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Archive for the ‘particle physics’ category: Page 186

Mar 26, 2023

New LHC experiments enter uncharted territory

Posted by in categories: cosmology, particle physics

Although neutrinos are produced abundantly in collisions at the Large Hadron Collider (LHC), until now no neutrinos produced in such a way had been detected. Within just nine months of the start of LHC Run 3 and the beginning of its measurement campaign, the FASER collaboration changed this picture by announcing its first observation of collider neutrinos at this year’s electroweak session of the Rencontres de Moriond. In particular, FASER observed muon neutrinos and candidate events of electron neutrinos. “Our statistical significance is roughly 16 sigma, far exceeding 5 sigma, the threshold for a discovery in particle physics,” explains FASER’s co-spokesperson Jamie Boyd.

In addition to its observation of neutrinos at a particle collider, FASER presented results on searches for dark photons. With a null result, the collaboration was able to set limits on previously unexplored parameter space and began to exclude regions motivated by dark matter. FASER aims to collect up to ten times more data over the coming years, allowing more searches and neutrino measurements.

FASER is one of two new experiments situated at either side of the ATLAS cavern to detect neutrinos produced in proton collisions in ATLAS. The complementary experiment, SND@LHC, also reported its first results at Moriond, showing eight muon neutrino candidate events. “We are still working on the assessment of the systematic uncertainties to the background. As a very preliminary result, our observation can be claimed at the level of 5 sigma,” adds SND@LHC spokesperson Giovanni De Lellis. The SND@LHC detector was installed in the LHC tunnel just in time for the start of LHC Run 3.

Mar 25, 2023

A cavity leads to a strong interaction between light and matter

Posted by in categories: computing, particle physics, quantum physics

Researchers have succeeded in creating an efficient quantum-mechanical light-matter interface using a microscopic cavity. Within this cavity, a single photon is emitted and absorbed up to 10 times by an artificial atom. This opens up new prospects for quantum technology, report physicists at the University of Basel and Ruhr-University Bochum in the journal Nature.

Quantum physics describes photons as light particles. Achieving an interaction between a and a is a huge challenge due to the tiny size of the atom. However, sending the past the atom several times by means of mirrors significantly increases the probability of an interaction.

In order to generate photons, the researchers use artificial atoms, known as . These semiconductor structures consist of an accumulation of tens of thousands of atoms, but behave much like a single atom: when they are optically excited, their energy state changes and they emit a photon. “However, they have the technological advantage that they can be embedded in a ,” says Dr. Daniel Najer, who conducted the experiment at the Department of Physics at the University of Basel.

Mar 25, 2023

Beaming in a Spin Texture

Posted by in categories: materials, particle physics

Researchers use an optical vortex beam to create a stable pattern of electron spins in a thin layer of semiconductor material.

Spin-based electronic, or “spintronic,” devices can benefit from techniques that coax electron spins into static spatial patterns called spin textures. A new experiment demonstrates that an optical vortex—a light beam that carries orbital angular momentum—can generate a stable spin texture in a semiconductor [1]. The research team showed that the vortex generates a pattern of stripes that has potential uses in processing spin information. Previous experiments have optically stimulated these striped textures, but the optical vortex has a structure that approximately overlaps with the stripe pattern, allowing faster spin-texture formation.

The spins of unbound electrons in a material can be aligned by a magnetic field or by polarized light. But as these electrons move—either through diffusion or through conduction—their spins will begin to rotate in response to so-called spin-orbit interactions within the material. The direction and rate of these rotations for any given electron depend on the path that it takes. Thus, two nearby electrons that start out aligned will become misaligned as they move along different paths, even if they arrive at the same destination. So maintaining an electronic spin texture seems like a doomed enterprise.

Mar 25, 2023

Graphene grows—physicists find a way to visualize it

Posted by in categories: materials, particle physics

Graphene is one of the strongest materials. On top of that, it is exceptionally good at conducting heat and electrical currents, making it one of the most special and versatile materials we know. For all these reasons, the discovery of graphene was awarded the Nobel Prize in Physics in 2010.

Yet, many properties of the material and its cousins are still poorly understood—for the simple reason that the atoms they are made up of are very difficult to observe. A team of researchers from the University of Amsterdam and New York University have now found a surprising way to solve this issue.

Two-dimensional materials, consisting of a hyper-thin single layer of atomic crystal, have attracted a lot of attention recently. This well-deserved attention is mainly due to their unusual properties, very different from their three-dimensional ‘bulk’ counterparts. Graphene, the most famous representative, and many other , are nowadays researched intensely in the laboratory.

Mar 24, 2023

New experiment translates quantum information between technologies in an important step for the quantum internet

Posted by in categories: computing, internet, particle physics, quantum physics

Researchers have discovered a way to “translate” quantum information between different kinds of quantum technologies, with significant implications for quantum computing, communication, and networking.

The research was published in the journal Nature on Wednesday. It represents a new way to convert from the format used by quantum computers to the format needed for quantum communication.

Photons—particles of light—are essential for , but different technologies use them at different frequencies. For example, some of the most common technology is based on , such as those used by tech giants Google and IBM; these qubits store quantum information in that move at microwave frequencies.

Mar 24, 2023

ATLAS and CMS observe simultaneous production of four top quarks

Posted by in category: particle physics

Today, at the Moriond conference, the ATLAS and CMS collaborations have both presented the observation of a very rare process: the simultaneous production of four top quarks. They were observed using data from collisions during Run 2 of the Large Hadron Collider (LHC).

Both experiments’ results pass the required five-sigma to count as an observation—ATLAS’s observation with 6.1 sigma, higher than the expected significance of 4.3 sigma, and CMS’s observation with 5.5 sigma, higher than the expected 4.9 —making them the first observations of this process.

The top quark is the heaviest particle in the Standard Model, meaning it is the particle with the strongest ties to the Higgs boson. This makes top quarks ideal for looking for signs of physics beyond the Standard Model.

Mar 24, 2023

Single-atom vibrational spectroscopy now sensitive at the level of chemical bonds

Posted by in categories: chemistry, particle physics

Researchers led by Prof. Zhou Wu from the University of Chinese Academy of Sciences (UCAS) and Prof. Sokrates T. Pantelides of Vanderbilt University have pushed the sensitivity of single-atom vibrational spectroscopy to the chemical-bonding-configuration extreme, which is critical for understanding the correlation of lattice vibrational properties with local atomic configurations in materials.

Using a combination of experimental and theoretical approaches, the researchers demonstrated the effect of chemical-bonding configurations and the atomic mass of impurity atoms on local vibrational properties at the single-atom level.

The study was published in Nature Materials.

Mar 23, 2023

The Crazy Mass-Giving Mechanism of the Higgs Field Simplified

Posted by in category: particle physics

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REFERENCES:
Where 99% of mass comes from: https://youtu.be/KnbrRhkJCRk.
ElectroWeak Unification: https://youtu.be/u05VK0pSc7I
Symmetry Breaking: https://youtu.be/yzqLHiA0uFI

Continue reading “The Crazy Mass-Giving Mechanism of the Higgs Field Simplified” »

Mar 23, 2023

Laser-cooled atoms bring networks of quantum computers a step closer

Posted by in categories: computing, particle physics, quantum physics

Rubidium atoms are used to convert between millimetre-wave photons and optical-wavelength photons.

Mar 23, 2023

New ATLAS result weighs in on the W boson

Posted by in categories: futurism, particle physics

For the past 40 years, the W boson has been making headlines. In the 1980s, the announcement of its discovery helped confirm the theory of the electroweak interaction – a unified description of electromagnetic and weak forces. Today, measurements of its mass (mW) are testing the consistency of the Standard Model it helped to form. Figure 1: The measured value of the W-boson mass is compared to other published results. The vertical bands show the Standard Model prediction, and the horizontal bands and lines show the statistical and total uncertainties of the published results. (Image: ATLAS Collaboration/CERN) The W-boson mass is closely related to the masses of nature’s heaviest particles, including the top quark and the Higgs boson. However, if additional heavy particles exist, the mass might deviate from the Standard Model prediction. By comparing direct measurements of the W-boson mass to theoretical calculations, physicists are looking for deviations that could be an indicator of new phenomena. To be sufficiently sensitive to such deviations, mass measurements need to have amazingly small uncertainties, of the order of 0.01%. In 2017, the ATLAS Collaboration at CERN published the LHC’s first measurement of the W-boson mass, giving a value of 80,370 MeV with an uncertainty of 19 MeV. At the time, this measurement was the most precise single-experiment result, and was in agreement with the Standard Model prediction and all other experimental results. Last year, the CDF Collaboration at Fermilab published an even more precise measurement of the W-boson mass, analysing the full dataset provided by the Tevatron collider. With a value of 80,434 MeV and an uncertainty of 9 MeV it differed significantly from the Standard Model prediction and from the other experimental results. In a new preliminary result released today, the ATLAS Collaboration reports an improved re-analysis of its initial W-boson mass measurement. ATLAS finds mW to be 80,360 MeV, with an uncertainty of just 16 MeV. The measured value is 10 MeV lower than the previous ATLAS result and is in agreement with the Standard Model. The ATLAS Collaboration has measured the W boson mass to be 80,360 MeV with an uncertainty of 16 MeV – in agreement with the Standard Model. Figure 2: The 68% and 95% confidence-level contours of the indirect determination of the W-boson and top-quark mass from the global electroweak fit are compared to the 68% and 95% confidence-level contours of the ATLAS measurements of the W-boson and top-quark masses. (Image: ATLAS Collaboration/CERN) For this new analysis, ATLAS physicists revisited its data collected in 2011 at a centre-of-mass energy of 7 TeV (corresponding to 4.6 fb-1, also used in ATLAS’ previous measurement). Researchers employed improved statistical methods and refinements in the treatment of the data, enabling them to reduce the uncertainty of their mass measurement by more than 15%. Researchers focused on collision events where the W boson decays into an electron or a muon (leptons), and a corresponding neutrino. The W-boson mass was then determined by fitting the kinematic distributions of the decay leptons in simulation to the data. The main difference between the 2017 and the new measurement is in the method used to perform these fits. While the previous measurement used the available data solely to determine the W-boson mass, with systematic uncertainties added after the fact, the new measurement simultaneously adjusts the systematic uncertainties together with the W-boson mass. This improvement reduced several systematic uncertainties, particularly those related to the theoretical modelling of W-boson production and decay. The W-boson transverse momentum distribution has as much of an influence on the lepton-decay distributions as the W-boson mass itself – and is therefore an important source of uncertainty. As the resolution of the 2011 data was too poor to verify the modelling of this distribution in detail, researchers instead used data recorded in 2017 during a special, low-luminosity proton-proton run at a centre-of-mass energy of 5 TeV. They found the data agreed with predicted distributions, thus validating the model. Also crucial to the measurement were the parton distribution functions (PDFs) of the proton, which model the relative momenta of its quark and gluon constituents. PDFs incorporate a multitude of data from different particle physics experiments. Since the previous measurement, these sets have been refined by including more data. The new ATLAS measurement evaluated the dependence of the measured W-boson mass on PDFs sets considering these more recent versions. Future measurements of the W-boson mass are expected by other LHC experiments, as well as further studies by ATLAS using data samples recorded in different pile-up conditions and at different centre-of-mass energies. These will provide independent evaluations of the experimental results obtained so far. About the event display in the banner: Display of a candidate W→μν event using proton-proton collisions at 7 TeV centre-of-mass energy at the LHC. Starting from the centre of the ATLAS detector, the reconstructed tracks of the charged particles in the Inner Detector (ID) are shown as cyan lines. The energy deposits in the electromagnetic (the green layer) and hadronic (the red layer) calorimeters are shown as yellow boxes. The identified muon is shown with its reconstructed track (blue line) passing through the muon chambers (blue layers). The muon has a transverse momentum of pT=36 GeV, whereas the missing transverse energy (red arrow) is 35 GeV and corresponds to the muon neutrino energy. The transverse mass of the W boson candidate is 71 GeV. (Image: ATLAS Collaboration/CERN) Explore the interactive event display Dynamic view of a candidate W→μν event using proton-proton collisions at 7 TeV centre-of-mass energy at the LHC. Starting from the centre of the ATLAS detector, the reconstructed tracks of the charged particles in the Inner Detector (ID) are shown as red lines. The energy deposits in the calorimeters are shown as yellow boxes. The identified muon is shown as a longer red dashed line. The missing transverse momentum is shown by a green dashed line. Learn more Improved W boson Mass Measurement using 7 TeV Proton-Proton Collisions with the ATLAS Detector (ATLAS-CONF-2023–004) Improved ATLAS result weighs in on the W boson, CERN Press Release, March 2023 Moriond EW 2023 presentation by Matthias Schott: EWK highlights from ATLAS High-precision measurement of the W boson mass with the CDF II detector (Science, Vol 376, Issue 6589) Briefing to previous W boson mass measurement, Physics Briefing, December 2016 First high-precision measurement of the mass of the W boson at the LHC, CERN Press Release, February 2018.