Showing posts with label lhc. Show all posts
Showing posts with label lhc. Show all posts

Four all new exotic particles

LHCb has recently observed four new exotic-like particles in the decay of the $B^+$:
he properties of these structures are consistent with their interpretation as four-quark particles, which are considered as "exotic", (hence the "exotic-like" name in the title), although the details of the four quark $c{\bar c}s{\bar s}$ binding mechanism is still under discussion.
Read also paper 1 and paper 2

Hints of physics behind standard model?

The LHCb collaboration is studying the decay of mesons $B$ in order to find some violations in standard model rules. In particular LHCb has measured a particular ratio, named $R (D^*)$, between two decay modes of $\overline{B}^0$ and they find a violation from the standard model prediction that is compatible with other similar measures:
In the SM all charged leptons, such as taus ($\tau$) or muons ($\mu$), interact in an identical fashion (or, in physicists' language, have the same "couplings"). This property is called "lepton universality". However, differences in mass between the leptons must be accounted for, and affect decays involving these particles. The $\tau$ lepton is much heavier than the $\mu$ lepton and therefore the SM prediction for the ratio $R(D^*)$ is substantially smaller than 1. This ratio is considered to be precisely calculable thanks to the cancellation of uncertainties associated with the $B$ to $D^*$ meson transition.
But there is another hint of new physics. At the end of July Nature Physics published a new paper from the LHCb collaboration about the possible existence of a new particle:
The LHCb collaboration published in Nature Physics a paper based on run 1 data which reports the determination of the parameter $|V_{ub}|$ describing the transition of a $b$ quark to a $u$ quark. This measurement was made by studying a particular decay of the $\Lambda_b^0$ baryon. Other measurements of $|V_{ub}|$ by previous experiments had returned two sets of inconsistent results, depending on which method was used to determine the parameter. Theorists had suggested that this discrepancy could be explained by the presence a new particle contributing to the decay process, which affected the result differently, depending on the measurement method. Today's result from LHCb removes the need for this new particle, while the puzzle of why the original sets of measurements do not agree persists.
where $|V_{ub}|$ is connected to the Cabibbo-Kobayashi-Maskawa matrix.

Quarks of power

about @LHCbExperiment #pentaquark discovery
Once upon a time, there was a controversy in particle physics. There were some physicists who denied the existence of structures more elementary than hadrons, and searched for a self-consistent interpretation wherein all hadron states, stable or resonant, were equally elementary. Others, appalled by the teeming democracy of hadrons, insisted on the existence of a small number of fundamental constituents and a simple underlying force law. In terms of these more fundamental things, hadron spectroscopy should be qualitatively described and essentially understood just as are atomic and nuclear physics.(11)
The need of the partons
When we descrive the collisions between particles, we calculate the cross section, the area of the distribution of the collisions' products. The mathematical object used to calculate the cross section are the structure functions, that mathematically describes the inner structure of the particle. In 1969 studying the deep inelastic scattering J. D. Bjorken(4, 18), in order to explain the experimental results, proposed a particular property for the hadronic structure function in the cross section called scaling. In the same year Richard Feynman(5, 18) suggested the necessity to adopt a new description of hadrons: they had to be made by smaller components, more elementary than the hadrons themselves. These components are called partons.
The Feynman's thesys was immediatly verified by Bjorken and Paschos(6, 7, 18), in this way starting a great discussion about the parton models, described in the paper by De Rújula, Georgi and Glashow quoted at the beginning of the post(11) (an interesting review of the parton model and its story is in Greenberg(18)).
Probably the most strong motivation to adopt the parton model to describe hadrons is the great production of particles in the ring particles accelerators(5). So, theoretical physicists produced a lot of model, but the most succesfull is the quarks model, developed by Murray Gell-Mann(1) and Georg Zweig(2, 3), that introduced a new quantum number, the flavor. The first formulation involved three type of quarks (and so three flavors): up, down and strange. To this first set of elementary particles in 1970 the quark charm was added by Glashow, Iliopulos and Maiani(8) and finally in 1973 Kobayashi and Maskawa(9) completed the family with the two last quark, top and bottom, named by Harari(10) in 1975.
Three quarks for Muster Mark!
Sure he has not got much of a bark
And sure any he has it's all beside the mark.
from Finnegan's Wake by James Joyce

LHC restars at 13 TeV

http://t.co/jLPjvDAT6V greeting to @CERN from @ulaulaman and all network
Today at CERN, LHC restarts after a stopping period, at the energy of 13 TeV. It's a great day because we expect signals of new physics beyond particle standard model.

Fabiola Gianotti, Director General at CERN

http://t.co/rYzcXWlvR0 about #FabiolaGianotti #CERN #ATLAS
Fabiola Gianotti is an Italian particle physicist, a former spokesperson of the ATLAS experiment at the Large Hadron Collider (LHC) at CERN in Switzerland, considered one of the world's biggest scientific experiments. She has been selected as the next Director-General of CERN, starting on 1 January 2016.
She is the 4th italian particle physicist to became Director General at CERN after Amaldi (1952-1954), Rubbia (1989-1993) and Maiani (1999-2003).
A bit concession to the SEO!

Planck results, ATLAS and the dark matter

http://t.co/jJxD8rhCr6 by @ulaulaman about #Planck, #ATLAS, #DarkMatter at #LHC
The last issue of Astronomy & Astrophysics (that it's free) is devoted to the Planck 2013 results:
This collection of 31 articles presents the initial scientific results extracted from this first Planck dataset, which measures the cosmic microwave background (CMB) with the highest accuracy to date. It provides major new advances in different domains of cosmology and astrophysics.
In the first paper there is an overview of 2013 science results, and we can read:
The Universe observed by Planck is well-fit by a six parameter, vacuum-dominated, cold dark matter (ACDM) model, and we provide strong constraints on deviations from this model.
But, in the meanwhile, ATLAS published a preprint about the quest of the dark matter in LHC:
The data are found to be consistent with the Standard Model expectations and limits are set on the mass scale of effective field theories that describe scalar and tensor interactions between dark matter and Standard Model particles. Limits on the dark-matter--nucleon cross-section for spin-independent and spin-dependent interactions are also provided. These limits are particularly strong for low-mass dark matter. Using a simplified model, constraints are set on the mass of dark matter and of a coloured mediator suitable to explain a possible signal of annihilating dark matter.
Tommaso Dorigo, examining ATLAS' results, concludes:
the ATLAS search increases significantly the sensitivity with respect to past searches, but no signal is found. As attractive as DM existence is as an economical explanation of a wealth of cosmological observations, the nature of dark matter continues to remain unknown.

via phys.org

Carlo Rubbia and the discoveries of the weak bosons

http://t.co/KGVNarwZMG by @ulaulaman about #CarloRubbia #NobelPrize #physics #particlephysics
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On that day 30 years ago, I was almost certainly at school. Physics still was not my passion. Of course I started very well: when the teacher asked what is the space, I thought immediately to the universe, but the question was not referring to that "space", but in another, the geometric. But it is not about those memories that I have to indulge, but on a particular photo, in which Carlo Rubbia and Simon van der Meer, with two goblets, presumably of wine in hand, are celebrating the announcement of the Nobel Prize for Physics
for their decisive contributions to the large project, which led to the discovery of the field particles W and Z, communicators of weak interaction
The story of this Nobel, however, began eight years earlier, in 1976. In that year, in fact, SPS, the Super Proton Synchrotron, begins to operate at CERN, originally designed to accelerate particles up to an energy of 300 GeV.
The same year David Cline, Carlo Rubbia and Peter McIntyre proposed transforming the SPS into a proton-antiproton collider, with proton and antiproton beams counter-rotating in the same beam pipe to collide head-on. This would yield centre-of-mass energies in the 500-700 GeV range(1).
On the other hand antiprotons must be somehow collected. The corresponding beam was then
(...) stochastically cooled in the antiproton accumulator at 3.5 GeV, and this is where the expertise of Simon Van der Meer and coworkers played a decisive role(1).

Fifty years of CP violation

via @CERN http://t.co/9Rac42mBVh #CPviolation #CPsymmetry #matter #antimatter
The CP violation is a violation of the CP-symmetry, a combination between the charge conjugation symmetry (C) and the parity symmetry (P).
CP-symmetry states that the laws of physics should be the same if a particle is interchanged with its antiparticle, and then its spatial coordinates are inverted.
The CP violation is discovered in 1964 by Christenson, Cronin, Fitch, and Turlay (Cronin and Fitch awarded the Nobel Prize in 1980) studying the kaons' decays and it could have a key-role in the matter-antimatter imbalance.
Now the CERN Courier dadicated a special issue about the fifty years of the discovery (download here).
Christenson, J., Cronin, J., Fitch, V., & Turlay, R. (1964). Evidence for the 2π Decay of the K_{2}^{0} Meson Physical Review Letters, 13 (4), 138-140 DOI: 10.1103/PhysRevLett.13.138

LHComedy: CERN After Dark

LHComedy brings science-themed stand-up comedy to the Geneva area. Bringing our audience a mixture of laughs and insight, we bring our passion about science and technology to the world with our own stories and experiences of life at CERN.
(more at lhcomedy.web.cern.ch)

The B mesons and the new physics

posted by @ulaulaman via @LHCbExperiment #newphysics #Bmesons #LHC #CERN #particlephysics
The search about B mesons decays has a great importance in physics for the possible clues of new physics that could be discovered. So theoretical phisicists have developed some new observables in order to test this possibility. LHCb produced new results about these new parameters, in particular the so called $P_5'$.
According to Joaquim Matias from Universitat Autonoma de Barcelona and colleagues the deviation in $P_5'$ and small discrepancies in the other angular observables for this decay, follow a pattern. In a recent paper the authors claim that a global analysis of the LHCb data, together with previous measurements, show a deviation of $4.5 \sigma$ with respect to Standard Model expectations, which can be explained with the same mechanism. This demands further investigation, in particular to re-evaluate all the sources of theoretical uncertainty, and to understand the effects of correlations between the experimental measurements.
(via LHCb)
The image shows the distribution of the $P_5'$ observable as a function of the $\mu^+ \mu^-$ invariant mass squared $q^2$. The black data points are compared with the Standard Model prediction.

First evidence of photon polarisation in a quark transition

posted by @ulaulaman via @LHCbExperiment #newPhysics #StandardModel #LHC #CERN
There are a lot of model about physics beyond standard model, and the experimental work is concentrate to search signals to select the new models for the future. LHCb has recently released a press release about the transition of a b-quark to an s-quark with the emission of a photon. This transition
is considered a very important process to investigate possible manifestation of new physics. This decay process is forbidden in the first approximation in the Standard Model (SM) of particle physics and moreover in the second-order processes that govern the process in the SM the emitted photon is expected to be strongly polarised. Therefore it is very sensitive to new physics effects arising from the exchange of new heavy particles in electroweak penguin diagrams (see 14 June 2013 news). Indeed, several models of new physics predict that the emitted photon should be less polarised than in the SM. Up to now different experiments have measured the decay rate of this process, ruling out significant deviations of the rate from the SM prediction and strongly reducing the allowed parameter space of new physics models. The photon polarisation was, however, never previously observed.
I think that this is a really intriguing news for a particle physics point of view.

The boson, the spin and the graviton

Some days ago, ATLAS has been released a draft about the spin of the new boson. The decay channels studied are the fab four: $H \rightarrow \gamma \gamma$, $H \rightarrow WW^*$, $H \rightarrow l\nu l\nu$, $H \rightarrow ZZ^* \rightarrow 4l$. The idea is combining data from the four channels in order to understand the spin of the new boson, in detail to distinguish between two cases: spin 0 ($J^P = 0^+$), and so a boson compatible with the Standard Model, and spin 2 ($J^P = 2^+$), that it could be connected with a model (arXiv) that represents a light coupling between the Standard Model's fields and the hypothetical graviton.
These the ATLAS' conclusions:
The data are in good agreement with the expected distributions of a $J^P=0^+$ particle while the graviton-inspired $J^P=2^+$ model, that is expected to be produced dominantly via the gluon fusion process, is excluded at more than 99.9% confidence level.
We could say that it starting the elimination process of the models that would lead the research of the new physics beyond the Standard Model for the next years. A good luck to all of them, but we don't forget the key role of the Standard Model, that is in some sense confirmed by this last draft from ATLAS.

Play the game with the Higgs boson

In the mid-March at Moriond 2013 ATLAS and CMS presented the last results about the research of the Higgs' boson. While CMS reduced the excess for the $H \rightarrow \gamma \gamma$ decay channell, ATLAS continued to observe it. This result could be a clue that the boson discovered and announced last year is only the first of a series of Higgs' bosons. Indeed, following Albert De Roeck of CSM, the photon decay could be connected with...
new physics and there are a great deal of models that can come with such a number
In order to resolve the question (is the new boson the only Higgs' boson or simply a Higgs' boson?) we have to wait the end of the maintenance work of LHC, but in the meantime we could play with the Quark Matter Card Game, in particular the variant named Higgs Boson - on Your Own!
Object of the game: to win, by detecting a decay of a Higgs boson. If this does not happen in a given game, one can win by statistics, by collecting the largest number of particle cards.
The proposed game is a variation of Memory

Mickey Mouse at the CERN

The most famous laboratory of the year is certanly the CERN thanks to the discovery of a new boson that it seems equal to the boson predicted by Peter Higgs et al.
CERN was established in 1952 and formed in 1954. Currently the experiments are carried with the LHC (Large Hadron Collider), but the previous accelerator ring was LEP, Large Electron-Positron Collider, that was used from 1989 to 2000. In particular in 1985 Alessandro Bencivenni, an italian disney writer, went at CERN and, inspired by the announced LEP, he wrote a story setted at the swiss laboratory, Mickey Mouse and the nuclear accelerator (Topolino e l'acceleratore nucleare), never published in english, so I decided to translate the cartoons about the explanation of the device and the experiment.
The popularizer is Atomo Bleep-Bleep, a charachter created by Romano Scarpa in Mickey Mouse and the Delta Dimension (first italian edition: 1959; first english edition: 1981 in Great Britain). I hope to write something about Atomo Bleep-Bleep, Doctor Einmug and the Delta Dimension in a future post, but for now I hope you can enjoy with this extract from the story, drawned by Massimo De Vita (I must remember that copyright is Disney):

Is it the Higgs? The spin will tell us!

a couple of video about #Higgs via @CMSexperiment posted by @ulaulaman
The CMS experiment posted on its Google Plus page a couple of video about the new boson and the future research of its spin, an important tool in order to understand if the new particle is a Higgs boson or someone like it, but with some, little differences:

Habemus papers (about the new boson)

posted by @ulaulaman thanks to @tanzmax @spimpompam #Higgs #boson #newboson #LHC #CMS #ATLAS #CERN
Finally Physics Letters B published the two papers by ATLAS and CMS about the discovery of the new boson at LHC (via tanzmax):
A search for the Standard Model Higgs boson in proton–proton collisions with the ATLAS detector at the LHC is presented. The datasets used correspond to integrated luminosities of approximately $4.8 \, fb^{−1}$ collected at $\sqrt{s} = 7$ TeV in 2011 and $5.8 \, fb^{−1}$ at $\sqrt{s} = 8$ TeV in 2012. Individual searches in the channels $H \rightarrow ZZ^{(*)} \rightarrow 4l$, $H \rightarrow \gamma \gamma$ and $H \rightarrow WW^{(*)} \rightarrow e \nu \mu \nu$ in the 8 TeV data are combined with previously published results of searches for $H \rightarrow ZZ^{(*)}$, $WW^{(*)}$, $b \bar{b}$ and $\tau^+ \tau^-$ in the 7 TeV data and results from improved analyses of the $H \rightarrow ZZ^{(*)} \rightarrow 4l$ and $H \rightarrow \gamma \gamma$ channels in the 7 TeV data. Clear evidence for the production of a neutral boson with a measured mass of 126.0 ± 0.4 (stat) ± 0.4 (sys) GeV is presented. This observation, which has a significance of 5.9 standard deviations, corresponding to a background fluctuation probability of 1.7 × 10−9, is compatible with the production and decay of the Standard Model Higgs boson.
Aad, G., Abajyan, T., Abbott, B., Abdallah, J., Abdel Khalek, S., Abdelalim, A.A., Abdinov, O., Aben, R., Abi, B., Abolins, M. & (2012). Observation of a new particle in the search for the Standard Model Higgs boson with the ATLAS detector at the LHC, Physics Letters B, 716 (1) 29. DOI: 10.1016/j.physletb.2012.08.020
Results are presented from searches for the standard model Higgs boson in proton–proton collisions at $\sqrt{s} =$ 7 and 8 TeV in the Compact Muon Solenoid experiment at the LHC, using data samples corresponding to integrated luminosities of up to $5.1 fb^{−1}$ at 7 TeV and $5.3 fb^{−1}$ at 8 TeV. The search is performed in five decay modes: $\gamma \gamma$, $ZZ$, $W^+ W^−$, $\tau^+ \tau^-$, and $b \bar{b}$. An excess of events is observed above the expected background, with a local significance of 5.0 standard deviations, at a mass near 125 GeV, signalling the production of a new particle. The expected significance for a standard model Higgs boson of that mass is 5.8 standard deviations. The excess is most significant in the two decay modes with the best mass resolution, $\gamma \gamma$ and $ZZ$; a fit to these signals gives a mass of 125.3 ± 0.4 (stat.) ± 0.5 (syst.) GeV. The decay to two photons indicates that the new particle is a boson with spin different from one.
Chatrchyan, S., Khachatryan, V., Sirunyan, A.M., Tumasyan, A., Adam, W., Aguilo, E., Bergauer, T., Dragicevic, M., Erö, J., Fabjan, C. & (2012). Observation of a new boson at a mass of 125 GeV with the CMS experiment at the LHC, Physics Letters B, 716 (1) 61. DOI: 10.1016/j.physletb.2012.08.021

To the previous papers, I add also the following (via spimpompam), that it could be interesting to read:
Following recent ATLAS and CMS publications we interpret the results of their Higgs searches in terms of Standard Model operators. For a Higgs mass of 125 GeV we determine several Higgs couplings from 2011 data and extrapolate the results towards different scenarios of LHC running. Even though our analysis is limited by low statistics we already derive meaningful constraints on modified Higgs sectors.
Klute, M., Lafaye, R., Plehn, T., Rauch, M. & Zerwas, D. (2012). Measuring Higgs Couplings from LHC Data, Physical Review Letters, 109 (10) DOI: 10.1103/PhysRevLett.109.101801 (arXiv)

Linux at CERN

#linux #cern #lhc #physics #newboson #Higgs
On reddit (via Ubuntu Vibes) an anonimous researcher from CERN published the following message:
I don't see any CERN related things here, so I want to mention how Linux (specifically, Scientific Linux and Ubuntu) had a vital role in the discovery of the new boson at CERN. We use it every day in our analyses, together with hosts of open software, such as ROOT, and it plays a major role in the running of our networks of computers (in the grid etc.) used for the intensive work in our calculations.
Yesterday's extremely important discovery has given us new information about how reality works at a very fundamental level and this is one physicist throwing Linux some love.
If you want, you can download the distributions used at CERN at the page Linux @ CERN. The CERN distribution is a Scientific Linux (a distribution used also at Fermilab) rebuilded with the Red Hat. In general the Linux distributions are the most used in the scientific world, in particular in physics and mathematics, and the reasons are the same that the anonimous research writes in another comment:
In terms of data analysis, Windows could be used in principle. We could also use some type of device that manipulates symbols on a strip of tape according to a simple table of rules. Linux is used because it is most appropriate for the job. Linux is ubiquitous in HPC and we use a lot of computing power in LHC physics, so the arguments for the use of Linux in HPC are very similar to the arguments for the use of Linux in LHC physics analyses. Naturally, it's important to have an operating system that is free, open source and reliable (Scientific Linux is basically Red Hat Linux), but here's a quotation from the Scientific Linux website that should give some idea of why Scientific Linux is needed:
"Our main goal for the base distribution is to have everything compatible with Enterprise, with only a few minor additions or changes. Examples of items that were added are Alpine, and OpenAFS.
Our secondary goal is to allow easy customization for a site, without disturbing the Scientific Linux base. The various labs are able to add their own modifications to their own site areas. By the magic of scripts, and the anaconda installer, each site is to be able to create their own distributions with minimal effort. Or, if a user wishes, they can simply install the base SL release."
I work primarily in physics, not in computing, so I doubt that I am able to argue very competently for Linux over something such as BSD. The fact is that Linux was the operating system used in the overwhelming majority of the analyses contributing to the discovery, so, in that sense I think I am justified in claiming that Linux played a vital role in the discovery.
And he also writes about Apple and Comic Sans:
In many ways, some Apple fans are similar to religious people in their devotion to something; that is, their support is not really derived from a critical appraisal of the technical standard of Apple products. I don't identify with this kind of motivation, but I am much happier seeing people religiously attached to new technological gadgetry than to invisible sky daddies.
Similarly, Comic Sans is grotesque, but if it contributes to directing attention to the recent discovery, then it could be argued that it is a good thing.
In direct answer to your question, I think that you can thank Microsoft Bob for the existence of Comic Sans.
And finally he explain (one of many) that, with the data collected since june 2012, we can say that the new particle is a new boson, but we are not certain that it is a Higgs boson:
The properties of the discovered boson have yet to be scrutinised thoroughly before one can reliably claim it to be a Higgs boson (note that I do not claim the discovered boson to be the Higgs particle in the post). This is a phase of analysis we are now moving into.
And don't forget to read the post about the discover of the new boson!

Discovering a boson

posted by @ulaulaman #Higgs #ICHEP2012
I'm partially wrong! Yesterday I write that no Higgs could be announced, but today ATLAS and CMS presented the observation of a new boson, that it's to soon to identify with certainty like the Higgs boson, but it is certainly a new boson to add to the picture of the universe. The next quest is to find its properties and to confront with the theoretical properties of the Higgs boson. It could be that the new boson presented today could be different for a bit of properties from the Higgs, but this is not so incredible: like I write, with a Higgs boson with a mass around 125 GeV, we need other ingredients to complete a picture of our stable universe.

Candidate Higgs decay to four electrons recorded by ATLAS in 2012 (source ATLAS)
But... what did it happen today?
The two experiments, CMS, represented by Joe Incandela, and ATLAS, represented by Fabiola Gianotti, showed the results of their last data elaboration about Higgs research. The results come from the combination of the complete data set from 2011 (see, for example, the ATLAS' preprint) with the first part of data from 2012. The conclusions are: CMS sees an excess with $m_H = 125.3 \pm 0.6 GeV$ with a significance of $4.9 \sigma$; ATLAS sees an excess with $m_H = 126.5 GeV$ with a significance of $5.0 \sigma$, that it means discover!

CMS' final result

ATLAS' final result