P < 0.001) at a significantly lower radiation dose (mean CTDIvol ± SD, 3.33 ± 0.82 vs. 7.19 ± 3.57 mGy; P < 0.001). Conclusion: Whole-body PCD-CT provides significantly higher subjective and objective image quality at significantly reduced radiation doses than the current clinical standard EID-CT protocols, along with readily available multi-spectral data, facilitating the potential for further advanced post-processing.

Measurement of fluorecence decay times of single molecules in solution (용액내 단분자의 형광소멸시간 계측)

  • 고동섭
    • Korean Journal of Optics and Photonics
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    • v.10 no.1
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    • pp.1-4
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    • 1999
  • A confocal microscope system was used to study the bursts of fluorescence photons from single dye molecules excited at 638 nm by a short-pulsed diode laser with a repetition rate of 17 MHz. A red dye, JA22, in ethylene glycol solution was used as a sample. The fluorescence decay curves of single molecules were acquired using a time-correlated single photon counting and analyzed by a maximum likelihood estimator. It was possible to measure the fluorescence decay times with an error probability of 21% at photon number of more than 40 per dye molecule.

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Absolute Measurement of the Quantum Efficiency of Photodetectors Using Correlated Photon Pairs (광자쌍을 이용한 광검출기의 양자효율 절대측정)

  • 안경진
    • Korean Journal of Optics and Photonics
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    • v.4 no.4
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    • pp.452-456
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    • 1993
  • The quantum efficiencies of photomultiplier tubes were measured by counting the coincidence photon pairs generated in the process of spontaneous parametric down-conversion. They were measured within 3% accuracy over the range of wavelength from 560 to 850 nm without any standard light source or detector. The values for 633 nm correspond to those obtained with a calibrated laser power meter within the measurement error.

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Study for energy transfer from Rhodamime 6G to Rhodamine B using time correlated single photon counting method (시간 상관 단일 광자 계수법에 의한 Rhodamine 6G에서 Rhodamine B로의 에너지 전달에 관한 연구)

  • 엄효순
    • Proceedings of the Optical Society of Korea Conference
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    • 1991.06a
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    • pp.69-73
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    • 1991
  • 모드 동기된 아르곤 이온 레이저를 여기광원으로 사용한 시간상관 단일 광자 계수장치를 이용하여 에탄올 용액 내에서 Rhodamine 6G에서 Rhodamine B로의 에너지 전달에 관하여 연구하였다. 측정된 형광 소멸 곡선은 본 실험실에서 개발한 full-fit program으로 deconvolution 하여 reduced concentration 과 critical transfer distance를 구했다. donor 의 농도가 acceptor의 농도보다 작을 경우에는 Foster 모델이 클 경우에는 Huber 모델이 잘 맞음을 확인하였다.

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Time-resolved UV Fluorescence Spectroscopy of Aorta and its Related Chromophores, Collagen and Elastin, Using 320 nm Excitaion

  • Park, Young D.
    • Bulletin of the Korean Chemical Society
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    • v.15 no.3
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    • pp.249-256
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    • 1994
  • Fluorescence time decay of human aorta has been measured at 380, 440, 480 nm using 320 nm excitation and time-correlated single photon counting technique. Fluorescence decay was found to be nonexponential at all emission frequencies. The normal and diseased sample showed significantly different fluorescence behaviors at 380 nm while this time decay difference was decreased in the fluorescence at 440 and 480 nms. The decay data were multiexponential and were analyzed with two exponential decay constants. The fluorescence decays were compared with and analyzed in terms of collagen and elastin.

Development of a Multi-Channel Photoelectric Photometer Using Optical Fiber

  • Lee, W.B.;Kim, H.I.;E.C.Sung;Moon, I.K.
    • Bulletin of the Korean Space Science Society
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    • 1992.10a
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    • pp.231-238
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    • 1992
  • We have developed a proto-type four-channel photoelectric photometer and control software for the 61-cm reflector of the Sobaeksan Astronomy Observatory. The photometer consists of five main units which has a manipulator, a set of four-opticsassemblies, a light detection units, Pulse counting electronics and a host computer. The software to control the chopper, filter wheel and photon counter has also been developed..

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Polarized Light Emission of Liquid Crystalline Polymer Blends (액정성 고분자 블렌드의 편발광)

  • 김영철;조현남;김동영;홍재민;송남웅
    • Polymer(Korea)
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    • v.24 no.2
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    • pp.211-219
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    • 2000
  • Fluorene-based light emitting polymer blends with liquid crystalline characteristics were studied on effective energy transfer and dichroic characteristics. Incorporating 0.5 wt% of the non-liquid crystalline into the liquid crystalline polymer suppressed the PL emission at 420 nm on photoexcitation at 360 nm, but generated a new PL emission of the non-liquid crystalline polymer at 480 nm. The highest PL intensity at 480 nm, which was 13 times stronger than those of the two polymers before blending, was observed for a blend with 2.0 wt% of the non-liquid crystalline polymer. When the molecules of the blends were aligned on a rubbed polyimide surface by a heating-cooling process, the dichroic ratio and the order parameter were 2.0 and 0.25, respectively. Time-correlated single photon counting (TCSPC) study revealed that the time required for energy transfer between the two chromophores was shortened by 93 ps when the blends were aligned on the rubbed polyimide surface by the heating-cooling process. The thermal treatment also enhanced the energy transfer efficiency by 9%.

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The fourth-order interference between entangled state photon pairs with different frequencies (진동수가 서로 다른 얽힘상태 광자쌍의 4차 간섭)

  • Kim, Heon-Oh;Ko, Jeong-Hoon;Kim, Tae-Soo
    • Korean Journal of Optics and Photonics
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    • v.13 no.4
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    • pp.308-313
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    • 2002
  • One of the nonclassical effects in two-photon interference experiments, spatial quantum beating, is observed in fourth-order interference with pairs of photons produced by a spontaneous parametric down-conversion process. When photon pairs in different frequencies $\omega1$ and $\omega2$ are mixed together, and directed to two detectors, the coincidence counts exhibit a cosine modulation with difference frequency | $\omega1$- $\omega2$|. The measured coincidence counts turned out to have an interference pattern with periodicity of 10.45 ㎛ in position or 34.82fs in time delay, which corresponds to the period 2$\pi$/| $\omega1$- $\omega2$| for the beat frequency of 0.29${\times}10^{14}$Hz.

Quantum Interference Experiments with Frequency Entangled Photon Pairs at 1.5 ㎛ Telecommunication Band (1.5 ㎛ 통신파장대역 진동수 얽힘 광자쌍의 양자간섭)

  • Kim, Heon-Oh;Kim, Yong-Soo;Youn, Chun-Ju;Cho, Seok-Beom
    • Korean Journal of Optics and Photonics
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    • v.22 no.6
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    • pp.276-282
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    • 2011
  • We performed experiments on Hong-Ou-Mandel type two-photon interference with frequency entangled photon pairs at 1.5 ${\mu}m$ telecommunication band generated through femtosecond pulsed spontaneous parametric down-conversion. Two different angular frequencies ${\omega}_1$ and ${\omega}_2$ were selected using CWDM(coarse wavelength division multiplexing) filters at the output ports of the interferometer. The coincidence counting rates were measured with varying path-length difference between the two interferometer arms to observe the two-photon interference patterns of spatial beating. The obtained visibilities in the net coincidence were close to the theoretical limit of 100%.

Improvement of Hong-Ou-Mandel Interference Visibility by Using a Single-Mode Optical-Fiber Photon Collector (단일모드 광섬유 집광기를 이용한 Hong-Ou-Mandel 간섭 가시도 향상)

  • Han, Sung-Wook;Kim, Heonoh;Seo, Joo Yeon;Kim, Myung-Whun
    • New Physics: Sae Mulli
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    • v.68 no.12
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    • pp.1374-1377
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    • 2018
  • We achieved 95% visibility in the Hong-Ou-Mandel interference experiment while we achieved only 56% visibility in a previous report. We used a 120 mW 405 nm single-mode continuous wave laser, a 5-mm-thick type-1 ${\beta}$-barium borate single crystal, standard Hong-Ou-Mandel interferometer optics, two avalanche photodiode single-photon counters, and a homemade coincidence counting unit. The photon collection unit was the key difference between the present study and the previous study. In the present experiment, we used single-mode optical fibers for photon collection, which suppressed accidental coincidence between-different mode photons by acting as a spatial filter because of its core size being much smaller than a multi-mode fiber.