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Prof. Klaus Kirch (ETHZ & PSI)21/10/2019, 09:00Oral
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Angela Papa (PSI and UniPi)21/10/2019, 09:05Invited Talk
Charged-lepton flavour-violating (cLFV) processes provide a unique discovery potential
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for physics Behind Standard Model (BSM). These cLFV processes explore new physics parameter space in a manner complementary to the collider, dark matter, dark energy, and neutrino physics programmes. Furthermore the observation of neutrino oscillations has clearly demonstrated that neutral lepton flavour is... -
Stefan Ulmer (RIKEN, Ulmer Fundamental Symmetries Laboratory, Saitama, Japan)21/10/2019, 09:35Invited Talk
The striking imbalance of matter and antimatter in our universe is one of the hottest topics of modern physics, which inspires experiments to compare the fundamental properties of matter-antimatter conjugates at lowest energy and with great precision. The BASE collaboration at the antiproton decelerator of CERN is performing such high-precision comparisons with protons and antiprotons. Using...
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Peter Geltenbort (Institut Laue-Langevin)21/10/2019, 10:05Invited Talk
Due to their outstanding property to be storable and hence observable for long periods of time (several hundreds of seconds) in suitable material or magnetic traps, ultracold neutrons (UCNs) with energies around hundred nanoelectron-volts are a unique tool to study fundamental properties of the free neutron, like its beta-decay lifetime, its electric dipole moment and its wave properties.
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The... -
Nicholas Hutzler (Caltech)21/10/2019, 11:05Invited Talk
The fact that the universe is made entirely out of matter, and contains no free anti-matter, has no physical explanation. While we cannot currently say what process created the matter in the universe, we know that it must violate a number of fundamental symmetries, including those that forbid the existence of certain electromagnetic moments of fundamental particles. We can search for...
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Fabian Allmendinger (Physikalisches Institut, Uni Heidelberg)21/10/2019, 11:35Oral
We present our recently published [1] measurement of the CP-violating permanent Electric Dipole Moment (EDM) of the neutral $^{129}$Xe atom. Our experimental approach is based on the detection of the free precession of co-located nuclear spin-polarized $^3$He and $^{129}$Xe samples. The EDM measurement sensitivity benefits strongly from long spin coherence times of several hours achieved in...
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Katharina Rolfs (Physikalisch Technische Bundesanstalt)21/10/2019, 11:55Oral
We describe a new technique used to measure the EDM of 129Xe with 3He comagnetometry. Both
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species are polarized using spin-exchange optical pumping, transferred to a measurement cell with doped silicon electrodes, and
transported into the BMSR2 magnetically shielded room at PTB-Berlin, where SQUID magnetometers detect free precession
in applied electric and magnetic fields. Two campaigns... -
Cristina Lazzeroni (University of Birmingham, UK)21/10/2019, 12:15Oral
The decay K+→π+vv, with a very precisely predicted branching ratio of less than 10exp(-10), is one of the best candidates to reveal indirect effects of new physics at the highest mass scales. The NA62 experiment at the CERN SPS is designed to measure the branching ratio of K+→π+vv with a decay-in-flight technique. NA62 took data so far in 2016-2018. Statistics collected in 2016 allowed NA62 to...
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Tobias JENKE (Institut Laue-Langevin)21/10/2019, 14:30Invited Talk
Neutrons are excellent probes to test gravity at short distances – electrically neutral and only hardly polarizable. Furthermore, very slow, so-called ultracold neutrons form bound quantum states in the gravity potential of the Earth. This allows combining gravity experiments at short distances with powerful resonance spectroscopy techniques, as well as tests of the interplay between gravity...
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Rajan Gupta (Los Alamos National Laboratory)21/10/2019, 15:00Oral
Steadily improving bounds on the neutron EDM provide stringent bounds on new interactions and theories at the TeV scale. To leverage this connection requires precise results on matrix elements of the Theta and novel CP violating interactions at the TeV scale. In this talk, I will update our results for the contributions of the quark EDM operator that are already being used in phenomenology,...
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Beatrice Franke (TRIUMF, Vancouver, Canada)21/10/2019, 15:20Invited Talk
We live in a matter dominated Universe. Naively assuming a preference of nature for symmetries, it’s somewhat unexpected that we observe much larger amounts of matter over antimatter. Asking our very successful Standard Model of Particle Physics for insight on this Baryon Asymmetry in the Universe (BAU), we learn that the observed asymmetry is actually even much larger than expected - by...
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Prof. Robert Golub (North Carolina State University)21/10/2019, 15:50Oral
We outline the principles of the method for searching for a neutron edm using super-thermal production of UCN in He4, a dilute solution of He3 as a co-magneotmeter and critical spin dressing and report on recent progress in designing and constructing the various sub-systems of the experiment.
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Sven Sturm (MPIK)21/10/2019, 16:40Invited Talk
The ultra-precise determination of the $g$-factor of highly charged ions is a unique possibility to test the validity of the Standard Model, particularly Quantum Electrodynamics (QED) in extreme electric fields up to $10^{16}$ V/cm. While the weak-field regime has been exquisitely tested, in the presence of strong fields higher-order contributions beyond the Standard Model might become...
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Sonia Bacca (JGU)21/10/2019, 17:10Invited Talk
The measurement of the Lamb shift in muonic hydrogen and the subsequent emergence of the proton radius puzzle have motivated an experimental campaign devoted other light muonic atoms, such as muonic deuterium and helium. For these systems nuclear structure corrections are the largest source of uncertainty and consequently the bottle-neck for exploiting the experimental precision to extract the...
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Frederik Wauters (Johannes Gutenberg University Mainz)21/10/2019, 17:40Oral
Negative muons at rest quickly get captured by nearby atoms and subsequently de-exite via radiative and Auger transitions until the muon ends up in the 1s orbital. At the lower orbits, there is substantial overlap between the muon wave function and the nucleus, making this system an excellent laboratory to study the interaction between the muon and atomic nucleus. With a physics program...
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Bastian Märkisch (Technische Universität München)22/10/2019, 09:00Invited Talk
Precision experiments on neutron beta decay are used to determine the CKM matrix element $V_{ud}$ and to search for novel scalar and tensor couplings beyond the axial-vector and vector couplings of the standard model. In this presentation, I will discuss the result of PERKEO III on the parity-violating beta asymmetry obtained using a pulsed cold neutron beam at the ILL. The result confirms...
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Prof. Werner Heil (Institute of Physics , JGU Mainz, Germany)22/10/2019, 09:30Oral
We report on a precise measurement of the electron-antineutrino angular correlation (a coeffcient) in free neutron beta-decay from the aSPECT experiment. The a coefficient is inferred from the recoil energy spectrum of the protons which are detected in 4pi by the aSPECT spectrometer using magnetic adiabatic collimation with an electrostatic filter. Data are presented from a 100 days run at the...
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Dr Benjamin Heacock (Nation Institute of Standards and Technology)22/10/2019, 09:50Oral
When neutrons are Bragg diffracted from a crystal slab, Bloch waves form in the crystal. Interference between the Bloch waves cause oscillations in the diffracted beam whose phase is a function of neutron energy and the thickness of the crystal slab. This phenomenon is known as pendellosung interference and has a spatial period, called the pendellosung length, that is on the order of 50...
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Christopher Crawford (University of Kentucky)22/10/2019, 10:10Oral
We report the parity violating proton asymmetry $A_p$ in the reaction $\vec{\mbox{n}}$ + $^{3}$He $\to$ p + $^{3}$H (the n-$^3$He experiment), the most precise hadronic asymmetry ever measured. Hadronic parity violation offers a unique probe of nucleon structure and the underlying non-perturbative behavior of low-energy QCD. The hadronic weak interaction is characterized by five spin and...
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Aldo Antognini (ETH)22/10/2019, 11:00Invited Talk
By means of laser spectroscopy we have measured several 2S-2P transitions in muonic hydrogen. From these measurements we have extracted a proton charge radius 20 times more precise than obtained from electron-proton scattering and hydrogen high-precision laser spectroscopy but at a variance of 7 sigma from these values. This discrepancy referred to as the ``proton radius puzzle’’ has prompted...
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Eric Hessels (York University)22/10/2019, 11:45Invited Talk
We have measured the Lamb shift in atomic hydrogen using a new FOSOF (Frequency Offset Separated Oscillatory Fields) method. We measure the 2S$_{1/2}$(F=0)-to-2P$_{1/2}$(F=1) interval to be 909.8717(32) MHz, from which an rms proton charge radius of 0.833(10) fm can be determined.
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Alexander Golossanov (PSI - Paul Scherrer Institut)22/10/2019, 12:15Oral
It is rare to have a discrepancy in such a basic property as proton size, and yet during the past decade measurements of proton charge radius using muons and electrons have disagreed by almost six standard deviations. The MUon proton Scattering Experiment (MUSE) at PSI aims to shed more light on this puzzle, by measuring the elastic scattering of muons, electrons, and positrons on protons in...
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Marianna Safronova (University of Delaware)22/10/2019, 14:30Invited Talk
The extraordinary advances in quantum control of matter and light have been transformative for precision measurements with atoms. For example, the development of atomic clocks enabled searches for the variation of fundamental constants, dark matter, violations of Einstein equivalence principle, and other applications. I will give an overview of precision fundamental studies with atoms...
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Prof. Hidetoshi Katori (The University of Tokyo)22/10/2019, 15:00Invited Talk
Clocks are devices that allow us to share time by taking advantage of ubiquitous oscillatory phenomena in nature. We once relied on astronomical observations, and today we use far regular oscillations of cesium atoms to define the international system of unit (SI) for time, i.e., the SI second. Recent optical atomic clocks have achieved 100-fold improvement over cesium clocks [1]. This extreme...
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Ioanna Arapoglou (Max Planck Institute for Nuclear Physics, Saupfercheckweg 1, 69117 Heidelberg, Germany)22/10/2019, 15:30Oral
The ALPHATRAP $g$-factor experiment is a high-precision Penning-trap experiment located at the Max Planck Institute for Nuclear Physics in Heidelberg. It has been designed for performing high-precision $g$-factor measurements on heavy highly charged ions (HCI), such as hydrogenlike $^{208}\mathrm{Pb}^{81+}$ and boronlike $^{208}\mathrm{Pb}^{77+}$, which will be externally produced and injected...
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Fabian Heiße (Max Planck Institute for Nuclear Physics)22/10/2019, 15:50Oral
Please find the abstract attached.
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Dr Wieslaw Sobkow (Institute of Theoretical Physics, University of Wroclaw)22/10/2019, 16:45Poster
Possibility of using elastic scattering of low energy electron neutrinos ($\nu_e$s) on polarized electron target (PET) for testing time reversal symmetry violation (TRSV) and neutrino nature (NN) in leptonic interactions is considered. We analyze the two theoretically possible scenarios of physics beyond the Standard Model (SM) in which flavor-conserving (FC) standard and non-standard...
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Patrick Schwendimann22/10/2019, 16:49Poster
In the field of charged lepton flavour violation (cLFV), one is investigating various decays, some of which contain photons in the final state. To discriminate between signal and background, detectors providing excellent resolutions in all particle variables are crucial.
The photons in muonic charged lepton flavour violating decays are expected to be on an energy scale in the range of 10 to...
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Niklaus Berger (Mainz University, Insititute for Nuclear Physics)22/10/2019, 16:50Poster
The Mu3e Experiment at PSI is designed to search for the lepton-flavour violating decay of a positive muon to two positrons and an electron with an ultimate sensitivity of one in 1016 muon decays. The detector is based on ultra-thin high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurement. Already in the first phase of...
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Joachim Monnard (University of Bern)22/10/2019, 16:51Poster
At the present level of uncertainty, the EM radiative corrections to the pion vector form factor become relevant in the HVP contribution to the anomalous magnetic moment of the muon. So far, their treatment is based essentially on scalar QED. In order to have a better understanding of these radiative corrections, we use unitarity and dispersion relations to express them in terms of integrals...
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Dr Vira Bondar (ETH Zurich)22/10/2019, 16:52Poster
We report on a Hanle-type magnetometer that uses the same physics package as the free spin preccession magnetometer published in [1]. The magnetometer is most sensitive at zero magnetic field and uses four laser beams to gain measurements of the magnetic field vector components along two orthogonal directions. The influence of the common mode power fluctuations in the laser beams is greatly...
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Kazuki Toyoda (The University of Tokyo)22/10/2019, 16:53Poster
A study on the aging of the photomultiplier tubes used in the liquid xenon calorimeter for the MEG and the MEG II experiment
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Jan Kahlenberg, Kim Ulrike Ross (Johannes-Gutenberg-University Mainz)22/10/2019, 16:54Poster
The $\tau$SPECT experiment aims to measure the neutron lifetime $\tau_n$ using a 3D magnetic storage technique. Due to the neutron’s magnetic moment, very low-energetic neutrons (ultracold neutrons, UCN) with a maximum energy of $\approx 50\,\mathrm{neV}$ can be stored in the magnetic trap with a volume of $\approx 8$ litres. $\tau$SPECT is designed to determine $\tau_n$ using two independent...
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Prof. Martin Fertl (Johannes Gutenberg Universitaet Mainz)22/10/2019, 16:55Poster
Neutrino flavor oscillation experiments prove that neutrinos have non-zero masses. Extensions to the Standard Model of Particle Physics have been developed to explain the non-zero masses and can be directly tested by a measurement of the absolute neutrino mass scale. The mass of the electron antineutrino $m_\bar{\nu_e}$ can be determined from the highest precision measurement of the...
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Ivo Schulthess (Universität Bern)22/10/2019, 16:56Poster
The current best estimate for the universe’s matter content consists of 84% dark matter, and the search for its composition remains of great interest. One possible candidate is a so far undetected ultra-low-mass axion. Various astronomical observations, and only one laboratory experiment, using ultra-cold neutrons, currently constrain the axion mass and its interaction strength in the allowed...
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Kosuke Yanai (University of Tokyo)22/10/2019, 16:57Poster
Scintillation detectors read out by silicon photomultipliers (SiPMs) are used in a variety of experiments as a means to detect charged particles. In particular, series connection of SiPMs have recently been attracting more and more attention for precise timing measurement. Series-connected SiPMs yield smaller capacitance than a single SiPM, which leads to narrower signal waveform and better...
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Frederik Wauters (Johannes Gutenberg University Mainz)22/10/2019, 16:58Poster
The first phase of the Mu3e experiment will search for the charged flavour violating decay of a positive muon into 2 positrons and one electron with a single events sensitivity of 2e-15. For this purpose, a DC muon beam will be stopped inside a Si pixel tracker constructed from High-Voltage Monolithic Active Pixel Sensors (HV-MAPS), complemented with timing detectors. The entire experiments...
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Charlotte König (Max-Planck-Institut für Kernphysik; 2Universität Heidelberg)22/10/2019, 16:59Poster
The electron capture (EC) decay of $^{163}$Ho to $^{163}$Dy is a promising candidate for the determination of the electron neutrino mass in the sub-eV range. For this purpose the ECHo collaboration [1] aims to perform a calorimetric measurement of the $^{163}$Dy$^{*}$ de-excitation spectrum. With its Penning-trap setup the \textsc{Pentatrap} [2] experiment performs a precision mass...
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Mr Jianqi Chen (Laboratoire de physique corpusculaire, Caen, France), Mr William Saenz (Laboratoire de physique corpusculaire, Caen, France)22/10/2019, 17:00Poster
A new ultra-cold neutron (UCN) detector is required for the n2EDM experiment since the previous $^6$Li-doped glass scintillator (NANOSC) model, used in the nEDM experiment, is constrained by its small size and high price (\textcolor{red}. Hence, the authors propose a novel detector (GADGET) composed of a chamber filled with $^3$He and CF$_4$ gases, and three perpendicular photo-multiplier...
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Mikio Sakurai (ETH Zürich)22/10/2019, 17:01Poster
We are studying in detail the feasibility of a dedicated search for a permanent electric dipole moment (EDM) of the muon at PSI. This would be the first dedicated search with a potential sensitivity of $5\times10^{-23}~e\!\cdot\!\mathrm{cm}$ employing the frozen-spin method in a compact magnetic storage ring. Such an experiment is an excellent probe for physics beyond the Standard Model (SM)...
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Nicholas Ayres (ETH Zurich)22/10/2019, 17:02Poster
Measurements for Control of Magnetic Field Related Systematic Effects for the PSI Neutron Electric Dipole Moment Experiment
N. J. Ayres on behalf of the PSI nEDM Collaboration
The neutron's electric dipole moment (nEDM) is an observable with extraordinary sensitivity to CP violating new physics phenomena. While the Standard Model predicts a negligibly small value, a wide variety of...
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POLINA KRAVCHENKO22/10/2019, 17:03Poster
The measurement of cross-section for the nuclear fusion reaction $d+^3He{\to}^4He+p$ at ultra-low energies is of interest in pure and applied physics. This fusion process is involved in the primordial nucleo-synthesis of the light elements in the early Universe. This reaction is a mirror reaction of the $d+t{\to}^4He+n$ fusion process and can be considered as a perspective source of...
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Emilio Depero (ETH)22/10/2019, 17:04Poster
NA64 is a fixed target experiment at the CERN SPS aiming at a sensitive search for hidden sectors. In this talk, we will present our latest results on the search for a new sub-GeV vector gauge boson (A′) mediated dark matter (χ) production. The A′, called dark photon, could be generated in the reaction e−Z→e−ZA′ of 100 GeV electrons dumped against an active target which is followed by the...
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Daniel Salvat (Indiana University)22/10/2019, 17:05Poster
The COHERENT collaboration operates multiple detectors at Oak Ridge National Laboratory to measure coherent elastic neutrino-nucleus scattering (CEvNS) in a variety of target nuclei. CEvNS cross sections scale as the square of the number of constituent neutrons in a given nucleus, thus giving large event rates compared to other neutrino detection modes. At the same time, the low recoil...
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Elise Wursten (CERN/RIKEN)22/10/2019, 17:06Poster
The Baryon Antibaryon Symmetry Experiment (BASE) at the antiproton decelerator of CERN is dedicated to high-precision measurements of the fundamental properties of the proton and the antiproton. Using single-particle multi-Penning-trap techniques, we compare the proton/antiproton charge-to-mass ratios [1] and magnetic moments [2,3] with ultra-high precision. Such experiments provide stringent...
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Ryoto Iwai (ETH Zürich)22/10/2019, 17:07Poster
At the Paul Scherer Institute, we are developing a novel positive muon beam at low energy with high brightness by compressing the 6-dimensional phase space of a standard surface muon beam.
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Muons are stopped in a helium gas target with a density gradient at cryogenic temperature and compressed by making use of complex-shaped B- and E-fields. Compression stages that act along two different... -
Mr Christoph Schweiger (Max-Planck-Institut für Kernphysik)22/10/2019, 17:08Poster
High-precision mass-ratio measurements with relative uncertainties below $10^{-11}$ have applications, among others, in tests of the theory of special relativity (SRT) [1], bound-state quantum electrodynamics (QED) [2] and neutrino physics research [3, 4]. This precision is achievable in Penning-trap mass spectrometry, where the mass of a charged particle is determined by measuring its free...
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Dr Christian Schmidt (Johannes Gutenberg-Universität Mainz)22/10/2019, 17:09Poster
The $a$SPECT experiment is a retardation spectrometer built to measure the proton energy spectrum in free neutron $\beta$-decay. From the shape of the spectrum, the $\beta$-$\overline{\nu}_e$ angular correlation coefficient $a$ can be derived and thus $\lambda(a)$, the ratio of the weak axial-vector $(A)$ to vector $(V)$ coupling constant $\lambda=g_A/g_V$.
In 2013, $a$SPECT had a...
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Jochen Krempel (ETH Zürich), on behalf of the nEDM collaboration22/10/2019, 17:10Poster
Currently a new experiment is being built for the measurement of the neutron
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electric dipole moment at PSI called n2EDM.
Compared to its predecessor, many improvements will be made not only to
the apparatus itself, but also to the supervisory control and data acquisition
system.
For nEDM it is essential to not only record, but also to influence the
experiment automatically which... -
Niklaus Berger (Mainz University, Insititute for Nuclear Physics)22/10/2019, 17:11Poster
The Mu3e Experiment at PSI is designed to search for the lepton-flavour violating decay of a positive muon to two positrons and an electron with an ultimate sensitivity of one in 1016 muon decays. The detector is based on ultra-thin high-voltage monolithic active pixel sensors combined with scintillating fibres and tiles for precise timing measurement. The poster will discuss...
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Dagmara Rozpedzik (Jagiellonian University)22/10/2019, 17:12Poster
The energy spectrum of ultra-cold neutrons (UCN) is an important factor in determining the systematic effects in precision measurements utilizing UCN. The oscillating ultra-cold neutron spectrometer (OTUS) is a new tool designed for monitoring the energy distribution and its time evolution in different places of the transport system connecting a UCN source with experiments. We will present the...
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Stergiani Marina Vogiatzi (PSI - Paul Scherrer Institut, ETH Zurich)22/10/2019, 17:13Poster
An ongoing experiment at PSI aims to determine the nuclear charge radius of $^{226}$Ra - needed by an experiment aiming at measuring atomic parity violation in a radium ion - by means of muonic atom spectroscopy. An intermediate test was performed with a $^{185,187}$Re target which is the last stable element whose nuclear charge radius has not been measured and shows similar nuclear structure...
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Mr Thomas B. Meijknecht (Van Swinderen Institute, University of Groningen and Nikhef, National Institute for Subatomic Physics)22/10/2019, 17:14Poster
As the NL-eEDM collaboration, we are searching for a permanent electric dipole moment on the electron (eEDM) in a BaF molecular beam. In preperation of such an experiment we have performed spectroscopic measurements in a supersonic BaF beam. The lifetimes of the $A^{2}Π_{1/2}$ and $A^{2}Π_{3/2}$ states were obtained using short light pulses generated from a CW laser beam with a pulsed...
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Masashi Usami (The Univ. of Tokyo, ICEPP)22/10/2019, 17:15Poster
The MEG II experiment is designed to achieve the world’s most sensitive $\mu^+ \rightarrow e^+\gamma$ decay search with the most intense muon beam ($7 \times 10^7 \mu^+ / s$) in Paul Scherrer Institut . This decay is prohibited in the standard model theory but predicted to occur in the many beyond standard model theories. Thus, to find this decay means to find the new physics.
To discover...
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Narongrit Ritjoho (PhD at Paul Scherrer Institut)22/10/2019, 17:16Poster
Recently, we have performed measurements on vacuum muonium formation at room and cryogenic temperatures at the the Paul Scherrer Institute. These measurements were conducted in the context of our efforts on the investigation of the gravitational interaction of antimatter and second-generation particles. In our room temperature setup, the muon beam impinged on several targets such as zeolite...
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Mr Simon Vanlangendonck (KULeuven)22/10/2019, 17:17Poster
There are indications that the measured number of antineutrinos emerging from reactor fission fragments inside a reactor is lower than theoretically predicted. Moreover, there is an additional anomaly in the energy spectrum of the antineutrinos. These observations are the reactor neutrino anomaly. One of the uncertainties in the theoretical description is the QCD influence on the β-decay of...
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Ingo Rienäcker (PSI)22/10/2019, 17:18Poster
Ultracold neutrons (UCN) with energies below 300 neV can be trapped for hundreds of seconds in containments made of materials with high optical potential. They are used in experiments that benefit greatly from long storage times, like the n2EDM experiment currently assembled at PSI, searching for a permanent electric dipole moment of the neutron. The PSI UCN source makes use of solid deuterium...
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Estelle Chanel (Universitat barn)22/10/2019, 17:19Poster
The search for a neutron electric dipole moment (EDM) is of significant interest in understanding the observed baryon asymmetry in the universe. Historically, two methods have been employed to measure an EDM, storage of ultracold neutrons (UCN) and cold neutron beams, with the latter being abandoned in the 1980s due to a limiting relativistic systematic effect. The Beam EDM experiment...
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Rina Onda (Tokyo Univ.)22/10/2019, 17:21Poster
Results of PDE measurements for VUV-MPPCs irradiated by $\gamma$, neutron or VUV light
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Dr Jacob Thorne (Universität Bern)22/10/2019, 17:22Poster
We present details of the simulations, design, and half scale initial tests of the Ramsey Chamber apparatus for the n2EDM experiment. The Chamber is a double chamber cylindrical geometry with a 80 cm internal diameter. The two UCN volumes are stacked vertically and separated by a central high voltage electrode. The volumes are sealed on top and bottom by an insulating spacer and ground...
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J. M. Cornejo (Leibniz Universität Hannover)22/10/2019, 17:23Poster
We present an experimental approach based on quantum logic inspired cooling and readout techniques to contribute to CPT tests in the baryonic sector. Within the BASE collaboration [1], these techniques would allow to cool single (anti-)protons to sub-Doppler temperatures by means of coupling to a laser-cooled beryllium ion [2, 3]. For this purpose, both ions will be co-trapped in an advanced...
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Mr Prajwal Mohanmurthy (ETH Zurich, PSI)22/10/2019, 17:24Poster
Neutron to mirror-neutron oscillations [1] could be an observable baryon number violating process. Baryon number violation is required for baryogenesis in order to explain the observed asymmetry between matter and antimatter in the universe. Two separate groups [2],[3] performed experiments in search of mirror-neutron oscillations and reported having found no evidence. The limit set on the...
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Daniel Moser (Stefan-Meyer-Institut, OEAW)22/10/2019, 17:25Poster
The beta decay of the free neutron provides several probes to test the Standard Model of particle physics as well as to search for extensions thereof. NoMoS, the neutron decay products momentum spectrometer, presents a novel method of momentum spectroscopy: it utilizes the R × B drift effect to disperse charged particles dependent on their momentum in an uniformly curved magnetic field. The...
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Mrs Karishma Dhanmeher (Institute of Nuclear Physics, Polish Academy of Sciences)22/10/2019, 17:26Poster
Neutron and nuclear beta decay correlation coefficients are sensitive to the exotic scalar and tensor interactions that are not included in the Standard Model (SM). The BRAND experiment will measure simultaneously 11 neutron correlation coefficients (a, A, B, D, H, L, N, R, S, U, V ) where 7 of them (H, L, N, R, S, U, V ) depend on the transverse electron polarization – a quantity which...
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Jonas Nuber22/10/2019, 17:27Poster
Spectroscopy of muonic hydrogen ($\mu$p) atoms allows for precise investigations of the proton’s electromagnetic structure. At PSI we want to measure the groundstate hyperfine-splitting of muonic hydrogen, from which the Zemach radius of the proton can be deduced. The experiment will use a new detection scheme which is based on the diffusion of laser-excited $\mu$p atoms inside a gas cell...
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Mr Andreas Lanz (Stefan Meyer Institute)22/10/2019, 17:28Poster
The [ASACUSA][0] (Atomic Spectroscopy And Collisions Using Slow Antiprotons) Collaboration of the AD-facility at CERN aims to measure the ground-state hyperfine structure of antihydrogen to test the CPT-Theorem [1]. For this purpose, a spectroscopy apparatus has been built and tested with hydrogen [2]. An upgrade of the interaction region enabled to induce two transitions between the hyperfine...
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70. Design of the detection system for the measurement of the hyperfine splitting in muonic hydrogenLaura Sinkunaite (Paul Scherrer Institute/ ETH Zürich)22/10/2019, 17:29Poster
Muonic hydrogen, ground-state hyperfine splitting, detection system, MeV-energy X-rays, scintillation detectors.
Muonic hydrogen ($\mu$p) is a bound-state of a negative muon and a proton. Since a muon is 207 times heavier than an electron, the energy levels of $\mu$p are very sensitive to the nuclear structure. By means of laser spectroscopy, we are aiming at...
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Gianluca Janka (ETH Zürich)22/10/2019, 17:30Poster
Antihydrogen studies aim to shed light on the observed
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baryon/antibaryon asymmetry in the Universe by comparing the properties
of matter and antimatter with very high precision. In the context of the
GBAR experiment [1] located at CERN, our aim is to perform a measurement
of the antihydrogen Lamb shift with an uncertainty of 100 ppm, which
allows extracting the antiproton charge radius at... -
Dr Gunther Wichmann (ETH Zürich)22/10/2019, 17:31Poster
Our scheme aims to measure the parity violating energy difference between the enantiomers of chiral molecules which has been predicted to be very small, e.g. about 100 aeV for CHFClBr [2] and 1 feV for 1,2 Dithiine [3], but so far has never been measured. The effect might be important for the origin of biomolecular homochirality and for precision tests of the standard model of particle physics...
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Alexey Fomin (Petersburg Nuclear Physics Institute)22/10/2019, 17:32Poster
The possibility of experimentally determining the ratio λ of the axial weak-interaction constant G$_A$ to the vector weak-interaction constant G$_V$ by simultaneously measuring the electron and neutrino asymmetries at the same setup is discussed. The proposed measurement and data-processing procedures are described. The determination of λ by the method in question permits disregarding the...
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Niklaus Berger (Mainz University, Insititute for Nuclear Physics)22/10/2019, 17:33Poster
The P2 experiment at the new electron accelerator MESA in Mainz aims for a determination of the weak mixing angle at low momentum transfer with unprecedented precision. To this end, the parity violating asymmetry in electron proton scattering is studied with integrating Cherenkov detectors at very high rates of scattered electrons. In order to determine the average momentum transfer...
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Mr Tim Engel (Paul Scherrer Institut/Universität Zürich)22/10/2019, 17:34Poster
Low-energy experiments with leptons such as MEG, Mu3e, MUonE and MUSE complement the research at the high-energy frontier. However, to fully exploit the experimental data, the corresponding Standard Model background has to be known to a high accuracy. For this reason we calculate the fully differential NNLO QED corrections to the processes $\mu\rightarrow e\nu\nu$, $\mu e\rightarrow \mu e$,...
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Mr Simon Scheidegger (ETH Zurich)22/10/2019, 17:35Poster
The first experiments designed to control the translational motion and the internal state of the hydrogen atom were performed almost 100 years ago by Rabi [1] using the beam methods developed by Gerlach and Stern [2]. We present a method with which paramagnetic atoms and molecules can be generated in a specific magnetic sublevel of a selected internal state and with which the atom or molecule...
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Alexander Albert Skawran22/10/2019, 17:36Poster
Presentation of the preparations regarding the nuclear charge radius measurement of radium.
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Dr Ying-nan Mao (National Center for Theoretical Sciences (Hsinchu, Taiwan))22/10/2019, 17:37Poster
I. Brief Intriduction to 2HDM with Soft CP-violation (Type I,II,III,IV)
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II. Current Constriants through Collider, Flavor, S-T parameter, and especially the ACME II electron EDM measurement;
III. The importance of neutron EDM: current constraint on CP-even and -odd mixing angle, and why is it irreplacement in constraining Type II and III models: possible cancellation in electron EDM;
IV.... -
Satoru Kobayashi (The University of Tokyo)22/10/2019, 17:38Poster
- Development of calibration measurements for VUV-sensitive MPPCs in MEG II Liquid Xenon Gamma-ray detector
- Performance evaluation of VUV-sensitive MPPCs under high-intensity muon beam
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Mr Waleed Khalid (SMI, ÖAW), Dr Manfred Valentan (SMI, ÖAW)22/10/2019, 17:39Poster
NoMoS, the neutron decay products momentum spectrometer, aims to measure the momentum spectra of the charged decay products (electron and proton) in neutron beta decay with high precision. It uses the so-called R x B effect in a uniformly curved magnetic field to separate and a spatially resolving detector to measure the charged decay particles according to their momentum. In this poster, the...
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Lennert De Keukeleere22/10/2019, 17:40Poster
Beyond Standard Model (BSM) theories can be probed in two types of experiments. In collider experiments, such as those carried out at LHC, exotic bosons are directly produced in high-energy proton - proton collisions. Another way to test BSM's, is by studying low-energy observables. This is facilitated by the small effects/currents of the same exotic bosons on these observables[1]. The shape...
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Mr Amit Nanda (Stefan Meyer Institute, Austrian Academy of Sciences)22/10/2019, 17:41Poster
The ASACUSA (Atomic Spectroscopy And Collisions Using Slow Antiprotons) collaboration, based at the Antiproton Decelerator facility of CERN aims to measure the ground state hyperfine structure of antihydrogen at a ppm level relative precision with a Rabi-type beam experiment [1,2]. ASACUSA produces antihydrogen atoms by the mixing of antiprotons with positrons in a double cusp trap with strong...
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Dr Sushil Sharma (Jagiellonian University)22/10/2019, 17:43Poster
Positronium is a purely leptonic object self annihilating into photons. It is an atom bound by a central potential and thus the states of positronium are parity eigenstates. Furthermore, as an atom composed of a particle (e-) and its antiparticle (e+), it is an eigenstate of the charge conjugation operator. Therefore, the positronium is a unique laboratory to study discrete symmetries whose...
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Philipp Schmidt-Wellenburg (Paul Scherrer Institut)22/10/2019, 17:45Poster
An electric dipole moment of the neutron (nEDM) is intrinsically violating the combined symmetry of charge and parity (CP). One necessary condition to create a matter/antimatter asymmetric universe from symmetric starting conditions is a sufficiently strong source of charge/parity violation (CPV) in the fundamental physics describing the early Universe. A discovery of a nEDM value larger than...
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Wolfgang Schreyer (TRIUMF)22/10/2019, 17:46Poster
The goal of the TUCAN collaboration is to measure the electric dipole moment (EDM) of the neutron with a sensitivity of $10^{-27}$ ecm. To achieve this within a reasonable time, we are building the world's strongest ultracold-neutron source, based on superthermal conversion of cold neutrons in superfluid helium. At TRIUMF, we recently commissioned a new proton beamline with a beam power of up...
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Prof. Valery Fedorov (NRC "Kurchatov Institut" - PNPI)22/10/2019, 17:47Poster
The effect of neutron spin rotation at Laue diffraction in a weakly deformed neutron-transparent
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noncentrosymmetric crystal has been described theoretically and studied experimentally. The effect is due to the bending of a Kato trajectory of the neutron in the deformed crystal. At a certain type of the deformation, one of two neutron waves excited at Laue diffraction, which propagate in... -
Dr Luca De Paolis (National Laboratory of Frascati (LNF) of INFN)22/10/2019, 17:48Poster
The VIP2 experiment is a major upgrade of the VIP (Violation of the Pauli exclusion principle) experiment and is testing the Pauli Exclusion Principle (PEP) for electrons, looking for a possible forbidden transition energy which could point out a violation of PEP.
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The transition energy monitored in VIP and VIP2 is that of the Kα1 line of the copper atom, which is 8047.8 eV. The transition... -
Dieter Ries (Johannes Gutenberg Universität Mainz)22/10/2019, 17:50Poster
Ultracold Neutrons (UCN) provide a unique tool for fundamental neutron research with long observation times.
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The τSPECT experiment, which is currently being commissioned at the pulsed UCN source of the TRIGA Mainz research reactor, aims to utilize this fact in order to precisely measure the free neutron lifetime. In order to reduce systematic errors with respect to storage experiments using... -
Andreas Crivellin (PSI&UZH)22/10/2019, 17:51Poster
We investigate the correlations between tauonic B meson decays (e.g. B→τν, B→D(∗)τν, B→πτν) and electric dipole moments (EDMs), in particular the one of the neutron, in the context of the S1 scalar leptoquark (LQ). This LQ naturally arises in the R-parity violating MSSM as the right-handed down-squark. We perform the matching of this model on the effective field theory taking into account the...
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Dmitrii Shapiro22/10/2019, 17:52Poster
There are 4 known types of interaction in nature, but nowadays the existence of a new force mediated by new unknown bosons is widely discussed in the literature [1], [2]. This work deals with the application of neutron scattering technique for the search for a new short-range interaction and for setting constraints on the coupling constant of such interaction.
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The main idea is to perform an... -
Prof. Sabin Stoica (International Centre for Advanced Training and Research in Physics)22/10/2019, 17:53Poster
Possible deviations from Lorentz invariance in the framework of the Standard Model Extension are more and more studied at present, including the neutrino sector. Observable effects due to the so-called countershaded operator cannot be investigated by measurements of neutrino oscillations and time of flight, but can be in double-beta decay (DBD) experiments, for example by a detailed analysis...
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Maud Versteegen (CENBG)22/10/2019, 17:54Poster
Nuclear beta decay offers a very powerful tool to test the Standard Model (SM) in the electroweak sector. The wide variety of nuclei and beta transitions allows us to choose the perfect candidate for specific tests of the SM which are complementary to high energy physics studies [1]. In particular, the possible existence of scalar (resp. tensor) currents in the well-established vector −...
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Joachim Bosina (Atominstitut TU Wien)22/10/2019, 17:55Poster
This talk focuses on the control and understanding of a gravitationally interacting elementary quantum system using gravity resonance spectroscopy (GRS) with ultracold neutrons (UCN). This technique offers a new way of looking at gravitation at short distances based on quantum interference.
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In the past years, the qBOUNCE collaboration has designed and built a new Ramsey-type GRS experiment at... -
Dr Ekaterina Korobkina (North Carolina State University)22/10/2019, 17:56Poster
Measuring particle EDMs is one of the most challenging experiments in the field of high precision physics. Present neutron EDM experiments are approaching limits of the traditional measurement technique due to both, statistic and systematic limitations. nEDM@SNS collaboration is working on realization of new approach, which employs production of trapped neutrons and measurement of neutron...
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Patrizia Cenci (INFN Perugia (IT))22/10/2019, 17:57Poster
The features of the NA62 experiment at the CERN SPS - high-intensity setup, trigger-system flexibility, high-frequency tracking of beam particles, redundant particle identification, and
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ultra-high-efficiency photon vetoes - make it particularly suitable to search for long-lived, weakly-coupled particles within Beyond the Standard Model physics.
We report the results of a search for π0 decays... -
Mr Duarte Vicente Pais (Paul Scherrer Insitut, ETH Zürich)22/10/2019, 17:58Poster
The search for the neutron electric dipole moment $d_n$, carried on by the n2EDM experiment at PSI could provide a better insight on the baryon asymmetry of the universe and/or new physics. The experimental goal to reach an order of magnitude higher sensitivity than previous efforts, means its systematic effects need to be better controlled. The appearance of a false $d_n$ ($d_{Hg→n}^{false}$)...
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Heerak Banerjee (Indian Association for the Cultivation of Science)22/10/2019, 17:59Poster
We propose that the $\gamma + \not{\hspace{-0.3em}E}$ signal at the Belle-II detector will be a smoking gun for supersymmetry (SUSY) in the presence of a gauged $U(1)_{L_{\mu}-L_{\tau}}$ symmetry. A striking consequence of breaking the enhanced symmetry appearing in the limit of degenerate (s)leptons is the nondecoupling of the radiative contribution of heavy charged sleptons to the $\gamma -...
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Dr Geza Zsigmond (Paul Scherrer Institut)22/10/2019, 18:00Poster
on behalf of the nEDM collaboration at PSI
The quest of a permanent electric dipole moment of the neutron, a CP-violating property, is one of the highest priorities in low-energy particle physics. The design of the n2EDM apparatus, now under construction at the PSI ultracold neutron (UCN) source, was strongly supported by neutron optics simulations using the MCUCN code. In order to obtain...
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Mrs Solange Emenegger (ETH Zuerich)22/10/2019, 18:01Poster
on behalf of the nEDM collaboration at PSI
The n2EDM experiment hosted at the Paul Scherrer Institute is seeking an improvement in the measurement of the neutron electric dipole moment (nEDM) by one order of magnitude.
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In order to achieve this goal, it is crucial to stabilize the magnetic fields inside the precession chamber, where neutrons are stored and Ramsey measurements are... -
Gabriele Piperno22/10/2019, 18:02Poster
A possible solution to the dark matter problem is to speculate that it lives in a separate sector with respect to the SM and that it interacts with it only by means of new particles called portals. The simplest one foresees an additional U(1) symmetry, whose mediator, the dark photon $A'$, could mix with the standard photon and faintly interact with SM particles.
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The PADME experiment, hosted... -
Dr Erwin Gutsmiedl (Senior Scientist Physics Department E18 TUM)22/10/2019, 18:03Poster
Karina Bernert, Roman Gernhäuser,Stefan Huber, Igor Konorov, Bastian Märkisch, Stephan Paul, Christoph Roick, Heiko Saul, Wolfgang Schott, Suzana Spasova - Physik-Department, Technische Universität München, D-85748 Garching, Germany;
Ralf Engels - Institut für Kernphysik, Forschungszentrum Jülich, D-52425 Jülich, GermanyIn order to improve the non- Standard Model weak interaction scalar...
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Pin-Jung Chiu (Paul Scherrer Institut and ETH Zurich)22/10/2019, 18:04Poster
on behalf of the nEDM Collaboration at PSI
There is so far no experimental evidence of CP violation found in the strong interaction. The non-observation of a neutron electric dipole moment (nEDM) constrains the CP violating term ($\theta$-term) in the QCD Lagrangian to be nine orders of magnitude smaller than naturally expected [1]. A solution proposed in 1977 postulated that an additional...
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Jakob Micko (Institut Laue-Langevin)22/10/2019, 18:05Poster
The qBOUNCE experiment investigates gravity at small distances. This is done using high precision frequency based spectroscopic methods. Ultracold neutrons (UCNs) form macroscopic bound states above a flat surface in the gravity potential of the Earth, connecting the quantum mechanical neutron wavefunction and gravity. Using this system we developed techniques for Gravity Resonance...
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Lukas Gerritzen (ETH Zurich)22/10/2019, 18:06Poster
Mu3e is a dedicated experiment searching for the charged lepton-flavour violating decay µ+ -> e+ e+ e-. The experiment consists of three subdetectors: A central barrel tracking device realised as two double layers of HV-CMOS pixel detectors, a scintillating fibre detector for timing measurements in the central region and a scintillating tile detector for timing in the end regions.
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The... -
Ms Swathi Karanth (Institute of Physics, Jagiellonian University in Krakow)22/10/2019, 18:07Poster
A particle called the axion has been proposed to explain the small size of the CP violating term in quantum chromodynamics. It would be light in weight and weakly coupled to nucleons. If sufficiently abundant, it might be a candidate for dark-matter in the universe. Axions or axion-like particles (ALPs), when coupled with gluons, introduce an oscillating Electric Dipole Moment (EDM) along the...
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Daniya Zinatulina (Joint Institute for Nuclear Research)22/10/2019, 18:08Poster
In the poster we observe our previous experience at the PSI muon facility, namely high precision gamma-spectroscopy with negative slow muons on the μE-4 and μΕ-1 beams with HPGe – detectors and with isotopically enriched targets (solid and gas). Such experiments could be divided in to three parts: 1) Doppler profile of gamma-lines following OMC (angular correlation with neutrino) ; 2) Partial...
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Arthur Olin (TRIUMF/UVic)22/10/2019, 18:09Poster
Nuclear muon capture (NMC) begins with a weak interaction process occurring within the nuclear volume. Information about NMC comes from the final-state particles, of which protons and deuterons are important components. However, published information is
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rather limited despite being important for the design of some current searches for lepton flavor violation. $\mu^-$ Al data taken using the... -
Dr Paul Jansen (ETH Zurich)22/10/2019, 18:10Poster
Paul Jansen, Luca Semeria, and Frédéric Merkt
Laboratory of Physical Chemistry, ETH Zurich, CH-8093 Zurich, SwitzerlandMeasurements of the level energies of few-electron atoms and molecules provide reference data to test the results of quantum chemical calculations. In recent years, molecular spectroscopy has reached the level of precision at which such measurements can play a role in...
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Miroslaw Marszalek22/10/2019, 18:11Poster
The measurement of the hyperfine splitting (HFS) in muonic hydrogen at the ppm level by means of pulsed laser spectroscopy allows for extraction of the Zemach radius of the proton at the per mille level. This measurement, ongoing at the Paul Scherrer Institute, features a novel laser system to excite the HFS transition at 6.8 µm. To increase the transition probability, we will use a multi-pass...
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Ulserik Moldanazarova (University of Liverpool)22/10/2019, 18:12Poster
Matching conditions for photon penguin diagrams in the generically extended Standard Model.
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Francesco Renga (INFN Roma)22/10/2019, 18:13Poster
The search for the Lepton Flavor Violating decay $\mu \to e \gamma$ exploits the most intense continuous muon beams, which can currently deliver ∼ 108 muons per second. In the next decade, accelerator upgrades are expected in various facilities, making it feasible to have continuous beams with an intensity of $10^9$ or even $10^{10}$ muons per second. We investigate the experimental limiting...
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Geoffrey Greene (University of Tennessee)22/10/2019, 18:14Poster
Neutron beta decay is an archetype for all semi-leptonic charged-current weak processes. A precise value for the neutron lifetime is required for consistency tests of the Standard Model and is needed to predict the primordial 4He abundance from the theory of Big Bang Nucleosynthesis. An effort is under way for an in-beam measurement of the neutron lifetime that is able to evaluate the...
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Dinko Pocanic (University of Virginia)23/10/2019, 09:00Invited Talk
Relatively simple dynamics, and extremely well controlled radiative and loop corrections, ensure that pion and muon decays are described with unprecedented precision within the Standard Model, typically with relative uncertainties of $\sim 10^{-4}$ or lower. This theoretical precision makes the $\pi$ and $\mu$ decays suitable as a sensitive means of testing the underlying symmetries,...
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Prof. Douglas Bryman (University of British Columbia and TRIUMF)23/10/2019, 09:30Invited Talk
Since the discovery of the muon, the lack of understanding of flavor is one of the most intriguing and persistent problems in particle physics. Many hypotheses which extend the Standard Model suggest that observations of non-universal charged current interactions could be due to effects at high mass scales, possibly approaching 1000 TeV, or to the existence of sterile neutrinos. Measurement of...
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Dr Stefano Di Falco (INFN Pisa)23/10/2019, 10:00Oral
The Mu2e experiment at Fermilab will search for the neutrinoless conversion of a muon into an electron in the field of an aluminum nucleus. A clear signature of this charged lepton flavor violating coherent two-body process is the monoenergetic conversion electron of 104.97 MeV produced in the final state. The experiment will have a single-event sensitivity of ~$2\times 10^{-17}$, and either...
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John Quirk (Boston University, AlCap Collaboration)23/10/2019, 10:20Oral
presented on behalf of the AlCap collaboration
Observation of neutrinoless muon-to-electron conversion in the presence of a nucleus would be unambiguous evidence of physics Beyond the Standard Model. Two experiments, COMET at J-PARC and Mu2e at Fermilab, are under construction and will search for this process with a detection sensitivity of $10^{-16}$, 10,000 times better than previously...
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Holger Mueller (UC Berkeley)23/10/2019, 11:10Invited Talk
The fine-structure constant $\alpha$ is ubiquitous in physics, and a comparison among different experiments provides a powerful test of the Standard Model of particle physics. The most precise measurement of $\alpha$ (to date) is our recently published result, $α = 1/137.035\,999\,046(27),$ with an uncertainty of 200 parts per trillion (ppt). A $2.5-\sigma$ tension with the value obtained...
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Matteo Fael (KIT Karlsruhe)23/10/2019, 11:40Oral
Recent improvements of the Large Hadron Collider luminosity and the beginning of Belle II experiment will increase the sensitivity to tau lepton-flavour violating modes. In particular, it has been claimed by Pham in hep-ph/9810484 that $BR(\tau \to 3 \mu)$ could be as large as $10^{−14}$ in the Standard Model with massive neutrinos, contradicting earlier predictions for $BR(\mu \to 3e)$. If...
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Yannick Ulrich (PSI / UZH)23/10/2019, 12:00Oral
Past years have seen an impressive progress in perturbative calculations. We apply these techniques to compute high-precision QED contributions to low-energy processes involving muons and other leptons.
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In this talk, I will review the current situation. -
Prof. George W.S. Hou (National Taiwan University)23/10/2019, 12:20Oral
The h(125) boson was discovered at the LHC in 2012, but as Run 2 has ended, nothing beyond the Standard Model (SM) has emerged, be it supersymmetry, extra gauge bosons, or any new particle. We call this situation, Dyssymmetry, as spoken by Nature. As such, we take the simplicity path to reexamine any presumed symmetries. In particular, we scrutinize the usual Z2 symmetry associated with having...
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Dr Rachel Ryan (University of Washington)23/10/2019, 14:30Invited Talk
The MuSun experiment utilizes a unique cryogenic time projection chamber to extract the $\mu d$ capture rate to better than 1.5% precision via determination of the $10^{-3}$ deviation of the muon lifetime in deuterium gas from the free muon lifetime. This measurement will lead to a benchmark result in calibrating weak interactions in the two nucleon system, relevant for calculating fundamental...
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Peter Winter (Argonne National Laboratory)23/10/2019, 15:00Invited Talk
The Muon g-2 experiment E989 at Fermilab will measure the anomalous magnetic moment of muon, a$^{}_\mu$, with a precision goal of 140 part-per-billion (ppb). The experiment is aiming to resolve the discrepancy of more than 3 standard deviations between the previous measurements dominated by the Brookhaven E821 result and the Standard Model calculation of a$^{}_\mu$.
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The experimental concept... -
Clara Hormigos-Feliu23/10/2019, 15:30Oral
The anomalous magnetic moments of the electron and the muon hint at lepton-nonuniversality from physics beyond the Standard Model (SM). We propose a natural explanation in the framework of an asymptotically safe SM, with an extended scalar sector and Yukawa couplings between vector-like fermions and ordinary leptons, which links flavor to new physics. Both leptons' magnetic moments are induced...
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Franziska Hagelstein (Universität Bern)23/10/2019, 15:50Oral
In their 2004 paper, Melnikov and Vainshtein derive a short-distance constraint for the pseudoscalar-pole light-by-light four-point function. To satisfy this constraint, Melnikov and Vainshtein dropped the pseudoscalar transition form factor at the vertex where the external photon is hooked. We present a way to satisfy the short-distance constraint of Melnikov and Vainshtein with an infinite...
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Prof. Nicola Serra (University of Zurich)23/10/2019, 16:40Invited Talk
Some recent measurements of b-hadron decays at the LHCb experiment and B-factories show a discrepancy with respect to Standard Model expectations. They consists of test of lepton flavour universality in rare and semileptonic decays and measurements of rare semi-muonic decays. While each of these measurements has a limited statistical significance, intriguingly, they seem to form a coherent...
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Andreas Crivellin (PSI&UZH)23/10/2019, 17:10Oral
We consider possible beyond-the-Standard-Model (BSM) effects that can accommodate both the long-standing tension in the anomalous magnetic moment of the muon, aμ=(g−2)μ/2, as well as the emerging 2.5σ deviation in its electron counterpart, ae=(g−2)e/2. After performing an EFT analysis, we consider BSM physics realized above the electroweak scale and find that a simultaneous explanation becomes...
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Alexander Saunders (Los Alamos National Lab)24/10/2019, 09:00Invited Talk
Measurement of free neutron decay to a proton, electron, and antineutrino provides information about the fundamental parameters of the charged weak current of the nucleon and constrains many extensions to the Standard Model at and above the TeV scale. Knowledge of the lifetime to an accuracy of better than 1 s is necessary to improve BBN predictions of elemental abundances and to search...
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Mr Victor Ezhov (1Petersburg Nuclear Physics Institute NRS KI, Gatchina, Russia)24/10/2019, 09:30Oral
Precision measurements of the neutron lifetime provide stringent tests of the standard electroweak model [1] as well as crucial inputs for Big-Bang nucleosynthesis calculations [2]. When combined with measurements of other neutron beta decay correlation coefficients [1], the neutron lifetime enables the determination of the Vud element of the Cabbibo-Kobayashi-Maskawa quark mixing matrix,...
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Yoshio Kamiya (International Center for Elementary Particle Physics, The University of Tokyo)24/10/2019, 09:50Oral
Gravitationally bound quantum states of ultracold neutrons, which have been measured using pixelated silicon imaging sensor for cold neutrons[1], would be an unique and interesting system to see gravity-like phenomena beyond Newtonian expressions or the general relativity. We are now designing and developing the experimental details to manipulate this quantum system to fit our planning...
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Alexander Frank (JINR)24/10/2019, 10:10Oral
The report is devoted to the evolvement of views at the Accelerating Medium Effect, which consists in changing the frequency of a wave passing through a refracting sample moving with acceleration. At different times, theoretical predictions of such a change in frequency were made for electromagnetic waves passing through a dielectric plate moving with acceleration [1], neutron waves passing...
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Makoto Fujiwara (TRIUMF)24/10/2019, 11:10Invited Talk
It has been 20 years since the start of the Antiproton Decelerator (AD) facility at CERN. During this time, tremendous progress has been made in synthesizing, trapping, and interrogating cold antihydrogen atoms. The field of antihydrogen physics has now arguably advanced from the proof-of-principle stage to the precision physics stage. This talk will review recent progress, with some focus on...
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Alexey Fomin (Petersburg Nuclear Physics Institute)24/10/2019, 11:40Oral
The search for neutron-antineutron oscillations is currently of great interest as a process with baryon number violation. The results of the Monte Carlo simulations of the experiment based on the storage of ultracold neutrons in a material trap and of the experiment at cold neutron beam are presented. The possibilities of increasing the sensitivity of the experiment due to the accumulation of...
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Prof. Vladimir Voronin (NRC "Kurchatov institute"-PNPI)24/10/2019, 12:00Oral
Recently proposed ultra-precise neutron spectrometry technique based on the effects of dynamic neutron Laue-diffraction in perfect crystals was experimentally tested.
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This technique is based on the effect of enhancement of angular deviation of neutron trajectory inside the crystal when the angle of neutron incidence on the crystal is slightly varied. Moreover, there is an additional gain... -
Mr Noah Birge (University of Tennessee)24/10/2019, 12:20Oral
The Standard Model (SM) has become one of the most complete theories encapsulating fundamental particle interactions. Despite its far ranging success, neutrino flavor oscillations, the observed baryon asymmetry, the dark matter puzzle, and complete absence of gravity from the theory makes it clear that there must exist interactions and particles beyond the standard model (BSM). A nonzero Fierz...
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Dr Elise Novitski (University of Washington)24/10/2019, 14:30Invited Talk
Measurements of the $\beta^-$ spectrum of tritium give the most precise directly measured limits on neutrino mass. Cyclotron Radiation Emission Spectroscopy (CRES) is a new experimental technique that has the potential to surmount the systematic and statistical limitations of current-generation direct measurement methods and reach an effective electron antineutrino mass sensitivity of...
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Prof. Michael Kohl (Hampton University)24/10/2019, 15:00Oral
Experiment E36 has recorded stopped-kaon decay data at the J-PARC K1.1BR beamline for a precision measurement of the ratio of decay widths BR($K^+ \rightarrow e^+\nu_e$) and BR($K^+ \rightarrow \mu^+ \nu_\mu$), respectively, to test lepton universality, and to search for rare decay modes producing light neutral bosons. An overview of the experiment and analysis status will be...
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Jimmy Caylor (The University of Tennessee - Knoxville)24/10/2019, 15:20Oral
Neutron beta decay is the simplest example of semi-leptonic decay. A precise measurement of the neutron lifetime and $\lambda$, the ratio of axial vector and vector coupling constants of the weak interaction, allow for a determination of the CKM matrix element $V_{ud}$ that is free from nuclear structure effects. The neutron lifetime provides an important test of unitarity and consistency of...
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Christopher Morris (LANL)24/10/2019, 15:40Oral
C. L. Morris for the UCNTau collaboration
A new method for counting surviving neutrons in neutron lifetime measurements, using bottled ultracold neutrons, which provides better characterization of systematic uncertainties and enables higher precision than previous measurement techniques will be described. An active detector that can be lowered into the trap has been used to measure the...
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Prof. Zurab Berezhiani (Univ. L'Aquila and LNGS)24/10/2019, 16:30Invited Talk
After the recent high precision determinations of $V_{us}$ and $V_{ud}$, the first row of the CKM matrix shows more than $4\sigma$ deviation from unitarity. Two possible scenarios beyond the Standard Model can be investigated in order to fill the gap. If a 4th quark $b'$ participates in the mixing, with $\vert V_{ub'} \vert \simeq 0.04$, then its mass should be no more than 6 TeV or so. A...
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DMITRY BUDKER (Helmholtz Institute Mainz)24/10/2019, 17:00Invited Talk
I will survey some of the recent experiments, including the Cosmic Axion Spin-Precession experiments (CASPEr), the use of sensor networks to detect topological dark matter, possibly trapped in the gravitational potential of the Earth, as well as experiments looking for scalar dark-matter fields oscillating at frequencies of up to hundreds of megahertz.
Some references can be found at:...
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24/10/2019, 17:30Oral
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Joerg Jaeckel (ITP Heidelberg)25/10/2019, 09:00Invited Talk
Very light and very weakly coupled particles, including in particular axion-like particles, provide interesting opportunities for dark matter. We consider a variety of different types of such light dark matter candidates and explore possible experimental and observational tests.
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Prof. Laura Baudis (University of Zurich)25/10/2019, 09:30Invited Talk
Neutrinos are the only known elementary particles that are Majorana fermion candidates, implying that they would be their own antiparticles. The most sensitive and perhaps only practical probe the Majorana nature of neutrinos is an extremely rate nuclear decay process, the neutrinoless double beta decay. I will present the experimental techniques to search for this decay, show current results...
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Anatolii Serebrov (Petersburg Nuclear Physics Institute)25/10/2019, 10:00Oral
Present status of experiment Neutrino-4 search for sterile neutrino is discussed. The effect of oscillations into sterile neutrino with parameters Δm$^2_{14}$$\approx$7.3 eV$^2$, sin$^2$2θ$_{14}$$\approx$0.39 is observed at the 2.8σ level. The detailed analysis of possible systematic errors is presented. Plans to improve the existing installation and create a new installation with a...
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Ms Ivana Belosevic (IPA, ETH Zurich)25/10/2019, 10:20Oral
Experiments with muons ($\mu^{+}$) and muonium atoms ($\mu^{+}e^{-}$) offer several promising possibilities for testing fundamental symmetries of particle physics with high precision. Examples of such tests include the search for the muon electric dipole moment, measurement of the muon $g-2$ and muonium laser spectroscopy. These experiments could benefit from a high-quality muon beam at low...
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Frédéric Merkt (ETH Zurich, Laboratory of Physical Chemistry)25/10/2019, 11:10Invited Talk
Few-electron molecules are attractive systems for precision spectroscopy because their properties can be calculated with high accuracy by quantum-chemical methods.$^{1,2,3}$ The measurements serve to test theoretical predictions, ideally at the level where their accuracy is limited by the uncertainties of the fundamental constants or by unrecognized physical effects. I will report on precision...
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Prof. Detlev Gotta (Forschungszentrum Jülich)25/10/2019, 11:40Invited Talk
Exotic atoms allow studies in the fields of particle and nuclear physics as well as atomic and molecular phenomena. Inherent to exotic-atom research is a low count rate in the presence of demanding background conditions. Therefore, facilities providing high muon, pion and antiproton fluxes are mandatory in particular for ultimate resolution spectroscopy when using crystal spectrometers. Such...
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Mr Shun Seo (The University of Tokyo, RIKEN)25/10/2019, 12:10Oral
MuSEUM (Muonium Spectroscopy Experiment Using Microwave) collaboration aims to perform a precise spectroscopy of the ground state muonium hyperfine structure (MuHFS) with high-intensity pulsed muon beam at J-PARC. Our goal is a ten-fold of improvement in a precision of MuHFS compared to the preceding experiment at LAMPF [1]. Muonium is the bound state of a positive muon and an electron. Its...
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Zakary Burkley (ETH Zürich, Institute for Particle Physics and Astrophysics)25/10/2019, 12:30Oral
Positronium and Muonium are excellent systems to test bound-state QED theory to high precision. This has motivated numerous precise experiments aimed at measuring the hyperfine splitting and 1S-2S transition of these atoms.
Currently, there is some disagreement with the most recent bound-state QED calculations for the hyperfine splitting in positronium. Our approach to resolve this, PHySES,...
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25/10/2019, 14:00
note that the registration for the EQLIPS Workshop is outside the auditorium WHGA/001
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you need to go there in order to obtain the access badge necessary to reach the WBGB/019 lecture hall -
25/10/2019, 14:00
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25/10/2019, 14:00
registration desk is outside the auditorium WHGA/001
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25/10/2019, 14:00
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Dr Valentina Santoro (ESS)Oral
The European Spallation Source (ESS) is being constructed in Lund, Sweden, to be the brightest cold (< 0.025 eV) spallation neutron source in the world. The facility uses a 2 GeV proton beam hitting a tungsten target to produce neutrons via spallation. The neutrons are then moderated in cold and thermal moderators consisting of liquid hydrogen and water, respectively. Surrounding the...
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