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2.
Phys Rev Lett ; 86(9): 1698-701, 2001 Feb 26.
Artigo em Inglês | MEDLINE | ID: mdl-11290227

RESUMO

The process e(+)e(-)-->mu(+)mu(-) has been studied by the SND detector at the VEPP-2M e(+)e(-) collider in the phi(1020)-resonance energy region. The measured effective phi meson leptonic branching ratio B(phi-->l(+)l(-)) identical with square root of B(phi-->e(+)e(-))B(phi-->mu(+)mu(-))] = (2.89 +/- 0.10 +/- 0.06) x 10(-4) agrees well with the Particle Data Group value B(phi-->e(+)e(-)) = (2.91 +/- 0.07) x 10(-4), confirming mu-e universality. Without additional assumption of mu-e universality the branching ratio B(phi-->mu(+)mu(-)) = (2.87 +/- 0.20 +/- 0.14) x 10(-4) was obtained.

3.
J Synchrotron Radiat ; 5(Pt 3): 176-8, 1998 May 01.
Artigo em Inglês | MEDLINE | ID: mdl-15263474

RESUMO

The main aim of the next-generation synchrotron radiation sources is to provide diffraction-limited undulator radiation in the 0.1-4 nm range with an average power of 10-1000 W and monochromaticity of 10(-3)-10(-4). A review of new accelerator technologies that could be used for the construction of such types of synchrotron radiation sources is given.

4.
J Synchrotron Radiat ; 5(Pt 3): 360-2, 1998 May 01.
Artigo em Inglês | MEDLINE | ID: mdl-15263510

RESUMO

A low-energy positron beam is a unique probe of materials. In high-energy electron and positron storage rings it is possible to generate intense synchrotron radiation with a photon energy of 1-3 MeV by installing a high-field (8-10 T) superconducting wiggler. High-energy photons are converted to low-energy positrons by using a suitable target-moderator system. For an 8 GeV electron storage ring at a beam current of 100 mA, final yields are estimated to be about 10(8)-10(10) slow-e(+) s(-1) or larger depending on the moderation efficiency, with the size of the positron source 10(1)-10(2) cm(2). In the present work a wiggler magnetic system of 10 T is proposed. The main parameters of the superconducting wiggler are presented.

5.
J Synchrotron Radiat ; 3(Pt 5): 201-6, 1996 Sep 01.
Artigo em Inglês | MEDLINE | ID: mdl-16702679

RESUMO

A low-energy positron beam is a unique probe of Fermi surfaces, defects, surfaces and interfaces. In high-energy electron and positron storage rings (E > 6 GeV) it is possible to generate intense synchrotron radiation with 1-3 MeV photons by installing a high-field superconducting wiggler. The strength of the wiggler should be ~8-12 T. High-energy photons are emitted from the wiggler and converted to low-energy positrons by using a suitable target-moderator system. For an 8 GeV electron storage ring at a beam current of 100 mA, final yields are estimated to be ~10(10)-10(12) (slow-e(+) s(-1)) with the size of positron source ~10(2)-10(3) cm(2). The possibility of increasing the brightness of the low-energy positron beam is discussed. Advantages of using synchrotron radiation for producing positrons are pointed out. The effect of a superconducting wiggler on the stored electron beam is also discussed.

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