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An efficient scheme of generating ultra-tightly focused proton bunch with radius in nanometer scale is proposed. A needlelike proton filament of transverse size in nanometer scale with the density of and charge quantity is obtained based on…

Accelerator Physics · Physics 2022-05-18 Q. Yu

We present the design of a Faraday cup-like charged particle detector in a four quadrant configuration aimed at facilitating the alignment of low-intensity beams of exotic particles. The device is capable of assessing the current on the…

Instrumentation and Detectors · Physics 2024-02-13 Kilian Brenner , Michael Zimmermann , Maik Butterling , Andreas Wagner , Christoph Hugenschmidt , Francesco Guatieri

We investigate the possibility that particles that are long-lived on cosmological scales, making up part or all of the dark matter, decay to neutrinos that have present-day energies around an eV. The neutrinos from these decays can…

High Energy Physics - Phenomenology · Physics 2019-07-23 David McKeen

Laser speckle, the granular intensity pattern arising from random optical interference, provides a high-dimensional encoding of spectral information that can be exploited for precision metrology. Speckle-based spectrometers have advanced…

The KArlsruhe TRItium Neutrino experiment (KATRIN) aims to measure the absolute neutrino mass scale with an unprecedented sensitivity of 0.2 eV/c2 (90% C.L.), using beta decay electrons from tritium decay. The kinetic energy of the decay…

Instrumentation and Detectors · Physics 2018-09-26 J. Letnev , W. Hazenbiller , A. Osipowicz , A. Beglarian , H. Bouquet , G. Drexlin , F. Glück , J. Garbe , H. Hillmer , P. Marte , T. Thümmler , Ch. Weinheimer

We propose a new experiment to search for a sterile neutrino in a few keV mass range at the "Troitsk nu-mass" facility. The expected signature corresponds to a kink in the electron energy spectrum in tritium beta-decay. The new goal…

The KATRIN experiment is designed to measure the absolute neutrino mass scale with a sensitivity of 200 meV at 90% C.L. by high resolution tritium beta-spectroscopy. A low background level of 10 mHz at the beta-decay endpoint is required in…

Instrumentation and Detectors · Physics 2015-06-04 S. Mertens , G. Drexlin , F. M. Fraenkle , D. Furse , F. Glueck , S. Goerhardt , M. Hoetzel , W. Kaefer , B. Leiber , T. Thuemmler , N. Wandkowsky , J. Wolf

Positronium is an ideal system for the research of the QED, especially for the QED in bound state. The discrepancy of 3.9\sigma is found recently between the measured HFS values and the QED prediction ($O(\alpha^3)$). It might be due to the…

High Energy Physics - Experiment · Physics 2015-03-13 S. Asai , T. Suehara , T. Yamazaki , G. Akimoto , A. Miyazaki , T. Namba , T. Kobayashi , H. Saito , T. Idehara , I. Ogawa , Y. Urishizaki , S. Sabchevski

Transmission electron microscopy (TEM) has reached ~ 50 picometer resolution in a high vacuum, enabling single-atom sensitive imaging of nanomaterials. Extending this capability to gaseous environments would allow for similar visualizations…

An ultra thin silicon detector called U3DTHIN has been designed and built for neutral particle analyzers (NPA) and thermal neutron detection. The main purpose of this detector is to provide a state-of-the-art solution for detector system of…

Instrumentation and Detectors · Physics 2018-01-03 F. Garcia , G. Pellegrini , M. Lozano , J. P. Balbuena , C. Fleta , C. Guardiola , D. Quirion

Monolithic CMOS pixel detectors have emerged as competitive contenders in the field of high-energy particle physics detectors. By utilizing commercial processes they offer high-volume production of such detectors. A series of prototypes has…

The new concept of the spherical TPC aims at relatively large target masses with low threshold and background, keeping an extremely simple and robust operation. Such a device would open the way to detect the neutrino-nucleus interaction,…

A custom, flat field, extreme ultraviolet EUV spectrometer built specifically for use with low power light sources that operate under ultrahigh vacuum conditions is reported. The spectral range of the spectrometer extends from 4 nm to 40…

The shape of the beta decay energy distribution is sensitive to the mass of the electron neutrino. Attempts to measure the endpoint shape of tritium decay have so far seen no distortion from the zero-mass form, thus placing an upper limit…

Nuclear Experiment · Physics 2009-09-24 Benjamin Monreal , Joseph A. Formaggio

The KATRIN experiment will probe the neutrino mass by measuring the beta-electron energy spectrum near the endpoint of tritium beta-decay. An integral energy analysis will be performed by an electro-static spectrometer (Main Spectrometer),…

Instrumentation and Detectors · Physics 2016-05-04 M. Arenz , M. Babutzka , M. Bahr , J. P. Barrett , S. Bauer , M. Beck , A. Beglarian , J. Behrens , T. Bergmann , U. Besserer , J. Blümer , L. I. Bodine , K. Bokeloh , J. Bonn , B. Bornschein , L. Bornschein , S. Büsch , T. H. Burritt , S. Chilingaryan , T. J. Corona , L. De Viveiros , P. J. Doe , O. Dragoun , G. Drexlin , S. Dyba , S. Ebenhöch , K. Eitel , E. Ellinger , S. Enomoto , M. Erhard , D. Eversheim , M. Fedkevych , A. Felden , S. Fischer , J. A. Formaggio , F. Fränkle , D. Furse , M. Ghilea , W. Gil , F. Glück , A. Gonzalez Urena , S. Görhardt , S. Groh , S. Grohmann , R. Grössle , R. Gumbsheimer , M. Hackenjos , V. Hannen , F. Harms , N. Hauÿmann , F. Heizmann , K. Helbing , W. Herz , S. Hickford , D. Hilk , B. Hillen , T. Höhn , B. Holzapfel , M. Hötzel , M. A. Howe , A. Huber , A. Jansen , N. Kernert , L. Kippenbrock , M. Kleesiek , M. Klein , A. Kopmann , A. Kosmider , A. Kovalík , B. Krasch , M. Kraus , H. Krause , M. Krause , L. Kuckert , B. Kuffner , L. La Cascio , O. Lebeda , B. Leiber , J. Letnev , V. M. Lobashev , A. Lokhov , E. Malcherek , M. Mark , E. L. Martin , S. Mertens , S. Mirz , B. Monreal , K. Müller , M. Neuberger , H. Neumann , S. Niemes , M. Noe , N. S. Oblath , A. Off , H. -W. Ortjohann , A. Osipowicz , E. Otten , D. S. Parno , P. Plischke , A. W. P. Poon , M. Prall , F. Priester , P. C. -O. Ranitzsch , J. Reich , O. Rest , R. G. H. Robertson , M. Röllig , S. Rosendahl , S. Rupp , M. Rysavy , K. Schlösser , M. Schlösser , K. Schönung , M. Schrank , J. Schwarz , W. Seiler , H. Seitz-Moskaliuk , J. Sentkerestiova , A. Skasyrskaya , M. Slezak , A. Spalek , M. Steidl , N. Steinbrink , M. Sturm , M. Suesser , H. H. Telle , T. Thümmler , N. Titov , I. Tkachev , N. Trost , A. Unru , K. Valerius , D. Venos , R. Vianden , S. Vöcking , B. L. Wall , N. Wandkowsky , M. Weber , C. Weinheimer , C. Weiss , S. Welte , J. Wendel , K. L. Wierman , J. F. Wilkerson , D. Winzen , J. Wolf , S. Wüstling , M. Zacher , S. Zadoroghny , M. Zboril

A generalization of Buttiker's voltage probe concept for nonzero temperatures is an open third terminal of a quantum thermoelectric circuit. An explicit analytic expression for the thermoelectric correction to an ideal quantum voltage…

Mesoscale and Nanoscale Physics · Physics 2015-06-22 Justin P. Bergfield , Charles A. Stafford

Two laboratory emission spectrometers have been designed and described previously. Here, we present a follow-up study with special focus on absolute intensity calibration of the new SURFER-spectrometer (SUbmillimeter Receiver For Emission…

Instrumentation and Methods for Astrophysics · Physics 2020-10-14 Nadine Wehres , Kirill Borisov , Katharina von Schoeler , Patrick Pütz , Cornelia E. Honingh , Frank Lewen , Stephan Schlemmer

A new type of radiation detector, a p-type modified electrode germanium diode, is presented. The prototype displays, for the first time, a combination of features (mass, energy threshold and background expectation) required for a…

Nuclear Experiment · Physics 2011-05-12 P. S. Barbeau , J. I. Collar , O. Tench

The challenges of precision neutrino physics require measurements of absolute neutrino cross sections at the GeV scale with exquisite (1%) precision. This precision is presently limited by the uncertainties on neutrino flux at the source;…

Instrumentation and Detectors · Physics 2017-05-02 Fabio Pupilli
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