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Malbrunot C, Amsler C, Arguedas Cuendis S, Breuker H, Dupre P, Fleck M, Higaki H, Kanai Y, Kolbinger B, Kuroda N, Leali M, Mäckel V, Mascagna V, Massiczek O, Matsuda Y, Nagata Y, Simon MC, Spitzer H, Tajima M, Ulmer S, Venturelli L, Widmann E, Wiesinger M, Yamazaki Y, Zmeskal J. The ASACUSA antihydrogen and hydrogen program: results and prospects. Philos Trans A Math Phys Eng Sci 2018; 376:rsta.2017.0273. [PMID: 29459412 PMCID: PMC5829175 DOI: 10.1098/rsta.2017.0273] [Citation(s) in RCA: 6] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Accepted: 12/18/2017] [Indexed: 06/08/2023]
Abstract
The goal of the ASACUSA-CUSP collaboration at the Antiproton Decelerator of CERN is to measure the ground-state hyperfine splitting of antihydrogen using an atomic spectroscopy beamline. A milestone was achieved in 2012 through the detection of 80 antihydrogen atoms 2.7 m away from their production region. This was the first observation of 'cold' antihydrogen in a magnetic field free region. In parallel to the progress on the antihydrogen production, the spectroscopy beamline was tested with a source of hydrogen. This led to a measurement at a relative precision of 2.7×10-9 which constitutes the most precise measurement of the hydrogen hyperfine splitting in a beam. Further measurements with an upgraded hydrogen apparatus are motivated by CPT and Lorentz violation tests in the framework of the Standard Model Extension. Unlike for hydrogen, the antihydrogen experiment is complicated by the difficulty of synthesizing enough cold antiatoms in the ground state. The first antihydrogen quantum states scan at the entrance of the spectroscopy apparatus was realized in 2016 and is presented here. The prospects for a ppm measurement are also discussed.This article is part of the Theo Murphy meeting issue 'Antiproton physics in the ELENA era'.
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Affiliation(s)
- C Malbrunot
- Experimental Physics Department, CERN, Genève 23, 1211, Switzerland
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
| | - C Amsler
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
| | - S Arguedas Cuendis
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
| | - H Breuker
- Ulmer Fundamental Symmetries Laboratory, RIKEN, Wako, Saitama 351-0198, Japan
| | - P Dupre
- Ulmer Fundamental Symmetries Laboratory, RIKEN, Wako, Saitama 351-0198, Japan
| | - M Fleck
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
| | - H Higaki
- Graduate School of Advanced Sciences of Matter, Hiroshima University, Hiroshima 739-8530, Japan
| | - Y Kanai
- Nishina Center for Accelerator-Based Science, RIKEN, Wako, Saitama 351-0198, Japan
| | - B Kolbinger
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
| | - N Kuroda
- Institute of Physics, The University of Tokyo, Komaba, Meguro-ku, Tokyo 153-8902, Japan
| | - M Leali
- Dipartimento di Ingegneria dell'Informazione, Università di Brescia, Brescia 25133, Italy
- Istituto Nazionale di Fisica Nucleare, Sez. di Pavia, 27100 Pavia, Italy
| | - V Mäckel
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
| | - V Mascagna
- Dipartimento di Ingegneria dell'Informazione, Università di Brescia, Brescia 25133, Italy
- Istituto Nazionale di Fisica Nucleare, Sez. di Pavia, 27100 Pavia, Italy
| | - O Massiczek
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
| | - Y Matsuda
- Institute of Physics, The University of Tokyo, Komaba, Meguro-ku, Tokyo 153-8902, Japan
| | - Y Nagata
- Department of Physics, Tokyo University of Science, Shinjuku, Tokyo 162-8601, Japan
| | - M C Simon
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
| | - H Spitzer
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
| | - M Tajima
- Institute of Physics, The University of Tokyo, Komaba, Meguro-ku, Tokyo 153-8902, Japan
| | - S Ulmer
- Ulmer Fundamental Symmetries Laboratory, RIKEN, Wako, Saitama 351-0198, Japan
| | - L Venturelli
- Dipartimento di Ingegneria dell'Informazione, Università di Brescia, Brescia 25133, Italy
- Istituto Nazionale di Fisica Nucleare, Sez. di Pavia, 27100 Pavia, Italy
| | - E Widmann
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
| | - M Wiesinger
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
| | - Y Yamazaki
- Ulmer Fundamental Symmetries Laboratory, RIKEN, Wako, Saitama 351-0198, Japan
| | - J Zmeskal
- Stefan-Meyer-Institut für Subatomare Physik, Österreichische Akademie der Wissenschaften, Boltzmanngasse 3, 1090 Wien, Austria
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Dupre P, Muller M, Wong Chi Man N, Le Penndu H, Foll Y, Collet M. Follow-Up of BI-RADS 3 Breast Mammograms, Results of a West France “Departement” Breast Cancer Screening Programme. Cancer Res 2009. [DOI: 10.1158/0008-5472.sabcs-09-4013] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 11/16/2022]
Abstract
Abstract
Background: French breast cancer screening program lies on a decentralized system. Each administrative division of a region (departement) organizes, coordinates and assesses their programme under the aegis of the French National Cancer Institute (INCa).The screening programme includes every two years, for women between 50 and 74 years of age a clinical examination and a breast mammogram. Conclusions are reported using the Breast Imaging and Reporting Data System (BI-RADS) of the American College of Radiology (ACR).French recommendations for low-suspicion lesions of the breast (BI-RADS 3) consist in a new screening 4 or 6 months later, then another one at one year and a third one year later before returning to the breast screening programme.Objectives: To evaluate the medical organisation and patients' observance for the follow-up of low suspicion breast lesions (BI-RADS 3).Material and Methods: Between January 2005 and January 2007 every BI-RADS 3 breast mammogram exams were listed in our departement and each radiologist was asked about their patient's health status.Patients who had not had their control mammogram were contacted.Their general practitioners were asked in case of no response.Results: Between January 2005 and January 2007 126 385 women were invited to take part in the breast cancer screening programme (screening rate 59.55%).2 209 exams were considered BI-RADS 3 (2.90%).383 patients (17.5%) were lost of sight.2111 women underwent an ultrasound scan examination (40.67%).20 women had MRI (0.39%).182 had biopsies (8.23%).BI-RADS 3 predictive value for a breast cancer lesion was 3.35%.Control mammograms were proposed at 4 months for 339 patients (18.7%) and 6 months for 1 125 patients (62.1%).1247 patients had only one control mammogram (60.9%), 388 (18.9%) patients had two and 60 (2.9%) had at least 3 controls.47.2% of BI-RADS 3 was re classified after first control and 60% after second control.Patients' observance was 91.26% for the first control, 62.9% for the second and decreased to 27% at fourth.1226 (55.5%) were re classified BI-RADS 1 or 2.185 (8.4%) were up graded to BI-RADS 4 or 5.154 (7%) are on attempt of re classification, 152 (6.90%) had no definitive conclusion after 24 months and 109 (4.90%) declined the medical follow-up supervision.The median time needed for re classified BI-RADS 3 was 276 days.Discussion: Our BI-RADS 3 rate (2.90%) is similar to those already published (3-7.7%).French recommendations are applied for the first and second control.Our cancer rate for BI-RADS 3 lesions (3.35%) is higher than those published (0.3%-1.7%).Patients' observance decreases rapidly, and patients' loss-of-sight remains high (17.3%).Initial BI-RADS 3 classification must be improved and recommendations for follow-up may be modified into a delayed control at 9 months that could settle for a BI-RADS 2 classification or lead to a histopathological exam.Waiting for new recommendations, we now contact each woman with BI-RADS 3 one month before control and in the absence of control we contact radiologist and general practitioner to improve observance and reduce the number of lost-of-sight patients.
Citation Information: Cancer Res 2009;69(24 Suppl):Abstract nr 4013.
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Affiliation(s)
- P. Dupre
- 1University Medical Center, Finistere, France
| | - M. Muller
- 1University Medical Center, Finistere, France
| | | | | | | | - M. Collet
- 1University Medical Center, Finistere, France
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Dupre P. Quasiunimodal tunable pulsed dye laser at 440 nm: theoretical development for using a quad prism beam expander and one or two gratings in a pulsed dye laser oscillator cavity. Appl Opt 1987; 26:860-871. [PMID: 20454235 DOI: 10.1364/ao.26.000860] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.1] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/29/2023]
Abstract
In the first section of this paper a theoretical discussion is presented for the performance of a pulsed dye laser oscillator cavity, without an intracavity etalon, using the Gaussian beam approximation. Optimal conditions for achievement of narrow spectral linewidth are discussed (location of the grating or of the beam expander). Various configurations of oscillator cavities are investigated, including a dispersive device composed of one grating and one virtual grating. The use of a beam expander is treated. We find that the same spectral linewidth is obtained theoretically for the optical cavity with two gratings as with one grating and a virtual grating. In the second part we describe the performance (in terms of spectral linewidth 1.3-GHz FWHM quasiunimodal structure, divergence of the beam, etc.) of the dye laser in light of the theoretical arguments. The complete laser contains an oscillator stage, a preamplifier stage, and an amplifier stage, each pumped by an UV beam (355 nm) from a pulsed Nd:YG laser.
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